This post shows the derivation of the model between two motion variables, velocity and time, of an object experiencing free-fall motion with simple resistance.
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This post shows the solution of the ordinary differential equation (ODE) for falling bodies with fluid resistance Ff=kv, velocity-time, v-t. If you wish to discover how the ODE was derived, read here first.

dvdt+kmv=g

  • The variable v refers to the velocity of the falling objects
  • Variable t refers to the time
  • The variable k refers to the drag proportionality constant.
  • Variable m is the object's mass
  • Constant g refers to the acceleration due to gravity.

Finding the Solution for Velocity-Time

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General Solution

Given the differential equation, dvdt+kmv=g, find its general solution:

Let A=km:

dvdt+Av=g

Apply the separation of variables and integrate both sides of the equation:

dv=(gAv)dt

dvgAv=dt

1Aln(gAv)=t+C1

Distribute A:

ln(gAv)=AtC1A

Convert to exponential notation:

gAv=eAteC1A

Let eC1A=C:

gAv=CeAt

Isolate v:

v=gCeAtA

Return A:

v=m(gCekmt)k

Particular Solution

Let's find a particular solution to model the event of free-fall with simple resistance. In free-fall, we know that the initial velocity is zero at the very start t=0. If we substitute this into the general solution, we will obtain C=g; hence, the particular answer is:

v=mg(1ekmt)k

Created On
June 5, 2023
Updated On
February 23, 2024
Contributors
Edgar Christian Dirige
Founder
References

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