How Do You Solve for Position x(t) Given a Force Dependent on Velocity?

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The discussion focuses on solving for the position x(t) of a particle subjected to a force defined by F(v) = bv², where b is a constant and v is the velocity. The initial conditions are set with an initial position of zero and an initial speed of v_i. The participants derive the equation m*dv/dx*v = -bv² and discuss the integration process, emphasizing the importance of correctly applying constants during integration. The constants represent the initial conditions, with the lower limits corresponding to the initial position and velocity.

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A particle of mass m is subject to a force F(v) = bv^2. The initial position is zero, and the initial speed is vi find x(t)

so far

m*dv/dx*v = -bv^2
m*dv/dx = -bv
integral m/-bv*dv = integral dx
m/-b*ln(v) + a = x + b

What do I do with the constants? i thought i was suppose to put in 'a' as vi and b as 0, but then when i integrate again for v, so i can get x(t) function, what do i use to fill in that constant?
 
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Where does m*dv/dx*v = -bv^2 come from? Newton's second law of motion implies F=m*dv/dt.
 
dv/dx*v=dv/dx*dx/dt = dv/dt = a
 
OK. You use your constants in the integrations: the lower constant on the dx integral is the starting location = 0, and the lower constant on the dv integral is the initial velocity = v_i.

The upper constants are the unknowns ... your integral equation will provide a relation between them.
 

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