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\r\n\tRadiation monitoring deals with the sampling and measurement of different products found in different radiation pathways from the environment ending with consumption in humans. Gamma-spectroscopy is the main tool for measurement of these radiations.
\r\n\r\n\tThe aim of this book is to investigate the radionuclide concentrations in the most consumable food products, air, water and soil. Particularly, it is essential to investigate the radiations level in the surroundings of a nuclear facility.
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Elif Korcan",authors:[{id:"5974",title:"Prof.",name:"Muhsin",middleName:null,surname:"Konuk",fullName:"Muhsin Konuk",slug:"muhsin-konuk"},{id:"11967",title:"Dr.",name:"İbrahim",middleName:null,surname:"Hakkı Ciğerci",fullName:"İbrahim Hakkı Ciğerci",slug:"ibrahim-hakki-cigerci"},{id:"11968",title:"Dr.",name:"Safiye",middleName:null,surname:"Elif Korcan",fullName:"Safiye Elif Korcan",slug:"safiye-elif-korcan"}]},{id:"6815",title:"Bioelectronic Noses Based on Olfactory Receptors",slug:"bioelectronic-noses-based-on-olfactory-receptors",signatures:"Jasmina Vidic",authors:[{id:"6403",title:"Dr.",name:"Jasmina",middleName:null,surname:"Vidic",fullName:"Jasmina Vidic",slug:"jasmina-vidic"}]}]}],publishedBooks:[{type:"book",id:"413",title:"Environmental Biosensors",subtitle:null,isOpenForSubmission:!1,hash:"ac77d5b581e7145c0302087d80651749",slug:"environmental-biosensors",bookSignature:"Vernon Somerset",coverURL:"https://cdn.intechopen.com/books/images_new/413.jpg",editedByType:"Edited 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Somerset"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"3484",title:"State of the Art in Biosensors",subtitle:"Environmental and Medical Applications",isOpenForSubmission:!1,hash:"b84ae4104612ff69dc3061cf297137f7",slug:"state-of-the-art-in-biosensors-environmental-and-medical-applications",bookSignature:"Toonika Rinken",coverURL:"https://cdn.intechopen.com/books/images_new/3484.jpg",editedByType:"Edited by",editors:[{id:"24687",title:"Dr.",name:"Toonika",surname:"Rinken",slug:"toonika-rinken",fullName:"Toonika Rinken"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}]},onlineFirst:{chapter:{type:"chapter",id:"81426",title:"Quality and Fatigue Assessment of Welded Railway Bridge Components by Testing",doi:"10.5772/intechopen.104439",slug:"quality-and-fatigue-assessment-of-welded-railway-bridge-components-by-testing",body:'Bridges are engineering structures which are subjected to dynamic actions, variable in time—repeated millions of times, and inconsistently. The endurance of steel bridges in service is determined mainly by fatigue, which usually causes catastrophic failures, and corrosion, which ordinarily results in degradation failures [1, 2, 3]. Many early welded bridges in Europe were fractured over the period 1925–1936 and later [4]. Many failures and catastrophic events happened due to fatigue and fracture despite the pioneering works of August Wöhler and other scientists [5, 6]. As a result, the limit state analysis of structures with a probabilistic approach became necessary.
Fractures led to a prohibition on using welding for early high-strength steels [7, 8]. As a result, welding was allowed only on mild steels. It was not until the late 1950s that some fatigue requirements were introduced into the design of steel railway bridges. It took another decade for these to be considered for road bridges; this started the modern approach to fatigue.
Each welded structure possesses discontinuity, or cracks and other imperfections resulting from manufacture or welding. These do not show any growth or instability while the loading rate is relatively low, below threshold fatigue strength. This means that such a stress range does not cause crack propagation. The endurance of steel structures or fatigue details with imperfections may be determined by testing small specimens or numerical analysis.
There are still many welded steel bridges in service which were manufactured in periods of poor quality of both materials and welded joints as well as few requirements for fatigue. After many years in service, each steel structure also undergoes what is known as functional aging, and its structural steel is subjected to structural aging. The mechanism of the aging process may be described by the classical separation theory or the newer dislocation blocking theory.
The quantitative results of welded butt splice quality obtained over 37 years of the testing of welded railway bridges in Poland are given. The radiographic examinations were conducted by the Steel Construction Chair at the West Pomeranian University of Technology in Szczecin [3]. The radiographic tests on the welded joints were supplemented by laboratory fatigue tests and more recently by Finite Element Method (FEM) analysis.
It is assumed that the basic factor describing the properties of a material is the changes in internal material structure resulting from the structural degradation processes described among other things in [3, 9, 10, 11]. This is mainly concerned with the decreasing value of the impact strength, sometimes even by several times. The comparison level for such a phenomenon is the difference in material properties of actual steel versus normalized, as the other has material properties from the time of the structure’s construction. The simulation of these properties is carried out by thermal annealing. For this purpose, specimens are annealed at a temperature of 930°C (steels of C ≤ 0.26%) for an hour and then cooled in air. This way the minimal possible grain size in the steel is achieved.
This process increases yield strength and at the same time lowers the ductile-brittle transition temperature, i.e. significantly increases mechanical properties (Figure 1). Sometimes, astonishing results are obtained. For example, from the railway bridge over the Warta River in Gorzów Wielkopolski (western Poland), two types of steel specimens were tested for Charpy impact energy.
Impact energy KV(T) for naturally aged (S) and normalized (N) specimens from a plate girder railway bridge constructed in 1938.
The bridge was constructed for the German Railways in 1938, using German normalized mild steel St37-12 (Figure 1). The tests refer to specimens which were
naturally aged S without any measures;
normalized N, i.e. annealed at 930°C for an hour and then cooled in air.
A significant aging effect was found in the structural steel after 77 years in service. At −20°C, the impact energy was 19.2 times higher.
