The changes in macroscopic properties of asphalt during UV aging are all generated by the motion collisions of microscopic particles, which originate from the transfer and transformation of energy between objects. Therefore, the change of system energy is introduced to analyze the effect of UV aging on the motion and aggregation behavior among asphalt components; the change of density and volume is introduced to analyze the effect of UV aging on the four-component structure of asphalt molecules; the glassy transition behavior is introduced to analyze the effect of UV aging on the motion state of asphalt internal chain segments; the WLF model of glass transition temperature was used to predict the viscosity of asphalt molecules in UV aging and compared with the results of the viscosity test to verify the reliability of the results of this simulation.
4.1 System energy variation
The molecular dynamics simulation results of 298K were chosen to establish the total energy variation curves and the energy variation curves at all levels for the molecular systems of normal asphalt and UV-aged asphalt, and the results are shown in Figs. 5 and 6 below.
As can be seen from Fig. 5, only at the beginning of the kinetic simulation had not yet reached equilibrium, the energy excitation inside the molecules of UV-aged asphalt was more than that of normal asphalt, and the excitation of energy inside the molecular model of normal asphalt was generally higher than that of UV-aged asphalt in the rest of the stage. The results indicated that UV aging reduced the activity of the molecules inside the asphalt and reduced the number of active molecules in the excited state, resulting in a low energy state of the system. Combined with the detailed graphs of energy changes at all levels in Fig. 6, it could be seen that with the increasing simulation time, the total energy fluctuations within the molecular system of normal asphalt and UV-aged asphalt gradually tended to a stable value, and the kinetic simulation reached an equilibrium state. Although the total energy and kinetic energy of the equilibrium normal asphalt molecular system were higher than the UV-aged asphalt molecules, and the overall energy fluctuation was more obvious, the potential energy is lower than that of the UV-aged asphalt molecular system, and the magnitude of the asphalt molecular potential energy was inversely proportional to the distance between the components. This shown that UV aging reduced the activity of asphalt molecules while increasing the distribution width between the components of asphalt molecules.
The properties of polymer molecules are not only related to the relative molecular mass and molecular structure, but also to the aggregation state between molecules. Asphalt is a polymer with light and heavy components blended together. The dispersion of molecular weight means that there is a significant interaction between the light and heavy components, and the high potential energy storage between the components ensures that they have sufficient capacity to resist stripping, giving the asphalt molecules a strong bond. Therefore, although UV aging reduced the activity of asphalt molecules and led to the weakening of the mechanical strength of asphalt, it increased the interaction between the components of asphalt molecules and improved the adhesion of asphalt molecules.
4.2 Density and volume
During molecular dynamics simulations, the density and volume of the dispersed phase are inversely proportional to each other, and density and volume are direct output parameters. However, because the molecular structure and periodic boxes of asphalt nanoaggregates in the simulation are in the same order of magnitude, the molecules of each component of asphalt undergo regional aggregation, resulting in large fluctuations of the dispersed phase density with the simulation step, so the equilibrium state density is chosen as the output with high accuracy. In order to obtained accurate simulation results, the density and volume of the dispersed phase in the last frame of the simulation step (251 frame) were selected as the output results in this paper. The simulation results of density and volume of normal asphalt and UV-aged asphalt molecules at different temperatures are shown in Table 3.
Table 3
Density and volume of asphalt molecules
Temperature(K)
|
Normal asphalt model
|
UV-aging asphalt model
|
Density(g/cm3)
|
Volume(Å3)
|
Density(g/cm3)
|
Volume(Å3)
|
195K
|
0.945
|
17162.174
|
0.985
|
13578.59
|
235K
|
0.943
|
17293.988
|
0.981
|
13669.431
|
255K
|
0.942
|
17393.866
|
0.977
|
13738.832
|
275K
|
0.939
|
17550.733
|
0.975
|
13786.749
|
295K
|
0.934
|
17860.281
|
0.966
|
13908.804
|
325K
|
0.927
|
18270.985
|
0.938
|
14251.773
|
As shown in Table 3, the kinetic behavior of the equilibrium state of both normal asphalt molecules and UV-aged asphalt molecules showed that the density of the dispersed phase decreased with the increase of the simulation temperature, while the volume gradually increased, and the density and volume of the dispersed phase showed an obvious inverse proportional relationship, which was mainly due to the kinetic simulation of the isothermal isobaric system (NPT) selected, in which the total number of molecules remained constant, the density and volume has an obvious inverse linear relationship, which also illustrates the accuracy of the asphalt model from the side.
