Differential equation for grav, boyant and drag force

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SUMMARY

The discussion focuses on deriving a time-dependent distance equation for a falling object considering buoyant force, gravitational force, and drag force. The relevant equations include the drag force equation (Fd = Cd * A * pa * v^2 / 2), buoyant force equation (Fb = mg * pa / pc), and gravitational force equation (Fg = mg). The final velocity equation is v(t) = (A/B)^(1/2) * (1 + C1 * e^(-2(BA)^(1/2)t)) / (1 - C1 * e^(-2(BA)^(1/2)t)), leading to the distance formula X(t) = (A/B)^(1/2)t + (1/B) * ln(1 - C1 * e^(-2(BA)^(1/2)t)) + C2. The discussion emphasizes checking the dimensional correctness of the resulting equations and analyzing special cases.

PREREQUISITES
  • Understanding of differential equations
  • Familiarity with forces in physics, specifically buoyant and drag forces
  • Knowledge of integration techniques
  • Basic understanding of dimensional analysis
NEXT STEPS
  • Explore the derivation of the drag force equation in fluid dynamics
  • Study the principles of buoyancy and Archimedes' principle
  • Learn about the applications of differential equations in physics
  • Investigate dimensional analysis and its importance in verifying equations
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Students studying physics, particularly those focusing on mechanics and fluid dynamics, as well as educators looking for examples of applying differential equations to real-world problems involving forces.

Agustin
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Homework Statement


So there is a falling object, you have to take into account the boyant force, the pull of gravity and the drag force
A time dependent distance equation is what we're looking for

Homework Equations


Fd=CdApav2/2
Where
Fd is the drag force
Cd is the drag coefficient
A is the area exposed to the fall
pa the air density
v the immediate velocity

Fb=mgpa/pc
Fb is the boyant force
mg is the weight of the object
pc is the object's density
Note ( this equation is found from the original equation Fb=Volume submerged x air density x gravity; where the submerged volume is m/pc)

Fg=mg

The Attempt at a Solution


ma=mg - mgpa/pc - CdApav2/2
Or
dv/dt = A - Bv2
Where
A=g( 1 - pa/pc)
B=CdApa/2m

I solve for v

v (t) = (A/B)1/2 (1 + C1e-2(BA)1/2t)/( 1 - C1e-2(BA)1/2t)

Where C1 is some arbitrary constant

Integrating we get the distance formula:

X (t) = (A/B)1/2t+(1/B)ln( 1 - C1e-2 (BA)1/2t) + C2
I don't know wether it's correct or not. I've used techniques i found on the internet for the integration. http://www.freemathhelp.com/forum/threads/47073-integral-(1-(e-x-1))-dx-Using-Partial-Fractions
 
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See if it gives the right answers in special cases. For example, what does your result say for the case of no buoyant force and no drag force? What happens as ## t \rightarrow \infty ##, and what would you expect physically in this case? There are lots of things like this to look into.

Oh, and can you check that the resulting equation is dimensionally correct?
 

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