Electrospinning parameters affecting fiber morphology.
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The generation of a wave train is a preoccupying subject in the realm of nonlinear science. This is mainly due to two effects: nonlinearity and dispersion. These two notions are essential in the propagation of the wave over long distances and the optical pulse resulting from this interaction gives rise to an optical soliton. The dynamic evolution of nonlinear pulses in nonlinear optical systems can be modeled by the well known nonlinear Schrödinger (NLS) equation which represents the lowest-order nontrivial condition describing the propagation process [1]. The co-propagation of two nonlinear waves in nonlinear optical Kerr media under a slowly varying amplitude approximation is made by using extensions of the NLS equation, whose analytical results provide the dispersion relation, the unstable conditions, as well as the gain spectra. This extension of NLS equation can take into account a large variety of physical properties such as higher-orders dispersion (like third-order dispersion (TOD) and fourth-order dispersion (FOD)) [2, 3, 4, 5, 6, 7, 8, 9]; multiple optical beams [10]; negative index material [11]; saturable nonlinearity [12]; and non-instantaneous nonlinear response [13]. Third-order dispersion is used to describe the proprieties of ultrashort pulses in the subpicosecond to femtosecond domain. Usually in nonlinear optic, Kerr nonlinearity is used to compensate the dispersion effects leading to the formation of soliton. Due to this property, focusing Kerr-type media promote the stable propagation of bright solitons [14]. Despite this, the diffraction effect is not enough to balance the self-focusing in focusing quintic nonlinear media and therefore the pulse undergoes critical collapse [15]. Thus, higher-order nonlinearities (HON) play an important role in the description and the propagation of the pulses in Kerr media. Consequently, the extension of NLS equation can also take into account the effect of HON. Reyna et al. [16, 17, 18] have experimentally and numerically investigated the nonlinearity management and spatial modulation instability for cubic, quintic, and septic nonlinearity for optical beams propagation in metal-dielectric nanocomposites.
The study of the propagation of an intense optical beams through a nonlinear and dispersive media may lead to fascinating effects such as exponential growth of amplitude due to modulation in amplitude and frequency. This effect is called modulation instability (MI). Modulation instability is a fundamental phenomenon firstly detected in hydrodynamic systems [19] and appears in most nonlinear wave systems. In nonlinear Kerr media such as optical fiber, MI results from the interaction between the nonlinear and dispersive effects [20] characterized by the instability undergone by a continuous wave (cw) or quasi-cw when it propagates inside a nonlinear dispersive system with low noise [21]. Modulation instability has been studied for waves in fluids dynamics [22], plasmas physic [23], dielectric media [24], electrodynamics [25], and atomic Bose-Einstein condensates [26, 27] and was first analyzed theoretically in glass fiber by Hasegawa and Brinkman [28] in 1984 to study the generation of ultrashort optical beams. This phenomenon is generally studied in the anomalous dispersion regime, but it can also be observed in normal dispersion regime when the pumping is carried out close to the zero dispersion subject to certain conditions on the higher order dispersion (HOD) coefficients [29, 30]. Cavalcanti et al. [31] predicted the possibility of MI to occur even in normal group velocity dispersion regime due to the negative values of fourth-order dispersion (FOD). The effects of FOD was also been investigated by many authors who show their inclusion leads to generation of new spectral window. Tchofo et al. have analytically and numerically investigated the behavior of MI under the combined effects of HOD and delayed Raman response [5, 6]. In Ref. [7], the authors shown that FOD shifts the MI peak gain to the higher frequency side and also increases the instability region. Nithyanandan et al. [8] analyzed that the cumulative effect of HOD and walk-off brings new characteristic spectral bands at a definite frequency window.
Wang et al. have shown in their work that the distribution of speed of system flow and the speed of sound determining the occurrence of the sonic horizon is in agreement with the corresponding quantities obtained from a pure numerical evaluation for quantum system incorporating septic nonlinearity modeled by NLS equation [32]. An essential manifestation of the intensity dependence of the refractive index in nonlinear optical media rises through self-phase modulation (SPM) [33], which leads to spectral spreading of optical pulses. It is well known that the co-propagation of two optical waves in nonlinear Kerr media is coupled due to refractive index of the media through the nonlinear phenomenon called cross-phase modulation (XPM) [29, 34].
In this paper, we study the MI in non-instantaneous Kerr media with cubic-quintic-septic nonlinearity, described by a system of two-coupled NLS equation. We mainly focus on revealing the contribution of group velocity mismatch
The optical electromagnetic field propagations are described, under a slowly varying amplitude approximation by a coupled nonlinear Schrödinger equation (CNLSE) with higher order dispersion [8] in a single-mode optical Kerr media where higher-order nonlinearities [16] are taken into account. These equations result from two optical beams at different frequencies and the same polarizations where time-dependent nonlinear response is incorporated in the system. The governing systems are read as:
The nonlinear Kerr parameters
Reyna et al. [16] have proposed this class of HON to study the spatial phase modulation induced by quintic and septic nonlinearities for optical beams propagation in metal colloids, where septic nonlinearity arises from the development up to seventh-order susceptibility of theoretical treatment of Maxwell-Garnett model. Quintic nonlinearity has been considered by Kumar [35] to show the influence of spatial delay on the modulational instability in a composite system with a controllable nonlinearity.
We extend the previous works on MI taking into account the CNLS with higher-order effects and using the linear stability approach. Therefore, we study the stability of the steady-state solution of the above dynamical equations against the small harmonic perturbations; the steady-state solution of the continuous wave (cw) is obtained by setting the time derivative in Eqs. (1)–(4) to zero. This leads the exacts solution in the form:
and
where
with
where
where
where the parameters of this equation are defined by the following relation:
With the parameters
Hence, for usual Kerr approach
The condition so that MI can occur read as:
This condition shows that MI depends on the sign of
By considering the effects of relaxation time
We investigate the effect of HON on MI gain in the case of low dispersion regime (
First, let us briefly consider the case of instantaneous response time
MI gain spectra
Now, considering the effect of delay response time by setting GVM null, Eq. (15) leads to four unstable modes which turns to two as given in Figure 1(b). We note from this figure that, for ultra-fast response time, the behavior is as for fast response time for cubic nonlinearity, and the rest of the curves is as described in quintic nonlinearity [39]. As already mentioned, the non-instantaneous response time brings new bands attributed to Raman effect involves in the fibers.
Taking into account the combined effects of delay response time and GVM, Eq. (15) leads to four unstable modes that turns to two for response time reaching certain value
MI gain spectra
Now considering that GVM varies with fixed nonlinear response time, we have observed that when the GVM increases, the behavior of the MI gain spectra changes drastically as given in Figure 3 for mixed GVD. In this figure, the four unstable modes coalesce into one at high frequencies.
MI gain spectra
However, for fast response time gives in Figure 3(a), we observe that for conventional and Raman band, the magnitude increases when
In the case of anomalous dispersion regime, the four unstable mode turns to two modes as given in Figure 4. One can observe from this figure that, for conventional spectral band, as GVM increases, the MI gain decreases, while for Raman band (second spectral band), it is inverted. However, the behavior of the MI gain spectra is different from these panels and we can see that as nonlinear response time increases, the magnitude of the gain decreases. In panel (a), we note that before extended in all frequencies, the curves are neutralized at a given frequency and move slowly toward high frequencies while in panel (b), they move rapidly as GVM increases.
MI gain spectra
In the case of normal dispersion regime, for slow response time [panel (a)], the two unstable modes turn to one for lower frequencies and to two at characteristic frequency until colliding to one at high frequencies. The previous description in anomalous case remains the same. Meanwhile for fast response time [panel (b)], the situation is slightly different where one can observe two unstable modes that collid to one as GVM increases. Figure 5 portrays this feature. The Raman and sporadic peaks observed previously in Figure 3 disappeared in these figures due probably to the sign of SOD (they have the same sign).
MI gain spectra
It has been shown that HOD effects such as FOD and TOD are most essential and give rise to a wide diversity of information concerning the MI dynamics.