The results of impact energy tests at temperature −20°C for nine steel grades from eight bridges constructed in the years 1887–1938 are shown in Figure 2. Two types of specimens were tested: naturally aged and normalized. The steel in post-service conditions showed a very small KV impact energy value.
Notch toughness of tested bridge steels at temperature −20°C for naturally aged (S) and normalized (N) specimens.
The actual ascertained KV values are only from 4 to 12 J. This dependence concerns all the steels tested independently of carbon content from 0.016% to 0.258%.
Such a condition shows brittleness in the material; this is a particular danger when it is located in areas of stress concentrations, for example around welding imperfections (WIs) in a weld – Figure 3. Welding imperfections (WIs) are crack initiators when the loads reach a prescribed critical value. The largest concentration of normal stresses σx is caused by ellipsoidal welding imperfections and longitudinal ones with elliptical cross sections. For these two groups of welding imperfections, the maximum stress gradient increases as the curvature radius value of the sharpest shape of welding imperfections lowers.
Stress distribution σx near welding imperfections: longitudinal – I, ellipsoidal – II, and globular – III [
For example, for welding imperfections with shape characteristic t/ρ = 100, the shape coefficient values u = y/t = 1 are 13.63 and 21.00 Figure 3. In the case of globular welding imperfections of a small stress concentration—class III with a sharp shape—it is independent from the imperfection size and is σx = 2.04·σ [3, 12], where σ is the design stress.
Tensile stresses near a notch may be the effect of external loading, residual stresses, or both simultaneously [13]. It is not possible to exclude brittle fracture even if there is no external loading.
According to the literature [14], the fatigue strength at 105 cycles to strength at 2·106 cycles ratio is in the range 1.44–2.45, with the average value 1.85. Similar values of 1.75 and 1.73 were obtained for Polish mild steel (St3SX: C = 0.160%, Mn = 0.498%) [15] – Figure 4. Tested were as follows:
naturally aged specimens S, for 35 years (fy = 260 MPa, fu = 405 MPa),
artificially overaged specimens NN (fy = 495 MPa, fu = 515 MPa).
Regression straights obtained from fatigue tests on: naturally aged specimens (S) and additionally aged specimens (NN) [
Specimens NN were cold-deformed up to 10% relative elongation and then heated up to temperature 250°C, kept at this temperature for an hour, and then cooled in air.
The value of the infinitive fatigue strength Zrj = 145.3 MPa of naturally aged steel for 35 years is 55.9% of its yield strength fy = 260 MPa and for the overaged steel this value is Zrj = 157.3 MPa which constitutes only 31.8% of its yield strength. As a result of additional aging (specimens NN), there was an unexpected very large increase in steel yield strength fy of 90.4%, and ultimate strength fu increased by 27.1%.
The specific character of bridge loadings and the structural changes in steels due to aging are the main reasons why a general hypothesis for their fatigue estimation has yet to be proposed [16]. Phenomenological models are still used despite the significant number of studies undertaken, especially for riveted structures, and more excellent research tools for testing have appeared as well as the possibility of numerical analysis. A problem has arisen as to how to adapt the information from laboratory fatigue tests to the design for the durability of structures in service. Knowledge of both the loading spectrum which a structure will be carrying and problems with butt splices have become necessary.
Welded structures under high stresses are damaged mainly by fatigue crack growth or brittleness. Hence, fracture mechanics has recognized the most important issues:
discovering and locating flat welding imperfections in a welded joint,
determining flat welding imperfection dimensions precisely, especially in the joint depth.
Over the years 1970–1980, the International Welding Institute introduced the “fitness for purpose” criterion, which relies on the formulation of fracture mechanics calculations for determining the permissible size of welding imperfections, thereby confirming the required quality and durability of structures according to standards and technical requirements. The determination of specific quality levels and example calculations as well as the determination of safety coefficients are given in [17, 18].
The aging of metallic materials favors the formation of brittle cracks as the ductile-brittle transition temperature clearly approaches higher values. Strains associated with aging depend on the location in the structure. They are particularly dangerous in stress concentration areas, e.g. around welding imperfections (WIs) and in heat-affected zones (HAZs). According to Neuber [3, 12], the largest concentration of stresses is associated with ellipsoidal and longitudinal welding imperfections with an elliptical cross section (Figure 3).These types of imperfections include cracks and lack of fusion, as well as band slag intrusion and incomplete side fusion. This issue is becoming particularly significant for bridges constructed after 1936, considering the poor quality of connecting welds. This has been confirmed by radiographic tests performed on bridges in service on Polish railway lines [3].
The Steel Structure Chair at the Technical University in Szczecin (now WPUT) carried out radiological tests on butt splices in the steel girders of around 200 railway bridges on the Polish railway network. For 154 bridges, including 124 plate girder bridges and 30 truss bridges, the exact time of construction was also established.
The range and results of in situ nondestructive radiological tests on the railway bridges are given in two histograms (Figures 5 and 6). The tests consist of the sum of 5-year intervals which take into account the bridge construction period from 1936 to 1975. Figure 5, in the upper part of the histogram, shows the number of bridges tested and the number of X-rays taken over a particular 5-year interval. At the same time, the number of internal structural cracks in connecting welds is given. These cracks were discovered on 437 X-rays. They constitute 2.8% of the total number of welds tested, equaling 15,875 units. This number includes 10,507 X-rays on butt joints in tensile components and the remaining 5368 X-rays on compress components. Simultaneously, the lower part of the histogram gives the number of welded joints tested over given 5-year intervals.
Numerical specification of the bridges and welded joints tested.
Specification for bridges and joints with hot cracks.
Figure 6 shows the proportional and numerical specification of hot cracks detected in bridge structures for given 5-year intervals of construction. Apart from one crack from 1974, the remaining cracks were ascertained in bridges constructed before 1960. According to Eurocode 1993-1-9 for the design of steel structures, such cracks do not exclude structures from service. The upper parts of the histogram (Figure 6) show the proportional and numerical specification of bridges with internal cracks in welded butt splices. Of note is that the majority of cracks were found in the oldest historical bridges from the years 1936–1940. For the seven bridges from that period tested, cracks were discovered in six structures, which constitute 85.7%. They were discovered on 124 welded butt splices from the general lot of 696 pieces tested.
