Compute the velocity of a free-falling parachutist using Euler's method

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SUMMARY

The discussion focuses on computing the velocity of a free-falling parachutist using Euler's method, specifically addressing the second-order drag model represented by the equation dv/dt = g - (Cd/m)v². The parameters include a mass (m) of 80 kg and a drag coefficient (Cd) of 0.25 kg/m, with an initial upward velocity of 20 m/s. The calculations are performed from t = 0 to t = 20 seconds, with a step size of 1 second, and a change in drag coefficient to 1.5 kg/m at t = 10 seconds. Key insights include the necessity of establishing a consistent sign convention for velocity and acceleration to accurately model the physics of the scenario.

PREREQUISITES
  • Understanding of Euler's method for numerical integration
  • Familiarity with drag force concepts in physics
  • Knowledge of basic calculus, specifically derivatives
  • Proficiency in applying sign conventions in physics equations
NEXT STEPS
  • Research "Euler's method for solving differential equations" for deeper insights
  • Study "drag force equations in fluid dynamics" to understand drag effects
  • Explore "sign conventions in physics" to clarify velocity and acceleration relationships
  • Learn about "numerical stability in iterative methods" to improve computational accuracy
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This discussion is beneficial for physics students, computational scientists, and engineers involved in modeling motion under drag forces, particularly those interested in numerical methods for solving differential equations.

thornear
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Homework Statement



For the second order drag model (Eq. 1.8), compute the velocity of a free-falling parachutist using Euler's method for the case where,

m = 80 kg
Cd = .25 kg/m

Perform the calculation from t = 0 to 20 with a step size of 1 s. Use an initial condition that the parachutist has an upward velocity of 20 m/s at t = 0. At t=10 s, assume that the chute is instantaneously deployed so that the drag coefficient jumps to 1.5 kg/m.

Homework Equations



Eq. 1.8,

dv/dt = g-((Cd)/m)*v2

The Attempt at a Solution



Used equation v(ti+1) = v(ti) + [g - (Cd/m)*v(ti)2](ti+1 - ti)v

(Used in example in book, unfortunately no example w/ an initial condition with an "upward velocity" though)

Plugged in the values to achieve,

t = 0... V = 20 + [9.81 - (.25/80)(0)2] *1 = 29.81m/s
t= 1...V = 29.81 + [9.81 - (.25/80)2]*1 = 36.51m/s
t =2....V=36.51 + [9.81-(.25/80)2]*1 = 42.15 m/s
...so on until t = 10 where Cd changes from .25 to 1.5

Am I doing this right? I don't know how the "upward velocity = 20" works into this. I assumed that it is the initial v(ti) as you can see from the first solution I have where t = 0, which may or may not be horribly wrong.

Thanks, much appreciated.
 
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Since you are representing an upward velocity as positive, you must have g as negative here. Try making g negative.
 
Making g negative makes sense to me but it begins to produce negative velocities. Also I made a mistake in the above post,

t = 0... V = 20 + [9.81 - (.25/80)(0)2] *1 = 29.81m/s
t= 1...V = 29.81 + [9.81 - (.25/80)2]*1 = 36.51m/s
t =2....V=36.51 + [9.81-(.25/80)2]*1 = 42.15 m/s
...so on until t = 10 where Cd changes from .25 to 1.5

Should read

t = 0... V = 20 + [9.81 - (.25/80)(0)2] *1 = 29.81m/s
t= 1...V = 29.81 + [9.81 - (.25/80)(29.81)2]*1 = 36.51m/s
t =2....V=36.51 + [9.81-(.25/80)(36.51)2]*1 = 42.15 m/s
...so on until t = 10 where Cd changes from .25 to 1.5

But in looking at that I realize perhaps that v(ti)2 should be 202 initially rather than 02.

Thoughts? Help?

Thanks
 
Let's step back and think about the math here, and the physics as well.

You initially have the parachutist going upwards. Gravitational acceleration is obviously directed downwards. You will need some sign convention on velocity and acceleration to handle this scenario. If you choose the sign convention such that downward velocity is positive, your value for g will be positive and your initial velocity will be negative. If you choose the sign convention such that upward velocity is positive, your value for g will be negative and your initial velocity will be positive.

That is not enough to cover this scenario. The other problem is drag. Drag is always directed against the velocity vector. If your velocity is positive (regardless of sign convention), the drag acceleration must be negative. If your velocity is negative, the drag acceleration must be positive. You have drag acceleration as - (c_d/m)v^2, so it is always negative. This is incorrect for negative velocities. One way to correct this is to compute the drag acceleration as - (c_d/m)(v^3/|v|).
 
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