Figure 3.
The evolution of the scale of the fireball (left), its time derivative (center), and the temperature (right) as a function of time for an exact solution of the non-relativistic Navier-Stokes equations for fixed = 250 MeV, = 5 fm and = 0 initial parameters. We assume a nuclear fluid here with m = 940 MeV particle mass and a constant, temperature-independent κ parameter: κ = 3. The solid black line stands for a perfect fluid solution, while the dashed blue, the dotted–dashed green, the dashed yellow, and the dotted–dashed red lines correspond to our new viscous solution of non-relativistic Navier-Stokes equations for different values of but for the same initial conditions.
Figure 3.
The evolution of the scale of the fireball (left), its time derivative (center), and the temperature (right) as a function of time for an exact solution of the non-relativistic Navier-Stokes equations for fixed = 250 MeV, = 5 fm and = 0 initial parameters. We assume a nuclear fluid here with m = 940 MeV particle mass and a constant, temperature-independent κ parameter: κ = 3. The solid black line stands for a perfect fluid solution, while the dashed blue, the dotted–dashed green, the dashed yellow, and the dotted–dashed red lines correspond to our new viscous solution of non-relativistic Navier-Stokes equations for different values of but for the same initial conditions.
Figure 4.
The evolution of the scale of the fireball (left), the scale velocity (center), and the temperature (right) as a function of time for the solution of the non-relativistic Navier-Stokes equations for = 250 MeV, = 5 fm, and = 0 initial parameters, utilising an m = 940 MeV for the particle mass and a constant, temperature-independent κ = 3. The solid black line stands for a perfect fluid solution, and this perfect fluid curve labelled by zero bulk viscosity is approached by each of the shown exact viscous solutions asymptotically, ~ . The dashed blue, the dotted–dashed green, the dashed yellow, and the dotted–dashed red lines correspond to our new viscous solution of non-relativistic Navier-Stokes equations for different values of , but for the same asymptotic solutions.
Figure 4.
The evolution of the scale of the fireball (left), the scale velocity (center), and the temperature (right) as a function of time for the solution of the non-relativistic Navier-Stokes equations for = 250 MeV, = 5 fm, and = 0 initial parameters, utilising an m = 940 MeV for the particle mass and a constant, temperature-independent κ = 3. The solid black line stands for a perfect fluid solution, and this perfect fluid curve labelled by zero bulk viscosity is approached by each of the shown exact viscous solutions asymptotically, ~ . The dashed blue, the dotted–dashed green, the dashed yellow, and the dotted–dashed red lines correspond to our new viscous solution of non-relativistic Navier-Stokes equations for different values of , but for the same asymptotic solutions.