Similar unfavorable test results were obtained during examination of the bridges constructed over the years 1946–1950. Cracks were found in 18 structures (37.5%) on 270 X-rays (5.5%).
All the cracks in the butt splices of the bridge structures are internal hot cracks. They arise in the weld metal and HAZ of a joint during the crystallization process in the liquidus–solidus temperature range (Figure 3).
Service fatigue cracks appear in stress concentration zones caused by structural details and increase their value by a concentration factor caused by nonmetallic inclusions. Therefore, the development of a fatigue crack depends on many factors: the shape and dimensions of a structural component as well as the way and magnitude of loading. The larger the structure, the smaller the critical crack length necessary to cause the final brittle fracture [3, 18]. Development of fatigue cracking appears in stages under fluctuating loads, and their increase is caused by the weakening of a structure’s strength. This is why, in the literature, the stress is put down to the influence of the imperfection’s geometry and its location in the weld.
The literature gives different models for the initiation and proliferation of fatigue cracks in a nondeterministic approach. Despite many attempts to describe the fatigue mechanism, given in 64 hypotheses [19], no general hypothesis has yet to be formulated [18, 20, 21]. We are still stuck in the phenological description, despite having more and better research tools and numerical calculations. It appears that when assessing the endurance of bridges with cracks in their welded joints, it is highly useful to analyze their service behavior and the results of laboratory tests.
In Poland, the pioneer of the in situ field testing of welded butt splices on railway bridges was Professor Andrzej Fabiszewski from the Technical University of Szczecin. The procedure understood the principle that a weld is the weakest point in welded structures. The results of these tests were a great surprise to the organizers. In 34 bridges, internal technological cracks and hot cracks were ascertained in 437 welded butt splices (Figure 6).
To answer the question, “What do we do with theses bridges?”, laboratory fatigue strength tests were carried out on three typical structural solutions which reflected the details in the early welded bridges. Specimens U, C, and P and the test results are given in Figure 7. The tests were carried out on 60 specimens, each time loaded at 5 loading levels. The tests are presented more precisely in [3]. They allowed, using the least-square method, fatigue class values according to EN ISO 5817: 2014 to be estimated [22, 23]. The following fatigue classes (ΔσC) were obtained for individual specimens from different constructions:
specimens U with butt welds of an acceptable quality level, fatigue class ΔσC = 125 MPa.
specimens C with an internal crack in the butt welds, fatigue class ΔσC = 90 MPa.
specimens P with butt welds covered by one-sided rhombic cover plates, fatigue class ΔσC = 79 MPa.
Fatigue strength test results for U – Sound welds (uncracked), C – Welds with internal cracks, and P – Welds covered by one-sided rhomboid cover plates.
The tests were carried out using a pulsator of frequency 5 Hz and stress ratio R = 0.1. Of note is the low fatigue class ΔσC = 79 MPa for specimens “strengthened” with rhombic cover plates. The rhombic cover plates had been intended to secure welded butt splices in early welded bridges, but the fatigue effects appeared to be quite the opposite. The results of the tests (Figure 7) clearly show that for the number of load cycles Ni larger than 1.1·106, the fatigue strength of the specimens with cover plates is lower than the fatigue strength of the specimens with cracked butt welds (type C).
The results of fatigue tests on 16 specimens with rhomboid cover plates give cause for reflection (Figure 8). Specimens with dimensions 180×12×720 mm were manufactured from Polish mild steel St3M for bridges (C = 0.19%, Mn = 0.66%) of fy = 312 MPa and fu = 452 MPa. The tests were carried out according to the Polish standard on fatigue tests on metals using five stress levels: 75, 80, 100, 120, and 140 MPa. The tests were performed on a pulsator with 5-Hz frequency. The first cracks appeared near the welded end of the cover plate and spread toward the specimen edges. In three specimens with stress levels 80, 100, and 140 MPa, the cracks appeared at 99·103, 168.9·103, and 20·103 cycles before total fracture. However, two specimens at stress level 80 MPa were not damaged, despite being loaded by 1819.8·103 and 836.8·103 cycles after the first cracks appeared (Figure 9). The test results for 13 damaged specimens allow us to work out the logarithmic regression equation.
Fatigue test results on 16 specimens and regression analysis.
Undamaged specimens after 3637·103 and 2827·103 load cycles (cracks after 1817.2·103 and 1990.2·103 load cycles).
The tests show stress concentrations by rhomboid cover plates mainly at their ends [14]. The fatigue strength value resulting from using cover plates depends on their shapes, as well as their length (Table 1). The lowest value is reached when the additional element is shortened up to 300 mm.
Effect of cover plates on the fatigue strength.
The fatigue behavior of metals is determined precisely in [20, 24, 25, 26]. Fatigue hypotheses, dislocation structures, fatigue cracking, and their fractures are given there. The issue of no crack growth in existing structures in service is also discussed there. Such cracks appear when the initiation crack stress is lower than the value of stress necessary for crack propagation. The undamaged service of these structures and the lack of propagation cracks is because no situation has arisen during service which would lead to their appearance. Many hypotheses resulting from laboratory tests have been put forward, including the oldest tests on wagon axle models (Ø 50 mm), carried out by T.V. Buchwalter as early as 1938 [27, 28]. Generally, there is no one solution for the three-dimensional problem of fatigue fractures. However, a material experiment review laid out the directions for further research to find a more precise solution to the problem. There is the optimistic fact that as early as 1965, Kudriawcew [29] stated “structural sections in which non-propagating cracks develop may be stronger than sections constructed with notches.”