The inclusion of FOD brings a great change to the MI spectrum and we obtain for each GVM value four gain spectra. In the case of mixed dispersion regime, from Figure 6 we note that, the spectrum presents two regions of instability which are connected to each other. The first one at the pump frequency is separated to the second one due to the effect of FOD. Thus in the case of fast delay response time gives in panel (a), one can observe that for the first instability region, the primary band remains unchanged for all GVM values; while for the Raman band as GVM increases, the MI gain spectra increase. For the second instability region, the situation remains the same as in the mixed case for weak dispersion regime (Figure 3(a)). In panel (b), our work unveiled that for first instability region, the conventional spectral MI gain decreases as GVM increases, while it is inverted for Raman bands. According to the second instability region, we revealed the presence of Raman and sporadic peaks that magnitude and width decrease as GVM increases and they move toward high frequencies. The fourth unstable mode turns to one at high frequencies. In addition at around
MI gain spectra
Taking into account the propagation with anomalous GVM qualitatively changes the MI spectrum, like shape as in Figure 7 that for the primary spectral band as GVM increases, the MI gain spectra decrease, contrarily to the Raman bands which increase as GVM increases. In addition, when increasing the delay response time, the magnitude and the width of MI gain spectra decrease considerably with a singularity around
MI gain spectra
MI gain spectra
We now shift our analysis to the effect of walk-off and delay response time in virtue of TOD. In the case of mixed GVD as seen in Figure 9, the spectra hardly change for
MI gain spectra
In the case of anomalous dispersion regime, the four obtained solution leads to four unstable modes that coalesce to one at higher frequencies. Figure 10 depicts the MI gain spectrum for some GVM value. One observed two singularities due certainly by HOD effects. In the case of fast response time, for first spectral region in panel (a), the primary and Raman bands decrease as GVM increases while for spectra obtained at low MI gain in this region the situation is inverted. In the second region, the inclusion of TOD brings Raman and sporadic peaks that shifted toward higher frequencies due to GVM effect. For slow response time given in panel (b), the situation is almost different as earlier. The sporadic and Raman peaks get shrink and still move toward higher frequencies. It is to explain the behavior of the obtained modes at lower frequencies coalesce to two at middle frequencies and to one at high frequencies. Contrarily to what observed in the case of quintic nonlinearity, in these figures (Figure 10), HOD acts in the case of septic nonlinearity.
MI gain spectra
We now turn our attention to the case of normal dispersion regime as given in Figure 11. We note that, the second spectral region remains almost the same as described in previous figure. However, in the first spectral region, the four solution leads to two unstable modes in panel (a) and to one in panel (b) for lower frequencies. The effect of FOD vanishes due probably to the dominance of SOD and HON. Obviously, we note that as response time increases, the Raman and sporadic peaks get shrink.
MI gain spectra
Figure 12 depicts the evolution of MI gain spectra in the case of “total mixed” GVD. It is obvious to see from panel (a) (fast response time) that as GVM increases, the conventional bands decrease while it is inverted for Raman bands. The effects of TOD is visible around
MI gain spectra
We generally note from these different figures that, the inclusion of TOD and FOD increases considerably the MI gain spectrum and their width. In addition, the formation of Raman and sporadic peaks observed is due on the one hand to the combined effect of SOD and relaxation time and on the other hand due to the combined effect of TOD. They move toward high frequencies due to the effect of GVM. From fast to slow response time, we note that the magnitude of MI gain spectra decreases considerably. The MI occurs in the case of HOD and septic nonlinearity only when the interactions between beams are less (gives here by walk-off parameter
To better appreciate the effect of septic nonlinearity on MI gain, we portrayed the latter versus
We have plotted the behavior of the MI gain in Figure 13 for normal GVD. We observe from this figure that MI appears on both side of
MI gain spectra
In the case of anomalous dispersion regime plotted in Figure 14, we notice that the side bands brought by FOD are suppressed due to their opposite sign with the sign of SOD, the latter dominates and leads to the observed spectrum. Apart from this difference, the information obtained in the normal case remains almost the same. We now turns our attention in the case of mixed dispersion regime gives in Figure 15. Our results show that contrarily to what are observed in previous figures, the bandwidth is clearly visible for
MI gain spectra
MI gain spectra
In this work, we have investigated analytically and numerically the MI process in nonlinear Kerr media with delayed Kerr nonlinearity and subjected to XPM, described by a system of two coupled NLS equation with cubic-quintic-septic nonlinearities, experiencing diverse GVD regime. The system is considered by incorporating the Debye relaxational time-dependent nonlinearities in NLS equation with combined high-order effects modeling the propagation of ultrashort optical pulses in highly nonlinear Kerr media. By considering a small harmonic perturbations to the stationary solutions, we derive the exact dispersion relation for the components of the perturbation fields that include both the XPM and relaxation effects. Our study revealed the effects of septic nonlinearity in the case of the pulses co-propagating in diverse GVD regime. Obviously from our work, the incorporation of septic nonlinearity increases considerably the MI gain spectrum with the emergence of new instabilities frequencies contrarily to that was observed in Ref. [8, 9, 38, 39], while the increase of delay response time decreases the magnitude and the width of the MI gain.
Our study unveiled in the case of weak dispersion regime that, in instantaneous Kerr media, the typical frequency converges to finite value for mixed GVD regime with two gain maxima for certain GVM, meanwhile the MI gain continuously grows with the GVM until it reaches certain values before decays. In non-instantaneous Kerr media, we note the appearance of Raman band with the emergence of Raman peaks for slow response time
Now considering the effect of HOD, we observed that their incorporation hardly change the spectrum. The inclusion of FOD does’t affect the MI gain in normal dispersion regime contrarily to the works done in the case of cubic and quintic nonlinearities [8, 9, 39] where the effect of FOD vanishes in the case of anomalous GVD. The effects of TOD vanish in the case of mixed dispersion regime. However, in the case of anomalous and normal dispersion regime, we note the appearance of Raman peaks that width and magnitude decrease as GVM increases and get shrink as response time increases. In addition, the four unstable modes observed in fast response time leads to two unstable modes for slow response time. For “total mixed” dispersion regime, we also note the appearance of Raman peaks that slightly shifted toward higher frequencies due to the effects of GVM. The effects of septic nonlinearity was also portrayed and our results unveil the appearance of instability in both side of septic nonlinearity parameter. This aspect shows that MI can be investigated as well as in focusing nonlinearity as in defocusing nonlinearity.
Due to the fact that the MI gain increases when taking into account the effect of HON, we can conclude that the system is more stable against harmonic perturbations. In addition, the incorporation of higher order effects lead to the emergence of Raman peaks on the Raman bands. This means that the incident particles after collision with the molecules of the medium, diffuse with a new energy thus creating the Raman peaks observed resulting to the generation of new frequencies range. The study of MI gain has aroused great enthusiasm within the scientific community, motivated in large part by their potential in innovative applications in information technology and telecommunications.
Electrospinning is the most preferred method because of its low cost compared to nanofiber production methods, production of long and continuous nanofibers, controllable nanofiber diameter, and industrial processing potential. When all these properties are evaluated, it would be appropriate to produce a nanofiber for wound healing by electrospinning. On the other hand, in recent years, interest in polymer materials obtained by the electrospinning method has increased significantly. Materials such as polymers and nanofiber composites can be produced directly by electrospinning. The post-processing of electrospun fibers forms other materials, such as ceramics and carbon nanotubes [1]. Polymer nanofibers obtained by the electrospinning method have a high surface area-volume ratio, flexible in surface functions, have superior mechanical performance, and are versatile in design [2].
Because of all these advantages, the most common and simple method used for tissue framework production is electrospinning. The principle of operation is based on filling the syringe with the polymer solution or melting in the high potential area and spraying it from the tip of the syringe to the collector by applying a voltage to an electrode connected to the tip of the syringe (Figure 1). Here, since the solution sprayed from the syringe is subjected to an electrical field, it elongates at the tip of the needle, and a conical appearance called a Taylor cone is obtained. A typical electrospinning process must be between a high voltage source with positive or negative polarity and a grounded surface so that the fibers can clump together. Spraying the solution in the syringe starts when the potential difference applied from the voltage source reaches the threshold value and equalizes to the electrostatic forces, and is completed by spraying it on the grounded surface. Since the fibers collected on the surface are sprayed with a high amount of pulling, they should be in a fine and regular structure [3, 4, 5].
Schematic representation of the electrospinning process.
The surface tension of the liquid (γ), and the gravitational force (Fg) affect the droplet when the solution, which is the first step of the electrospinning process, comes out of the syringe by forming a droplet. The capillary of internal radius (R), density of the liquid (ρ), and gravitational constant (g) values of the pipe through which the polymer flows are effective in the formation of the radius of the droplet (r0).
When a sufficiently high voltage is applied, the electric force FE, the gravitational force Fg encounter surface forces (Fγ = FE + Fg), and the radius of the droplet decreases from (r0) to r (r < r0) [6].
After droplet formation, the polymer solution overcomes the surface forces under the influence of Coloumb repulsive forces, forming a Taylor cone with an apex angle of 49.3°. Initially straight, the jet segment may become unstable over time and may show twisting and undulating movements as it passes toward the collector. The jet in this region exhibits components of predominantly non-axial electrostatic repulsion forces. Three types of instability can occur as demonstrated by the polymer jet. These instability forms are listed as classical Rayleigh instability, axisymmetric electric field current, and whipping instability. Whipping instability results in a radial torque from the center of the jet, resulting in a high degree of bending instability. The resulting radial jets push each other and separate from the main jet. The interaction between increasing charge density on the one hand and viscous and surface tension forces resisting elongation on the other determines the complexity of the resulting instability [6, 7].
