Integrating the force equation when velocity drops to zero

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i have a force acting on and object and I've gotten the question down to when i have to intergrate but I'm stuck on the intergral
[tex]F=-(f+cv^2)[/tex]
[tex]m \frac{dv}{dx} \frac {dx}{dt} = -(f+cv^2)[/tex]
f and c are constants
[tex]mvdv=-(f+cv^2)dx[/tex]
[tex]\frac{mvdv}{f+cv^2}=-dx[/tex]
now how do i intergrat them from [tex]v_{o} to 0 and 0 to x[/tex]
 
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This is the kind where the numerator has to be expressed as a constant times the derivative of the denominator. Find the constant and you're through. Simply put, differentiate the denominator and observe the similarity with the numerator.
 


To integrate this equation, we can use the method of partial fractions. First, we can rewrite the equation as:

\frac{mvdv}{f+cv^2}=-dx

Next, we can use the substitution u = f+cv^2, du = 2cv dv to rewrite the integral as:

\frac{m}{2c}\int\frac{du}{u}=-\int dx

Solving for u, we get:

u = f+cv^2 = f+\frac{m}{2c}\frac{du}{dv}

Substituting this back into the integral, we get:

\frac{m}{2c}\int\frac{du}{u}=-\int dx

Solving for v, we get:

v = \sqrt{\frac{2c}{m}}\sqrt{u-f}

Now, we can integrate this equation from v_{o} to 0 and 0 to x to find the final solution for v(x):

v(x) = \sqrt{\frac{2c}{m}}\left(\sqrt{f}-\sqrt{f+cx^2}\right)

This is the final solution for the velocity of the object as a function of its position. To find the position of the object, we can simply integrate the velocity function with respect to x:

x(t) = \frac{1}{c}\left(\sqrt{f}x-\frac{m}{4c}x^2+\frac{m}{4c}x_{o}^2\right)

where x_{o} is the initial position of the object.