The prediction of eventual fatigue cracking in welded butt splices in the railway bridges tested was assessed on the basis of strength analysis for three selected bridges. These are plate girder bridges constructed in 1938, 1938, and 1947 on different railway lines. Their technical characteristics are given in Table 2. This is a compilation of requirements collated in two papers [7, 16] relating to the structures.
Bridge No. (year built) | Number | Span length | Stress σ, MPa | ||||
---|---|---|---|---|---|---|---|
Girder (tested) | X-rays (cracks) | Dead load | Live actions | Dead + measured | |||
LM 71 | Service | ||||||
1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 |
I (1938) | 6 (2) | 128 (8) | 22.40 | a = 10/14 | 81/108 | 47/63 | |
b = 12/14 | 94/111 | 54/64 | |||||
c = 13/15 | 99/114 | 57/65 | |||||
II (1939) | 6 (1) | 144 (39) | 20.20 | a = 14/17 | 116/137 | 68/80 | |
b = 15/17 | 122/138 | 74/84 | |||||
c = 15/17 | 124/137 | 72/80 | |||||
III (1947) | 12 (3) | 360 (5) | 21.20 | a = 9/10 | 80/93 | 47/55 | 50/59 |
b = 10/11 | 89/101 | 52/59 | 52/61 |
Bridges, their technical data, and normal stresses in butt welds with cracks as well as behind cover plates.
The analysis was undertaken on the three bridges. They were constructed either side of WWII. In total, there were six examinations of the welded butt splices, and three additional tests limited to the testing of splices with cracks. The additional examinations were executed in 5–8-year time intervals. Overall, 632 X-rays were taken and 49 technological hot cracks were discovered. The calculated stress values at the butt splice locations in the lower chords of the plate girders are given in columns 5–7 in Table 2. Column 8 shows the results of service stresses measured on the welded joints of bridge III located on the Katowice–Tczew coal railway line. The permanent load and the electric locomotive ST-21 (live load) are taken into account. The great similarity of stresses calculated theoretically (column 7) and stresses measured “in situ” on bridge III (column 8) are of note.
Locations of welded butt splices:
The calculations assume the creation of a national set of standards, i.e. Polish bridge standards: PN-85/S-10030 and PN-82/S-10052 for actions and steel bridges, respectively. The characteristic values of the live action effects with dynamic factor Φ are taken into account. The standard load model in the form of the contemporary Eurocode railway traffic model LM 71 for loading class k = +2 is under consideration. The stresses were determined on the butt weld and cover plate axis as well as in the flange plates just behind the ends of the rhombic plates (values in denominators). It is easy to see that the service values of stresses in column 7 are from 60 to 70% of the stress values for the standard loading (LM 71) in column 6. This means that they are also lower than the values of Zrj = ΔσC = 79 MPa determined according to Figure 7, i.e. the service stresses are lower than the limit value for such joints determined in [3].
Considering the load spectra recommended by the JRC (Joint Research Centre) for railway bridges [1], the above value of loading will be smaller. The authors conducted such analyses and described them in [2, 30].
The load spectrum given in Figure 10 according to the old British standard BS 153 was established in structural calculations [29, 30, 31]. The method allows the service life of bridge structures to be prolonged by as much as three times. The authors recommend this method for the endurance assessment of historical bridges.
Stress ratio frequency.
In some countries, the results of traffic load measurements have been published, giving the load spectra for analyzing existing bridges [32, 33]. New standards and guides for the testing and assessment of existing bridges have appeared [19, 34, 35, 36, 37].
The first welded bridge designers were aware that “a weld is the weakest place in the structure.” Because of welding imperfections, their resistance is lower than that of the welded material. The simplest and the most economical way to eliminate these differences seemed to be enlargement of the welded joint section by adding cover plates which compensated for the weakened section. In the welded plate girders of railway bridges constructed up to 1939 and in the period from 1945 to 1953, the butt splices of webs and flanges were covered with one- or two-sided cover plates [3].
In the 154 railway bridges which were checked radiographically, internal cracking was discovered in 438 welded joints. In this group, there were 28 plate girder structures; the constructions of their lower flanges are shown in Figure 11. In 18 structures, their butt splices are covered with one-sided rhomboid cover plates from the side of the girder longitudinal axis. The rhomboid cover plates are from 90 to 200 mm in width and from 160 to 340 mm long.
Details of welded butt splices with cracks in 28 plate girder bridges.
To assess the endurance of such types of joints, fatigue strength tests were undertaken, which were discussed in Section 4. The results of the tests and the regression line are given in Figure 8. The determined infinitive fatigue strength value Zrj = 79 MPa at Ni = 2·106 load cycles constitutes only 26% of yield strength fy = 302 MPa for the steel of the specimens tested. It is worth mentioning that for three stress levels σ = 80, 100, and 140 MPa, on five specimens seven cracks appeared, as shown in Figure 12.
Cracks in flanges with rhomboid cover plates after fatigue tests: The top three specimens – Damaged and the bottom two specimens – Undamaged.
The results of the fatigue tests show a very low fatigue limit value for the welded butt splices covered with rhomboid plates. The problem was solved numerically using an FEM model as shown in Figure 13. More details of the numerical analysis are given in [38, 39].
Numerical model for analysis of a welded butt splice with cover plates.
For the numerical analysis, the welded splice was modeled using the FEM method (Figure 14) with Inventor Nastran software. Material parameters for structural steel are fy = 249 MPa and fu = 360 MPa. The stresses were calculated in four cross sections and on nine points for each section. Loading was modeled as 162, 173, 216, 260, and 303 kN tensile forces with 75, 80, 100, 120, and 140 MPa course tensile stresses in the flange. The same stress levels were formulated as for the laboratory fatigue tests.
Details of the numerical model with cracks and structural steel material data.