This chapter focused that the electrospinning process, parameters affecting the process such as solution and ambient. After then, it was explained herbal extracts were used to obtain nanofibers by electrospinning method and their application areas. This chapter will provide an overview of the principles of the electrospinning process with various herbal extracts for potential applications in many fields especially biomedical areas.
There are three main parameters of the electrospinning process. These are due to the polymer solution, process, and environmental conditions. In this section, the factors affecting each parameter will be discussed in detail. These parameters and their effects in Table 1 are also shown.
Parameters | Effect of Fiber Morphology |
---|---|
Solution Viscosity ↑ | Fiber Diameter ↑ (within the optimum range) |
Surface Tension↓ | Fiber Diameter ↑ |
Solution Conductivity ↑ | Fiber Diameter ↓(wide diameter distribution) |
Solution Dielectric Constant↑ | Fiber Diameter ↓ |
Voltage ↑ | Fiber Diameter ↓ later ↑ |
Flow Rate ↑ | Fiber Diameter ↑ (if the flow rate is too high, a bead appearance occurs.) |
Temperature↑ | Fiber Diameter ↓ (as the viscosity will decrease) |
Distance Between Tip and Collector↑ | Fiber Diameter ↓ (if the distance between the tip and the collector is too short, a bead appearance occurs) |
Humidity (Moisture) ↑ | Fiber Diameter ↑ (with the optimum range) |
Electrospinning parameters affecting fiber morphology.
To carry out the electrospinning process, the polymer must be in liquid form, in the form of a molten polymer or polymer solution. The physical and chemical properties of the solutions play an active role in the electrospinning process and the resulting fiber morphology. During the electrospinning process, the polymer solution is drawn from the tip of the needle. For this reason, the electrical properties, surface tension, and viscosity of the solution determine the amount of stress in the solution. The evaporation rate also affects the viscosity of the solution as it is stretched. The solubility of the polymer in the solvent determines not only the viscosity of the solution but also the types of polymers that can be mixed with each other [1].
Viscosity is the most important factor determining the flow rate of the solution. In the electrospinning process, the flow rate increases at low viscosity [8]. However, when the viscosity of the solution is too low, fluidity may occur and polymer particles may form instead of fibers. In solutions with lower viscosity, the polymer chain is generally less synthesized with each other [9], less chain entanglement occurs, and thus jet stability is lost. The fibers are collected into the collector as droplets, which first turn into spindle-like structures and then into beaded nanofibers [3]. As the viscosity increases, the formation of the bead structure decreases, and more regular nanofibers are obtained [9]. Therefore, factors that affect the viscosity of the solution also affect the electrospinning process and the resulting fibers.
The molecular weight of the polymer used in the electrospinning process has a direct effect on properties such as viscosity, surface tension, and conductivity, and this interaction determines the nanofiber formation. Molecular weight is explained as the length of the chains of the polymer from which nanofibers will be obtained [4]. The length of the polymer chain will determine the amount of entanglement of the polymer chains in the solvent [1]. Since the viscosity will be higher in polymer solutions with high molecular weight, the formation of beads decreases [10]. Although the increase in molecular weight provides regular fiber formation, if this increase is high, it causes the formation of microstrip structure [11, 12].
When a very small drop of waterfalls into the air, the droplet usually takes on a spherical shape. The liquid surface property that causes this phenomenon, which occurs when the electrical forces are around zero, is known as surface tension [1]. An excessive increase in surface tension adversely affects the electrospinning process. Some surfactants with low concentrations are used to lower the surface tension. The decrease in the surface tension of the solution ensures the formation of finer and smoother fibers and a problem-free electrospinning process [4]. The concentration change in the solutions used directly affects the surface tension [13].
Electrospinning is a method of obtaining nanofibers that repel the charges on the surface by stretching the solution and transfer the electric charge from the electrode to the polymer solution [1, 14]. In the electrospinning system, low electrical conductivity can form beaded fibers as it will create instability and cause the jet to not be able to extend sufficiently, while with high electrical conductivity, the polymer jet can stretch more with the loads it carries and form fibers with a smoother and finer structure [3]. For this reason, it is aimed to increase the electrical conductivity by increasing the concentration. Some additives can also be added to increase conductivity in low-concentration or insufficiently ionic solutions [4]. If the conductivity of the solution increases, the electrospinning jet can carry more charge. For example, the conductivity of the solution can be increased by the addition of ions [1]. By adding salt to an uncharged solution, although electrical neutrality is maintained, salt molecules can dissociate into independently acting positive and negative ions, thereby increasing the electrical conductivity of a solution [15, 16]. These ions can also be obtained by dissolving most drugs or proteins in water. As a result, when a small amount of salt or polyelectrolyte is added to the solution, the increased loads carried by the solution will increase the stretching of the solution and the formation of beaded fibers will be prevented [1].
The insulation constant or dielectric constant is defined as a coefficient that measures the ability of a material to store charge on it [17]. As the dielectric constant of the solutions increases, the charge distribution across the surface of the bubble formed at the needle tip will be more uniform, as there will be more net charge density. Therefore, the ordered structure of the obtained nanofiber is also increasing [3, 4]. It is thought that as the dielectric constant increases, obtaining finer and smoother fibers is due to the application of more tension force to the fluid jet [18].
Another important parameter affecting the electrospinning process is various external factors applied to the electrospinning jet. These factors are voltage, flow rate, temperature, collector effect, nozzle diameter, and the distance between the tip and the collector. Although these parameters are less important than solution parameters, they have a certain effect on fiber morphology.
Voltage is a parameter that induces charges in the solution, overcomes electrostatic forces, and initiates the electrospinning process [1]. As the amount of applied voltage increases, the diameters of the obtained nanofibers will decrease [4]. There are three main reasons for this. The first reason is because of a higher voltage will lead to greater stretching of the solution due to the larger columbic forces in the jet and the stronger electric field. This will reduce the fiber diameter. The second factor is that by using a lower viscosity solution, at a higher voltage, the formation of secondary jets during electrospinning is achieved. Thus, the fiber diameters can become narrower. Another factor that can affect the fiber diameter is the flight time of the electrospinning jet. A longer flight time will allow more time for the fibers to stretch and elongate before being placed on the collecting plate. Therefore, at a lower voltage, the diminished acceleration of the jet and the weaker electric field can increase the flight time of the electrospinning jet, facilitating the formation of finer fibers [1].
In many studies [19, 20, 21], it was observed that the formation of beads on the surface formed with the increase of voltage increased. The increase in bead density due to tension is explained because of increased instability of the jet as it is drawn into the syringe needle in the Taylor cone [1]. Here, bead formation occurs with the excessive acceleration of voltage increase, jet movement, and evaporation [4]. It is also suggested that increasing voltage will increase bead density and at even higher voltage, beads will form fibers of thicker diameter [1].
Despite these studies that the voltage increase creates a bead surface, it has been observed that the production of nanofibers at very low voltage also creates a beaded surface [22]. In this sense, the important thing is to work at a voltage where the flow balance will be stable. With the increase in voltage, the jets coming out of the cone tip reach the collector in an orderly manner, increasing their speed in the electrical field. Here, excessive speed increase or decrease is a factor that will lead to the formation of a beaded surface. In other words, the applied voltage must have an upper and lower limit.
The feeding rate determines the amount of feed in the electrospinning system. A certain feeding rate is needed to maintain the Taylor cone in the system. When the feeding rate increases, there will be an increase in the fiber diameter or the size of the beads formed in the fibers, as there will be more solution volume at the nozzle tip [1]. At low feeding rate, nanofiber production will not be possible because there will not be sufficient feed for the Taylor cone.
As the applied voltage changes, the resulting Taylor cone will also change. At low applied voltages, a hanging drop forms at the tip of the array. The Taylor cone is then formed at the tip of the array. However, as the applied voltage increases (moving from left to right), the volume of the hanging drop decreases until a Taylor cone is formed at the tip of the array. Increasing the applied voltage results in the ejection of the spray through the syringe, which is associated with an increase in bead formation [5].
The temperature parameter consists of three environmental variables: melt temperature, solution temperature, and ambient temperature. As the melt temperature increases, less tension is required due to the decrease in viscosity and fiber diameters decrease [7]. Similar to melt temperature, the temperature of a solution has the effect of both increasing the evaporation rate and reducing the viscosity of the polymer solution. This is because the solution has a lower viscosity and greater solubility of the polymer in the solvent, allowing the solution to be stretched more evenly. With a lower viscosity, Columbic forces can exert a greater tensile force on the solution, thus resulting in smaller diameter fibers [1].
