Thermophysical properties of some common PCMs with high latent heat.
Here,
The hydraulic fracture propagation in cohesive zone model can be applied by the traction-separation law:\n
where
where
Here,
Hydraulic fracture in naturally fractured reservoirs is faced with a unique situation which may increase the possibility of deviation from symmetrical propagation. Experimental results reveal that three scenarios may occur at the propagation stage and beyond the collision stage of fluid-driven in hydraulic fracture interaction with the natural fracture, namely diversion, penetration, and containment. Diversion is the situation in which the collided hydraulic fracture has an effective stress too low to initiate new fracture at the front wall of preexisting joint, and as a result the fluid-driven propagates along the natural fracture axis. Many studies have been investigated in order to specify the possibility of occurrence of these scenarios.
\nHanson et al. and later Shaffer et al. represented that the magnitude of difference between the young modulus of the two intersected interface has significant influence on increasing the possibility of arresting hydraulic fracture [21, 22]. Based on their experimental reports, as the hydraulic fracture propagates from higher modulus into lower interface, the arresting phenomena increase. In addition to the young modulus, experimental results and numerical analysis reveal the effect of the frictional coefficient on the containment of hydraulic fracture. These results show that if the hydraulic fracture propagates from higher frictional coefficient pathway and collides to lower frictional coefficient interface at the natural fracture, the strain increases parallel to the hydraulic fracture due to the increase in the motion rate at interface region. This increase may result in an abrupt fracture seizing. Daneshy also discussed about the possibility of seizing the growth of hydraulic fracture at the intersection stage based on the opening interface of the natural fracture [23]. Another significant parameter that can influence the crossing criteria of hydraulic fracture is the approaching angle. Blanton using different angle-approaching experiments concluded that the presence of high differential stress and high intersection angle can improve the crossing of hydraulic fracture.
\nThe hydraulic fracture can keep on planar propagation beyond the collision point. However, because of the energy dissipation at the contacting stage, the crossing criteria cannot exactly determine if the hydraulic fracture will penetrate through the other side of weakness plane. The fluid-driven energy must be high enough in order to separate the natural fracture bonding at the intact side of the wall. However, breakage at the other side of the wall might have some offset with the collision point, which originates from the preexisted flaw or mini-cracks along the intact side. Based on Blanton’s results, the reduction of the stress anisotropy and treatment pressure may lead to increase in the possibility of diversion and dissipation of fluid-driven along the natural fracture path and also to complex natural fracture network [24, 25]. Later, Beugelsdijk using laboratory experimental results concluded that at high principle stress difference, the hydraulic fracture may have no interaction with the preexisting discontinuities and may turn around them [26]. In addition to the mentioned scenarios, hydraulic fracture may also cause dilation, long slippage along the natural fracture interface, or may turn around and bypass discontinuities. Inclined weakness plane at the propagation path of induced fracture has high tendency to divert the fluid-driven. However, all of the mentioned scenarios can only be estimated and visually represented using an experimental method. The containment stage is the only stage which can approximate the interaction on the natural fracture and fluid-driven. Beyond this stage, no other method can exactly approve the crossing criteria or diversion.
\nHydraulic fracture propagation in the naturally fractured reservoirs plays a different role than the conventional porous media. As the hydraulic fracture passes beyond the induced stress of drilled well, the hydraulic fracture propagation reorientates through the maximum stress principle. The hydraulic fracture propagation in homogeneous porous media is approximately near to the straight path; however, in a real reservoir rock media, because of discontinuities and inhomogeneity, the induced fracture trajectory waver is perpendicular with the minimum compressional stress. The hydraulic fracture tip tends to propagate through the local direction, which has the maximum energy release rate and minimum resistance. Still, there is the possibility of curving and increasing the deviation of hydraulic fracture from straight trajectory by increasing the shearing intensity factor. As long as the induced fracture propagates in opening mode, its fracture trajectory is near to the straight line. When the fracture faced the two materials with different Young’s modulus, the angle of deflection tends to rematch the tip direction in accordance with the lower Young’s modulus material. By increasing the hydraulic fracture length by the propagation of the tip of the hydraulic fracture away from the wellbore, the curvature of hydraulic fracture tends to be decreased. In addition to the rock mechanic properties, the fracturing fluid properties and flow rate injection also have a great impact on the straightness stability. Also, increasing the fracturing fluid viscosity will decrease the leak-off rate and tortuosity of the fracture, but it requires a higher rate of treatment pressure [27]. However, increasing the fluid viscosity in fracturing treatment leads to an abrupt increase in fluid pressure at the fracture path and reduces the flow rate at the fracture tip, because of the uniformity in pressure profile within the hydraulic fracture path. High rate of pressure difference between the fracture tip and the mouth region causes an inhomogeneity in the geometry of the fracture path and lowers the rate of growth [28]. Unlike the high viscosity, lower viscosity will cause a uniform pressure profile within the hydraulic fracture path increasing fluid leakage rate to the adjacent layer. Increasing the fluid leak-off rate will cause a perturbation in the local stress regime and increase the possibility of zigzag fracture pattern. Natural fractures have different response in alteration of the rate of injection and fracturing fluid properties. In the naturally fractured reservoir, increasing the flow rate injection will increase the leak-off rate to the adjacent layer and subsequently cause debonding of the natural fracture in tensile mode [29]. From the studies, reducing the fluid flow injection rate and viscosity of fracturing fluid in fractured media will greatly reduce the possibility of complex fracture network generation [30].
\nAfter initiation and propagation stage of hydraulic fracture beyond the far-field stress region, the hydraulic fracture tries to rematch its orientation by the maximum stress principle. The hydraulic fracture direction is almost parallel with the orientation of maximum stress principle but not exactly perpendicular to the minimum compressional stress, because it tends to orient its trajectory in porous media along the path of minimum resistance. Despite the stress direction in the local field, the induced fracture trajectory may have a wavy shape because of the inhomogeneity of the porous media along its path. The local stress component at the neighborhood of the fracture tip can be expressed by the following equation:\n
where (
where
In numerical modeling, we can only predict the local displacement within the natural fracture only at the
where
where
where
where
As mentioned earlier, when the hydraulic fracture propagates through the 90° natural fracture, at the early stage of approaching, the natural fracture is almost closed. By approaching the hydraulic fracture to the natural fracture interface, some activation may occur which may change the local physical properties at that region. In addition to the hydraulic fracture acting stress, the natural fracture also perturbs the stress regime around its area, which is directly proportional to its length. In reality, we cannot represent that if the approaching angle is 90°, then the collision angle is orthogonal too. This is due to the fact that the local perturbation and acting stress in coalescence process are mutual. Natural fracture by acting stress to the tip of the hydraulic fracture will cause deviation on its overall propagation, which may lead to deviation from the 90°. The magnitude of this stress can be expressed by the following equation [33]:\n
where
From Figure 2, assume that the approaching angle is the same as collision angle which is 90°. As seen in Figure 2, the hydraulic fracture approaches the natural fracture in an orthogonal angle. The tensile and shear debonding can be evaluated at the approaching stage of the hydraulic fracture tip to the natural fracture interface in a, b and c areas. a and b areas are located, respectively, at 10- and 5-cm distances from the 50-cm length natural fracture interface, and c area is precisely located at the collision point of the hydraulic fracture to the natural fracture. Stress condition is assumed to be isotopic.
\nEvaluated areas for debonding of natural fracture when induction fracture is 90° angle.
The maximum opening and shearing displacement in perpendicular approaching stage approximately occurs at the 20-cm distance from the north tip of the natural fracture. The maximum tensile and debonding size and location in the orthogonal approaching stage are the same. Moreover, debonding evaluation indicates that the minimum debonding size occurs at the 30-cm distance from the north of the natural fracture tip. As already mentioned, in the realistic-induced fracture propagation, debonding displacement alteration in tensile and shearing mode happens because changing the propagation angle at the perturbed stress region is not monotonic.
\nPerturbation of stress regime around the approaching hydraulic fracture tip will lead to the activation of natural fracture interface prior to the collision stage. In normal opening mode prior to the collision stage, debonding occurs at the time that the pore pressure within the natural fracture dominates the normal closure stress of the natural fracture (
Tensile and shear displacements along the deboned zone shown in
Approaching stage of hydraulic fracture and shear dilation caused by remote stress around induced fracture.
Another main approaching angle, which can be investigated in our study, is an inclined natural fracture with the 45° angle with respect to the propagated hydraulic fracture. In an inclined mode, the lower rate of energy is required in order to reactivate the natural fracture interface at the same distance compared with the perpendicular mode (Figure 5). Unlike many earlier models, the hydraulic fracture is propagated through the interface of the natural fracture, which means that the touching moment of the left side is the same as the right side. Tensile and shear displacements along the debonded crack (45°) are shown in Figure 6. When the induction with 45° angle is close to the natural fracture in the c area, tensile failure phenomenon is such that the natural fracture had an angle of 90°, because the middle area of the natural fracture becomes debonded and the maximum value of debonding occurs at the collision point. But with less distance between the natural and induced fractures, the condition is slightly different. When the hydraulic fracture approaches the 10-cm distance from the natural fracture, the 12-cm distance from the north tip of the natural fracture becomes compressed and the other part becomes debonded. The maximum value of debonding is at the collision point but the symmetry of the debonding zone in the natural fractures with 90° angle does not take place here. After the cutoff point, the natural fracture by hydraulic fracture (c area) of the upper part of the kink point becomes debonded and the lower part becomes compressed (Figure 6). In 45° angle propagation angle, the shear displacement magnitude has a higher value than the tensile opening. In this case, the lower part of the coalescence point has the tendency to bind because of the compression and the upper part in tension turns into debonding (Figure 7).
\nAreas of study for debonding investigation when natural fracture with a 45° angle relative to the hydraulic fracture spread.
Tensile and shear displacements along the debonded zone shown in
In low approaching angle (45°) at the isotropic stress ratio, the shearing displacement is much larger than the tensile mode; however, with an increase in the stress ratio the difference between shearing and tensile opening remains closed to each other [34]. The natural fracture length increases the remote stress caused by the tip of the hydraulic fracture that has a tendency to increase the debonding of the natural fracture [35, 36].
\nDebonding induced by the approaching hydraulic fracture to natural fracture.
The approaching stage of the hydraulic fracture was not fully investigated and carried out in a numerical way. As mentioned previously, considering stress regime perturbation around the natural fracture location will cause a deflection on the approaching angle of the hydraulic fracture. As the hydraulic fracture grows toward the natural fracture, influenced by the interaction stress of the natural fracture, the nearest tip edge will be active in a shorter time leading to the propagation of hydraulic fracture in a mixed mode. By increasing the shearing intensity factor, the hydraulic fracture path tends to be more kinked and deviates through the natural fracture interface. The following equation can compute the deflection angle of induced fracture (α) under mixed-mode propagation:\n
The curvature of the hydraulic fracture by the propagation of the hydraulic fracture will dramatically increase in stress-perturbed zone [33]. If the opening mode dominates in the tip of the hydraulic fracture, the fracture trajectory will tend to be more singular and straight. The rate of the hydraulic fracture deflection highly depends on the treatment pressure, leak-off rate, length of the natural fracture, and stress anisotropy. In this study, we assume that the hydraulic fracture is subjected to an isotropic principle stress. At the early stage of deviation, the natural fracture walls tend to stick together and are almost completely closed. In parallel natural fracture case, in addition to the distance parameter, the alteration of the approaching angle is another factor which was considered. Figure 8 shows the distance from the deviated hydraulic fracture tip on the natural fracture at 10 (a) and 5 m (b) and the exact coalescence (c) of the hydraulic and natural fractures. When the hydraulic fracture reaches the point a, the natural fracture reaches the activation threshold. When the hydraulic fracture approaches the natural fracture (Figure 8b and c), normal displacement occurs, and the natural fracture interface nearly fully separates. As seen in Figure 8, the approaching of the induced fracture will lead to an abrupt increase in the propagation angle and oriented near to perpendicularly. Increases in the values for the deviation angle and interaction stress increase the possibility of natural fracture collision.
\nApproaching stage of induced fracture and shear dilation caused by remote stress around hydraulic fracture.
If the collision point in the approaching stage of the hydraulic fracture is assumed to lie at the midpoint of the natural fracture in the isotropic principle stress situation, the tensile displacement is as shown in Figure 9. At the approaching stage, the shear displacement increases nonlinearly because, at a constant shear stress, the shear displacement is also a function of the normal displacement. By increasing the normal displacement of natural fracture interface, the shear displacement has lower resistance to shearing. Moreover, because of continuous changing of approaching angle besides the distance, the shearing, and opening displacement both of them have non-monotonic behavior. As the hydraulic fracture approaches the natural fracture, the approaching angle of the hydraulic fracture increases with respect to the natural fracture location, which leads to a decrease in shearing compression. Surprisingly, the influence of the approaching angle on the shear slippage as the hydraulic fracture approaches the natural fracture is greater than the influence of the distance. As Figure 9 shows, the approaching angle of the hydraulic fracturing tip is 66 (a), 49 (b), and 34° (c). As seen in Figure 10, the deviation of the intersection angle from the perpendicular will result in discrepancies in the natural fracture tip displacement. As the hydraulic fracture interacts with the natural fracture, the pore pressure within the natural fracture changes, which leads to compression and extension within the natural fracture.