Comparing the density and volume of normal asphalt and UV-aged asphalt molecules, it could be seen that the volume of UV-aged asphalt molecules is smaller than normal asphalt molecules at the same temperature, while the density is larger. As can be seen, the internal structural composition of asphalt molecules changed during the UV aging process, which was manifested by the degradation of polar small molecules and aggregation into large molecules, reducing the volume of asphalt molecules while increasing the density of the dispersed phase of asphalt. With the deepening of UV aging, the transformation of lighter components to heavier components in asphalt molecules became more and more obvious, which intensified the aging rate of asphalt.
4.3 Glass state transition behavior
The glassy transition behavior of the asphalt model is characterized by the thermal expansion and contraction of the occupied and free volumes of the polymer as the temperature of the system changes. However, when the temperature of the system reaches a certain temperature, only the occupied volume undergoes thermal expansion and contraction, while the free volume inside the asphalt reaches a critical value and the molecular and chain segment motions are frozen. The glass transition temperature of the asphalt polymer is the critical temperature that describes this change.
Based on the data of density and volume of normal and UV-aged asphalt molecules in Table 3, scatter graphs of density and volume at different temperatures were plotted, and linear regression curves were fitted on each side of the curve inflection point to predict the glass transition temperature of the system [Du et al. 2012]. Because of the inverse relationship between density and volume, the intersection of the two linearly fitted density scatter curves should be consistent with the intersection of the fitted volume scatter curves, and the intersection point is the glass transition temperature of the asphalt model. The density-volume scatter of normal asphalt and UV-aged asphalt molecules were linearly fitted to obtain the density-volume linear fitting curves of asphalt before and after UV-aging as shown in Fig. 7.
As can be seen from Fig. 7: the glass transition temperature of normal asphalt (Tg,Normal=268K) was about 20K lower than that of UV-aged asphalt (Tg,UV=288K). Above the glassy temperature, the density-volume variation of normal asphalt and UV-aged asphalt molecules was significant, while on the contrary, below the glassy temperature, the density-volume variation trend was flat and the asphalt molecular model was approximately in a frozen state. As the UV-aged asphalt molecules had a higher glass transition temperature, with the decrease of temperature, the free volume inside the UV-aged asphalt molecules was more likely to reach the critical value, which reduced the active state of each component molecule and chain segment, and the asphalt molecules showed low rheological behavior. Therefore, with the deepening of UV aging, the glass transition temperature of asphalt molecules increased, resulting in the movement state of asphalt molecules gradually being solidified and difficult to occur rheological behavior, reducing the low temperature resistance of asphalt molecules.
In order to present the motion of asphalt molecules more intuitively, the last frame (251 frames) of each simulation stage was selected to construct the free volume visualization of normal asphalt and UV-aged asphalt molecules (see Fig. 8), and the free volume change curves were drawn through the free volume visualization of each stage (see Fig. 9) to deeply explore the nature of the glassy state transition behavior of the asphalt model.
As can be seen from Fig. 8: Surrounding the free volume of asphalt molecules (blue area) were the chain hydrocarbon molecules and aromatic ring molecules. Referring to the structural composition of asphalt molecules, it can be found that the saturated and aromatic of the four components mainly occupy the free volume of asphalt molecules. Compared to asphaltene and resin molecules, saturated and aromatic molecules had large space for movement and high motility, and the molecules behave in an active state, which improved the overall energy of the system. This is an important reason to ensure the mobility of asphalt molecules. Combined with the detailed diagram of the free volume change of asphalt molecules in Fig. 9, the rate of free volume increase of UV-aged asphalt molecules was flatter than that of normal asphalt, indicating that UV-aging caused the reduction of components such as saturated and aromatic in the structural composition of asphalt molecules, which corroborated the conclusion of the previous section.
In summary, UV aging caused the saturated and aromatic of the asphalt molecular structure to degrade and aggregate into asphaltenes and resin, reducing the free volume of asphalt molecules while decreasing the activity of chain segment movement within the asphalt molecule. With the increase of temperature, the low activity of UV-aged asphalt molecules led to low rheological behavior of asphalt molecules, thus it can be seen that UV-aging enhances the high temperature stability performance of asphalt molecules. However, because the UV-aged asphalt molecules had a higher glass transition temperature, the chain movement inside the molecule was easily frozen, resulting in the UV-aged asphalt molecules in a solid state at low temperatures, while UV aging led to the increase of asphaltenes, resin and other macromolecular components in the asphalt molecules, which aggravated the degree of deterioration in the low-temperature resistance of UV-aged asphalt.