Analysis of the tensile stresses in the welded joint allowed us to formulate some remarks:
rhomboid cover plates do not lower the stresses in a butt weld as was initially assumed (see Table 1); it was expected that the resistance of the joint would be increased by 25.9%;
cover plates appeared to be unnecessary components, causing some additional fatigue problems;
at the ends of the cover plates, the concentration of stresses appear within a range of 1.47–1.69;
the stress concentration together with the smallest concentration factor for globular (spherical) nonmetallic inclusions of 2.04 are the reasons for the formation of one-sided stochastic cracking already at the 80-MPa stress level (Figure 13); thus σ = 80.1.69.2.04 = 275 MPa which is greater than the steel yield strength fy = 249 MPa [39].
Cracks appeared at three stress levels, σ = 80, 100, and 140 MPa, with a varied number of load cycles from 535,000 to 990,200.
These are fatigue cracks developing in stages, as opposed to the rapidly developing cracks in the fatigue tests of welded joints on specimens U, C, and P (Figure 8). All the cracks had a similar fracture as shown in Figure 15, with three developing trajectories: I – crack initiations, II – growth, and III – final fracture. The scheme of fatigue crack zones is shown in Figure 16.
Fracture surface of a broken specimen after the fatigue testing (see
Scheme of a fatigue crack: Zone I – Origin, zone II – Fatigue zone and zone III – Final fracture.
The stress distribution on the circumference of the cracks is similar, with the smallest values in the upper zone. The values are equal to the upper values of yield strength fy = 280 MPa, while the maximum stress σ ∼ 306 MPa appeared at the crack tip.
A study of the literature shows that no direct criterion has been established for precise cracking in zones I and II, e.g. the zones of settled crack growth, and zone III (unstable crack growth). This has not been achieved since 1913 (C. E. Inglis) despite the development of 64 growing hypotheses at the microstructure level and thousands of publications [27, 28, 40, 41]. For example, after the chapter, “Fatigue crack growth” in [27], there is a list of 469 supplementary readings. Crack growth is described there probabilistically in a way that is comprehensible only for specialists.
Considering the results of the numerical calculations of stresses in cracked joints in Figure 17, a new way for describing ductile fracture growth (zone II) may be suggested. The analysis takes into account two laws of physics:
ductile fracture growth may be restrained at any moment by lowering stresses below the material’s yield strength;
the moving peaks of the upper size of the fracture with length 2 t on the top surface will first reach the elastic stress area σ = 99–100 and 100–104 MPa at stress level 100 MPa as well as σ = 172–180 and 176–180 MPa at stress level 140 MPa – see Figure 17. This is guaranteed by the geometry of the fracture t/h ∼ 2 and is assured by fracture surface analysis which shows that the fracture growth is along the top surface rather than into the material.
Concentration of stresses at the ends of cover plates for stress levels: 100 and 140 MPa.
There is a reduction in edge surface stresses on the top surface to the measured values 274–310 MPa, i.e. to the upper yield strength of the material fyH = 280 MPa. The growth of ductile fracture disappears at the edge points on the top surface. This phenomenon evolves in the nearby “deep” points of the fracture and according to the stress equalizing rule, it gradually restrains a two-sided fracture from proceeding to the tip of the fracture. The cracking growth in zone II disappears totally.
Generally, it should be stated that no comprehensive model for a general description of fatigue fractures has yet been devised. All models described in the literature relate only to growth zones I and II. The only known model for transition from fracture zone to final fracture, zone III, was devised by A.H. Cottrel and N.J. Petch [40, 42]. The Cottrel–Petch theory describes the ductile-brittle transition properties of steel. A basis for the transition is assumed yield strength σpl.
When the yield strength is larger than the fracture growth stress, then the material is brittle and vice versa. “Brittle fracture will occur when the work of applied stress σ during fracture growth reaches the effective energy of newly formed surfaces.” This means that brittle fracture will occur under stress σ = σpl (Figure 17).
An explanation for this phenomenon in relation to the five cracks in the three damaged joints (Figure 12) is given in [38]. In the analysis, the results obtained during fatigue strength tests for three types of joints were used (Figure 7). Practically, this applies to the infinitive fatigue strength values Zrj given as a function of load cycles Ni.
During their service life, bridges, like other structures, undergo functional and material degradation. In many cases, tests show that despite non-strict conformity with actual design standards, they are able to carry actual service loadings. According to [1], calculations of existing steel bridges resistance should be carried out more precisely and in a more readable manner following a three-phase assessment: a preliminary evaluation, a detailed investigation, and an expert investigation. Some other studies have recommended using five assessment levels: a bridge rating, a preliminary evaluation, a detailed investigation, an expert investigation, and advance testing [16, 35, 36, 37]. Application of the assessment procedure led to improvements in knowledge and a calibration of confidence factors.
At the same time, the project “Sustainable bridges – assessment for future traffic demands and longer lives” with nine packages, deals with the increasing capacity and service life of existing railway bridges [35]. New methods for the resistance assessment of existing bridges were developed in standards and guidelines using calibrated partial safety coefficients.
The Steel Structure Chair at the Technical University in Szczecin (now WPUT) contributed to these issues by carrying out a multiyear program for the quality-level assessment of welded butt splices in existing railway bridges in service in Poland. Radiological tests on butt splices in the steel girders of around 200 railway bridges were carried out. Nearly, 200 bridges were tested using X-ray examination over a 37-year period. The number of joints tested was over 15,000; cracks were discovered in 400 welded joints in 34 bridges tested. Repeated tests on welded joints with cracks were undertaken as well as laboratory investigations for their complex assessment. Partial results of the laboratory fatigue testing are given in the paper.
Numerical analysis of tensile stresses in welded splices was undertaken to support and confirm the results of laboratory fatigue tests. The results of the FEM analysis of tensile stresses in welded joints with rhomboid cover plates are given. The FEM method allowed us to determine tensile stresses at each service stage. The analysis allowed for:
negative assessment of the welded joint type with cover plates – total disqualification of cover plates;
suggesting a new hypothesis for the initiation and growth of the surface fatigue fractures;
conformity assessment for the Cottrell–Petch theory for the transition from ductile fracture to brittle state at the final fracture.