\nTensile and shear displacements along the debonded zone shown in
Deviation of the intersection angle from the perpendicular will result in discrepancies in natural fracture tip displacement.
Formerly, re-meshing technique has been greatly implemented in order to align the mesh with the tip of the hydraulic fracture for tracking the propagating direction. However, in our study by utilizing the XFEM as no-re-meshing tools can greatly track the hydraulic fracture trajectory to capture the stress and strain field around the tip of the hydraulic fracture. The accuracy of fracture propagation trajectory by refining the mesh around the crack tip can be improved. Stress singularity at the fracture tip is eliminated by the implementation of cohesive zone model in XFEM. Refining the mesh can provide more accurate calculation in the propagation of hydraulic fracture through natural fractures based on shearing or opening mode by computation stress concentration around the fracture tip. The number of iteration to reach convergence in our fracture tip is 5–7. The error between our numerical result and the analytical result is lower than 1%.
\nNatural fractures can have a significant effect on the hydraulic fracture growth and achieve successful treatment. Spacing and trajectory of natural fractures in fractured blocks with respect to the induced fracture propagation has a significant effect on the accuracy of interaction prediction. Numerical analysis of hydraulic fracturing propagation in the naturally fractured reservoir and the interaction between the induced fracture and the natural fracture are the main objectives of this paper. Numerical simulation can be used as a tool to solve this engineering problem.
\nIn this paper, the extended finite element method (XFEM) has been implemented to simulate the coalescence stage of hydraulic fracture and natural fractures. Analysis of interaction between the induced and natural fractures in the fractured reservoirs was discussed in this study. The interaction between the induced and natural fractures depends on the collide angle. Induced fracture causes the opening of the preexisting natural fractures. The tensile and shear debonding of natural fractures in 90 and 45° displayed different behavior caused induced and variations in stresses at the natural fractures. A critical point in interaction between the hydraulic fracture and the natural fractures is the dilation caused by shearing and opening from the northing to the southing along the natural fracture in both degrees which play different scenarios. Decreasing the approaching angle from perpendicular to 45° intensifies the displacement by shearing much more than tensile. In low collision angle, the top stage of the interception point has the maximum debonding in shearing mode and the lower stage has the maximum bonding.
\nThere may not be a precise background to the first discovery and application of phase change materials (PCMs). Perhaps, from the earliest days where human has acquired the intellect, he has realized the existence of these substances or, maybe, has used them without recognizing their nature. Throughout science and technology evolution, more precisely, since the heat capacity of materials and sensible or latent heats have been known, their ability to store and release thermal energy has also been considered. However, A. T. Waterman submitted the first report of discovery in the early 1900s. In recent years, scientists have paid particular attention to these materials, and their commercialization began from those years.
Perhaps the main reason for this attention was the problems caused by energy mismanagement and improper use of it. Today, inadequate energy management, especially fossil fuels, has caused many environmental and economic problems. Therefore, the necessity of efficient energy demand as well as development of renewable energies and energy storage systems is highly significant. One of the important topics in this field is the design of special energy storage equipment to other types. Energy storage not only reduces the discrepancy between energy supply and demand but also indirectly improves the performance of energy generation systems as well as plays a vital role in saving of energy by converting it into other reliable forms. Hence, this matter saves high-quality fuels and reduces energy wastes [1, 2, 3].
Energy storage is one of the important parts of renewable energies. Energy can be stored in several ways such as mechanical (e.g., compressed air, flywheel, etc.), electrical (e.g., double-layer capacitors), electrochemical (e.g., batteries), chemical (e.g., fuels), and thermal energy storages [4].
Among several methods of energy storage, thermal energy storage (TES) is very crucial due to its advantages. TES is accomplished by changing the internal energy of materials, such as sensible heat, chemical heat, latent heat, or a combination of them.
In sensible heat storage (SHS) systems, heat can be stored by increasing the temperature of a material. Hence, this system exploits both the temperature changes and the heat capacity of the material to store energy. The amount of heat stored in this system depends on the specific heat, temperature differences, and amount of material; thus it requires a large amount of materials, whereas Latent heat storage (LHS) is generally based on the amount of heat absorbed or released during the phase transformation of a material. Lastly, In the chemical heat storage (CHS), heat is stored by enthalpy change of a chemical reaction.
Among the aforementioned heat storage systems, the LHS is particularly noteworthy. One of the special reasons is its ability to store large amount of energy at an isothermal process [5, 6, 7].
Any high-performance LHS system should contain at least one of the following terms:
Appropriate PCM with optimum melting temperature range
Desirable and sufficient surface area proportional to the amount of heat exchange
Optimal capacity compatible with PCM
Phase change materials perform energy storage in LHS method. In this case, a material during the phase change absorbs thermal energy from surrounding to change its state, and in the reverse process, the stored energy is released to the surrounding. PCMs initially behave likewise to other conventional materials as the temperature increases, but energy is absorbed when the material receives heat at higher temperatures and close to the phase transformation. Unlike conventional materials, in PCMs absorption or release of thermal energy is performed at a constant temperature. A PCM normally absorbs and releases thermal energy 5–14 times more than other storage materials such as water or rock [8, 9].
PCMs can store thermal energy in one of the following phase transformation methods: solid-solid, solid-liquid, solid-gas, and liquid-gas. In the solid-solid phase change, a certain solid material absorbs heat by changing a crystalline, semicrystalline, or amorphous structure to another solid structure and vice versa [10]. This type of phase change, usually called phase transitions, generally has less latent heat and smaller volume change comparing to the other types. Recently, this type of PCM has been used in nonvolatile memories [11].
Solid-liquid phase change is a common type of commercial PCMs. This type of PCM absorbs thermal energy to change its crystalline molecular arrangement to a disordered one when the temperature reaches the melting point. Unlike solid-solid, solid-liquid PCMs contain higher latent heat and sensible volumetric change. Solid-gas and liquid-gas phase changes contain higher latent heat, but their phase changes are associated with large volumetric changes, which cause many problems in TES systems [8]. Although the latent heat of solid-liquid is less than liquid-gas, their volumetric change is much lower (about 10% or less). Therefore, employing PCMs based on solid-liquid phase change in TES systems would be more economically feasible.
The overall classification of energy storage systems as well as phase change materials is given in Figure 1.
Overview of energy storage and classification of phase change materials.
As mentioned in the previous section, despite the high thermal energy absorption capacity, PCMs in liquid-gas and solid-gas transitions have extremely high volume changes. On the other hand, solid-solid PCMs also have a lower thermal energy storage capacity. Therefore, the abovementioned PCMs, with the exception of specific cases, have not received much attention to commercialization. Currently, the most common type of transition that has been mass-marketed is solid-liquid PCMs. The classification of phase change materials is schematically given in Figure 1. Solid-liquid PCMs are generally classified as three general organics, inorganic, and eutectics [12, 13]. However, in some references they are classified into two major organics and inorganics.
Inorganic PCMs mainly have high capacity for thermal energy storage (about twice as much as organic PCMs) as well as have higher thermal conductivity. They are often classified as salt hydrates and metals.
At the phase transition, the hydrate crystals are subdivided into anhydrous (or less aqueous) salt and water. Although salt hydrates have several advantages, some deficiencies make restrictions in their application. One of these problems is incongruent melting behavior of salt hydrates. In this problem the released water from dehydration process is not sufficient for the complete dissolution of the salts. In this case, the salts precipitate and as a result phase separation occurs. In order to prevent this problem, an additional material such as thickener agent is added to salt hydrates. Another major problem with salt hydrates is the supercooling phenomenon. In this phenomenon, when crystallization process occurs, the nucleus formation is delayed; therefore, even at temperatures below freezing, the material remains liquid [7, 11, 14].
Overall, the most attractive properties of salt hydrate are (i) high alloy latent temperature, (ii) relatively high thermal conductivity (almost two to five times more than paraffin), and (iii) small volume changes in melting. They are also very low emitting and toxic, adaptable to plastic packaging, and cheap enough to use [15].
Some metals such as indium, cesium, gallium, etc. are used for low-temperature PCMs, while others such as Zn, Mg, Al, etc. are used for high temperatures. Some metal alloys with high melting points (in the range of 400–1000°C) have been used for extremely high temperature systems. These metal alloys as high-temperature PCMs can be used in the field of solar power systems [16, 17]. They can also be used in industries that require temperature regulation in furnaces or reactors with high operating temperatures.
Perhaps the most important fragment is the organic PCMs. Organic PCMs show no change in performance or structure (e.g., phase separation) over numerous phase change cycles. In addition, supercooling phenomena cannot be observed in organic PCMs. The classification of organic PCMs is unique. This division is mainly based on their application contexts. In general, they are classified into two major paraffin and non-paraffin sections.
Although non-paraffin organic PCMs have high latent heat capacity, they have weaknesses such as flammability, low thermal conductivity, low combustion temperatures, and transient toxicity. The most important non-paraffinic PCMs are fatty acids, glycols, polyalcohols, and sugar alcohols.
Fatty acids [CH3(CH2)2nCOOH] also have high latent heat. They can be used in combination with paraffin. Fatty acids exhibit high stability to deformation and phase separations for many cycles and also crystallize without supercooling. Their main disadvantages are their costs. They are 2–2.5 times more expensive than technical grade paraffins. Unlike paraffins, fatty acids are of animal or plant origin. Their properties are similar to those of paraffins, but the melting process is slower. On the other hand, they are moderately corrosive as well as generally odorous [21].
A eutectic contains at least two types of phase change materials. Eutectics have exceptional properties. In eutectics, the melting-solidification temperatures are generally lower than the constituents and do not separate into the components through the phase change. Therefore, phase separation and supercooling phenomena are not observed in these materials.
Eutectics typically have a high thermal cycle than salt hydrates. Inorganic-inorganic eutectics are the most common type of them. However, in recent studies, organic-inorganic and organic-organic varieties have received more attention. The major problem of eutectics is their commercialization. Their cost is usually two to three times higher than commercial PCMs [22, 23].
Some of the above PCMs and their thermal properties, which are competitive with paraffins in terms of latent heat capacity, are summarized in Table 1.
Type of PCMs | Materials | Melting point (°C) | Latent heat (kJ/kg) | Density* (kg/m3) | Thermal conductivity (W/mK)** | Ref. | |
---|---|---|---|---|---|---|---|
Inorganic salt hydrates | LiClO3·3H2O | 8 | 253 | 1720 | [24, 25] | ||
K2HPO4·6H2O | 14 | 109 | [24] | ||||
Mn(NO3)2·6H2O | 25.8 | 126 | 1600 | [14, 25] | |||
CaCl2·6H2O | 29.8 | 191 | 1802 | 1.08 | [24, 25] | ||
Na2CO3·10H2O | 32–34 | 246–267 | [14, 24] | ||||
Na2SO4·10H2O | 32.4 | 248, 254 | 1490 | 0.544 | [14, 26] | ||
Na2HPO4·12H2O | 34–35 | 280 | 1522 | 0.514 | [15, 26] | ||
FeCl3·6H2O | 36–37 | 200, 226 | 1820 | [25, 26] | |||
Na2S2O3·5H2O | 48–49 | 200, 220 | 1600 | 1.46 | [15, 26] | ||
CH3COONa·3H2O | 58 | 226, 265 | 1450 | 1.97 | [15, 26] | ||
Non-paraffinic organic PCMs | Fatty acids | Formic acid | 8.3 | 247 | 1220 | — | [1, 25] |
n-Octanoic acid | 16 | 149 | 910 | 0.148 | [21, 27] | ||
Lauric acid | 43.6 | 184.4 | 867 | [21, 25] | |||
Palmitic acid | 61.3 | 198 | 989 | 0.162 | [21, 27] | ||
Stearic acid | 66.8 | 259 | 965 | 0.172 | [21, 25] | ||
Polyalcohols | Glycerin | 18 | 199 | 1250 | 0.285 | [1, 25] | |
PEG E600 | 22 | 127.2 | 1126 | 0.189 | [27] | ||
PEG E6000 | 66 | 190 | 1212 | [27] | |||
Xylitol | 95 | 236 | 1520 | 0.40 | [28] | ||
Erythritol | 119 | 338 | 1361 | 0.38 | [28] | ||
Others | 2-Pentadecanone | 39 | 241 | [1, 25] | |||
4-Heptadekanon | 41 | 197 | [1, 25] | ||||
D-Lactic acid | 52–54 | 126, 185 | 1220 | [1, 25] | |||
Eutectics | O-O, O-I, I-I *** | CaCl2·6H2O + MgCl2·6H2O | 25 | 127 | 1590 | [27] | |
Mg(NO3)2·6H2O + MgCl2·6H2O | 59 | 144 | 1630 | 0.51 | [27] | ||
Trimethylolethane + urea | 29.8 | 218 | [21] | ||||
CH3COONa·3H2O + Urea (60:40) | 31 | 226 | [27] | ||||
Metals | Mg-Zn (72:28) | 342 | 155 | 2850 | 67 | [16, 17] | |
Al-Mg-Zn (60:34:6) | 450 | 329 | 2380 | [16, 17] | |||
Al-Cu (82:18) | 550 | 318 | 3170 | [16, 17] | |||
Al-Si (87.8:12.2) | 580 | 499 | 2620 | [16, 17] |
Thermophysical properties of some common PCMs with high latent heat.