4.4 Viscosity simulation prediction
The viscosity of asphalt, as a characteristic most closely related to the mechanical behavior of asphalt pavements, is one of the main aspects of the research of asphalt road performance. The WLF model based on the glass transition temperature is mainly used in the asphalt molecular model to calculate the viscosity index parameters [He et al. 2020], and the detailed description of the asphalt model viscosity calculation is shown below.

Where η(T): Polymer viscosity at a temperature of T; η(Tg): Viscosity of asphalt polymers at glassy temperature, most amorphous polymers have a viscosity of about 1012 Pa·s at glassy temperature; Tg: Glass transition temperature of asphalt polymers.
Through the above Eq. (1), the viscosity of normal asphalt and UV-aged asphalt molecules at different temperatures were calculated respectively (see Table 4), and the viscosity change curve was plotted, and the results are shown in Fig. 10.
Table 4
Simulated predicted values of molecular viscosity of asphalt at different temperatures
Temperature(K)
|
lg(Simulated viscosity value)
|
Normal asphalt model
|
UV-aging asphalt model
|
295K
|
6.009
|
9.916
|
305K
|
4.716
|
7.678
|
315K
|
3.686
|
6.009
|
325K
|
2.846
|
4.716
|
335K
|
2.147
|
3.686
|
345K
|
1.557
|
2.846
|
As can be seen from Fig. 10, the viscosity of UV-aged asphalt molecules at the same temperature was higher than that of normal asphalt molecules. Due to UV aging, the saturated and aromatic fractions of the asphalt molecule were converted into asphaltene and resin. It can be inferred that heavy components such as asphaltene and gums provide viscosity to the asphalt molecules. It can be seen that UV aging enhances the viscosity of asphalt molecules and improves the high temperature stability performance of asphalt by increasing the heavy components in the asphalt molecules and increasing the distribution width between the asphalt molecule components.
Observing the curvature of the change of molecular viscosity of UV-aged asphalt in Fig. 10, it can be found that the rate of decrease of viscosity of UV-aged asphalt molecular gradually flattens out with the increase of temperature. If the change in viscosity is predicted from the rheological behavior of asphalt molecules, as the temperature increases, the asphalt molecules become more and more reactive, so the rate of decrease in the viscosity of the asphalt molecules should be more and more dramatic, but this assumption is the opposite of the results in Fig. 10. The factors that effect the change of viscosity of asphalt molecules are not only the activity of asphalt molecular, but also related to the structure and molecular weight of asphalt molecules. The increase in temperature leads to the activation of asphalt molecular energy, the molecular system energy is higher than the bond energy of branched chain hydrocarbon molecules, resulting in the degradation and aggregation of branched chain hydrocarbon molecules into heavy molecules, and the presence of heavy molecules is conducive to increasing the viscosity of asphalt molecules, thus delaying the rate of sharp decrease in viscosity of asphalt molecules due to the increase in temperature, presenting the simulation results in Fig. 10. Among the factors affecting the viscosity of asphalt molecular, the degree of effect of the molecular structure and molecular weight is significantly greater than the molecular activity. The addition of short branched chain hydrocarbon molecules to the UV-aged asphalt molecules could effectively reduce the viscosity of the asphalt molecules and improve the flowability of the asphalt molecules, thus enhancing the low-temperature resistance of UV-aged asphalt.
4.5 Experimental validation
The viscosity range that can be measured by rotational viscometer (RV) is 0.002 ~ 10000 Pa·s. The viscosity of 90# base asphalt before and after UV-aging in the temperature range of 60 ~ 120。C was determined by using RV, and the results are shown in Fig. 11.
As shown in Fig. 11, the viscosity of UV-aged asphalt was significantly higher than that of normal asphalt, indicating that UV-aging increased the viscosity of asphalt, which is consistent with the conclusions obtained from the previous kinetic simulations. With the increase of temperature, the viscosity of both UV-aged asphalt and normal asphalt decreased, and the rate of decrease gradually leveled off, and the trend of the test viscosity change curve was similar to the simulated viscosity. This verified the accuracy of the previous kinetic simulation results and conclusions.