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Shohel"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}]},subject:{topic:{id:"954",title:"Thermodynamics",slug:"thermodynamics",parent:{id:"158",title:"Metals and Nonmetals",slug:"metals-and-nonmetals"},numberOfBooks:2,numberOfSeries:0,numberOfAuthorsAndEditors:61,numberOfWosCitations:7,numberOfCrossrefCitations:10,numberOfDimensionsCitations:15,videoUrl:null,fallbackUrl:null,description:null},booksByTopicFilter:{topicId:"954",sort:"-publishedDate",limit:12,offset:0},booksByTopicCollection:[{type:"book",id:"8416",title:"Non-Equilibrium Particle Dynamics",subtitle:null,isOpenForSubmission:!1,hash:"2c3add7639dcd1cb442cb4313ea64e3a",slug:"non-equilibrium-particle-dynamics",bookSignature:"Albert S. 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Kim"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"7661",title:"Heat and Mass Transfer",subtitle:"Advances in Science and Technology Applications",isOpenForSubmission:!1,hash:"c29b5c2ce24925a935ca52b8344fbb99",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",bookSignature:"Alfredo Iranzo",coverURL:"https://cdn.intechopen.com/books/images_new/7661.jpg",editedByType:"Edited by",editors:[{id:"67352",title:"Dr.",name:"Alfredo",middleName:null,surname:"Iranzo",slug:"alfredo-iranzo",fullName:"Alfredo Iranzo"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}],booksByTopicTotal:2,seriesByTopicCollection:[],seriesByTopicTotal:0,mostCitedChapters:[{id:"67726",doi:"10.5772/intechopen.86322",title:"CFD Simulation of Heat and Mass Transfer for Climate Control in Greenhouses",slug:"cfd-simulation-of-heat-and-mass-transfer-for-climate-control-in-greenhouses",totalDownloads:1120,totalCrossrefCites:3,totalDimensionsCites:3,abstract:"Greenhouse plant production involves a number of processes such as transpiration, condensation, photosynthesis, and climate control. Such processes, in turn, set off mass and heat transfer phenomena that influence not only the quality and quantity of crop production but also its environmental cost. While these processes have considerably been analyzed in separate, they strongly interact with one another. For instance, increased radiation (mainly thermal infrared) increases temperature, reduces humidity, consequently increases transpiration, and affects CO2 exchange as well as other reaction rates. Computational fluid dynamics (CFD) is a numerical tool with a solid physical basis which allows, through the construction of a computational model, to simulate the fluid flow environment. Heating, ventilation, and condensation have been analyzed in the greenhouse environment with CFD techniques. The current challenge is the interaction of these processes and their impact on the production system. The present work summarizes some CFD investigations carried out in this topic, in order to analyze the processes of heat and mass transfer in a greenhouse for agronomic purposes.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Cruz Ernesto Aguilar Rodriguez and Jorge Flores Velazquez",authors:[{id:"173578",title:"Dr.",name:"Jorge",middleName:null,surname:"Flores-Velazquez",slug:"jorge-flores-velazquez",fullName:"Jorge Flores-Velazquez"}]},{id:"66158",doi:"10.5772/intechopen.84706",title:"Numerical Solution to Two-Dimensional Freezing and Subsequent Defrosting of Logs",slug:"numerical-solution-to-two-dimensional-freezing-and-subsequent-defrosting-of-logs",totalDownloads:620,totalCrossrefCites:3,totalDimensionsCites:3,abstract:"Two-dimensional mutually connected mathematical models have been created, solved, and verified for the transient non-linear heat conduction in logs during their freezing and subsequent defrosting. The models reflect the influence of the internal sources of latent heat of both the free and bound water on the logs’ freezing process and also the impact of the temperature on the fiber saturation point of wood species, with whose participation the current values of the thermo-physical characteristics in each separate volume point of the subjected to freezing and subsequent defrosting logs are computed. The chapter presents solutions of the models with explicit form of the finite-difference method and their validation towards own experimental studies. Results from experimental and simulative investigation of 2D non-stationary temperature distribution in the longitudinal section of beech and pine logs with a diameter of 0.24 m and length of 0.48 m during their many hours freezing in a freezer and subsequent defrosting at room temperature are presented, visualized, and analyzed.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Nencho Deliiski and Natalia Tumbarkova",authors:[{id:"43040",title:"Prof.",name:"Nencho",middleName:"Stanev",surname:"Deliiski",slug:"nencho-deliiski",fullName:"Nencho Deliiski"},{id:"284649",title:"Dr.",name:"Natalia",middleName:"Yordanova",surname:"Tumbarkova",slug:"natalia-tumbarkova",fullName:"Natalia Tumbarkova"}]},{id:"67626",doi:"10.5772/intechopen.86738",title:"The Boundary Element Method for Fluctuating Active Colloids",slug:"the-boundary-element-method-for-fluctuating-active-colloids",totalDownloads:920,totalCrossrefCites:0,totalDimensionsCites:2,abstract:"The boundary element method (BEM) is a computational method particularly suited to solution of linear partial differential equations (PDEs), including the Laplace and Stokes equations, in complex geometries. The PDEs are formulated as boundary integral equations over bounding surfaces, which can be discretized for numerical solution. This manuscript reviews application of the BEM for simulation of the dynamics of “active” colloids that can self-propel through liquid solution. We introduce basic concepts and model equations for both catalytically active colloids and the “squirmer” model of a ciliated biological microswimmer. We review the foundations of the BEM for both the Laplace and Stokes equations, including the application to confined geometries, and the extension of the method to include thermal fluctuations of the colloid. Finally, we discuss recent and potential applications to research problems concerning active colloids. The aim of this review is to facilitate development and adoption of boundary element models that capture the interplay of deterministic and stochastic effects in the