At 20°C.
Just above melting point (liquid phase).
Inorganic-inorganic (I-I), organic-inorganic (O-I), and organic-organic (O-O).
Paraffin is usually a mixture of straight-chain
Paraffins typically have high latent heat capacity. If the length of the chain increases, the melting ranges of waxes also increase, while the latent heat capacity of melting is not subject to any particular order (Table 2).
Materials | Melting point (°C) | Latent heat (kJ/kg) | Density* (kg/m3) | Thermal conductivity** (W/mK) |
---|---|---|---|---|
n-Tetradecane (C14) | 6 | 228–230 | 763 | 0.14 |
n-Pentadecane (C15) | 10 | 205 | 770 | 0.2 |
n-Hexadecane (C16) | 18 | 237 | 770 | 0.2 |
n-Heptadecane (C17) | 22 | 213 | 760 | 0145 |
n-Octadecane (C18) | 28 | 245 | 865 | 0.148 |
n-Nonadecane (C19) | 32 | 222 | 830 | 0.22 |
n-Eicosane (C20) | 37 | 246 | ||
n-Henicosane (C21) | 40 | 200, 213 | 778 | |
n-Docosane (C22) | 44.5 | 249 | 880 | 0.2 |
n-Tricosane (C23) | 47.5 | 232 | ||
n-Tetracosane (C24) | 52 | 255 | ||
n-Pentacosane (C25) | 54 | 238 | ||
n-Hexacosane (C26) | 56.5 | 256 | ||
n-Heptacosane (C27) | 59 | 236 | ||
n-Octacosane (C28) | 64.5 | 253 | ||
n-Nonacosane (C29) | 65 | 240 | ||
n-Triacontane (C30) | 66 | 251 | ||
n-Hentriacontane (C31) | 67 | 242 | ||
n-Dotriacontane (C32) | 69 | 170 | ||
n-Triatriacontane (C33) | 71 | 268 | 880 | 0.2 |
Paraffin C16-C18 | 20–22 | 152 | ||
Paraffin C13-C24 | 22–24 | 189 | 900 | 0.21 |
RT 35 HC | 35 | 240 | 880 | 0.2 |
Paraffin C16-C28 | 42–44 | 189 | 910 | |
Paraffin C20-C33 | 48–50 | 189 | 912 | |
Paraffin C22-C45 | 58–60 | 189 | 920 | 0.2 |
Paraffin C21-C50 | 66–68 | 189 | 930 | |
RT 70 HC | 69–71 | 260 | 880 | 0.2 |
Paraffin natural wax 811 | 82–86 | 85 | 0.72 (solid) | |
Paraffin natural wax 106 | 101–108 | 80 | 0.65 (solid) |
In general, paraffin waxes are safe, reliable, inexpensive, and non-irritating substances, relatively obtained in a wide range of temperatures. As far as economic issues are concerned, most technical grade waxes can be used as PCMs in latent heat storage systems. From the chemical point of view, paraffin waxes are inactive and stable. They exhibit moderate volume changes (10–20%) during melting but have low vapor pressure.
The paraffin-based PCMs usually have high stability for very long crystallization-melting cycles. Table 2 illustrates the thermal properties of some paraffin waxes.
Besides the favorable properties, paraffins also show some undesirable properties such as low thermal conductivity, low melting temperatures, and moderate-high flammability. Some of these disadvantages especially thermal conductivity and flammability can be partially eliminated with the help of additives or paraffin composites.
Measures must be taken to make the solid-liquid PCMs usable. For this purpose, there are several methods for stabilizing the shapes of paraffinic PCMs. Two main methods of them are discussed below.
Encapsulation is generally a worthy method to protect and prevent leakage of PCMs in the liquid state. The capsules consist of two parts, the shell and the core. The core part contains PCMs, whereas the shell part is usually composed of polymeric materials with improved mechanical and thermal properties. The shell part plays the role of protection, heat transfer, and sometimes preventing the release of toxic materials into the environment. In these cases, the shell must have appropriate thermal conductivity. Polymeric shells are also commonly used in encapsulating PPCMs. The choice of core part depends on its application field. The encapsulation of PPCMs is classified into three major parts: bulk or macroencapsulation, microencapsulation, and nano-encapsulation.
In order to increase the efficiency of heat transfer in these types of capsules, either the size of the capsules should be appropriately selected or suitable modifiers should be used. In general, the smaller the diameter of spherical capsules or cylinders, the better the heat transfer. In some cases, metal foams are used to improve the heat transfer properties of paraffin. Aluminum and copper open-cell foams are among the most studied, whereas, in other cases metal oxides, metals and graphite are used [30, 31].
There are various forms of macroencapsulation, such as ball shape, spherical shape, cylindrical, flat sheets, tubular, etc. [31]. Cylindrical tubes are one of the famous forms of macroencapsulated PPCMs. This type of encapsulation is most commonly used in buildings or in solar energy storage systems.
Most of the research carried out on macroencapsulated PPCMs has been focused on improving their thermal conductivity. In one of these studies, different metal oxide nanoparticles such as aluminum oxide, titanium oxide, silicon oxide, and zinc oxide were used to improve the thermal conductivity of paraffin. The results show that titanium oxide performs better under the same conditions than the other oxides [32]. In a similar study, copper oxide nanoparticles were used to improve thermal conductivity and performance of paraffin in solar energy storage systems [33]. In some studies, graphite flakes and expanded graphite have also been used as improving agent for heat conductivity [31].
Hong et al. have used polyethylene terephthalate pipes as a shell for paraffin. In this macroencapsulated system, introduced as cylinder modules, float stone has been added to paraffin as an enhancer of thermal conductivity. In this study, the effect of various parameters such as pipe diameter on heat transfer is investigated, and the results of experimental section are compared with modeling [34].
D. Etansova et al. studied numerical computation and heat transfer modeling of paraffin-embedded stainless steel macroencapsulates for use in solar energy storage systems. In this study, the effect of geometric size and shape on heat transfer was investigated [35].
In general, there are two major physical and chemical methods for microencapsulation. The most important physical methods are fluidized bed, spray dryer, centrifuge extruder, and similar processes. However, chemical methods are often based on polymerization. The most important techniques include in situ suspension and emulsion polymerization, interfacial condensation polymerization, and sol-gel method. The latter is sometimes known as the physicochemical method [12, 29].
In the suspension or emulsion polymerization method, the insoluble paraffin is first emulsified or suspended in a polar medium, which is predominantly aqueous phase, by means of high-speed stirring. Surfactants are used to stabilize the particles. Then, lipophilic monomers are added to the medium, and the conditions are prepared for polymerization. This polymer, which is insoluble in both aqueous and paraffin phases, is formed on the outer surface of paraffin particles and finally, after polymerization, encapsulates the paraffin as a shell. The size of these capsules depends on the size of emulsion or suspension of paraffin droplets. Sometimes certain additives are added to the medium to improve some of the polymer properties. For instance, in some studies, polyvinyl alcohol (PVA) has been added to the medium with methyl-methacrylate monomer, which is known as one of the most important shell materials. As a result, paraffin has been encapsulated by PVA modified polymethyl methacrylate (PMMA). Adding this modifier forms a smooth surface of the microencapsulates [36, 37].
In the interfacial method, soluble monomers in the organic phase with other monomers in the aqueous phase at the droplet interface form a polymer that precipitates on the outer layer of the organic phase.
The sol-gel method is a multi-step procedure. In this method, firstly, an organosilicon compound such as tetraethoxysilane (TEOS) is hydrolyzed in an acidic medium at low pH. The prepared homogenous solution is known as the sol part. Then, the paraffin emulsion is prepared in an aqueous medium and stabilized by special emulsifiers. Actually, these emulsifiers are the first layer of the shell. Subsequently, the sol solution is slowly added to the aqueous phase containing paraffin. The silicon compounds containing OH groups (silanols) form hydrogen bonding with polar side of emulsifiers, and finally the condensation process is carried out on the first layer interface. As a result, paraffin microencapsulates with an inorganic material that is often silica. Silica is one of the significant materials used as a shell for micro and nano-encapsulation. Silica has high thermal conductivity and on the other hand has better mechanical properties than some polymers [38, 39, 40, 41].
As mentioned, most of the materials used to microencapsulation are polymers. The main polymers used as shell materials are polymethyl methacrylate [42], polystyrene [43], urea-formaldehyde [44], urea-melamine-formaldehyde [45], polyaniline [46], etc. However, in many cases, these polymers are used in modified form. For example, polymethyl methacrylate modified with polyvinyl alcohol or with other methacrylates [36, 37], polystyrene copolymers [47], and melamine modified-formaldehyde with methanol [48] can be considered. Table 3 shows the most common polymers used as shell materials.
Core material PPCM | Shell material | Encapsulation method | Particle size (μm) | Recommended application | Ref |
---|---|---|---|---|---|
n-Nonadecane | Polymethyl methacrylate | Emulsion | ~ 8 | Smart building and textiles | [42] |
n-Heptadecane | Polystyrene | Emulsion | <2 | General fields | [43] |
Commercial paraffin wax | Polystyrene-co-PMMA | Suspension | ~ 20 | [50] | |
Commercial RT21 | PMMA | Suspension | 20–40 | [36] | |
Commercial RT21 | PMMA modified with PVA | Emulsion | 15 | Building | [37] |
Commercial paraffin wax | Polyaniline | Emulsion | <1 | [46] | |
Commercial paraffin wax | Urea-formaldehyde | In situ | ~ 20 | [44] | |
n-Octadecane, n-nonadecane | Urea-melamine-formaldehyde | In situ | 0.3-0.6 | [45] | |
Commercial paraffin wax | Methanol-melamine-formaldehyde | In situ | 10–30 | Building | [48] |
Commercial paraffin wax | Silica | Sol-gel | 4–10 | Textile | [38] |
Commercial paraffin wax | Silica | Sol-gel | 0.2–0.5 | [39] | |
n-Octadecane | Silica | Sol-gel | 7–16 | [40] | |
n-Pentadecane | Silica | Sol-gel | 4–8 | [41] |
Common materials for microencapsulation of PPCMs.
In addition to the aforementioned microencapsulation approaches, which mainly form polymeric materials as shells, other materials have been also recommended. For example, Singh and colleagues have used silver metal as a shell for paraffin microencapsulates. They first emulsified paraffin into small particles in water and then converted silver salts to metallic silver via an in situ reduction reaction. The average particle size of 329 μm has been reported, and the thermal properties of paraffin have been investigated using DSC and TGA. This type of metal shell microencapsulates has been suggested for use in microelectronics heat management systems [49].
There are several techniques to study the properties of micro and nano-encapsulates. In all studies, differential scanning calorimetry (DSC) and thermogravimetric analysis (TGA) have been used to determine the thermal properties of PPCMs, such as enthalpy of fusion, melting temperature, weight loss, degradation, etc. Various methods such as XRD, FTIR, and 12C NMR have been used to study the structure and chemical composition of PPCMs. The morphology and diameters of the microcapsules have often been studied by scanning electron microscopy (SEM) and particle size analyzer.
The latter technique is used to study the influence of different variables on the diameter of the microcapsules. One of these variables is the effect of stirring speed on emulsification of paraffin. The results of some studies show that higher stirring speed of emulsification process leads to decrease of the mean size of paraffin droplets [48].
Along with studies on the type of microcapsules, many studies have been conducted to improve thermal conductivity and mechanical properties of microencapsulates. Part of these studies has been dedicated to the effect of graphene and graphene oxide on the improvement of thermal conductivity [51]. L. Zhang et al. investigated the effect of graphene oxide on improving the mechanical properties and leakage protection as well as improving the thermal conductivity of melamine-formaldehyde as shell materials of PPCM microencapsulates [52]. In another part of studies, metals and metal oxides have been used. For example, 10 and 20 wt% of nanomagnetite (Fe3O4) with particle size from 40 to 75 nm increase the thermal conductivity by 48 and 60%, respectively [53]. Also, addition of TiO2 and Al2O3 nanoparticles in a mass fraction of 5% with respect to PPCM at the size range of 30–60 nm increases the thermal conductivity by 40 and 65%, respectively [54].
