MHB Manipulating Differential Equations with the Chain Rule

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can anyone please help me ?

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abhay said:
can anyone please help me ?
It would help us help you if you could tell us what you are able to do on this question.

-Dan
 
You "change variables" in a differential equation using the "chain rule".

That is, $$\frac{\partial u}{\partial x}= \frac{\partial u}{\partial \xi}\frac{\partial \xi}{\partial x}+ \frac{\partial u}{\partial\tau}\frac{\partial \tau}{\partial x}$$ and $$\frac{\partial u}{\partial t}= \frac{\partial u}{\partial \xi}\frac{\partial \xi}{\partial t}+ \frac{\partial u}{\partial\tau}\frac{\partial \tau}{\partial t}$$.

Here, we are given [math]\xi= x- Vt[/math] and [math]\tau= t[/math] so [math]\frac{\partial \xi}{\partial x}= 1[/math] and [math]\frac{\partial \tau}{\partial x}= 0[/math]. [math]\frac{\partial u}{\partial x}= \frac{\partial u}{\partial \xi}[/math].

Similarly [math]\frac{\partial u}{\partial t}= \frac{\partial u}{\partial \xi}\frac{\partial \xi}{\partial t}+ \frac{\partial u}{\partial \tau}\frac{\partial \tau}{\partial t}[/math]. Since [math]\frac{\partial \xi}{\partial t}= -V[/math] and [math]\frac{\partial \tau}{\partial t}= 1[/math], [math]\frac{\partial u}{\partial t}= -V\frac{\partial u}{\partial \xi}+ \frac{\partial u}{\partial\tau}[/math].

Repeat that to get the second derivatives.
 
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I have the equation ##F^x=m\frac {d}{dt}(\gamma v^x)##, where ##\gamma## is the Lorentz factor, and ##x## is a superscript, not an exponent. In my textbook the solution is given as ##\frac {F^x}{m}t=\frac {v^x}{\sqrt {1-v^{x^2}/c^2}}##. What bothers me is, when I separate the variables I get ##\frac {F^x}{m}dt=d(\gamma v^x)##. Can I simply consider ##d(\gamma v^x)## the variable of integration without any further considerations? Can I simply make the substitution ##\gamma v^x = u## and then...

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