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

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To solve for the position x(t) of a particle under the force F(v) = bv^2, the discussion begins with applying Newton's second law, leading to the equation m*dv/dx*v = -bv^2. The integration process involves determining the constants based on initial conditions, specifically setting the lower limit for x at zero and for v at the initial speed vi. The integration results in a relationship between the constants and the variables, which must be resolved to find x(t). Clarification is provided on using constants during integration, emphasizing that the upper constants remain unknowns that the final equation will relate. The discussion highlights the importance of correctly applying initial conditions to derive the function for position over time.
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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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