In recent years, research on polymeric matrix-based shape-stable PCMs has gained great importance. Among these types of phase change materials, the paraffin-polymer composite is particularly attractive. The combination of paraffin and polymers as new PCMs with a unique controllable structure can be widely used. This compound remains solid at paraffin melting point and even above without any softening, which is why this type of PCM is called shape-stable. These materials are well formed and have high-energy absorption capacity; hence they can be widely used as stable PCMs with specific properties. On the other hand, some problems such as high cost and difficulty of encapsulating processes could be resolved. Despite these advantages, some common disadvantages such as low thermal stability, low thermal conductivity, and relatively high flammability can restrict their application, particularly in building materials. For this reason, further studies are required to eliminate these disadvantages and improve the properties of these materials. A large part of research is relevant to increase or improve their thermal conductivity, flame retardation, and thermophysical and mechanical properties. Suitable additives are proposed to improve these properties [55, 56].
In some articles, a simple method involves mixing-melting of polyethylene and paraffin, consequently cooling the composite, or using a simple twin extruder to prepare a shape-stable PCM has been reported [57, 58]. When this compound contains sufficient polymer, a homogeneous mixture remains solid at temperatures above the melting point of paraffin and below the polymer melting point. During the preparation of these composites, no chemical reaction or chemical bonds are formed between the polymers and paraffin; therefore these types of compounds are considered as physical mixtures. Shape-stable PPCMs can be used in all previously described areas. Due to the thermoplastic properties of these composites, it is possible to melt and crystalize them for many cycle numbers. Shape-stable PPCMs have several advantages over other PCMs. They are also nontoxic and do not require high-energy consumption during production process.
Inaba and Tu [59] developed a new type of shape-stable PPCM and determined their thermophysical properties. These materials can be used without encapsulation. Feldman et al. [60] prepared plates of shape-stable PCM and determined their high thermal energy storage capacity when used in small chambers. In this type of polymer-based plates, fatty acids are used as PCMs that absorb or releases large amounts of heat during melting and solidification, without altering the composition of the shape-stable PCM. The same researchers determined the role of polymer-PCM sheets in stabilizing the shape and size of the plates when PCM was liquefied. The composition of paraffin and high-density polyethylene (HDPE) has been studied by Lee and Choi [61] and has been introduced as a shape-stable energy storage material. In this study, the amount of energy stored by the mentioned composites is also studied. They also studied the morphology of the high-density polyethylene crystal lattice (HDPE) and its effect on paraffin through scanning electron microscopy and optical microscopy (OM) analysis. On the other hand, they also reported of high thermal energy storage capacity of the prepared paraffin/HDPE-based shape-stable PCMs. Hong and Xin-Shi [62] synthesized polyethylene-paraffin as a shape-stable PCM and characterized its morphology and structure by scanning electron microscopy and its latent heat of melting by differential scanning calorimetry. In this study, a composition consisting of 75% paraffin as a cheap, effective, easy-to-prepare, low-temperature shape-stable PPCM is recommended. In another study, Xiao et al. [63] prepared a shape-stable PCM based on the composition of paraffin with a thermoplastic elastomer (styrene butadiene rubber) and determined its thermal properties. The obtained results show that the stable mixture has the phase changing property and the amount of latent heat of melting stored in this compound is estimated to be 80% of pure paraffin. In another part of this study, the thermal conductivity of PCMs was significantly increased by using graphite.
Despite the above benefits, some disadvantages of shape-stable PPCMs are also reported. One of the major problems is the softening and paraffin leakage phenomenon at elevated temperatures. Seiler partly resolved this problem by adding a different ratio of silica and copolymers to the polyethylene-paraffin composition [64]. Another problem is the low thermal conductivity of the polyethylene-paraffin compound. A lot of research has been conducted to increase this property. A. Sari [65] prepared two types of paraffin with different melting temperatures (42–44°C and 56–58°C) and combined each with HDPE as phase modifier. By addition of 3% expanded graphite, the thermal conductivity of composites increased by 14 and 24%, respectively. Zhang et al. [66] developed new PCMS based on graphite and paraffin with high thermal energy storage capacity and high thermal conductivity. Zhang and Ding et al. [67] have used various additives such as diatomite, Wollastonite, organic modified bentonite, calcium carbonate, and graphite to improve the thermal conductivity of shape-stable PCMs.
It should be noted that metal particles and metal oxides due to their higher thermal conductivity are widely used to improve this property of PCMs. One of the materials that has received more attention in recent years is alumina. Aluminum oxide nanoparticles were added to paraffin to increase its thermal conductivity in both liquid and solid states [57, 68]. This compound coupled with its high thermal conductivity is cheaper and more abundant than other metal oxides.
Another problem with shape-stable PPCMs is their flammability. The effect of various additives has been studied by scientists to eliminate this problem. One of the most effective of these substances is halogenated compounds, but they cause environmental pollution and also release toxic compounds while burning. Researchers have used hybrid and environmentally friendly materials to enhance the durability of flame retardant materials. They studied the effect of clay nanoparticles and organo-modified montmorillonite. Adding these materials not only increases their resistance to burning but also increases their mechanical and thermal properties [69, 70, 71]. In another study, Y. Cai et al. added paraffin, HDPE, and graphite, then added ammonium polyphosphate and zinc borate separately, and studied their resistance to burning. The results show that the addition of ammonium polyphosphate decreases flammability, while zinc borate increases the flammability risk [72]. One of the most interesting and harmless fire retardant compounds is metal hydroxides, especially aluminum hydroxide, magnesium hydroxide, or their combination [73, 74, 75].
Some researchers have used other advanced materials as supporting materials to prepare shape-stable PPCMs instead of using the polymer matrix [76, 77, 78]. Rawi et al. used acid-treated multi-walled carbon nanotubes (A-CNT). They reported that adding 5% by weight A-CNT to paraffin decreases 25% of the latent heat while increasing heat conductivity up to 84% [79]. Y. Wan et al. used pinecone biochar as the supporting matrix for PCMs. They prepared shape-stable PCM materials at different ratios and studied the leakage behavior. The optimal ratio is suggested as 60% of the PCM. For the above ratio, no PCM leakage was observed after the melting temperature. The results showed that the thermal conductivity of the same ratio shape-stable PCM increased by 44% compared to the pure PCM [80].
PCMs are available in a wide range of desired temperature ranges. Obviously, a PCM may not have all the properties required to store heat energy as an ideal material. Therefore, it would be more appropriate to use these materials in combination with either other PCMs or various additives to achieve the required features. However, as latent heat storage materials, while using PCMs, the thermodynamic, kinetic, and chemical properties as well as the economic and availability issues of them must be taken into account. Employed PCMs must have the optimum phase change temperature. On the other hand, the higher the latent heat of the material, the lower its physical size. High thermal conductivity also helps to save and release energy. From the physical and kinetic point of view, the phase stability of PCMs during melting and crystallization contributes to optimum thermal energy storage. Their high density also enables high storage at smaller material sizes. During phase change, smaller volume changes and lower vapor pressures are appropriate for continuous applications.
H. Nazir et al. in their review article [12] have explained the criteria for selection of PCMs as a pyramid. In this pyramid, at the bottom, known as the fundamentals, there are several items such as cost, regularity compliance, and safety. In the next section, the thermophysical properties such as energy storage capacity and runtime are discussed. In the upper section, reliability and operating environment consist of degradation, cycle life, shelf life, and thermal limits are reflected. Finally, at the top section of pyramid, user perception and convenience are located. These criteria help us to find a proper PCM for certain application fields.
These criteria may also be extended to paraffinic PCMs. Nowadays, paraffinic PCMs (PPCMs) are widely used as thermal energy storage materials, including solar energy storage systems, food industries, medical fields, electrical equipment protection, vehicles, buildings, automotive industries, etc. [24, 29, 81, 82, 83, 84, 85].
Generally, application fields of PPCMs can be considered in two main sections: thermal protection and energy storage purposes. The major difference between these two areas of application is in thermal conductivity of the PPCMs.
One of the studies related to these issues is the use of paraffin containing heavy alkanes to protect electronic devices against overheating. In this study, paraffin has been used as a protective coating for the resistor chip, and its effect on cooling of the devices has been investigated. Experimental results show that paraffin coating increases the relative duration of overheating by 50 to 150% over the temperature range of 110–140°C [88]. In another study, a mixture of paraffin and polypropylene has been used as an overheating protector in solar thermal collectors [89].
However,
One of the main drawbacks of lightweight building materials is their low thermal storage capacity, which results in extensive temperature fluctuations as a result of intense heating and cooling. Therefore, PPCMs have been used in buildings due to their ability to regulate and stabilize indoor temperatures at higher or lower outdoor temperatures [90].
Generally, PPCMs in buildings are used as thermal energy storage at daytime peak temperature, and they released the stored energy at night when temperatures are low. The result of this application is to set the comfort condition for a circadian period. This application minimizes the amount of energy consumed for cooling during the day and warming up at night.
In contrast, in order to stabilize the ambient conditions at low temperatures, some special PCMs are also used in air conditioner systems. In this case, cool air is stored during the night and released into the warm hours of the day.
Y. Cui et al. [91] in a review article categorized PPCM application methods based on their location of use such as PCMs in walls, floor heating systems, ceiling boards, air-based solar heating systems, free cooling systems (with ventilation systems), and PCM shutter (in windows). Both types of encapsulation and shape-stable PPCMs could be used in all of the above classification of building applications. Sometimes these materials can be added directly to concrete, gypsum, etc. [90, 92, 93, 94, 95].
In order to increase the performance of PPCMs in this application field, great deals of studies have also been done on improving their thermal conductivity. On the other hand, extensive research into safety issues has been done to reduce the flammability of PPCMs by adding flame retardants to these materials.
Overall, these studies cover the importance of using PPCMs in heating and cooling as well as indicate the general characteristics, advantages, and disadvantages of these materials used for thermal storage in buildings.
It is clear that at this time, where renewable energy is particularly important, the use of PPCMs is on the rise. As it has been mentioned, PPCMs have many application fields due to their advantages. For example, they can be used in the construction, pharmaceutical and medical industries, textiles, automobiles, solar power systems, transportation, thermal batteries, heat exchangers, and so on.
This chapter of the book has attempted to focus more on how to use paraffins. For this reason, two methods, namely, encapsulation and shape-constant, have been widely discussed. In addition, improving their weak properties such as thermal conductivity and flammability has also been studied. Depending on the benefits of paraffins, new applications are suggested every day. Extensive studies are underway on other new applications in recent years.
You have been successfully unsubscribed.
