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Post common envelope simulation
I put a 1 solar mass object at the origin of the simulation box. There is no outflow from 0 to 500 day. From 500 to 1000 day, there is outflow for the boundary of the object. I list the physical quantities below:
Radius of the object that has outflow: r=46.875R_{\odot}
Mass of the object: 1M_{\odot}
Density of the outflow: \rho=10^{-11}g\cdot cm^{-3}
Temperature of the object: T_{1}=30000K
The outflow is asymmetric, in the polar direction (theta=0 and theta=pi), the outflow velocity is the maximum; in the equatorial plane, the outflow velocity is 0. The outflow velocity is a function of polar angle, there are two kinds of functions, linear and Gaussian - to vary the open angle. The Gaussian is narrower.
Linear: v_{r}(\theta)=v_{max}\times\frac{\|\pi-2\theta\|}{\pi}
Gaussian: v_{r}(\theta)=v_{max}\times\exp(-10(\frac{\|\pi-\|2\theta-\pi\|\|}{\pi})^{2})
Spherical: v_{r}(\theta)=v_{max}
Below shows the linear and Gaussian velocity v.s. angle.
The outflow temperature: 30000K
Outflow duration: 500 day - 1000 day
Mass loss: \dot{M}=\int_0^{\pi}2\pi\rho r^{2}\sin\theta v_{r}(\theta)d\theta. However, much of the outflow will be impeded by the surrounding gas, the actual mass loss will be lower than the calculated ones.
ID | v_{r}(0)(km\cdot s^{-1}) | \rho (g\cdot cm^{-3}) | \dot{M}(M_{\odot}\cdot yr^{-1}) | simulation | approximate expansion velocity |
1 | 300 (linear) | 10^{-11} | 2.31\times10^{-4} | 120(km\cdot s^{-1}) | |
movies:density and temperature | |||||
2 | 400 (linear) | 10^{-11} | 3.07\times10^{-4} | ||
3 | 400 (gaussian) | 10^{-12} | 1.00\times10^{-5} | ||
4 | 400 (gaussian) | 10^{-11} | 1.00\times10^{-4} | 310(km\cdot s^{-1}) | |
movies:density and temperature | |||||
5 | 300 (spherical) | 10^{-11} | 6.35\times10^{-4} | 240(km\cdot s^{-1}) | |
movies:density and temperature |
Simulations that has indefinite outflow duration. (it is always on)
ID | v_{r}(0)(km\cdot s^{-1}) | \rho (g\cdot cm^{-3}) | \dot{M}(M_{\odot}\cdot yr^{-1}) | simulation | approximate expansion velocity |
6 | 300 (spherical) | 10^{-11} | 6.35\times10^{-4} | movies:density | |
2 | 1000 (spherical) | 10^{-16} | 2.12\times10^{-8} | ||
Some questions: where exactly does the jet emerge? What are the open angle and outflow velocity. What are the outflow density and temperature?
- Posted: 7 years ago (Updated: 7 years ago)
- Author: Zhuo Chen
- Categories: (none)
Attachments (5)
- gaussian.png (7.6 KB) - added by Zhuo Chen 7 years ago.
- linear.png (8.6 KB) - added by Zhuo Chen 7 years ago.
- 1_137.png (402.9 KB) - added by Zhuo Chen 7 years ago.
- 4_105.png (462.5 KB) - added by Zhuo Chen 7 years ago.
- 5_177.png (357.2 KB) - added by Zhuo Chen 7 years ago.
Download all attachments as: .zip
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