Parachutist falling with quadratic drag

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SUMMARY

The discussion centers on the physics of a parachutist experiencing quadratic drag during free fall. The parachutist, with a mass of 80 kg and a drag coefficient of C = 3.52, achieves a terminal speed of 14.92 m/s. The calculations for the height required for a 3-minute descent involve integrating the motion equations, specifically using the relationship ma = mg - Cv². The final solutions for the height calculations are derived through integration techniques, including the use of hyperbolic functions.

PREREQUISITES
  • Understanding of Newton's second law of motion (ma = mg - Cv²)
  • Familiarity with terminal velocity calculations (Vt = (mg/C)^(1/2))
  • Knowledge of integration techniques, particularly involving hyperbolic functions
  • Ability to manipulate and solve differential equations
NEXT STEPS
  • Study the derivation of terminal velocity in fluid dynamics
  • Learn advanced integration techniques, focusing on hyperbolic functions
  • Explore the implications of quadratic drag in various physical scenarios
  • Investigate numerical methods for solving differential equations in physics
USEFUL FOR

Physics students, educators, and anyone interested in the dynamics of free fall and drag forces will benefit from this discussion.

Jukai
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MAJOR EDIT: I fixed my position integral and got the answer to 1.ii)

Homework Statement



A parachutist jumps from a helicopter that's not moving. The mass of the person is 80kg, the quadratic drag is f = -Cv^2 where C = 3,52. Neglect the Earth's rotation effect. The parachute is opened as soon as the person jumps.

i) Is there a terminal speed? if yes, what is it?

ii) What is the height at which the helicopter must be so that the parachutist stays in the air exactly 3 minutes if her initial speed is 0.

iii) If the parachutist falls with a constant speed (the terminal speed), at what height must the helicopter be so that the person stays in the air exactly 3 minutes.

Homework Equations



ma = mg -Cv^2 (1)

Vt= (mg/C)^(1/2) where Vt : terminal speed

\int(1/(1 - ((x^2)/(a^2))) = a(arctanh(x/a))
\int((tanh(x)dx)= ln(cosh(x)))

tanh(x) = (e^x - e^-x)/(e^x + e^-x)
cosh(x) = (e^x + e^-x)/2

The Attempt at a Solution



i) I got this one right. I made the logical argument that if the parachutist reaches a terminal speed, there is no more acceleration, therefore (1) becomes
mg = CV^2 and Vt = 14,92 m/s

The next questions is where I'm having intense difficulty

ii) I divide by m everywhere in (1) and factor g from the right side and I get this:

dv/(1 - ((V^2)/(Vt^2))) = gdt

Integration gives me the following:

Vt((arctanh(V/Vt)) - (arctanh(Vo/Vt)) = g(t - to)

where to and Vo are the initial time and speed

Since I'm looking for height, I need to integrate V once more. I isolate V as follows and integrate as follows:

V = Vt( (tanh(g(t - to)/Vt)) + (arctanh(Vo/Vt)))

X - Xo = ((Vt^2)/g)(ln(cosh( (g(t-to)/Vt) + (arctanh(Vo/Vt)))))

Now when I put t = 180, it works.

iii) I'm not even sure how I'm supposed to integrate when V is constant throughout the fall...

For this question, my initial speed is Vt and the problem with arctanh(1) going to infinity persists..
 
Last edited:
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Jukai said:

Homework Equations



ma = mg -Cv^2 (1)

Vt= (mg/C)^(1/2) where Vt : terminal speed

\int(1/(1 - ((x^2)/(a^2))) = a(arctanh(x/a))
\int((tanh(x)dx)= ln(cosh(x)))

tanh(x) = (e^x - e^-x)/(e^x + e^-x)
cosh(x) = (e^x + e^-x)/2

The Attempt at a Solution



i) I got this one right. I made the logical argument that if the parachutist reaches a terminal speed, there is no more acceleration, therefore (1) becomes
mg = CV^2 and Vt = 14,92 m/s

The next questions is where I'm having intense difficulty

ii) I divide by m everywhere in (1) and factor g from the right side and I get this:

dv/(1 - ((V^2)/(Vt^2))) = gdt

Integration gives me the following:

Vt((arctanh(V/Vt)) - (arctanh(Vo/Vt)) = g(t - to)

where to and Vo are the initial time and speed

Since I'm looking for height, I need to integrate V once more. I isolate V as follows and integrate as follows:

V = Vt( (tanh(g(t - to)/Vt)) + (arctanh(Vo/Vt)))
Great job so far! :approve:. But you can simplify things quite a bit by defining v0 = 0 and t0 = 0. You don't really lose any generality by doing so for this particular problem, and it gets rid of that second term.
X - Xo = Vt(ln(cosh( (g(t-to)/Vt) + (arctanh(Vo/Vt)))))

when I put t = 3 minutes = 180 seconds, I don't get the right answer.
Try this on for size. You already know that

\int \tanh x \ dx= \ln (\cosh x) + K

where K is an arbitrary constant.

Substituting x = ay, where a is a constant, and noting that dx = a dy --> dy = (1/a)dx,

\int \tanh (ay) \ dy= \frac{\ln (\cosh ay)}{a} + K

Good luck! :smile:
 
Thank you very much =), it's too easy to forget the substitution trick for integration..

last edit: (for those who care =) )So I found out iii), I just had to integrate to x starting from ma= -CV + mg where the right side are constants.
 
Last edited:

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