Classical Mechanics - Drag Force

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SUMMARY

The discussion focuses on the analysis of a block sliding on a slippery horizontal surface subjected to a drag force defined by F = -cv^(3/2), where c is a positive constant. The user derived the velocity function as v = [v0^(1/2) / (1 + (cv0^(1/2)t / 2m))]^2, but encountered difficulties with integrating the velocity function to find the position. A correction was made regarding the integral of the drag force, clarifying that the integral Int [dv/v^(2/3)] is indeed v^(1/3) rather than v^(1/2). The discussion also highlights the need for proper substitution techniques to simplify the integral of time.

PREREQUISITES
  • Understanding of classical mechanics principles, specifically drag forces.
  • Familiarity with calculus, particularly integration techniques.
  • Knowledge of differential equations as applied to motion.
  • Basic physics concepts related to forces and motion on horizontal surfaces.
NEXT STEPS
  • Study integration techniques for solving differential equations in classical mechanics.
  • Learn about the implications of drag forces on motion in fluid dynamics.
  • Explore the use of substitution methods in calculus for simplifying integrals.
  • Investigate the limiting behavior of functions in physics, particularly in relation to motion under drag forces.
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Students and educators in physics, particularly those focusing on classical mechanics and drag force analysis, as well as anyone interested in applying calculus to physical problems.

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Homework Statement


Suppose a block sliding on a slippery horizontal surface experiences a drag force F=-cv3/2 where c is a positive constant. At time t=0, the block is at position x=0 with initial positive velocity. Find the velocity and position as a function of time. Derive an expression for the limiting distance the block travels, or show that there is no limit.

Homework Equations


F=-cv3/2

The Attempt at a Solution



For velocity:
I took the integral of the drag force

mdv = -cv3/2 dt

int [dv/v3/2]= -c/m * int[dt]

-2/v1/2 + 2/v01/2 = -c/m * t

Isolating for v:

v= [v01/2/ 1+ (cv01/2t/2m)]2

Can someone kindly check the arithmetic if I got it right.

As for position, I have trouble dealing with the integral of the velocity function. If someone can help me regarding this, it would be greatly appreciated.
 
Last edited:
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Int [dv/v2/3] is not v1/2 but v1/3. See the error?
 
Sourabh N said:
Int [dv/v2/3] is not v1/2 but v1/3. See the error?

Yes, sorry there's a typo in the original question I put up, the drag force is F = -cv3/2 and not 2/3. Sorry for this, I hope you can go through it again. Thanks!
 
Okay. After you put v = dx/dt, the integral looks like Int [dx] = Int [dt/(a + b*t)2] where a and b are some trivial constants, right? That t integral is easy to do, you know how?

I am sleepy (read sloppy) right now, so I'd rather not fix those constants for you.
 
Hmm, it made more sense the way you put it though I still cannot determine the integral of t.
 
A substitution a + b*t = w (some random variable) brings it in the form Int [dw/w2] with some constants I have suppressed. Does it look familiar now?
 

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