",metaTitle:"Unsubscribe Successful",metaDescription:"You have been successfully unsubscribed.",metaKeywords:null,canonicalURL:"/page/unsubscribe-successful",contentRaw:'[{"type":"htmlEditorComponent","content":""}]'},components:[{type:"htmlEditorComponent",content:""}]},successStories:{items:[]},authorsAndEditors:{filterParams:{sort:"featured,name"},profiles:[{id:"6700",title:"Dr.",name:"Abbass A.",middleName:null,surname:"Hashim",slug:"abbass-a.-hashim",fullName:"Abbass A. Hashim",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/6700/images/1864_n.jpg",biography:"Currently I am carrying out research in several areas of interest, mainly covering work on chemical and bio-sensors, semiconductor thin film device fabrication and characterisation.\nAt the moment I have very strong interest in radiation environmental pollution and bacteriology treatment. The teams of researchers are working very hard to bring novel results in this field. I am also a member of the team in charge for the supervision of Ph.D. students in the fields of development of silicon based planar waveguide sensor devices, study of inelastic electron tunnelling in planar tunnelling nanostructures for sensing applications and development of organotellurium(IV) compounds for semiconductor applications. I am a specialist in data analysis techniques and nanosurface structure. I have served as the editor for many books, been a member of the editorial board in science journals, have published many papers and hold many patents.",institutionString:null,institution:{name:"Sheffield Hallam University",country:{name:"United Kingdom"}}},{id:"54525",title:"Prof.",name:"Abdul Latif",middleName:null,surname:"Ahmad",slug:"abdul-latif-ahmad",fullName:"Abdul Latif Ahmad",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:null},{id:"20567",title:"Prof.",name:"Ado",middleName:null,surname:"Jorio",slug:"ado-jorio",fullName:"Ado Jorio",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Universidade Federal de Minas Gerais",country:{name:"Brazil"}}},{id:"47940",title:"Dr.",name:"Alberto",middleName:null,surname:"Mantovani",slug:"alberto-mantovani",fullName:"Alberto Mantovani",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:null},{id:"12392",title:"Mr.",name:"Alex",middleName:null,surname:"Lazinica",slug:"alex-lazinica",fullName:"Alex Lazinica",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/12392/images/7282_n.png",biography:"Alex Lazinica is the founder and CEO of IntechOpen. After obtaining a Master's degree in Mechanical Engineering, he continued his PhD studies in Robotics at the Vienna University of Technology. Here he worked as a robotic researcher with the university's Intelligent Manufacturing Systems Group as well as a guest researcher at various European universities, including the Swiss Federal Institute of Technology Lausanne (EPFL). During this time he published more than 20 scientific papers, gave presentations, served as a reviewer for major robotic journals and conferences and most importantly he co-founded and built the International Journal of Advanced Robotic Systems- world's first Open Access journal in the field of robotics. Starting this journal was a pivotal point in his career, since it was a pathway to founding IntechOpen - Open Access publisher focused on addressing academic researchers needs. Alex is a personification of IntechOpen key values being trusted, open and entrepreneurial. Today his focus is on defining the growth and development strategy for the company.",institutionString:null,institution:{name:"TU Wien",country:{name:"Austria"}}},{id:"19816",title:"Prof.",name:"Alexander",middleName:null,surname:"Kokorin",slug:"alexander-kokorin",fullName:"Alexander Kokorin",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/19816/images/1607_n.jpg",biography:"Alexander I. Kokorin: born: 1947, Moscow; DSc., PhD; Principal Research Fellow (Research Professor) of Department of Kinetics and Catalysis, N. Semenov Institute of Chemical Physics, Russian Academy of Sciences, Moscow.\r\nArea of research interests: physical chemistry of complex-organized molecular and nanosized systems, including polymer-metal complexes; the surface of doped oxide semiconductors. He is an expert in structural, absorptive, catalytic and photocatalytic properties, in structural organization and dynamic features of ionic liquids, in magnetic interactions between paramagnetic centers. The author or co-author of 3 books, over 200 articles and reviews in scientific journals and books. He is an actual member of the International EPR/ESR Society, European Society on Quantum Solar Energy Conversion, Moscow House of Scientists, of the Board of Moscow Physical Society.",institutionString:null,institution:{name:"Semenov Institute of Chemical Physics",country:{name:"Russia"}}},{id:"62389",title:"PhD.",name:"Ali Demir",middleName:null,surname:"Sezer",slug:"ali-demir-sezer",fullName:"Ali Demir Sezer",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/62389/images/3413_n.jpg",biography:"Dr. Ali Demir Sezer has a Ph.D. from Pharmaceutical Biotechnology at the Faculty of Pharmacy, University of Marmara (Turkey). He is the member of many Pharmaceutical Associations and acts as a reviewer of scientific journals and European projects under different research areas such as: drug delivery systems, nanotechnology and pharmaceutical biotechnology. Dr. Sezer is the author of many scientific publications in peer-reviewed journals and poster communications. Focus of his research activity is drug delivery, physico-chemical characterization and biological evaluation of biopolymers micro and nanoparticles as modified drug delivery system, and colloidal drug carriers (liposomes, nanoparticles etc.).",institutionString:null,institution:{name:"Marmara University",country:{name:"Turkey"}}},{id:"61051",title:"Prof.",name:"Andrea",middleName:null,surname:"Natale",slug:"andrea-natale",fullName:"Andrea Natale",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:null},{id:"100762",title:"Prof.",name:"Andrea",middleName:null,surname:"Natale",slug:"andrea-natale",fullName:"Andrea Natale",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"St David's Medical Center",country:{name:"United States of America"}}},{id:"107416",title:"Dr.",name:"Andrea",middleName:null,surname:"Natale",slug:"andrea-natale",fullName:"Andrea Natale",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Texas Cardiac Arrhythmia",country:{name:"United States of America"}}},{id:"64434",title:"Dr.",name:"Angkoon",middleName:null,surname:"Phinyomark",slug:"angkoon-phinyomark",fullName:"Angkoon Phinyomark",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/64434/images/2619_n.jpg",biography:"My name is Angkoon Phinyomark. I received a B.Eng. degree in Computer Engineering with First Class Honors in 2008 from Prince of Songkla University, Songkhla, Thailand, where I received a Ph.D. degree in Electrical Engineering. My research interests are primarily in the area of biomedical signal processing and classification notably EMG (electromyography signal), EOG (electrooculography signal), and EEG (electroencephalography signal), image analysis notably breast cancer analysis and optical coherence tomography, and rehabilitation engineering. I became a student member of IEEE in 2008. During October 2011-March 2012, I had worked at School of Computer Science and Electronic Engineering, University of Essex, Colchester, Essex, United Kingdom. In addition, during a B.Eng. I had been a visiting research student at Faculty of Computer Science, University of Murcia, Murcia, Spain for three months.\n\nI have published over 40 papers during 5 years in refereed journals, books, and conference proceedings in the areas of electro-physiological signals processing and classification, notably EMG and EOG signals, fractal analysis, wavelet analysis, texture analysis, feature extraction and machine learning algorithms, and assistive and rehabilitative devices. I have several computer programming language certificates, i.e. Sun Certified Programmer for the Java 2 Platform 1.4 (SCJP), Microsoft Certified Professional Developer, Web Developer (MCPD), Microsoft Certified Technology Specialist, .NET Framework 2.0 Web (MCTS). I am a Reviewer for several refereed journals and international conferences, such as IEEE Transactions on Biomedical Engineering, IEEE Transactions on Industrial Electronics, Optic Letters, Measurement Science Review, and also a member of the International Advisory Committee for 2012 IEEE Business Engineering and Industrial Applications and 2012 IEEE Symposium on Business, Engineering and Industrial Applications.",institutionString:null,institution:{name:"Joseph Fourier University",country:{name:"France"}}},{id:"55578",title:"Dr.",name:"Antonio",middleName:null,surname:"Jurado-Navas",slug:"antonio-jurado-navas",fullName:"Antonio Jurado-Navas",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/55578/images/4574_n.png",biography:"Antonio Jurado-Navas received the M.S. degree (2002) and the Ph.D. degree (2009) in Telecommunication Engineering, both from the University of Málaga (Spain). He first worked as a consultant at Vodafone-Spain. From 2004 to 2011, he was a Research Assistant with the Communications Engineering Department at the University of Málaga. In 2011, he became an Assistant Professor in the same department. From 2012 to 2015, he was with Ericsson Spain, where he was working on geo-location\ntools for third generation mobile networks. Since 2015, he is a Marie-Curie fellow at the Denmark Technical University. His current research interests include the areas of mobile communication systems and channel modeling in addition to atmospheric optical communications, adaptive optics and statistics",institutionString:null,institution:{name:"University of Malaga",country:{name:"Spain"}}}],filtersByRegion:[{group:"region",caption:"North America",value:1,count:5816},{group:"region",caption:"Middle and South America",value:2,count:5281},{group:"region",caption:"Africa",value:3,count:1754},{group:"region",caption:"Asia",value:4,count:10511},{group:"region",caption:"Australia and Oceania",value:5,count:906},{group:"region",caption:"Europe",value:6,count:15913}],offset:12,limit:12,total:119061},chapterEmbeded:{data:{}},editorApplication:{success:null,errors:{}},ofsBooks:{filterParams:{topicId:"1175"},books:[],filtersByTopic:[{group:"topic",caption:"Agricultural and Biological Sciences",value:5,count:26},{group:"topic",caption:"Biochemistry, Genetics and Molecular Biology",value:6,count:8},{group:"topic",caption:"Business, Management and Economics",value:7,count:3},{group:"topic",caption:"Chemistry",value:8,count:11},{group:"topic",caption:"Computer and Information Science",value:9,count:9},{group:"topic",caption:"Earth and Planetary Sciences",value:10,count:9},{group:"topic",caption:"Engineering",value:11,count:25},{group:"topic",caption:"Environmental Sciences",value:12,count:2},{group:"topic",caption:"Immunology and Microbiology",value:13,count:4},{group:"topic",caption:"Materials Science",value:14,count:7},{group:"topic",caption:"Mathematics",value:15,count:2},{group:"topic",caption:"Medicine",value:16,count:45},{group:"topic",caption:"Neuroscience",value:18,count:3},{group:"topic",caption:"Pharmacology, Toxicology and Pharmaceutical Science",value:19,count:3},{group:"topic",caption:"Physics",value:20,count:4},{group:"topic",caption:"Psychology",value:21,count:4},{group:"topic",caption:"Robotics",value:22,count:1},{group:"topic",caption:"Social Sciences",value:23,count:3},{group:"topic",caption:"Technology",value:24,count:1},{group:"topic",caption:"Veterinary Medicine and Science",value:25,count:2}],offset:12,limit:12,total:0},popularBooks:{featuredBooks:[{type:"book",id:"8472",title:"Bioactive Compounds in Nutraceutical and Functional Food for Good Human Health",subtitle:null,isOpenForSubmission:!1,hash:"8855452919b8495810ef8e88641feb20",slug:"bioactive-compounds-in-nutraceutical-and-functional-food-for-good-human-health",bookSignature:"Kavita Sharma, Kanchan Mishra, Kula Kamal Senapati and Corina Danciu",coverURL:"https://cdn.intechopen.com/books/images_new/8472.jpg",editors:[{id:"197731",title:"Dr.",name:"Kavita",middleName:null,surname:"Sharma",slug:"kavita-sharma",fullName:"Kavita Sharma"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9685",title:"Agroecosystems",subtitle:"Very Complex Environmental Systems",isOpenForSubmission:!1,hash:"c44f7b43a9f9610c243dc32300d37df6",slug:"agroecosystems-very-complex-environmental-systems",bookSignature:"Marcelo L. Larramendy and Sonia Soloneski",coverURL:"https://cdn.intechopen.com/books/images_new/9685.jpg",editors:[{id:"14764",title:"Dr.",name:"Marcelo L.",middleName:null,surname:"Larramendy",slug:"marcelo-l.