《新整理施工方案大全》翻 译 原 文.doc

翻 译 原 文Low-temperature failure behavior of bituminous binders and mixesABSTRACTA research including a large experimental campaign on the thermo-mechanical behavior of different bituminous materials in the large strain amplitude domain is proposed. The primary goal of this paper is to identify and determine the links between the failure properties of bituminous binders and those of mixes at low temperatures.The thermo-mechanical behavior of bituminous binders was evaluated with the tensile strength at a constant strain rate and constant temperatures. The thermo-mechanical behavior of bituminous mixes has been studied byperforming measurements of the coefficient of thermal dilatation and contraction, tensile tests at constant temperatures and strain rates, and Thermal Stress Restrained Specimen Tests. Some pertinent links between fundamental properties of binders and mixes are established. Some characteristics which appear as pertinent and discriminating enough with regard to the low-temperature failure properties of bituminous mixes are presented.Keywords : bitumens, bituminous mixes, rheological behavior, thermo-mechanical properties, failure properties, tensile strength, TSRST, low temperature, brittle, ductile, brittle/ductile transition temperature.INTRODUCTIONThe different domains of bitumen behavior can be illustrated according to the strain amplitude (_) and the temperature (T), at a given strain rate. FIGURE 1 (drawn from (1) and (2) points out : the brittle and ductile domains, where the tensile strength p can be measured, the brittle failure, which could be characterized by the fracture toughness Kc (Linear Elastic FractureMechanics), the linear elastic behavior, characterized by the moduli E and G, the linear viscoelastic domain, characterized by the complex moduli E* and G*, the purely viscous (Newtonian) behavior, characterized by the viscosity , for strains of a few percent, the domain where the behavior is highly non-linear.A bituminous mix has also a complex temperature-sensitive behavior. Its response to a given loading is strongly dependent on temperature and loading path. In addition, at a given temperature and a given strain rate, four main typical behaviors can be identified according to the strain amplitude () and the number of applied cyclic loadings (N) (see FIGURE 2, from (3).This paper is aimed at providing an assessment of the work conducted to date within the framework of a partnership between the “Département Génie Civil et Bâtiment” of the Ecole Nationale des TPE, Appia and Eurovia. This study focused on the thermo-mechanical behavior of different bituminous materials in both the small strain domain and the large strain domain, at low and mid temperatures, when considering only a small number of loadings This paper only deals with the characterization of the failure properties (i.e. in the large strain amplitude domain) of bituminous materials, at low and mid temperatures. It may be underlined that this paper completes two previous papers which focused on the linear viscoelastic behavior of bituminous materials (i.e. in the small strain domain) at low and intermediate temperatures (2) and (4).MATERIALSFour very different bitumens have been tested : two pure bitumens (10/20 and 50/70 penetration grade), and two polymer modified bitumens with a high content of polymer, one with plastomer and one with elastomer. The polymer modified binders are named hereafter PMB1 and PMB2. TABLE 1 presents the results of the conventional tests (the Fraass brittle point, the Penetration at 25°C and the Softening Point Ring and Ball) initially performed on the different binders.Four different bituminous mixes, made from the 10/20, 50/70, PMB1 and PMB2 bitumens with one type of aggregate and grading, have been tested. The mixture samples had a continuous 0/10mm diorite grading, a 3±1% void content and a binder content of 6% by dry weight of aggregate.TESTS ON BINDERSSHRP Direct Tensile Tests (DTT)As described in AASHTO TP3 and (5), the SHRP Direct Tensile Test consists in elongating 27mm high bitumen samples at 1mm/min and at constant temperatures. The corresponding strain rate () equals 2.22m/m/h. At least six repeats at each temperature were realized on unaged samples. Apart from the determination of the conventional temperature leading to failure at 1% strain, T=1%, our analysis also consists in characterizing a threshold temperature separating the brittle behavior and the ductile one. Moreover, the tensile strength (maximum tensile stress) and thecorresponding strain for each temperature are considered and represented in FIGURE 3.In our opinion, the ranking of binders in function of their strain tolerance using the parameter T=1% does not seem to be really pertinent in the sense that this approach is rather empirical. This parameter will be hereafter compared with a new concept of brittle/ductile transition temperature