dynamics of active colloids.",book:{id:"8416",slug:"non-equilibrium-particle-dynamics",title:"Non-Equilibrium Particle Dynamics",fullTitle:"Non-Equilibrium Particle Dynamics"},signatures:"William E. Uspal",authors:[{id:"279308",title:"Prof.",name:"William",middleName:null,surname:"Uspal",slug:"william-uspal",fullName:"William Uspal"}]},{id:"66487",doi:"10.5772/intechopen.85735",title:"Mean Aspects Controlling Supercritical CO2 Precipitation Processes",slug:"mean-aspects-controlling-supercritical-co-sub-2-sub-precipitation-processes",totalDownloads:736,totalCrossrefCites:1,totalDimensionsCites:2,abstract:"The use of supercritical CO2 is an excellent alternative in extraction, particle precipitation, impregnation and reaction processes due to its special properties. Solubility of the compound in supercritical CO2 drives the precipitation process in different ways. In supercritical antisolvent process, mass and heat transfers, phase equilibria, nucleation, and growth of the compound to be precipitated are the main phenomena that should be taken into account. Mass transfer conditions the morphology and particle size of the final product. This transfer could be tuned altering operating conditions. Heat transfer in non-isothermal process influences on mixing step the size of generated microparticles. In rapid expansion of supercritical solution, phenomena as the phase change from supercritical to a CO2 gas flow, rapid mass transfer and crystallization of the compound, and expansion jet define the morphology and size of the final product. These phenomena a priori could be modulated tuning a large number of operating parameters through the experiments, but the correlations and modeling of these processes are necessary to clarify the relative importance of each one. Moreover, particle agglomeration in the expansion jet and CO2 condensation are determinant phenomena which should be avoided in order to conserve fine particles in the final product.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Antonio Montes, Clara Pereyra and Enrique J. Martínez de la Ossa",authors:[{id:"55991",title:"Mr.",name:"Antonio",middleName:null,surname:"Montes",slug:"antonio-montes",fullName:"Antonio Montes"},{id:"55992",title:"Dr.",name:"Clara",middleName:null,surname:"Pereyra",slug:"clara-pereyra",fullName:"Clara Pereyra"},{id:"55993",title:"Dr.",name:"Enrique",middleName:null,surname:"Martinez De La Ossa",slug:"enrique-martinez-de-la-ossa",fullName:"Enrique Martinez De La Ossa"}]},{id:"66317",doi:"10.5772/intechopen.85254",title:"Review Heat Transfer of Non-Newtonian Fluids in Agitated Tanks",slug:"review-heat-transfer-of-non-newtonian-fluids-in-agitated-tanks",totalDownloads:1001,totalCrossrefCites:1,totalDimensionsCites:1,abstract:"The heating and cooling of non-Newtonian liquids in tanks with mechanical impellers are operations commonly employed as chemical reactors, heat exchangers, distillers, extractors, thinners and decanters. In particular, the design of heat exchangers (jackets, helical coils, spiral coils and vertical tubular baffles) in tanks requires the prior knowledge of the rheology of the liquid for the calculation of the convection coefficients and the Reynolds number, in order to obtain the area thermal exchange. This chapter aimed to present the basic concepts of tanks with agitation, non-Newtonian liquids, hydrodynamics, heat transfer and, finally, with a practical design example for engineers and undergraduate students.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Vitor da Silva Rosa and Deovaldo de Moraes Júnior",authors:[{id:"187128",title:"Ph.D.",name:"Vitor",middleName:null,surname:"Rosa",slug:"vitor-rosa",fullName:"Vitor Rosa"},{id:"188792",title:"Dr.",name:"Deovaldo",middleName:null,surname:"Moraes Júnior",slug:"deovaldo-moraes-junior",fullName:"Deovaldo Moraes Júnior"}]}],mostDownloadedChaptersLast30Days:[{id:"66878",title:"Design of Industrial Falling Film Evaporators",slug:"design-of-industrial-falling-film-evaporators",totalDownloads:1753,totalCrossrefCites:0,totalDimensionsCites:0,abstract:"The high performance evaporators are important for process industries such as food, desalination and refineries. The falling film evaporators have many advantages over flooded and vertical tubes that make them best candidate for processes industries application. The heat transfer area is the key parameter in designing of an evaporator and many correlations are available to estimate the size of tube bundle. Unfortunately, most of the correlation is available only for pure water and above 322 K saturation temperatures. Out of these conditions, the areas are designed by the extrapolation of existing correlations. We demonstrated that the actual heat transfer values are 2–3-fold higher at lower temperature and hence simple extrapolated estimation leads to inefficient and high capital cost design. We proposed an accurate heat transfer correlation for falling film evaporators that can capture both, low temperature evaporation and salt concentration effectively. It is also embedded with unique bubble-assisted evaporation parameter that can be only observed at low temperature and it enhances the heat transfer. The proposed correlation is applicable from 280 to 305 K saturation temperatures and feed water concentration ranges from 35,000 to 95,000 ppm. The uncertainty of measured data is less than 5% and RMS of regressed data is 3.5%. In this chapter, first part summarized the all available correlations and their limitations. In second part, falling film evaporation heat transfer coefficient (FFHTC) is proposed and model is developed. In the last part, experimentation is conducted and FFHTC developed and compared with conventional correlations.