Angular Momentum: Rotating Object

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Speedking96
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Homework Statement



I'm trying to understand an example from my textbook about angular momentum. This is the example given:
upload_2014-12-11_16-18-1.png


For the part in red: I don't understand where the cosine theta term came from. When you're calculating the magnitudes of torques, don't you just use FRsin(theta)? If someone could clear that up for me, it would be great! Thank you.
upload_2014-12-11_16-18-1.png

upload_2014-12-11_16-18-1.png
 
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Speedking96 said:
I don't understand where the cosine theta term came from. When you're calculating the magnitudes of torques, don't you just use FRsin(theta)?
If the theta is the angle between the force vector and the distance vector, yes. But in the diagram, the angle between the vectors is the angle between the vertical and the seesaw. Theta is the angle between the horizontal and the seesaw.
 
Ok. I think I get it; the cosine is used to get the moment arm in this case, correct?
 
Speedking96 said:
Ok. I think I get it; the cosine is used to get the moment arm in this case, correct?
That's one way to look at it. There are at least 3 ways, leading to the same answer:
- distance cos (theta) = moment arm.
- force cos (theta) = component of force perpendicular to distance
- vector product of force and distance = force * distance * sin(90-theta)
 
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Ok, I understand. Thank you very much.