of binders, which is introduced at the studied strain rate. The determination of this brittle/ductile transition temperature of binders is explained in the next paragraphs.Any isothermal direct tensile test yields much more data than just failure strain or stress values. In particular, the brittle-like or the ductile-like shape of the stress-strain curve can be examined at each temperature. Athigh temperatures, binders have a purely ductile behavior, whereas at very low temperatures their behavior is purely fragile. Following the considered temperature, the bitumen behavior sweeps from ductile (high temperature) to brittle (low temperature). Nevertheless, at intermediate temperatures, there is a slow evolution of the behavior from a ductile one to a brittle one when decreasing the temperature. Thus, practically, there is no determining an accuratetransition temperature directly from the examination of the shape of the stress-strain curve. In the best case, it is just possible to determine a more or less wide temperature range which corresponds to this slow transition of thephysical properties of binders.From our results, we introduce a brittle/ductile transition temperature of binders at the studied strain rate,Tbdb, which is the temperature at which the tensile strength peaks in the axes tensile strength-temperature (FIGURE3). This makes the determination of Tbdb easier and more accurate since the maximum of the tensile strength may be clearly identified. King et al. (5) have already noticed that when the temperature drops below about -15°C, the tensile strength of bituminous mixtures decreases and the tensile specimen fractures at low strain as a brittle failure.The brittle/ductile transition temperature, hereafter named Tbdb (for a strain rate of 2.22m/m/h), can be considered as a pertinent, handy and alternative low-temperature parameter. Its physical meaning is directly linked to the type of fracture process of specimens, which influences the shape of the stress-strain curves.The values of Tbdb are presented in TABLE 1 along with the temperature corresponding to a strain of 1% at failure, T=1%. Tbdb and T=1% are highly correlated with each other (r2=0.977). Nevertheless, further investigations onother bituminous binders are still needed before any definitive conclusion can be drawn.As shown in FIGURE 3, the failure stress results are noticeably scattered at low temperatures, where the behavior is brittle. However, the performance of such a test at intermediate and high temperatures leads to a minor scatter of results. Therefore, from our results on four very different binders, the maximum tensile stress (tensilestrength) seems to be all the more repeatable than the temperature is high (FIGURE 3). As assumed by Largeaud et al. (7), the scattering at low temperature could be explained by the detrimental influence of occlusions of air bubbles in the small section of binder samples.TESTS ON MIXESDirect Tensile Tests (DTT)DTT results on mixesThese tests were performed at constant temperatures between 5°C to -46°C at constant strain rate. Two very different strain rates (300 and 45000m/m/h) were chosen so as to study the influence of strain rate upon the failure properties of bituminous mixtures. 220mm high cylindrical (diameter=80mm) samples were tested in tension using a servo-hydraulic press at the Eurovia laboratory. The strain in the sample was considered as the mean value of the measures given by three transducers placed at 120° around the sample. Two or three test replicates were performedat each temperature.On one hand, as previously shown by Di Benedetto et al. (8) (9), the experimental results on the four studied bituminous mixtures evidence that the stress at failure (viscoplastic flaw) is highly dependent on the strain rate in the ductile domain (high temperature). On the other hand, the obtained stress at failure only slightly depends upon the strain rate in the brittle domain (low temperature). So, as a first approximation, the tensile strength in the brittle domain can be considered as independent of the chosen strain rate. This point is of primary importance since a high strain rate can be used in the brittle domain in order to save time. Nevertheless, it is noteworthy that Stock and Arand (10) previously stated that in the brittle domain, at very low temperatures, the tensile strength slightly decreases while increasing the strain rate. This point needs to be deepened with further investigation.Furthermore, in reference to the transition temperature concept presented for binders, we introduced the brittle/ductile transition temperature of bituminous mixes, Tfdm, which depends on the applied strain rate (). The difference for the two considered strain rates (300 and 45000m/m/h) can reach 9°C. This low-temperatureparameter is reported in TABLE 1 for the two considered strain rates.As illustrated in FIGURE 4 where all replicate results