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Sorry if this is a newby question, but it was something I was tinkering with a bit last night
"As an object increases its speed relative to you, its relative mass increases. Therefore, if a neutron star passes by you at a certain speed, it should turn into a black hole."
The schwartzchild radius is R = \frac{2MG}{c^2} (which can be derived by setting v=c in the escape velocity equation)
So a mass of M \geq \frac{Rc^2}{2G} will be a black hole.
Using special relativity,
M = \frac{m_0}{\sqrt{1-\frac{v^2}{c^2}}}
So we can solve the equation
\frac{m_0}{\sqrt{1-\frac{v^2}{c^2}}} \geq \frac{Rc^2}{2G} for v.
\therefore v \geq \sqrt{c^2-\left(\frac{2Gm_0}{Rc}\right)^2}
If we plug in the data for a neutron star,
\rho = 4.9 \times 10^{17}\ \mbox{kg/m}^3
r = 12 \times 10^3\ \mbox{m}
We get v > 0.9c, which is certainly achievable.
In your frame of reference, you would see the star collapse into a black hole. In the neutron star's frame of reference, nothing would happen.
Does that work?
"As an object increases its speed relative to you, its relative mass increases. Therefore, if a neutron star passes by you at a certain speed, it should turn into a black hole."
The schwartzchild radius is R = \frac{2MG}{c^2} (which can be derived by setting v=c in the escape velocity equation)
So a mass of M \geq \frac{Rc^2}{2G} will be a black hole.
Using special relativity,
M = \frac{m_0}{\sqrt{1-\frac{v^2}{c^2}}}
So we can solve the equation
\frac{m_0}{\sqrt{1-\frac{v^2}{c^2}}} \geq \frac{Rc^2}{2G} for v.
\therefore v \geq \sqrt{c^2-\left(\frac{2Gm_0}{Rc}\right)^2}
If we plug in the data for a neutron star,
\rho = 4.9 \times 10^{17}\ \mbox{kg/m}^3
r = 12 \times 10^3\ \mbox{m}
We get v > 0.9c, which is certainly achievable.
In your frame of reference, you would see the star collapse into a black hole. In the neutron star's frame of reference, nothing would happen.
Does that work?