One-dimensional motion with drag

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SUMMARY

This discussion focuses on solving one-dimensional motion problems involving drag forces. The user initially considered basic equations for motion but recognized the need for a more complex approach suitable for a higher-mark exam question. The key equations identified are the motion equation with drag, represented as ma = -sign(v)*F_d - mg, leading to the differential equation dv/dt = -sign(v)*b v^2 - g. The user aims to derive the functions v(t) and y(t) by integrating the motion equations.

PREREQUISITES
  • Understanding of differential equations
  • Familiarity with drag force concepts in physics
  • Knowledge of integration techniques
  • Basic principles of one-dimensional motion
NEXT STEPS
  • Study the derivation of drag force equations in one-dimensional motion
  • Learn about solving nonlinear differential equations
  • Explore numerical methods for integrating motion equations
  • Investigate the impact of varying drag coefficients on motion
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Students studying physics, particularly those focusing on mechanics and motion, as well as educators looking for examples of complex motion problems involving drag forces.

cupparamen
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Hi, this is my first time posting on this forum. This is a question about how to approach questions about one-dimensional motion with drag.

A link to the question:
http://puu.sh/5fOCO.png

While attempting this question, I thought the two equations they were referring to were:
dy/dt = v
dv/dt = -g

However, this would be far too basic for 4 marks (this is a past exam).

It would be much appreciated if you could help me out with this question.

Thanks.
 
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After some thinking, I got:

ma = -sign(v)*F_d - mg

So, a = -sign(v)*F_d/m - g

And of course I can sub in F_d which is given in the question. Not sure about how to get dy/dt though.
 
Fd is proportional to v2, say Fd/m=b.

You need to determine the functions v(t) and y(t), by solving the differential equation

dv/dt = -sign(v)*b v2 - g,

and then integrating v(t) = dy/dt to get y(t).


ehild
 

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