are plotted, the scatter of results is rather small whatever the strain rate and the temperature. The repeatability of such a test on mixes appears as especially good, as well in the fragile domain as in the ductile domain.FIGURE 5 sums up the influence of both the temperature and the strain rate on the brittle/ductile behavior for tensile tests at constant strain rate on binders and mixes.DTT on binders Vs DTT on mixesAs can be seen in FIGURE 6, the tensile strength of binders found with the SHRP Direct Tensile Tests at 1mm/min (2.22m/m/h) is quite close to the tensile strength of mixes at 300m/m/h. This point is noticeable and needs furtherinvestigation. Indeed, as testing bituminous mixtures is very expensive and time-consuming, one of the current great issues is to determine methods in which the properties of mixes could be evaluated with enough accuracy from the properties of the binder and from the mix composition. To confirm these results, next steps could consist in testing another strain rate for binders (150mm/min, i.e. 333m/m/h, if possible) and also different mix compositions. In addition, in the brittle domain at very low temperatures, and only as a first approximation (lack of repeatability), the previous observations (cf. FIGURE 6) allow to consider that the tensile strength of binders equals the tensile strength of mixes which does not depend on the strain rate (FIGURE 4). To our knowledge, this statement which is sometimes supposed to be valid has been but little experimentally checked. Moreover, this statement is of the utmost importance since the failure in mixes could be predicted, as a first approximation, from the failure in binders. For instance, as regards the current revision of the AASHTO low temperature specification MP1 (MP1A), the failure stress from DTT on binders is incorporated in a comprehensive model to calculate and predict the socalled critical cracking temperature of pavement (11) (12).Coefficient of thermal dilatation/contraction of bituminous mixesThe linear coefficient of thermal dilatation/contraction “” depends on the thermal characteristics of the components of the bituminous mixture (binder, aggregate and air). It especially highly depends on the binder content since thecoefficient of linear thermal dilatation/contraction of bitumen is some 30 times greater than that of the mineral aggregate (13) (14) (15). In our study, as only one mix design is considered, the influence of the amount of binder and aggregate can not be evaluated.Parallelepipedic asphalt samples (L*W*H = 16*4*4 cm3) of the four types of investigated mixes were laid on their length on a layer of small glass marbles coated with a silicone spray. This base provides nearly frictionless movement. Each sample was submitted to different plateaus of temperature in the range of +24 to 26°C. Thetemperature was held constant for about three-hour periods after each increment of around three degrees Celsius.Two identical strain gages are used for each test : the first one is glued on the upper part of the asphalt beam, the second one on the lower part, for not taking into account the flexion of the beam during the test. The average value is considered. A third strain gage was glued on a reference titanium silicate beam, of known -value(0.03m/m/°C), in order to account for and correct the effect of temperature. In addition, a temperature probe was used to measure the temperature at the surface of asphalt samples.The thermal strain can be written as follows :=T 1where : linear coefficient of thermal dilatation/contraction (m/m/°C)T : change in temperature (°C)Thermal equilibriumAfter each temperature change, the temperature is held constant during 3 hours so as to allow the specimen, the titanium silicate beam and the three strain gages to equilibrate at the considered temperature. At the onset of this plateau of temperature, a transitional period is first observed, in which each element is contracting (or dilating) until thermal equilibrium. The transitional period of each element depends i)on its dimensions (the strain gage reaches more quickly the thermal equilibrium than the mix sample), ii)on its thermo-physical coefficients, iii)on the temperature change amplitude, iv)etc. From our results, this transitional period lasts about 1 hour.Experimental coefficientsFIGURE 7 shows that the thermal dilatation coefficient of mixes and their thermal contraction coefficient are really close (see also (16). The two coefficients are hereafter considered as equal. Moreover, FIGURE 7 highlights that the four different mixes have very close thermal contraction coefficients over the considered range of temperature (from -26 to +24°C). As Di Benedetto and Neifar (16), using a specially designed test method, and Serfass et al. (17) have already shown, a linear relationship between the thermal contraction coefficient and the temperature can beconsidered, as a first app