There must be an electric field between the source and the collector (collector) for the electrospinning process to start. Therefore, in most electrospinning systems, the collector plate is made of a conductive material such as aluminum foil, which is electrically grounded such that there is a constant potential difference between the source and the collector. If a non-conductive material is used as a collector, charges from the electrospinning jet will quickly build upon the collector, resulting in less fiber deposition. Fibers collected on non-conductive material generally have a lower packing density than those collected on a conductive surface. This is due to the repulsive forces of the loads that build upon the collector as more fibers accumulate. For a conductive collector, the loads on the fibers are distributed so that more fibers are drawn into the collector. As a result, the fibers can be wrapped closely together [1].
The most commonly used collector types in the electrospinning method are generally flat plates, grids and frames. Apart from these, rotating cylinder, rotating disc, rotating cones, parallel rings, liquid bath and wrapper, pyramid-shaped platform, conveyor belt, two parallel frames, rotor, and thin conductive rod are listed as [7].
The nozzle diameter has a certain effect on the electrospinning process. As the nozzle diameter gets smaller, it provides clogging of the diameter and reduces the amount of beads on the nanofibers. The reduction in occlusion is due to less exposure of the solution to the atmosphere during electrospinning. The decrease in the inner diameter of the hole causes a decrease in the diameter of the nanofibers. As the size of the droplet at the tip of the hole decreases, the surface tension of the droplet increases. It reduces jet acceleration when the same amount of voltage is applied, allowing more time for the solution to stretch and stretch before the collector. The nanofibers formed in this way are finer [1].
The nozzle could be blockage when electrospinning with electrospinning chloroform solutions of PLA. When more than one nozzle is formed, the solvent density may increase, but this will increase the difficulty of solvent removal and nozzle cleaning and compose the deposition of nonwoven fiber in thicknesses >10 mm [23].
The distance between the needle tip and the collector provides the necessary time for the solvent in the polymer jet sprayed from the nozzle tip to evaporate [4]. Changing the distance between the tip and the collector has a direct effect on both the flight time and the electric field strength. As the distance between the tip and the collector decreases, the jet will have a shorter distance to travel before reaching the collector plate. In addition, the electric field strength will increase at the same time, which will increase the acceleration of the jet going to the collector. As a result, there may not be enough time for solvents to evaporate when they hit the collector. When the distance is too low, excess solvent causes the fibers to coalesce where they come into contact [1].
Environmental conditions in the electrospinning process are the factors affecting the electrospinning process. In this sense, humidity, atmospheric type, and pressure cause physical and morphological changes in the formed fibers.
The increase in humidity in the environment adversely affects the electrospinning process. High humidity causes circular pores to form on the nanofiber surfaces obtained. The pore depth increases with increasing humidity. However, the depth, diameter, and number of pores remain constant above a certain humidity [1]. It is not possible to carry out the electrospinning process at very high humidity values [3]. As the humidity level decreases, volatile solvents evaporate quickly, causing drying and making the electrospinning process difficult [9]. For this reason, keeping the humidity level at an optimum level is an important factor.
The type of atmosphere in which the electrospinning process takes place is very important for the smooth running of the process. Different gases have different behavior under the high electrostatic field. For example, helium decomposes under a high electrostatic field and therefore electrospinning is not possible [1]. For another example, with excessively volatile solvents the Taylor cone could dry out. To prevent evaporation in the cone, it is feasible to introduce a local stream of solvent-saturated gas around the cone [23]. The decrease in pressure in the environment adversely affects the electrospinning process [1].
Pressure changes in the electrospinning process make it difficult to ensure the stability of the drafting process. The reduction in pressure surrounding the electrospinning jet adversely affects the electrospinning process. When the ambient pressure drops below atmospheric pressure, the polymer solution in the syringe will have a greater tendency to flow through the needle, resulting in an unstable spray start. As the pressure decreases, rapid solution foaming occurs at the needle tip. At very low pressure, electrospinning is not possible due to the direct discharge of electric charges [1].
Reasons such as health problems, population density, environmental pollution, and increased consumption have encouraged people to seek natural solutions. The use of herbal products in the field of health for their healing properties is increasing day by day. In recent years, plants derived from natural substances such as flavonoids, terpenoids, steroids have received considerable attention due to their different pharmacological properties, including antibacterial, antioxidant, and anticancer activity.
The olive leaf plant, which draws attention with its biocompatible, biodegradable, antioxidant, and antimicrobial properties, has been used by many researchers [24, 25, 26, 27] in the electrospinning process for use in the biomedical field. Similarly, because of its biocompatible, biodegradable and antimicrobial properties, and rosemary plant [28, 29] has been used as a bioactive packaging material and to obtain nanofibers by electrospinning for use in the biomedical field. Many plant extracts such as aloe vera [30, 31], thyme [10], grape seed [32], chamomile [33], green tea [34], grewia mollis [35], gotu kola [36], calendula [37], mangosteen [38], lavender [39] are mixed with different polymers and used in the production of nanofibers for use in the medical field.
The fact that different plants grow in every geography, each plant has different and many effects and the ability to obtain biocompatible, sustainable, organic, and environmentally friendly products have encouraged researchers to work in this field. The use of plants obtained from natural sources as active agents is increasing day by day in areas such as wound healing, tissue engineering, and drug release.
The skin forms the largest part of body weight and is very vulnerable to external forces and effects such as tissue traumas and injuries. Today, wound dressings play a vital role in the healing of such wounds, and wound healing depends on several factors such as selection of wound dressing, physiological state of the wound, and degree of damage. An ideal wound dressing should facilitate wound healing, remove exudates from the wound bed, be non-toxic and allergenic, and act as a barrier against microbes [4, 30]. Conventional wound dressings are generally used to close the wound and absorb the excess discharge. Although in previous studies, it was stated that the dressing should keep the wound dry, it is known that a warm and moist environment on the wound increases the healing of the wound [40]. However, it is a fact that excessive moisture causes wetting and softening of the scar tissues and prolongs the wound healing process [4]. Keeping the humidity level at an optimum level is very important for wound treatment. In addition to the ideal moisture level of modern wound dressings, effective oxygen circulation, air permeability, and low bacterial contamination are the essential qualities sought [40].
Modern wound dressings are composed of water-absorbent granular hydrocolloids, alginate containing mannuronic and guluronic acids, and hydrogel, in which water-absorbing polymers are structured into a three-dimensional network [40]. In recent years, with the rapid development of tissue engineering, nanofiber-based ECM (extracellular matrix) scaffold structures have become widespread [4]. ECM is a collagenous substance commonly found in skin, tendons, cartilage, and bone [11]. Compared to other wound dressings, nanofiber wound dressings have advantages such as hemostasis, high porosity, good fluid absorption capacity, small pore sizes, and large surface area [4]. Hyaluronic acid, collagen, chitosan-based nanofibers are generally used in new generation nanofiber-containing bioactive wound dressings due to their biocompatible, biodegradable, and antibacterial properties [40]. Thus, it ensures the healing of the wound by releasing the active substance in the nanofiber structure onto the wound in a controlled manner.
In recent studies [24, 29, 41, 42, 43], herbal extracts seem to be helpful in fighting infection and accelerating the wound healing process. The use of herbal extracts as wound dressings can nourish the wound site with healing properties such as antimicrobial, anti-inflammatory, analgesic, and tissue regeneration [30]. The long-term toxicity and harmful side effects of herbal extracts are generally insignificant compared to synthetic drugs. The main disadvantage of herbal medicines is that they need to be used in higher dosages than synthetic medicines. Large amounts of herbal medicines extracted from plants reduce their solubility in water or other chemical solvents. Therefore, dissolution of plant extracts almost never occurs in polymer-carriers such as capsules, nanofiber mats, and casting films containing herbal medicines. This may cause adverse effects in applications such as drug release behavior. Despite these problems, herbal drugs promise great success compared to chemical drugs due to their superior performance in wound treatments [10]. The important point here is to extract the herbal extracts in a suitable solvent, to obtain a biocompatible polymer and a nanofibrous structure that preserves its existing effects such as anti-inflammatory and antibacterial and supports the repair of opened wounds.
Tissue engineering is a field that aims to heal damaged or diseased tissues/organs, to maintain, regenerate and develop the functions of normal tissues/organs, and to form tissue scaffolds with repair capability for this purpose. Electrospinning is an application with high potential in many tissue engineering fields such as vasculature, bone, neural, and tendon/ligament. With the electrospinning process, the ability to form aligned scaffolds for anisotropic mechanical and biological properties in the field of vascular grafts, as well as the ability to inhibit smooth muscle cell migration, is provided. In addition, possibilities have been presented to improve vascular grafts with tissue scaffolds that can be obtained by tissue engineering [5, 44].
