One-dimensional motion with drag

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The discussion focuses on solving a problem related to one-dimensional motion with drag, specifically how to approach the equations of motion when drag is involved. The initial equations considered were too simplistic for the exam context, prompting a more complex formulation involving acceleration and drag force. The key equation derived is ma = -sign(v)*F_d - mg, leading to a differential equation for velocity. To find the position function, the user must integrate the velocity function after solving the differential equation. The discussion emphasizes the importance of incorporating drag proportional to the square of velocity in the calculations.
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
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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