-larramendy",fullName:"Marcelo L. Larramendy"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8564",title:"Cell Interaction",subtitle:"Molecular and Immunological Basis for Disease Management",isOpenForSubmission:!1,hash:"98d7f080d80524285f091e72a8e92a6d",slug:"cell-interaction-molecular-and-immunological-basis-for-disease-management",bookSignature:"Bhawana Singh",coverURL:"https://cdn.intechopen.com/books/images_new/8564.jpg",editors:[{id:"315192",title:"Dr.",name:"Bhawana",middleName:null,surname:"Singh",slug:"bhawana-singh",fullName:"Bhawana Singh"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9629",title:"Electroencephalography",subtitle:"From Basic Research to Clinical Applications",isOpenForSubmission:!1,hash:"8147834b6c6deeeec40f407c71ad60b4",slug:"electroencephalography-from-basic-research-to-clinical-applications",bookSignature:"Hideki Nakano",coverURL:"https://cdn.intechopen.com/books/images_new/9629.jpg",editors:[{id:"196461",title:"Prof.",name:"Hideki",middleName:null,surname:"Nakano",slug:"hideki-nakano",fullName:"Hideki Nakano"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8760",title:"Structure Topology and Symplectic Geometry",subtitle:null,isOpenForSubmission:!1,hash:"8974840985ec3652492c83e20233bf02",slug:"structure-topology-and-symplectic-geometry",bookSignature:"Kamal Shah and Min Lei",coverURL:"https://cdn.intechopen.com/books/images_new/8760.jpg",editors:[{id:"231748",title:"Dr.",name:"Kamal",middleName:null,surname:"Shah",slug:"kamal-shah",fullName:"Kamal Shah"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9161",title:"Frailty in the Elderly",subtitle:"Understanding and Managing Complexity",isOpenForSubmission:!1,hash:"a4f0f2fade8fb8ba35c405f5ad31a823",slug:"frailty-in-the-elderly-understanding-and-managing-complexity",bookSignature:"Sara Palermo",coverURL:"https://cdn.intechopen.com/books/images_new/9161.jpg",editors:[{id:"233998",title:"Ph.D.",name:"Sara",middleName:null,surname:"Palermo",slug:"sara-palermo",fullName:"Sara Palermo"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8445",title:"Dam Engineering",subtitle:"Recent Advances in Design and Analysis",isOpenForSubmission:!1,hash:"a7e4d2ecbc65d78fa7582e0d2e143906",slug:"dam-engineering-recent-advances-in-design-and-analysis",bookSignature:"Zhongzhi Fu and Erich Bauer",coverURL:"https://cdn.intechopen.com/books/images_new/8445.jpg",editors:[{id:"249577",title:"Dr.",name:"Zhongzhi",middleName:null,surname:"Fu",slug:"zhongzhi-fu",fullName:"Zhongzhi Fu"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9385",title:"Renewable Energy",subtitle:"Technologies and Applications",isOpenForSubmission:!1,hash:"a6b446d19166f17f313008e6c056f3d8",slug:"renewable-energy-technologies-and-applications",bookSignature:"Tolga Taner, Archana Tiwari and Taha Selim Ustun",coverURL:"https://cdn.intechopen.com/books/images_new/9385.jpg",editors:[{id:"197240",title:"Associate Prof.",name:"Tolga",middleName:null,surname:"Taner",slug:"tolga-taner",fullName:"Tolga Taner"}],equalEditorOne:{id:"186791",title:"Dr.",name:"Archana",middleName:null,surname:"Tiwari",slug:"archana-tiwari",fullName:"Archana Tiwari",profilePictureURL:"https://mts.intechopen.com/storage/users/186791/images/system/186791.jpg",biography:"Dr. Archana Tiwari is Associate Professor at Amity University, India. Her research interests include renewable sources of energy from microalgae and further utilizing the residual biomass for the generation of value-added products, bioremediation through microalgae and microbial consortium, antioxidative enzymes and stress, and nutraceuticals from microalgae. She has been working on algal biotechnology for the last two decades. She has published her research in many international journals and has authored many books and chapters with renowned publishing houses. She has also delivered talks as an invited speaker at many national and international conferences. Dr. Tiwari is the recipient of several awards including Researcher of the Year and Distinguished Scientist.",institutionString:"Amity University",position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"3",totalChapterViews:"0",totalEditedBooks:"1",institution:{name:"Amity University",institutionURL:null,country:{name:"India"}}},equalEditorTwo:{id:"197609",title:"Prof.",name:"Taha Selim",middleName:null,surname:"Ustun",slug:"taha-selim-ustun",fullName:"Taha Selim Ustun",profilePictureURL:"https://mts.intechopen.com/storage/users/197609/images/system/197609.jpeg",biography:"Dr. Taha Selim Ustun received a Ph.D. in Electrical Engineering from Victoria University, Melbourne, Australia. He is a researcher with the Fukushima Renewable Energy Institute, AIST (FREA), where he leads the Smart Grid Cybersecurity Laboratory. Prior to that, he was a faculty member with the School of Electrical and Computer Engineering, Carnegie Mellon University, Pittsburgh, PA, USA. His current research interests include power systems protection, communication in power networks, distributed generation, microgrids, electric vehicle integration, and cybersecurity in smart grids. He serves on the editorial boards of IEEE Access, IEEE Transactions on Industrial Informatics, Energies, Electronics, Electricity, World Electric Vehicle and Information journals. Dr. Ustun is a member of the IEEE 2004 and 2800, IEC Renewable Energy Management WG 8, and IEC TC 57 WG17. He has been invited to run specialist courses in Africa, India, and China. He has delivered talks for the Qatar Foundation, the World Energy Council, the Waterloo Global Science Initiative, and the European Union Energy Initiative (EUEI). His research has attracted funding from prestigious programs in Japan, Australia, the European Union, and North America.",institutionString:"Fukushima Renewable Energy Institute, AIST (FREA)",position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"1",totalChapterViews:"0",totalEditedBooks:"0",institution:{name:"National Institute of Advanced Industrial Science and Technology",institutionURL:null,country:{name:"Japan"}}},equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8937",title:"Soil Moisture Importance",subtitle:null,isOpenForSubmission:!1,hash:"3951728ace7f135451d66b72e9908b47",slug:"soil-moisture-importance",bookSignature:"Ram Swaroop Meena and Rahul Datta",coverURL:"https://cdn.intechopen.com/books/images_new/8937.jpg",editors:[{id:"313528",title:"Associate Prof.",name:"Ram Swaroop",middleName:null,surname:"Meena",slug:"ram-swaroop-meena",fullName:"Ram Swaroop Meena"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"7031",title:"Liver Pathology",subtitle:null,isOpenForSubmission:!1,hash:"631321b0565459ed0175917f1c8c727f",slug:"liver-pathology",bookSignature:"Vijay Gayam and Omer Engin",coverURL:"https://cdn.intechopen.com/books/images_new/7031.jpg",editors:[{id:"273100",title:"Dr.",name:"Vijay",middleName:null,surname:"Gayam",slug:"vijay-gayam",fullName:"Vijay Gayam"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8158",title:"Veganism",subtitle:"a Fashion Trend or Food as a Medicine",isOpenForSubmission:!1,hash:"d8e51fc25a379e5b92a270addbb4351d",slug:"veganism-a-fashion-trend-or-food-as-a-medicine",bookSignature:"Miljana Z. Jovandaric",coverURL:"https://cdn.intechopen.com/books/images_new/8158.jpg",editors:[{id:"268043",title:"Dr.",name:"Miljana Z.",middleName:"Z",surname:"Jovandaric",slug:"miljana-z.-jovandaric",fullName:"Miljana Z. Jovandaric"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"2160",title:"MATLAB",subtitle:"A Fundamental Tool for Scientific Computing and Engineering Applications - Volume 1",isOpenForSubmission:!1,hash:"dd9c658341fbd264ed4f8d9e6aa8ca29",slug:"matlab-a-fundamental-tool-for-scientific-computing-and-engineering-applications-volume-1",bookSignature:"Vasilios N. Katsikis",coverURL:"https://cdn.intechopen.com/books/images_new/2160.jpg",editors:[{id:"12289",title:"Prof.",name:"Vasilios",middleName:"N.",surname:"Katsikis",slug:"vasilios-katsikis",fullName:"Vasilios Katsikis"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}}],offset:12,limit:12,total:5315},hotBookTopics:{hotBooks:[],offset:0,limit:12,total:null},publish:{},publishingProposal:{success:null,errors:{}},books:{featuredBooks:[{type:"book",id:"8472",title:"Bioactive Compounds in Nutraceutical and Functional Food for Good Human Health",subtitle:null,isOpenForSubmission:!1,hash:"8855452919b8495810ef8e88641feb20",slug:"bioactive-compounds-in-nutraceutical-and-functional-food-for-good-human-health",bookSignature:"Kavita Sharma, Kanchan Mishra, Kula Kamal Senapati and Corina Danciu",coverURL:"https://cdn.intechopen.com/books/images_new/8472.jpg",editors:[{id:"197731",title:"Dr.",name:"Kavita",middleName:null,surname:"Sharma",slug:"kavita-sharma",fullName:"Kavita Sharma"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9685",title:"Agroecosystems",subtitle:"Very Complex Environmental Systems",isOpenForSubmission:!1,hash:"c44f7b43a9f9610c243dc32300d37df6",slug:"agroecosystems-very-complex-environmental-systems",bookSignature:"Marcelo L. Larramendy and Sonia Soloneski",coverURL:"https://cdn.intechopen.com/books/images_new/9685.jpg",editors:[{id:"14764",title:"Dr.",name:"Marcelo L.",middleName:null,surname:"Larramendy",slug:"marcelo-l.-larramendy",fullName:"Marcelo L. Larramendy"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8564",title:"Cell Interaction",subtitle:"Molecular and Immunological Basis for Disease Management",isOpenForSubmission:!1,hash:"98d7f080d80524285f091e72a8e92a6d",slug:"cell-interaction-molecular-and-immunological-basis-for-disease-management",bookSignature:"Bhawana Singh",coverURL:"https://cdn.intechopen.com/books/images_new/8564.jpg",editors:[{id:"315192",title:"Dr.",name:"Bhawana",middleName:null,surname:"Singh",slug:"bhawana-singh",fullName:"Bhawana Singh"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9629",title:"Electroencephalography",subtitle:"From Basic Research to Clinical Applications",isOpenForSubmission:!1,hash:"8147834b6c6deeeec40f407c71ad60b4",slug:"electroencephalography-from-basic-research-to-clinical-applications",bookSignature:"Hideki Nakano",coverURL:"https://cdn.intechopen.com/books/images_new/9629.jpg",editors:[{id:"196461",title:"Prof.",name:"Hideki",middleName:null,surname:"Nakano",slug:"hideki-nakano",fullName:"Hideki Nakano"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8760",title:"Structure Topology and Symplectic Geometry",subtitle:null,isOpenForSubmission:!1,hash:"8974840985ec3652492c83e20233bf02",slug:"structure-topology-and-symplectic-geometry",bookSignature:"Kamal Shah and Min Lei",coverURL:"https://cdn.intechopen.com/books/images_new/8760.jpg",editors:[{id:"231748",title:"Dr.",name:"Kamal",middleName:null,surname:"Shah",slug:"kamal-shah",fullName:"Kamal Shah"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9161",title:"Frailty in the Elderly",subtitle:"Understanding and Managing Complexity",isOpenForSubmission:!1,hash:"a4f0f2fade8fb8ba35c405f5ad31a823",slug:"frailty-in-the-elderly-understanding-and-managing-complexity",bookSignature:"Sara Palermo",coverURL:"https://cdn.intechopen.com/books/images_new/9161.jpg",editors:[{id:"233998",title:"Ph.D.",name:"Sara",middleName:null,surname:"Palermo",slug:"sara-palermo",fullName:"Sara Palermo"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8445",title:"Dam Engineering",subtitle:"Recent Advances in Design and Analysis",isOpenForSubmission:!1,hash:"a7e4d2ecbc65d78fa7582e0d2e143906",slug:"dam-engineering-recent-advances-in-design-and-analysis",bookSignature:"Zhongzhi Fu and Erich Bauer",coverURL:"https://cdn.intechopen.com/books/images_new/8445.jpg",editors:[{id:"249577",title:"Dr.",name:"Zhongzhi",middleName:null,surname:"Fu",slug:"zhongzhi-fu",fullName:"Zhongzhi Fu"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"9385",title:"Renewable Energy",subtitle:"Technologies and Applications",isOpenForSubmission:!1,hash:"a6b446d19166f17f313008e6c056f3d8",slug:"renewable-energy-technologies-and-applications",bookSignature:"Tolga Taner, Archana Tiwari and Taha Selim Ustun",coverURL:"https://cdn.intechopen.com/books/images_new/9385.jpg",editors:[{id:"197240",title:"Associate