Nanofibers in tissue engineering must have such as biocompatible, biodegradable (with an acceptable shelf life), tissue-appropriate degradation rate, tissue-appropriate mechanical (strength, stiffness, and modulus) and structural (pore sizes, shape, and structure) properties, and sterilizability [45]. Tissues consist of multiple cell types and works in conjunction with the cell-surrounding extracellular matrix (ECM), which is the tissue scaffold, concealed by regular, micro-sized cells. The ECM is responsible for providing the cells with the needed mechanical support and protecting the cells. The materials used in tissue engineering applications should allow a certain interaction with the cell, the cell’s attachment, proliferation, change, ECM production, and proper progression of this process should be ensured. It should form a supporting function in the formation of new tissues [3, 44].
Approximately, 25% of current prescription drugs are derived from trees, medicinal plants, shrubs, and herbs in nature. The use of herbal extracts with nanofibers produced by electrospinning provides a good potential to form scaffolds for skin regeneration [46]. For example, it has been seen that the nanofibrous structure of the chamomile plant supports collagen fiber accumulation and tissue formation in the dermis [33], and the olive leaf plant has a good potential for tissue scaffolding in biomedical applications thanks to its high antioxidant effect [3]. There are studies on tissue scaffolds containing edible, non-toxic, biocompatible, biodegradable plant extracts with many different contents. It is thought that the applications of plant-based tissue scaffolds will increase in future studies.
Drug delivery systems aim to deliver the drug to the unhealthy region in a controlled and regular manner and to ensure its effectiveness in this region. While drug delivery is generally associated with the delivery of therapeutic agents for the treatment of certain disease states such as cancer, the delivery systems for tissue engineering applications can also apply to the delivery of bioactive agents such as proteins and DNA [5].
In conventional drug delivery systems, successive doses of the drug cause a fluctuating profile of the drug concentration in the blood throughout the treatment period. Therefore, at certain times, concentrations may exceed the recommended maximum (Cmax) concentration with the risk of biotoxicity or fall below the minimum concentration (Cmin), limiting the therapeutic effect. To obtain the highest therapeutic value from the drug, the optimum concentration (C), (Cmin < C < Cmax) in body tissue should be maintained throughout the entire treatment period. Via controlled delivery techniques, the bioavailability of the drug has been designed throughout to be close to this optimum value. In addition, the amount of drug required to be administered is relatively lower in the controlled release mode, minimizing potential side effects [6].
In tissue engineering, the design of the polymer scaffold requires the release of growth factors and other bioactive substances into the growing tissue over a period of time. In nanofiber applications such as wound dressings or artificial leather, the local controlled release of antibiotic substances can aid the healing process. Polymer-based delivery systems can produce controlled drug release by diffusion or chemical bioerosion of the matrix or biodegradation of the linkages connecting the drug to the matrix [6]. These advantages are of great importance in their preference and use.
Polymer-based drug delivery systems; nano or microparticles, hydrogels, micelles, and fibrillar systems. Fibrillated systems form nanofiber-based drug release systems [3]. The release kinetics of the drug is controlled by the morphology of the polymer/drug composite as well as the semi-crystalline structure of the polymer. First, the drug is dissolved at the molecular level in the polymer matrix. The drug is separated as crystalline or amorphous particles in the polymer matrix [6, 47].
The use of herbal-based nanofiber structures in drug delivery systems has increased in recent years. There are different applications such as designing coaxial nanofibers by using olive leaf extract as a bioactive agent [25], producing nanofiber membranes containing aloe vera [48], using nanofibers prepared using the bark of Tecomella undulate (rohida) plant in in-vitro drug release [49]. It is expected that nanofiber drug delivery systems containing herbal extracts will increase therapeutic efficacy, reduce toxicity and ensure compatibility with patients by delivering drugs to the affected area at a controlled rate for a certain period.
Electrospinning is a nanofiber production method that is the most preferred because it is simple, economical, and environmentally friendly, and has many production parameters including solution, process, and environmental conditions. Production of nanofibers by electrospinning process; It is a subject that draws attention with its applications in many fields such as tissue engineering, drug release, filtration, automotive, energy, food industry, cosmetics, agriculture, biosensing. Although polymer contents with synthetic infrastructures are generally preferred in these applications, approaches to using natural agents with few side effects, biocompatible, sustainable, economical, biodegradable, and free from toxic components are increasing [10, 27, 33, 41, 42]. The use of natural components containing active agents in the production of nanofibers is becoming more and more common in the fight against potential health problems that may occur due to the rapidly increasing world population and environmental pollution. Herbal extracts are promising in electrospinning applications with their biodiversity, ability to maintain their biological functionality even after exposure to high electrical voltage, and wound healing effects against pathogenic microorganisms. In addition, it is thought that the use of herbal extracts in different applications in the field of health will become widespread, as they have fewer side effects, and versatile therapeutic properties compared to chemical agents.
The authors declare no conflict of interest.
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Every year, the number of palm oil mills increases rapidly, thus increasing the capacity of fresh fruit bunch waste or effluent discharge. Based on the data from the Malaysian Palm Oil Board in 2012, Malaysia produced 99.85 million tons of fresh fruit bunch (FFB) per year. However, about 5–5.7 tons of water was required in order to sterilize the palm fruit bunches and clarify the extracted oil to produce 1 ton of crude palm oil resulting in 50% of the water turning into palm oil mill effluent (POME). POME is one of the major environmental pollutants in Malaysia. The characteristics of POME and its behavior, if discharged directly, in water are described in this chapter. The suspended solid and nutrient content in POME could be able to support the growth of algae. This chapter aims to demonstrate that POME could be used as a main source for algae production, and this effluent is one of the main environmental problems in the tropical region especially in Malaysia.",book:{id:"6730",slug:"palm-oil",title:"Palm Oil",fullTitle:"Palm Oil"},signatures:"Hesam Kamyab, Shreeshivadasan Chelliapan, Mohd Fadhil Md Din,\nShahabaldin Rezania, Tayebeh Khademi and Ashok Kumar",authors:[{id:"225957",title:"Dr.",name:"Hesam",middleName:null,surname:"Kamyab",slug:"hesam-kamyab",fullName:"Hesam Kamyab"},{id:"237449",title:"Dr.",name:"Shreeshivadasan",middleName:null,surname:"Chelliapan",slug:"shreeshivadasan-chelliapan",fullName:"Shreeshivadasan Chelliapan"},{id:"241504",title:"Dr.",name:"Mohd Fadhil",middleName:null,surname:"Md Din",slug:"mohd-fadhil-md-din",fullName:"Mohd Fadhil Md Din"},{id:"241505",title:"Dr.",name:"Shahabaldin",middleName:null,surname:"Rezania",slug:"shahabaldin-rezania",fullName:"Shahabaldin Rezania"},{id:"241506",title:"Dr.",name:"Tayebeh",middleName:null,surname:"Khademi",slug:"tayebeh-khademi",fullName:"Tayebeh Khademi"},{id:"241508",title:"Dr.",name:"Ashok",middleName:null,surname:"Kumar",slug:"ashok-kumar",fullName:"Ashok Kumar"}]},{id:"38711",doi:"10.5772/51238",title:"Hydrogen Storage for Energy Application",slug:"hydrogen-storage-for-energy-application",totalDownloads:12184,totalCrossrefCites:17,totalDimensionsCites:40,abstract:null,book:{id:"2873",slug:"hydrogen-storage",title:"Hydrogen Storage",fullTitle:"Hydrogen Storage"},signatures:"Rahul Krishna, Elby Titus, Maryam Salimian, Olena Okhay, Sivakumar Rajendran, Ananth Rajkumar, J. M. G. Sousa, A. L. C. Ferreira, João Campos Gil and Jose Gracio",authors:[{id:"25491",title:"Dr.",name:"Elby",middleName:null,surname:"Titus",slug:"elby-titus",fullName:"Elby Titus"}]},{id:"29876",doi:"10.5772/35875",title:"Petroleum