Integrating $\frac{dv}{dt}=g-kv^2$ from $v=0$ to $v_t$

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The discussion focuses on integrating the differential equation $\frac{dv}{dt} = g - kv^2$ from initial velocity $v=0$ to terminal velocity $v_t$, and from time $t=0$ to $t=t_f$. The user seeks guidance on achieving the correct integration result, which involves the hyperbolic tangent function. They realize that separating variables and integrating leads to the expression $\int_{0}^{v(t)}\frac{dv}{g-kv^2}=\int_0^t t'dt'$, which simplifies the problem. The user corrects a previous mistake regarding the inverse hyperbolic tangent function, clarifying its correct formulation. The conversation highlights the integration process and the realization of the hyperbolic function's role in the solution.
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I'm missing something simple here:

\frac{d\mbox{v}}{d\mbox{t}} = g - k\mbox{v}^2

I'm integrating from v=0 to v=v_t (where v_t is a known constant independant of velocity and time) and from t=0 to t=t_f, where t_f is the variable I wish to solve for in the end.

I'd rather not embarass myself by giving out the answer I produced. The actual answer has a hyperbolic tangent and I honestly am not sure how to get that. Could someone nudge me in the right direction?
 
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The inverse of the hyperbolic tangent, the Artanh function is given by:
Artanh(x)=log(\frac{1+x}{1-x})
 
You can separate the variables and integrate:

\int_{0}^{v(t<br /> )}\frac{dv}{g-kv^2}=\int_0^t t&#039;dt&#039;
 
Aha! And the derivative of that is:

\frac{1}{1-x^2} Which should take care of the problem. If only it had seemed more obvious before I had to ask! Thank you for your time arildno.
 
Thank you too for helping Galileo. I'm afraid this seems rather obvious in retrospect, which I thought it might be.

Have a good friday.
 
I'm sorry, I made a mistake:
We should have:
Artanh(x)=\frac{1}{2}log(\frac{1+x}{1-x})
This can be seen by solving for "y" from the following equation:
x=Tanh(y)\equiv\frac{e^{y}-e^{-y}}{e^{y}+e^{-y}}
 
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