Prof.",name:"Tolga",middleName:null,surname:"Taner",slug:"tolga-taner",fullName:"Tolga Taner"}],equalEditorOne:{id:"186791",title:"Dr.",name:"Archana",middleName:null,surname:"Tiwari",slug:"archana-tiwari",fullName:"Archana Tiwari",profilePictureURL:"https://mts.intechopen.com/storage/users/186791/images/system/186791.jpg",biography:"Dr. Archana Tiwari is Associate Professor at Amity University, India. Her research interests include renewable sources of energy from microalgae and further utilizing the residual biomass for the generation of value-added products, bioremediation through microalgae and microbial consortium, antioxidative enzymes and stress, and nutraceuticals from microalgae. She has been working on algal biotechnology for the last two decades. She has published her research in many international journals and has authored many books and chapters with renowned publishing houses. She has also delivered talks as an invited speaker at many national and international conferences. Dr. Tiwari is the recipient of several awards including Researcher of the Year and Distinguished Scientist.",institutionString:"Amity University",position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"3",totalChapterViews:"0",totalEditedBooks:"1",institution:{name:"Amity University",institutionURL:null,country:{name:"India"}}},equalEditorTwo:{id:"197609",title:"Prof.",name:"Taha Selim",middleName:null,surname:"Ustun",slug:"taha-selim-ustun",fullName:"Taha Selim Ustun",profilePictureURL:"https://mts.intechopen.com/storage/users/197609/images/system/197609.jpeg",biography:"Dr. Taha Selim Ustun received a Ph.D. in Electrical Engineering from Victoria University, Melbourne, Australia. He is a researcher with the Fukushima Renewable Energy Institute, AIST (FREA), where he leads the Smart Grid Cybersecurity Laboratory. Prior to that, he was a faculty member with the School of Electrical and Computer Engineering, Carnegie Mellon University, Pittsburgh, PA, USA. His current research interests include power systems protection, communication in power networks, distributed generation, microgrids, electric vehicle integration, and cybersecurity in smart grids. He serves on the editorial boards of IEEE Access, IEEE Transactions on Industrial Informatics, Energies, Electronics, Electricity, World Electric Vehicle and Information journals. Dr. Ustun is a member of the IEEE 2004 and 2800, IEC Renewable Energy Management WG 8, and IEC TC 57 WG17. He has been invited to run specialist courses in Africa, India, and China. He has delivered talks for the Qatar Foundation, the World Energy Council, the Waterloo Global Science Initiative, and the European Union Energy Initiative (EUEI). His research has attracted funding from prestigious programs in Japan, Australia, the European Union, and North America.",institutionString:"Fukushima Renewable Energy Institute, AIST (FREA)",position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"1",totalChapterViews:"0",totalEditedBooks:"0",institution:{name:"National Institute of Advanced Industrial Science and Technology",institutionURL:null,country:{name:"Japan"}}},equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"8937",title:"Soil Moisture Importance",subtitle:null,isOpenForSubmission:!1,hash:"3951728ace7f135451d66b72e9908b47",slug:"soil-moisture-importance",bookSignature:"Ram Swaroop Meena and Rahul Datta",coverURL:"https://cdn.intechopen.com/books/images_new/8937.jpg",editors:[{id:"313528",title:"Associate Prof.",name:"Ram Swaroop",middleName:null,surname:"Meena",slug:"ram-swaroop-meena",fullName:"Ram Swaroop Meena"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}},{type:"book",id:"7031",title:"Liver Pathology",subtitle:null,isOpenForSubmission:!1,hash:"631321b0565459ed0175917f1c8c727f",slug:"liver-pathology",bookSignature:"Vijay Gayam and Omer Engin",coverURL:"https://cdn.intechopen.com/books/images_new/7031.jpg",editors:[{id:"273100",title:"Dr.",name:"Vijay",middleName:null,surname:"Gayam",slug:"vijay-gayam",fullName:"Vijay Gayam"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}}],latestBooks:[{type:"book",id:"8472",title:"Bioactive Compounds in Nutraceutical and Functional Food for Good Human Health",subtitle:null,isOpenForSubmission:!1,hash:"8855452919b8495810ef8e88641feb20",slug:"bioactive-compounds-in-nutraceutical-and-functional-food-for-good-human-health",bookSignature:"Kavita Sharma, Kanchan Mishra, Kula Kamal Senapati and Corina Danciu",coverURL:"https://cdn.intechopen.com/books/images_new/8472.jpg",editedByType:"Edited by",editors:[{id:"197731",title:"Dr.",name:"Kavita",middleName:null,surname:"Sharma",slug:"kavita-sharma",fullName:"Kavita Sharma"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"8760",title:"Structure Topology and Symplectic Geometry",subtitle:null,isOpenForSubmission:!1,hash:"8974840985ec3652492c83e20233bf02",slug:"structure-topology-and-symplectic-geometry",bookSignature:"Kamal Shah and Min Lei",coverURL:"https://cdn.intechopen.com/books/images_new/8760.jpg",editedByType:"Edited by",editors:[{id:"231748",title:"Dr.",name:"Kamal",middleName:null,surname:"Shah",slug:"kamal-shah",fullName:"Kamal Shah"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9536",title:"Education at the Intersection of Globalization and Technology",subtitle:null,isOpenForSubmission:!1,hash:"0cf6891060eb438d975d250e8b127ed6",slug:"education-at-the-intersection-of-globalization-and-technology",bookSignature:"Sharon Waller, Lee Waller, Vongai Mpofu and Mercy Kurebwa",coverURL:"https://cdn.intechopen.com/books/images_new/9536.jpg",editedByType:"Edited by",editors:[{id:"263302",title:"Dr.",name:"Sharon",middleName:null,surname:"Waller",slug:"sharon-waller",fullName:"Sharon Waller"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"8564",title:"Cell Interaction",subtitle:"Molecular and Immunological Basis for Disease Management",isOpenForSubmission:!1,hash:"98d7f080d80524285f091e72a8e92a6d",slug:"cell-interaction-molecular-and-immunological-basis-for-disease-management",bookSignature:"Bhawana Singh",coverURL:"https://cdn.intechopen.com/books/images_new/8564.jpg",editedByType:"Edited by",editors:[{id:"315192",title:"Dr.",name:"Bhawana",middleName:null,surname:"Singh",slug:"bhawana-singh",fullName:"Bhawana Singh"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9629",title:"Electroencephalography",subtitle:"From Basic Research to Clinical Applications",isOpenForSubmission:!1,hash:"8147834b6c6deeeec40f407c71ad60b4",slug:"electroencephalography-from-basic-research-to-clinical-applications",bookSignature:"Hideki Nakano",coverURL:"https://cdn.intechopen.com/books/images_new/9629.jpg",editedByType:"Edited by",editors:[{id:"196461",title:"Prof.",name:"Hideki",middleName:null,surname:"Nakano",slug:"hideki-nakano",fullName:"Hideki Nakano"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9685",title:"Agroecosystems",subtitle:"Very Complex Environmental Systems",isOpenForSubmission:!1,hash:"c44f7b43a9f9610c243dc32300d37df6",slug:"agroecosystems-very-complex-environmental-systems",bookSignature:"Marcelo L. Larramendy and Sonia Soloneski",coverURL:"https://cdn.intechopen.com/books/images_new/9685.jpg",editedByType:"Edited by",editors:[{id:"14764",title:"Dr.",name:"Marcelo L.",middleName:null,surname:"Larramendy",slug:"marcelo-l.-larramendy",fullName:"Marcelo L. Larramendy"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9524",title:"Organ Donation and Transplantation",subtitle:null,isOpenForSubmission:!1,hash:"6ef47e03cd4e6476946fc28ca51de825",slug:"organ-donation-and-transplantation",bookSignature:"Vassil Mihaylov",coverURL:"https://cdn.intechopen.com/books/images_new/9524.jpg",editedByType:"Edited by",editors:[{id:"313113",title:"Associate Prof.",name:"Vassil",middleName:null,surname:"Mihaylov",slug:"vassil-mihaylov",fullName:"Vassil Mihaylov"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9280",title:"Underwater Work",subtitle:null,isOpenForSubmission:!1,hash:"647b4270d937deae4a82f5702d1959ec",slug:"underwater-work",bookSignature:"Sérgio António Neves Lousada",coverURL:"https://cdn.intechopen.com/books/images_new/9280.jpg",editedByType:"Edited by",editors:[{id:"248645",title:"Dr.",name:"Sérgio António",middleName:null,surname:"Neves Lousada",slug:"sergio-antonio-neves-lousada",fullName:"Sérgio António Neves Lousada"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9161",title:"Frailty in the Elderly",subtitle:"Understanding and Managing Complexity",isOpenForSubmission:!1,hash:"a4f0f2fade8fb8ba35c405f5ad31a823",slug:"frailty-in-the-elderly-understanding-and-managing-complexity",bookSignature:"Sara Palermo",coverURL:"https://cdn.intechopen.com/books/images_new/9161.jpg",editedByType:"Edited by",editors:[{id:"233998",title:"Ph.D.",name:"Sara",middleName:null,surname:"Palermo",slug:"sara-palermo",fullName:"Sara Palermo"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"8158",title:"Veganism",subtitle:"a Fashion Trend or Food as a Medicine",isOpenForSubmission:!1,hash:"d8e51fc25a379e5b92a270addbb4351d",slug:"veganism-a-fashion-trend-or-food-as-a-medicine",bookSignature:"Miljana Z. Jovandaric",coverURL:"https://cdn.intechopen.com/books/images_new/8158.jpg",editedByType:"Edited by",editors:[{id:"268043",title:"Dr.",name:"Miljana Z.",middleName:"Z",surname:"Jovandaric",slug:"miljana-z.-jovandaric",fullName:"Miljana Z. Jovandaric"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}]},subject:{topic:{id:"637",title:"Spatial Analysis",slug:"spatial-analysis",parent:{title:"Geography",slug:"geography"},numberOfBooks:7,numberOfAuthorsAndEditors:184,numberOfWosCitations:13,numberOfCrossrefCitations:34,numberOfDimensionsCitations:62,videoUrl:null,fallbackUrl:null,description:null},booksByTopicFilter:{topicSlug:"spatial-analysis",sort:"-publishedDate",limit:12,offset:0},booksByTopicCollection:[{type:"book",id:"9381",title:"Geographic Information Systems in Geospatial Intelligence",subtitle:null,isOpenForSubmission:!1,hash:"069b444029eceaad8ff557eca7bd713e",slug:"geographic-information-systems-in-geospatial-intelligence",bookSignature:"Rustam B. Rustamov",coverURL:"https://cdn.intechopen.com/books/images_new/9381.jpg",editedByType:"Edited by",editors:[{id:"59174",title:"Dr.",name:"Rustam B.",middleName:null,surname:"Rustamov",slug:"rustam-b.-rustamov",fullName:"Rustam B. Rustamov"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9846",title:"Spatial Variability in Environmental Science",subtitle:"Patterns, Processes, and Analyses",isOpenForSubmission:!1,hash:"cfa4fa7b982bbff46ffbe6fbdbffbdf1",slug:"spatial-variability-in-environmental-science-patterns-processes-and-analyses",bookSignature:"John P. Tiefenbacher and Davod Poreh",coverURL:"https://cdn.intechopen.com/books/images_new/9846.jpg",editedByType:"Edited by",editors:[{id:"73876",title:"Dr.",name:"John P.",middleName:null,surname:"Tiefenbacher",slug:"john-p.