A question about variables of integration

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SUMMARY

The discussion centers on the integration of the equation ##F^x=m\frac {d}{dt}(\gamma v^x)##, where ##\gamma## represents the Lorentz factor. The participant questions whether they can treat ##d(\gamma v^x)## as the variable of integration and if substituting ##\gamma v^x = u## simplifies the process. The conclusion reached is that the substitution is valid, and the integration follows the fundamental theorem of calculus, leading to the result ##\frac {F^x}{m}t=\gamma v^x##, confirming the textbook solution.

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TL;DR
an integral with a strange variable of integration
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 write ##\frac {F^x}{m}\int_0^t\,dt=\int_0^u\,du##? The solution would then be ##\frac {F^x}{m}t=u=\gamma v^x## as in the book. Is it really that simple? I feel uneasy about this because of the twofold dependence of ##\gamma v^x## on ##v^x##.
 
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I don't think you have to make any substitutions. In general, if:
$$f(t) = \frac{d}{dt}g(t)$$Then, by the fundamental theorem of calculus:
$$\int f(t) dt = \int \frac{d}{dt}g(t) dt = g(t) + C$$Or, in terms of the definite integral:
$$\int_{t_0}^{t_1} f(t) dt = \int_{t_0}^{t_1}\frac{d}{dt}g(t) dt = g(t_1) - g(t_0)$$
 
This is the typical example of integration: It looks awkward, but it works. What we have is
\begin{align*}
\dfrac{F^x}{m}&=\dfrac{d}{dt}\left(\gamma v^x\right)\\
\int \dfrac{F^x}{m}\,dt&=\int \dfrac{d}{dt}\left(\gamma v^x\right)\,dt \\
\dfrac{F^x}{m}\cdot t&\stackrel{u=\gamma v^x}{=}\int u'\cdot \dfrac{du}{u'}=\int du\\
\dfrac{F^x}{m}\cdot t&=u=\gamma v^x
\end{align*}
 
I made the substitution because without it my integral looked like this: ##\int d(\gamma v^x)##, which I found was a very odd looking integral. If instead I write it as ##\int \frac {d}{dt}(\gamma v^x)\,dt##, it does not look odd anymore and it all makes sense. Problem solved, thank you very much.
 

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