Asphaltenes",slug:"petroleum-asphaltenes",totalDownloads:14174,totalCrossrefCites:25,totalDimensionsCites:40,abstract:null,book:{id:"2288",slug:"crude-oil-emulsions-composition-stability-and-characterization",title:"Crude Oil Emulsions",fullTitle:"Crude Oil Emulsions - Composition Stability and Characterization"},signatures:"Lamia Goual",authors:[{id:"106226",title:"Dr.",name:"Lamia",middleName:null,surname:"Goual",slug:"lamia-goual",fullName:"Lamia Goual"}]},{id:"60752",doi:"10.5772/intechopen.76412",title:"Biomaterial from Oil Palm Waste: Properties, Characterization and Applications",slug:"biomaterial-from-oil-palm-waste-properties-characterization-and-applications",totalDownloads:2816,totalCrossrefCites:22,totalDimensionsCites:38,abstract:"Oil palm are among the best known and most extensively cultivated plant families, especially Indonesia and Malaysia. Many common products and foods are derived from oil palm, its making them one of the most economically important plants. On the other hand, declining supply of raw materials from natural resources has motivated researchers to find alternatives to produce new materials from sustainable resources like oil palm. Oil palm waste is possibly an ideal source for cellulose-based natural fibers and particles. Generally, oil palm waste such as oil palm empty fruit bunches, oil palm trunk, oil palm shell and oil palm ash are good source of biomaterials. Lack of sufficient documentation of existing scientific information about the utilization of oil palm waste raw materials for biomaterial production is the driving force behind the this chapter. Incorporation of various types of biomaterial derived from oil palm waste resources as reinforcement in polymer matrices lead to the development of biocomposites products and this can be used in wide range of potential applications. Properties and characterization of biomaterial from oil palm waste will not only help to promote further study on nanomaterials derived from non-wood materials but also emphasize the importance of commercially exploit oil palm waste for sustainable products.",book:{id:"6730",slug:"palm-oil",title:"Palm Oil",fullTitle:"Palm Oil"},signatures:"Rudi Dungani, Pingkan Aditiawati, Sri Aprilia, Karnita Yuniarti, Tati\nKarliati, Ichsan Suwandhi and Ihak Sumardi",authors:[{id:"220081",title:"Dr.",name:"Pingkan",middleName:null,surname:"Aditiawati",slug:"pingkan-aditiawati",fullName:"Pingkan Aditiawati"},{id:"234728",title:"Dr.",name:"Rudi",middleName:null,surname:"Dungani",slug:"rudi-dungani",fullName:"Rudi Dungani"},{id:"249537",title:"Dr.",name:"Sri",middleName:null,surname:"Aprilia",slug:"sri-aprilia",fullName:"Sri Aprilia"},{id:"249539",title:"Dr.",name:"Karnita",middleName:null,surname:"Yuniarti",slug:"karnita-yuniarti",fullName:"Karnita Yuniarti"},{id:"249541",title:"Dr.",name:"Tati",middleName:null,surname:"Karliati",slug:"tati-karliati",fullName:"Tati Karliati"},{id:"249542",title:"Dr.",name:"Ichsan",middleName:null,surname:"Suwandi",slug:"ichsan-suwandi",fullName:"Ichsan Suwandi"},{id:"249543",title:"Dr.",name:"Ihak",middleName:null,surname:"Sumardi",slug:"ihak-sumardi",fullName:"Ihak Sumardi"},{id:"256251",title:"Dr.",name:"Sri",middleName:null,surname:"Hartati",slug:"sri-hartati",fullName:"Sri Hartati"}]},{id:"52155",doi:"10.5772/64828",title:"EOR Processes, Opportunities and Technological Advancements",slug:"eor-processes-opportunities-and-technological-advancements",totalDownloads:5447,totalCrossrefCites:16,totalDimensionsCites:33,abstract:"Enhanced oil recovery (EOR) processes are well known for their efficiency in incrementing oil production; however, the selection of the most suitable method to adopt for specific field applications is challenging. Hence, this chapter presents an overview of different EOR techniques currently applied in oil fields, the opportunities associated with these techniques, key technological advancements to guide the decision‐making process for optimum applicability and productivity and a brief review of field applications.",book:{id:"5143",slug:"chemical-enhanced-oil-recovery-ceor-a-practical-overview",title:"Chemical Enhanced Oil Recovery (cEOR)",fullTitle:"Chemical Enhanced Oil Recovery (cEOR) - a Practical Overview"},signatures:"Lezorgia Nekabari Nwidee, Stephen Theophilus, Ahmed Barifcani,\nMohammad Sarmadivaleh and Stefan Iglauer",authors:[{id:"37799",title:"Dr.",name:"Stefan",middleName:null,surname:"Iglauer",slug:"stefan-iglauer",fullName:"Stefan Iglauer"},{id:"179076",title:"Dr.",name:"Lezorgia",middleName:"Nekabari",surname:"Nwidee",slug:"lezorgia-nwidee",fullName:"Lezorgia Nwidee"},{id:"179077",title:"Prof.",name:"Ahmed",middleName:null,surname:"Barifcani",slug:"ahmed-barifcani",fullName:"Ahmed Barifcani"},{id:"179078",title:"Prof.",name:"Stephen",middleName:null,surname:"Theophilus",slug:"stephen-theophilus",fullName:"Stephen Theophilus"},{id:"189371",title:"Dr.",name:"Mohammad",middleName:null,surname:"Sarmadivaleh",slug:"mohammad-sarmadivaleh",fullName:"Mohammad Sarmadivaleh"}]}],mostDownloadedChaptersLast30Days:[{id:"52155",title:"EOR Processes, Opportunities and Technological Advancements",slug:"eor-processes-opportunities-and-technological-advancements",totalDownloads:5449,totalCrossrefCites:16,totalDimensionsCites:33,abstract:"Enhanced oil recovery (EOR) processes are well known for their efficiency in incrementing oil production; however, the selection of the most suitable method to adopt for specific field applications is challenging. Hence, this chapter presents an overview of different EOR techniques currently applied in oil fields, the opportunities associated with these techniques, key technological advancements to guide the decision‐making process for optimum applicability and productivity and a brief review of field applications.",book:{id:"5143",slug:"chemical-enhanced-oil-recovery-ceor-a-practical-overview",title:"Chemical Enhanced Oil Recovery (cEOR)",fullTitle:"Chemical Enhanced Oil Recovery (cEOR) - a Practical Overview"},signatures:"Lezorgia Nekabari Nwidee, Stephen Theophilus, Ahmed Barifcani,\nMohammad Sarmadivaleh and Stefan Iglauer",authors:[{id:"37799",title:"Dr.",name:"Stefan",middleName:null,surname:"Iglauer",slug:"stefan-iglauer",fullName:"Stefan Iglauer"},{id:"179076",title:"Dr.",name:"Lezorgia",middleName:"Nekabari",surname:"Nwidee",slug:"lezorgia-nwidee",fullName:"Lezorgia Nwidee"},{id:"179077",title:"Prof.",name:"Ahmed",middleName:null,surname:"Barifcani",slug:"ahmed-barifcani",fullName:"Ahmed Barifcani"},{id:"179078",title:"Prof.",name:"Stephen",middleName:null,surname:"Theophilus",slug:"stephen-theophilus",fullName:"Stephen Theophilus"},{id:"189371",title:"Dr.",name:"Mohammad",middleName:null,surname:"Sarmadivaleh",slug:"mohammad-sarmadivaleh",fullName:"Mohammad Sarmadivaleh"}]},{id:"60752",title:"Biomaterial from Oil Palm Waste: Properties, Characterization and Applications",slug:"biomaterial-from-oil-palm-waste-properties-characterization-and-applications",totalDownloads:2823,totalCrossrefCites:22,totalDimensionsCites:38,abstract:"Oil palm are among the best known and most extensively cultivated plant families, especially Indonesia and Malaysia. Many common products and foods are derived from oil palm, its making them one of the most economically important plants. On the other hand, declining supply of raw materials from natural resources has motivated researchers to find alternatives to produce new materials from sustainable resources like oil palm. Oil palm waste is possibly an ideal source for cellulose-based natural fibers and particles. Generally, oil palm waste such as oil palm empty fruit bunches, oil palm trunk, oil palm shell and oil palm ash are good source of biomaterials. Lack of sufficient documentation of existing scientific information about the utilization of oil palm waste raw materials for biomaterial production is the driving force behind the this chapter. Incorporation of various types of biomaterial derived from oil palm waste resources as reinforcement in polymer matrices lead to the development of biocomposites products and this can be used in wide range of potential applications. Properties and characterization of biomaterial from oil palm waste will not only help to promote further study on nanomaterials derived from non-wood materials but also emphasize the importance of commercially exploit oil palm waste for sustainable products.",book:{id:"6730",slug:"palm-oil",title:"Palm Oil",fullTitle:"Palm Oil"},signatures:"Rudi Dungani, Pingkan Aditiawati, Sri Aprilia, Karnita Yuniarti, Tati\nKarliati, Ichsan Suwandhi and Ihak Sumardi",authors:[{id:"220081",title:"Dr.",name:"Pingkan",middleName:null,surname:"Aditiawati",slug:"pingkan-aditiawati",fullName:"Pingkan Aditiawati"},{id:"234728",title:"Dr.",name:"Rudi",middleName:null,surname:"Dungani",slug:"rudi-dungani",fullName:"Rudi Dungani"},{id:"249537",title:"Dr.",name:"Sri",middleName:null,surname:"Aprilia",slug:"sri-aprilia",fullName:"Sri