-tiefenbacher",fullName:"John P. Tiefenbacher"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9246",title:"Satellites Missions and Technologies for Geosciences",subtitle:null,isOpenForSubmission:!1,hash:"f23d04613b089dae40f81342c3e7c7f4",slug:"satellites-missions-and-technologies-for-geosciences",bookSignature:"Vladislav Demyanov and Jonathan Becedas",coverURL:"https://cdn.intechopen.com/books/images_new/9246.jpg",editedByType:"Edited by",editors:[{id:"154597",title:"Prof.",name:"Vladislav",middleName:null,surname:"Demyanov",slug:"vladislav-demyanov",fullName:"Vladislav Demyanov"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"7304",title:"Geospatial Analyses of Earth Observation (EO) data",subtitle:null,isOpenForSubmission:!1,hash:"e90c7cda0e7f94a6620d6ec83db808ae",slug:"geospatial-analyses-of-earth-observation-eo-data",bookSignature:"Antonio Pepe and Qing Zhao",coverURL:"https://cdn.intechopen.com/books/images_new/7304.jpg",editedByType:"Edited by",editors:[{id:"99269",title:"Dr.",name:"Antonio",middleName:null,surname:"Pepe",slug:"antonio-pepe",fullName:"Antonio Pepe"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"7362",title:"Geographic Information Systems and Science",subtitle:null,isOpenForSubmission:!1,hash:"b0ac3aa0063d6a10dd3fe90ff78cddd7",slug:"geographic-information-systems-and-science",bookSignature:"Jorge Rocha and Patrícia Abrantes",coverURL:"https://cdn.intechopen.com/books/images_new/7362.jpg",editedByType:"Edited by",editors:[{id:"145918",title:"Ph.D.",name:"Jorge",middleName:null,surname:"Rocha",slug:"jorge-rocha",fullName:"Jorge Rocha"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"7262",title:"Spatial Analysis, Modelling and Planning",subtitle:null,isOpenForSubmission:!1,hash:"ed7c7f4193e3951e715569ca454f7077",slug:"spatial-analysis-modelling-and-planning",bookSignature:"Jorge Rocha and José António Tenedório",coverURL:"https://cdn.intechopen.com/books/images_new/7262.jpg",editedByType:"Edited by",editors:[{id:"145918",title:"Ph.D.",name:"Jorge",middleName:null,surname:"Rocha",slug:"jorge-rocha",fullName:"Jorge Rocha"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"5241",title:"Applications of Spatial Statistics",subtitle:null,isOpenForSubmission:!1,hash:"acc5941907640ecc7a3e350c5fe3df19",slug:"applications-of-spatial-statistics",bookSignature:"Ming-Chih Hung",coverURL:"https://cdn.intechopen.com/books/images_new/5241.jpg",editedByType:"Edited by",editors:[{id:"184413",title:"Dr.",name:"Ming",middleName:"Chih",surname:"Hung",slug:"ming-hung",fullName:"Ming Hung"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}],booksByTopicTotal:7,mostCitedChapters:[{id:"52704",doi:"10.5772/65996",title:"Comparison of Spatial Interpolation Techniques Using Visualization and Quantitative Assessment",slug:"comparison-of-spatial-interpolation-techniques-using-visualization-and-quantitative-assessment",totalDownloads:2573,totalCrossrefCites:5,totalDimensionsCites:9,book:{slug:"applications-of-spatial-statistics",title:"Applications of Spatial Statistics",fullTitle:"Applications of Spatial Statistics"},signatures:"Yi-Hwa (Eva) Wu and Ming-Chih Hung",authors:[{id:"181853",title:"Dr.",name:"Yi-Hwa",middleName:null,surname:"Wu",slug:"yi-hwa-wu",fullName:"Yi-Hwa Wu"}]},{id:"69962",doi:"10.5772/intechopen.90039",title:"Nanosatellites and Applications to Commercial and Scientific Missions",slug:"nanosatellites-and-applications-to-commercial-and-scientific-missions",totalDownloads:805,totalCrossrefCites:3,totalDimensionsCites:8,book:{slug:"satellites-missions-and-technologies-for-geosciences",title:"Satellites Missions and Technologies for Geosciences",fullTitle:"Satellites Missions and Technologies for Geosciences"},signatures:"Adriano Camps",authors:[{id:"299991",title:"Prof.",name:"Adriano",middleName:null,surname:"Camps",slug:"adriano-camps",fullName:"Adriano Camps"}]},{id:"67619",doi:"10.5772/intechopen.86109",title:"Application of Topographic Analyses for Mapping Spatial Patterns of Soil Properties",slug:"application-of-topographic-analyses-for-mapping-spatial-patterns-of-soil-properties",totalDownloads:754,totalCrossrefCites:4,totalDimensionsCites:4,book:{slug:"geospatial-analyses-of-earth-observation-eo-data",title:"Geospatial Analyses of Earth Observation (EO) data",fullTitle:"Geospatial Analyses of Earth Observation (EO) data"},signatures:"Xia Li and Gregory W. McCarty",authors:[{id:"55106",title:"Dr.",name:"Gregory",middleName:null,surname:"McCarty",slug:"gregory-mccarty",fullName:"Gregory McCarty"},{id:"286359",title:"Dr.",name:"Xia",middleName:null,surname:"Li",slug:"xia-li",fullName:"Xia Li"}]}],mostDownloadedChaptersLast30Days:[{id:"52704",title:"Comparison of Spatial Interpolation Techniques Using Visualization and Quantitative Assessment",slug:"comparison-of-spatial-interpolation-techniques-using-visualization-and-quantitative-assessment",totalDownloads:2574,totalCrossrefCites:5,totalDimensionsCites:9,book:{slug:"applications-of-spatial-statistics",title:"Applications of Spatial Statistics",fullTitle:"Applications of Spatial Statistics"},signatures:"Yi-Hwa (Eva) Wu and Ming-Chih Hung",authors:[{id:"181853",title:"Dr.",name:"Yi-Hwa",middleName:null,surname:"Wu",slug:"yi-hwa-wu",fullName:"Yi-Hwa Wu"}]},{id:"63765",title:"Introductory Chapter: Spatial Analysis, Modelling, and Planning",slug:"introductory-chapter-spatial-analysis-modelling-and-planning",totalDownloads:2234,totalCrossrefCites:0,totalDimensionsCites:2,book:{slug:"spatial-analysis-modelling-and-planning",title:"Spatial Analysis, Modelling and Planning",fullTitle:"Spatial Analysis, Modelling and Planning"},signatures:"José António Tenedório and Jorge Rocha",authors:[{id:"145918",title:"Ph.D.",name:"Jorge",middleName:null,surname:"Rocha",slug:"jorge-rocha",fullName:"Jorge Rocha"},{id:"242032",title:"Dr.",name:"José António",middleName:null,surname:"Tenedório",slug:"jose-antonio-tenedorio",fullName:"José António Tenedório"}]},{id:"64204",title:"GIS and Remote Sensing for Mangroves Mapping and Monitoring",slug:"gis-and-remote-sensing-for-mangroves-mapping-and-monitoring",totalDownloads:1548,totalCrossrefCites:2,totalDimensionsCites:3,book:{slug:"geographic-information-systems-and-science",title:"Geographic Information Systems and Science",fullTitle:"Geographic Information Systems and Science"},signatures:"Hamdan Omar, Muhamad Afizzul Misman and Samsudin Musa",authors:[{id:"264176",title:"Dr.",name:"Hamdan",middleName:null,surname:"Omar",slug:"hamdan-omar",fullName:"Hamdan Omar"},{id:"272549",title:"Mr.",name:"Muhamad Afizzul",middleName:null,surname:"Misman",slug:"muhamad-afizzul-misman",fullName:"Muhamad Afizzul Misman"},{id:"272550",title:"Dr.",name:"Samsudin",middleName:null,surname:"Musa",slug:"samsudin-musa",fullName:"Samsudin Musa"}]},{id:"67895",title:"The Impact of Land Use and Land Cover Changes on the Nkula Dam in the Middle Shire River Catchment, Malawi",slug:"the-impact-of-land-use-and-land-cover-changes-on-the-nkula-dam-in-the-middle-shire-river-catchment-m",totalDownloads:653,totalCrossrefCites:0,totalDimensionsCites:0,book:{slug:"geospatial-analyses-of-earth-observation-eo-data",title:"Geospatial Analyses of Earth Observation (EO) data",fullTitle:"Geospatial Analyses of Earth Observation (EO) data"},signatures:"Maureen Kapute Mzuza, Weiguo Zhang, Fanuel Kapute and Xiaodao Wei",authors:[{id:"286469",title:"Dr.",name:"Maureen",middleName:null,surname:"Kapute Mzuza",slug:"maureen-kapute-mzuza",fullName:"Maureen Kapute Mzuza"},{id:"288469",title:"Prof.",name:"Weiguo",middleName:null,surname:"Zhang",slug:"weiguo-zhang",fullName:"Weiguo Zhang"},{id:"288470",title:"Prof.",name:"Fanuel",middleName:null,surname:"Kapute",slug:"fanuel-kapute",fullName:"Fanuel Kapute"},{id:"288471",title:"Mr.",name:"Xiaodao",middleName:null,surname:"Wei",slug:"xiaodao-wei",fullName:"Xiaodao Wei"}]},{id:"64243",title:"GIS and Big Data Visualization",slug:"gis-and-big-data-visualization",totalDownloads:1134,totalCrossrefCites:1,totalDimensionsCites:1,book:{slug:"geographic-information-systems-and-science",title:"Geographic Information Systems and Science",fullTitle:"Geographic Information Systems and Science"},signatures:"Junghoon Ki",authors:[{id:"271241",title:"Prof.",name:"Junghoon",middleName:null,surname:"Ki",slug:"junghoon-ki",fullName:"Junghoon Ki"}]},{id:"69962",title:"Nanosatellites and Applications to Commercial and Scientific Missions",slug:"nanosatellites-and-applications-to-commercial-and-scientific-missions",totalDownloads:806,totalCrossrefCites:3,totalDimensionsCites:8,book:{slug:"satellites-missions-and-technologies-for-geosciences",title:"Satellites Missions and Technologies for Geosciences",fullTitle:"Satellites Missions and Technologies for Geosciences"},signatures:"Adriano Camps",authors:[{id:"299991",title:"Prof.",name:"Adriano",middleName:null,surname:"Camps",slug:"adriano-camps",fullName:"Adriano Camps"}]},{id:"66971",title:"Introductory Chapter: Geographic Information Systems and Science",slug:"introductory-chapter-geographic-information-systems-and-science",totalDownloads:487,totalCrossrefCites:0,totalDimensionsCites:0,book:{slug:"geographic-information-systems-and-science",title:"Geographic Information Systems and Science",fullTitle:"Geographic Information Systems and Science"},signatures:"Cláudia M. Viana, Patrícia Abrantes and Jorge Rocha",authors:[{id:"145918",title:"Ph.D.",name:"Jorge",middleName:null,surname:"Rocha",slug:"jorge-rocha",fullName:"Jorge Rocha"},{id:"149241",title:"Prof.",name:"Patricia",middleName:null,surname:"Abrantes",slug:"patricia-abrantes",fullName:"Patricia Abrantes"},{id:"192917",title:"Dr.",name:"Cláudia",middleName:"Morais",surname:"Viana",slug:"claudia-viana",fullName:"Cláudia Viana"}]},{id:"67603",title:"The Color of Water from Space: A Case Study for Italian Lakes from Sentinel-2",slug:"the-color-of-water-from-space-a-case-study-for-italian-lakes-from-sentinel-2",totalDownloads:501,totalCrossrefCites:3,totalDimensionsCites:3,book:{slug:"geospatial-analyses-of-earth-observation-eo-data",title:"Geospatial Analyses of Earth Observation (EO) data",fullTitle:"Geospatial Analyses of Earth Observation (EO) data"},signatures:"Claudia Giardino, Kerttu-Liis Kõks, Rossano Bolpagni, Giulia Luciani, Gabriele Candiani, Moritz K. Lehmann, Hendrik Jan Van der Woerd and Mariano Bresciani",authors:[{id:"292340",title:"Dr.",name:"Claudia",middleName:null,surname:"Giardino",slug:"claudia-giardino",fullName:"Claudia Giardino"},{id:"300416",title:"Ms.",name:"Kerttu-Liis",middleName:null,surname:"Kõks",slug:"kerttu-liis-koks",fullName:"Kerttu-Liis Kõks"},{id:"300418",title:"Dr.",name:"Rossano",middleName:null,surname:"Bolpagni",slug:"rossano-bolpagni",fullName:"Rossano Bolpagni"},{id:"300419",title:"Dr.",name:"Giulia",middleName:null,surname:"Luciani",slug:"giulia-luciani",fullName:"Giulia Luciani"},{id:"300420",title:"Dr.",name:"Gabriele",middleName:null,surname:"Candiani",slug:"gabriele-candiani",fullName:"Gabriele Candiani"},{id:"300421",title:"Dr.",name:"Moritz K.",middleName:null,surname:"Lehmann",slug:"moritz-k.-lehmann",fullName:"Moritz K. Lehmann"},{id:"300423",title:"Dr.",name:"Mariano",middleName:null,surname:"Bresciani",slug:"mariano-bresciani",fullName:"Mariano Bresciani"},{id:"305861",title:"Dr.",name:"Hendrik",middleName:"Jan",surname:"Van Der Woerd",slug:"hendrik-van-der-woerd",fullName:"Hendrik Van Der Woerd"}]},{id:"70180",title:"The Impact of Space Radiation Environment on Satellites Operation in Near-Earth Space",slug:"the-impact-of-space-radiation-environment-on-satellites-operation-in-near-earth-space",totalDownloads:472,totalCrossrefCites:1,totalDimensionsCites:4,book:{slug:"satellites-missions-and-technologies-for-geosciences",title:"Satellites Missions and Technologies for Geosciences",fullTitle:"Satellites Missions and Technologies for Geosciences"},signatures:"Victor U. J. Nwankwo, Nnamdi N. Jibiri and Michael T. Kio",authors:[{id:"94563",title:"Dr.",name:"Nnamdi",middleName:null,surname:"Jibiri",slug:"nnamdi-jibiri",fullName:"Nnamdi Jibiri"},{id:"300878",title:"Dr.",name:"Victor",middleName:null,surname:"Nwankwo",slug:"victor-nwankwo",fullName:"Victor Nwankwo"},{id:"310318",title:"Dr.",name:"Michael",middleName:null,surname:"Kio",slug:"michael-kio",fullName:"Michael Kio"}]},{id:"62237",title:"Modelling Driving Forces of Urban Growth with Fuzzy Sets and GIS",slug:"modelling-driving-forces-of-urban-growth-with-fuzzy-sets-and-gis",totalDownloads:781,totalCrossrefCites:0,totalDimensionsCites:0,book:{slug:"spatial-analysis-modelling-and-planning",title:"Spatial Analysis, Modelling and Planning",fullTitle:"Spatial Analysis, Modelling and Planning"},signatures:"Khalid Al-Ahmadi",authors:[{id:"137051",title:"Dr.",name:"Khalid",middleName:null,surname:"Al-Ahmadi",slug:"khalid-al-ahmadi",fullName:"Khalid Al-Ahmadi"}]}],onlineFirstChaptersFilter:{topicSlug:"spatial-analysis",limit:3,offset:0},onlineFirstChaptersCollection:[],onlineFirstChaptersTotal:0},preDownload:{success:null,errors:{}},aboutIntechopen:{},privacyPolicy:{},peerReviewing:{},howOpenAccessPublishingWithIntechopenWorks:{},sponsorshipBooks:{sponsorshipBooks:[{type:"book",id:"10176",title:"Microgrids and Local Energy Systems",subtitle:null,isOpenForSubmission:!0,hash:"c32b4a5351a88f263074b0d0ca813a9c",slug:null,bookSignature:"Prof. Nick Jenkins",coverURL:"https://cdn.intechopen.com/books/images_new/10176.jpg",editedByType:null,editors:[{id:"55219",title:"Prof.",name:"Nick",middleName:null,surname:"Jenkins",slug:"nick-jenkins",fullName:"Nick Jenkins"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter"}}],offset:8,limit:8,total:1},route:{name:"profile.detail",path:"/profiles/255276/nadia-libia-ortiz-cornejo",hash:"",query:{},params:{id:"255276",slug:"nadia-libia-ortiz-cornejo"},fullPath:"/profiles/255276/nadia-libia-ortiz-cornejo",meta:{},from:{name:null,path:"/",hash:"",query:{},params:{},fullPath:"/",meta:{}}}},function(){var e;(e=document.currentScript||document.scripts[document.scripts.length-1]).parentNode.removeChild(e)}()