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Muhammad Wakil Shahzad, Muhammad Burhan and Kim Choon Ng",authors:[{id:"174208",title:"Dr.",name:"Muhammad Wakil",middleName:null,surname:"Shahzad",slug:"muhammad-wakil-shahzad",fullName:"Muhammad Wakil Shahzad"},{id:"249811",title:"Dr.",name:"Muhammad",middleName:null,surname:"Burhan",slug:"muhammad-burhan",fullName:"Muhammad Burhan"},{id:"254696",title:"Prof.",name:"Kim Choon",middleName:null,surname:"Ng",slug:"kim-choon-ng",fullName:"Kim Choon Ng"}]},{id:"66102",title:"Heat and Mass Transfer of Additive Manufacturing Processes for Metals",slug:"heat-and-mass-transfer-of-additive-manufacturing-processes-for-metals",totalDownloads:1302,totalCrossrefCites:0,totalDimensionsCites:0,abstract:"Additive manufacturing (AM), a method in which a part is fabricated layer by layer from a digital design package, provides the potential to produce complex components at reduced cost and time. Many techniques (using many different names) have been developed to accomplish this via melting or solid-state joining. However, to date, only a handful can be used to produce metallic parts that fulfill the requirements of industrial applications. The thermal physics and weld pool behaviors in metal AM process have decisive influence on the deposition quality, the microstructure and service performance of the depositions. Accurate analysis and calculation of thermal processes and weld pool behaviors are of great significance to the metallurgy analysis, stress and deformation analysis, process control and process optimization etc. Numerical modeling is also a necessary way to turn welding from qualitative description and experience-based art into quantitative analysis- and science-based engineering branch. In this chapter, two techniques for producing metal parts are explored, with a focus on the thermal science of metal AM: fluid flow and heat transfer. Selective laser melting (SLM) is the one that is most widely used because it typically has the best resolution. Another is named metal fused-coated additive manufacturing (MFCAM) that is cost competitive and efficient in producing large and middle-complex components in aerospace applications.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Zhengying Wei and Jun Du",authors:[{id:"47614",title:"Prof.",name:"Zhengying",middleName:null,surname:"Wei",slug:"zhengying-wei",fullName:"Zhengying Wei"},{id:"282052",title:"Dr.",name:"Jun",middleName:null,surname:"Du",slug:"jun-du",fullName:"Jun Du"}]},{id:"66563",title:"Heat and Mass Transfer in Outward Convex Corrugated Tube Heat Exchangers",slug:"heat-and-mass-transfer-in-outward-convex-corrugated-tube-heat-exchangers",totalDownloads:1037,totalCrossrefCites:0,totalDimensionsCites:1,abstract:"Heat and mass transfer in outward convex corrugated tube heat exchangers is of significant importance for the optimization, fabrication, and application of outward convex corrugated tube heat exchangers. This chapter gives a deep investigation of the heat and mass transfer in outward convex corrugated tube heat exchangers. Based on the experimental setup developed, the performances of a novel outward convex corrugated tube heat exchanger are presented. Simulation methods are then used to detail the heat and mass transfer at tube side and shell side of the outward convex corrugated tube heat exchanger, and these include the flow structure, temperature distribution, and turbulence kinetic energy. Heat and mass transfer enhancements of the outward convex corrugated tube heat exchanger are also studied, and they are from tube side, shell side, and overall system aspects. Finally, multi-objective optimization of the outward convex corrugated tube heat exchanger is conducted to obtain the optimal performances through using Response Surface Methodology (RSM) and Non-dominated Sorting Genetic Algorithm (NSGA-II). Main conclusions and future outlook are then briefly stated and summarized. We firmly believe that the contents presented in this chapter can not only enrich the knowledge of heat exchangers but also develop methods for studying heat exchangers.",book:{id:"7661",slug:"heat-and-mass-transfer-advances-in-science-and-technology-applications",title:"Heat and Mass Transfer",fullTitle:"Heat and Mass Transfer - Advances in Science and Technology Applications"},signatures:"Huaizhi Han, Bingxi Li, Yaning Zhang, Quan Zhu and Ruitian Yu",authors:[{id:"23828",title:"Dr.",name:"Quan",middleName:null,surname:"Zhu",slug:"quan-zhu",fullName:"Quan Zhu"},{id:"148369",title:"Prof.",name:"Bingxi",middleName:null,surname:"Li",slug:"bingxi-li",fullName:"Bingxi Li"},{id:"196928",title:"Dr.",name:"Yaning",middleName:null,surname:"Zhang",slug:"yaning-zhang",fullName:"Yaning Zhang"},{id:"281875",title:"Prof.",name:"Huaizhi",middleName:null,surname:"Han",slug:"huaizhi-han",fullName:"Huaizhi Han"},{id:"282268",title:"Mr.",name:"Ruitian",middleName:null,surname:"Yu",slug:"ruitian-yu",fullName:"Ruitian Yu"}]},{id:"66317",title:"Review Heat Transfer of Non-Newtonian Fluids in Agitated Tanks",slug:"review-heat-transfer-of-non-newtonian-fluids-in-agitated-tanks",totalDownloads:1001,totalCrossrefCites:1,totalDimensionsCites:1,abstract:"The heating and cooling of non-Newtonian liquids in tanks with mechanical impellers are operations commonly employed as chemical reactors, heat exchangers, distillers, extractors, thinners and decanters. In particular, the design of heat exchangers (jackets, helical coils, spiral coils and vertical tubular baffles) in tanks requires the prior knowledge of the rheology of the liquid for the calculation of the convection coefficients and the Reynolds number, in order to obtain the area thermal exchange. 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CSP plants utilize solar thermal energy to produce electrical energy based on different thermodynamic power cycles. Solar collectors, reflectors, receivers, thermal fluid, and turbines are the main components of each CSP plant and involve intensive heat transfer at all stages. This chapter illustrates the thermal characteristics of the main components used in CSP technology. In addition, the solar thermal fluid characteristics and its stable operational ranges are discussed in this chapter. Heat capacity, vapor pressure, volume expansion, density and viscosity of the thermal fluid should not differ significantly at different temperatures during various operation stages because these variations can cause failure in the system, which is designed at the fixed material properties. Currently, CSP technology is associated with a higher cost compared to the electricity generated through gas power plants. Many efforts are made to search for sustainable and inexpensive materials to minimize the cost of CSP. One critical issue faced by CSP technology is the intermittent nature of the sun. 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