Aprilia"},{id:"249539",title:"Dr.",name:"Karnita",middleName:null,surname:"Yuniarti",slug:"karnita-yuniarti",fullName:"Karnita Yuniarti"},{id:"249541",title:"Dr.",name:"Tati",middleName:null,surname:"Karliati",slug:"tati-karliati",fullName:"Tati Karliati"},{id:"249542",title:"Dr.",name:"Ichsan",middleName:null,surname:"Suwandi",slug:"ichsan-suwandi",fullName:"Ichsan Suwandi"},{id:"249543",title:"Dr.",name:"Ihak",middleName:null,surname:"Sumardi",slug:"ihak-sumardi",fullName:"Ihak Sumardi"},{id:"256251",title:"Dr.",name:"Sri",middleName:null,surname:"Hartati",slug:"sri-hartati",fullName:"Sri Hartati"}]},{id:"66623",title:"Catalytic Dehydration of Glycerine to Acrolein",slug:"catalytic-dehydration-of-glycerine-to-acrolein",totalDownloads:1418,totalCrossrefCites:1,totalDimensionsCites:3,abstract:"The biodiesel production yields glycerine as a by-product in quantities around 10 vol% of produced biodiesel. Acrolein can be obtained from glycerine by a dehydration reaction. Catalytic processes in gas phase have been developed to obtain acrolein from a renewable feedstock using heterogeneous catalysts. The main process variables are the reaction temperature, the concentration of glycerol in water, and the space velocity in fixed-bed reactors. A thermodynamic study of the equilibrium has been made to estimate the conversion to equilibrium as a function of temperature. The reactors have been heated usually between 523 and 603 K. Generally, an aqueous glycerol solution is preheated in a preheating zone at a temperature enough to vaporize the feedstock, between 473 and 533 K, depending on the concentration of reactant required in the feed. Some of the most active catalysts in the gas-phase reaction (yield >70%) were NH4-La-β zeolite, Pd/LaY zeolite, hierarchical ZSM-5, WO3/ZrO2, WO3/TiO2, ZrOx-NbOx, WOx-NbOx, WO3-SiO2/ZrO2, NbOx-WOx/Al2O3, H3PO4-MCM-41, SAPO-40, NbPSi, Pd-H3PW12O40/Zr-MCM-41, H3PW12O40/Cs-SBA-15, H3PW12O40/Nb2O5, Cs-doped H4SiW12O40/Al2O3, H4SiW12O40/TiO2, and H4SiW12O40/SiO2.",book:{id:"8448",slug:"glycerine-production-and-transformation-an-innovative-platform-for-sustainable-biorefinery-and-energy",title:"Glycerine Production and Transformation",fullTitle:"Glycerine Production and Transformation - An Innovative Platform for Sustainable Biorefinery and Energy"},signatures:"Israel Pala Rosas, Jose Luis Contreras Larios , Beatriz Zeifert and José Salmones Blásquez",authors:[{id:"94936",title:"Dr.",name:"José Luis",middleName:null,surname:"Contreras",slug:"jose-luis-contreras",fullName:"José Luis Contreras"},{id:"284261",title:"Ph.D.",name:"Israel",middleName:null,surname:"Pala-Rosas",slug:"israel-pala-rosas",fullName:"Israel Pala-Rosas"},{id:"284262",title:"Dr.",name:"Jose",middleName:null,surname:"Salmones",slug:"jose-salmones",fullName:"Jose Salmones"},{id:"284263",title:"Dr.",name:"Beatriz",middleName:null,surname:"Zeifert",slug:"beatriz-zeifert",fullName:"Beatriz Zeifert"},{id:"295779",title:"Prof.",name:"Jose Luis",middleName:null,surname:"Contreras",slug:"jose-luis-contreras",fullName:"Jose Luis Contreras"}]},{id:"64816",title:"PVT Properties of Black Crude Oil",slug:"pvt-properties-of-black-crude-oil",totalDownloads:1561,totalCrossrefCites:0,totalDimensionsCites:1,abstract:"Precise PVT studies and behavior of phase-equilibrium of petroleum reservoir fluids are essential for describing these fluids and appraising their volumetric behavior at several pressure stages. There are numerous laboratory studies that can be performed on a reservoir sample. The amount of data desired determines the number of tests to be performed in the laboratory. Generally, there are three laboratory tests which characterize hydrocarbon fluids, namely primary study, constant mass depletion, and differential vaporization test. Generally, PVT properties are determined either experimentally or calculated theoretically through published correlations. This chapter presents different PVT laboratory tests that are required to understand the phase behavior of black oils.",book:{id:"7323",slug:"processing-of-heavy-crude-oils-challenges-and-opportunities",title:"Processing of Heavy Crude Oils",fullTitle:"Processing of Heavy Crude Oils - Challenges and Opportunities"},signatures:"Abdelaziz El-Hoshoudy and Saad Desouky",authors:[{id:"201556",title:"Dr.",name:"Abdelaziz",middleName:"Nasr",surname:"El-Hoshoudy",slug:"abdelaziz-el-hoshoudy",fullName:"Abdelaziz El-Hoshoudy"},{id:"210639",title:"Dr.",name:"Saad M.",middleName:null,surname:"Desouky",slug:"saad-m.-desouky",fullName:"Saad M. Desouky"}]},{id:"64885",title:"Environmental Challenges Associated with Processing of Heavy Crude Oils",slug:"environmental-challenges-associated-with-processing-of-heavy-crude-oils",totalDownloads:876,totalCrossrefCites:2,totalDimensionsCites:6,abstract:"The petroleum industry is one of the largest industries in the world and plays a pivotal part in driving a nation’s economy. However, the exploration and exploitation of heavy crude oil have raised series of environmental challenges and caused increased concern for the communities where the oil refineries are cited. Activities such as gas flaring and oil spillage have led to the release of toxic organic and inorganic pollutants, which has resulted in acid rain, climate change, and contamination of soil, water, and air. These environmental hazards have caused adverse effects directly or indirectly to the ecosystem. This chapter offers a general overview of the processes involved in the processing and some of the potential environmental challenges associated with heavy crude oil processing.",book:{id:"7323",slug:"processing-of-heavy-crude-oils-challenges-and-opportunities",title:"Processing of Heavy Crude Oils",fullTitle:"Processing of Heavy Crude Oils - Challenges and Opportunities"},signatures:"Samuel O. 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Fungal infectious illness prevalence and prognosis are determined by the exposure between fungi and host, host immunological state, fungal virulence, and early and accurate diagnosis and treatment. \r\nPatients with both congenital and acquired immunodeficiency are more likely to be infected with opportunistic mycosis. Fungal infectious disease outbreaks are common during the post- disaster rebuilding era, which is characterised by high population density, migration, and poor health and medical conditions.\r\nSystemic or local fungal infection is mainly associated with the fungi directly inhaled or inoculated in the environment during the disaster. The most common fungal infection pathways are human to human (anthropophilic), animal to human (zoophilic), and environment to human (soilophile). Diseases are common as a result of widespread exposure to pathogenic fungus dispersed into the environment. \r\nFungi that are both common and emerging are intertwined. 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Biochemistry examines macromolecules - proteins, nucleic acids, carbohydrates, and lipids – and their building blocks, structures, functions, and interactions. Much of biochemistry is devoted to enzymes, proteins that catalyze chemical reactions, enzyme structures, mechanisms of action and their roles within cells. Biochemistry also studies small signaling molecules, coenzymes, inhibitors, vitamins, and hormones, which play roles in life processes. Biochemical experimentation, besides coopting classical chemistry methods, e.g., chromatography, adopted new techniques, e.g., X-ray diffraction, electron microscopy, NMR, radioisotopes, and developed sophisticated microbial genetic tools, e.g., auxotroph mutants and their revertants, fermentation, etc. More recently, biochemistry embraced the ‘big data’ omics systems. 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Dr. Blumenberg’s research is focused on the epidermis, expression of keratin genes, transcription profiling, keratinocyte differentiation, inflammatory diseases and cancers, and most recently the effects of the microbiome on the skin. He has published more than 100 peer-reviewed research articles and graduated numerous Ph.D. and postdoctoral students.",institutionString:null,institution:{name:"New York University Langone Medical Center",institutionURL:null,country:{name:"United States of America"}}},subseries:[{id:"14",title:"Cell and Molecular Biology",keywords:"Omics (Transcriptomics; Proteomics; Metabolomics), Molecular Biology, Cell Biology, Signal Transduction and Regulation, Cell Growth and Differentiation, Apoptosis, Necroptosis, Ferroptosis, Autophagy, Cell Cycle, Macromolecules and Complexes, Gene Expression",scope:"The Cell and Molecular Biology topic within the IntechOpen Biochemistry Series aims to rapidly publish contributions on all aspects of cell and molecular biology, including aspects related to biochemical and genetic research (not only in humans but all living beings). We encourage the submission of manuscripts that provide novel and mechanistic insights that report significant advances in the fields. Topics include, but are not limited to: Advanced techniques of cellular and molecular biology (Molecular methodologies, imaging techniques, and bioinformatics); Biological activities at the molecular level; Biological processes of cell functions, cell division, senescence, maintenance, and cell death; Biomolecules interactions; Cancer; Cell biology; Chemical biology; Computational biology; Cytochemistry; Developmental biology; Disease mechanisms and therapeutics; DNA, and RNA metabolism; Gene functions, genetics, and genomics; Genetics; Immunology; Medical microbiology; Molecular biology; Molecular genetics; Molecular processes of cell and organelle dynamics; Neuroscience; Protein biosynthesis, degradation, and functions; Regulation of molecular interactions in a cell; Signalling networks and system biology; Structural biology; Virology and microbiology.",annualVolume:11410,isOpenForSubmission:!0,coverUrl:"https://cdn.intechopen.com/series_topics/covers/14.jpg",editor:{id:"165627",title:"Dr.",name:"Rosa María",middleName:null,surname:"Martínez-Espinosa",fullName:"Rosa María Martínez-Espinosa",profilePictureURL:"https://mts.intechopen.com/storage/users/165627/images/system/165627.jpeg",institutionString:null,institution:{name:"University of Alicante",institutionURL:null,country:{name:"Spain"}}},editorTwo:null,editorThree:null,editorialBoard:[{id:"79367",title:"Dr.",name:"Ana Isabel",middleName:null,surname:"Flores",fullName:"Ana Isabel Flores",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRpIOQA0/Profile_Picture_1632418099564",institutionString:null,institution:{name:"Hospital Universitario 12 De Octubre",institutionURL:null,country:{name:"Spain"}}},{id:"328234",title:"Ph.D.",name:"Christian",middleName:null,surname:"Palavecino",fullName:"Christian Palavecino",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0033Y000030DhEhQAK/Profile_Picture_1628835318625",institutionString:null,institution:{name:"Central University of Chile",institutionURL:null,country:{name:"Chile"}}},{id:"186585",title:"Dr.",name:"Francisco Javier",middleName:null,surname:"Martin-Romero",fullName:"Francisco Javier Martin-Romero",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bSB3HQAW/Profile_Picture_1631258137641",institutionString:null,institution:{name:"University of Extremadura",institutionURL:null,country:{name:"Spain"}}}]},{id:"15",title:"Chemical Biology",keywords:"Phenolic Compounds, Essential Oils, Modification of Biomolecules, Glycobiology, Combinatorial Chemistry, Therapeutic peptides, Enzyme Inhibitors",scope:"Chemical biology spans the fields of chemistry and biology involving the application of biological and chemical molecules and techniques. In recent years, the application of chemistry to biological molecules has gained significant interest in medicinal and pharmacological studies. This topic will be devoted to understanding the interplay between biomolecules and chemical compounds, their structure and function, and their potential applications in related fields. Being a part of the biochemistry discipline, the ideas and concepts that have emerged from Chemical Biology have affected other related areas. 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Behind these definitions are hidden all the aspects of normal and pathological functioning of all processes that the topic ‘Metabolism’ will cover within the Biochemistry Series. Thus all studies on metabolism will be considered for publication.",annualVolume:11413,isOpenForSubmission:!0,coverUrl:"https://cdn.intechopen.com/series_topics/covers/17.jpg",editor:{id:"138626",title:"Dr.",name:"Yannis",middleName:null,surname:"Karamanos",fullName:"Yannis Karamanos",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002g6Jv2QAE/Profile_Picture_1629356660984",institutionString:null,institution:{name:"Artois University",institutionURL:null,country:{name:"France"}}},editorTwo:null,editorThree:null,editorialBoard:[{id:"243049",title:"Dr.",name:"Anca",middleName:null,surname:"Pantea Stoian",fullName:"Anca Pantea Stoian",profilePictureURL:"https://mts.intechopen.com/storage/users/243049/images/system/243049.jpg",institutionString:null,institution:{name:"Carol Davila University of Medicine and Pharmacy",institutionURL:null,country:{name:"Romania"}}},{id:"203824",title:"Dr.",name:"Attilio",middleName:null,surname:"Rigotti",fullName:"Attilio Rigotti",profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",institutionString:null,institution:{name:"Pontifical Catholic University of Chile",institutionURL:null,country:{name:"Chile"}}},{id:"300470",title:"Dr.",name:"Yanfei (Jacob)",middleName:null,surname:"Qi",fullName:"Yanfei (Jacob) Qi",profilePictureURL:"https://mts.intechopen.com/storage/users/300470/images/system/300470.jpg",institutionString:null,institution:{name:"Centenary Institute of Cancer Medicine and Cell Biology",institutionURL:null,country:{name:"Australia"}}}]},{id:"18",title:"Proteomics",keywords:"Mono- and Two-Dimensional Gel Electrophoresis (1-and 2-DE), Liquid Chromatography (LC), Mass Spectrometry/Tandem Mass Spectrometry (MS; MS/MS), Proteins",scope:"With the recognition that the human genome cannot provide answers to the etiology of a disorder, changes in the proteins expressed by a genome became a focus in research. Thus proteomics, an area of research that detects all protein forms expressed in an organism, including splice isoforms and post-translational modifications, is more suitable than genomics for a comprehensive understanding of the biochemical processes that govern life. The most common proteomics applications are currently in the clinical field for the identification, in a variety of biological matrices, of biomarkers for diagnosis and therapeutic intervention of disorders. From the comparison of proteomic profiles of control and disease or different physiological states, which may emerge, changes in protein expression can provide new insights into the roles played by some proteins in human pathologies. Understanding how proteins function and interact with each other is another goal of proteomics that makes this approach even more intriguing. Specialized technology and expertise are required to assess the proteome of any biological sample. Currently, proteomics relies mainly on mass spectrometry (MS) combined with electrophoretic (1 or 2-DE-MS) and/or chromatographic techniques (LC-MS/MS). MS is an excellent tool that has gained popularity in proteomics because of its ability to gather a complex body of information such as cataloging protein expression, identifying protein modification sites, and defining protein interactions. The Proteomics topic aims to attract contributions on all aspects of MS-based proteomics that, by pushing the boundaries of MS capabilities, may address biological problems that have not been resolved yet.",annualVolume:11414,isOpenForSubmission:!0,coverUrl:"https://cdn.intechopen.com/series_topics/covers/18.jpg",editor:{id:"200689",title:"Prof.",name:"Paolo",middleName:null,surname:"Iadarola",fullName:"Paolo Iadarola",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bSCl8QAG/Profile_Picture_1623568118342",institutionString:null,institution:{name:"University of Pavia",institutionURL:null,country:{name:"Italy"}}},editorTwo:{id:"201414",title:"Dr.",name:"Simona",middleName:null,surname:"Viglio",fullName:"Simona Viglio",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRKDHQA4/Profile_Picture_1630402531487",institutionString:null,institution:{name:"University of Pavia",institutionURL:null,country:{name:"Italy"}}},editorThree:null,editorialBoard:[{id:"72288",title:"Dr.",name:"Arli Aditya",middleName:null,surname:"Parikesit",fullName:"Arli Aditya Parikesit",profilePictureURL:"https://mts.intechopen.com/storage/users/72288/images/system/72288.jpg",institutionString:null,institution:{name:"Indonesia International Institute for Life Sciences",institutionURL:null,country:{name:"Indonesia"}}},{id:"40928",title:"Dr.",name:"Cesar",middleName:null,surname:"Lopez-Camarillo",fullName:"Cesar Lopez-Camarillo",profilePictureURL:"https://mts.intechopen.com/storage/users/40928/images/3884_n.png",institutionString:null,institution:{name:"Universidad Autónoma de la Ciudad de México",institutionURL:null,country:{name:"Mexico"}}},{id:"81926",title:"Dr.",name:"Shymaa",middleName:null,surname:"Enany",fullName:"Shymaa Enany",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRqB9QAK/Profile_Picture_1626163237970",institutionString:null,institution:{name:"Suez Canal University",institutionURL:null,country:{name:"Egypt"}}}]}]}},libraryRecommendation:{success:null,errors:{},institutions:[]},route:{name:"onlineFirst.detail",path:"/online-first/80458",hash:"",query:{},params:{id:"80458"},fullPath:"/online-first/80458",meta:{},from:{name:null,path:"/",hash:"",query:{},params:{},fullPath:"/",meta:{}}}},function(){var m;(m=document.currentScript||document.scripts[document.scripts.length-1]).parentNode.removeChild(m)}()