How do you decide whether to use cosine or sine when calculating torque?

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SUMMARY

The discussion centers on calculating torque using the correct trigonometric function, specifically cosine or sine, in relation to a particle attached to a rod. The torque equation is defined as τ = Frsin(θ), where θ is the angle between the force and position vector. The correct answer for the torque in this scenario is Lmg cos(θ), derived from the perpendicular component of the force vector to the lever arm or the perpendicular component of the lever arm to the force. Understanding the orientation of the angle in relation to the force and position vectors is crucial for determining whether to use cosine or sine.

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  • Understanding of torque and its calculation using τ = Frsin(θ)
  • Knowledge of vector decomposition in physics
  • Familiarity with gravitational force and its components
  • Basic trigonometry, specifically sine and cosine functions
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Homework Statement



I'm working through a problem:

"A particle of mass m is attached to a rod of negligible mass and length L. The rod is attached to the ground at point O. If the rod makes an angle \Theta with the horizontal as it falls, calculate the torque about point O.

Here's a rough sketch of the diagram:

scmWd.png


My book says that the equation for torque is \tau=Frsin\theta where \theta is the angle between the force and position vector.

The answer for this is Lmg cos\theta, but I don't understand why it's cosine. The book answer says to solve it in one of two ways: by multiplying the perpendicular component of the force vector to the lever arm, or by multiplying the perpendicular component of the lever arm to the force (indicating these two methods are equivilent).

How do you decide whether to use cosine or sine?

Thanks!
 
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Tybstar said:
How do you decide whether to use cosine or sine?

You basically do it like they said in your book

Tybstar said:
by multiplying the perpendicular component of the force vector to the lever arm

If you do it like this, the component of the force perpendicular to the lever arm is mgcosθ. Do you understand how the force is split into this components and a sine component parallel to the arm?

Tybstar said:
or by multiplying the perpendicular component of the lever arm to the force (indicating these two methods are equivilent).

The length of the lever arm perpendicular to the downward force mg is Lcosθ. This one should be easier to see.
 
rock.freak667 said:
If you do it like this, the component of the force perpendicular to the lever arm is mgcosθ. Do you understand how the force is split into this components and a sine component parallel to the arm?

Thanks for the help.

I do understand how the force is split with cosine and sine. My problem is figuring out which angle to use. Is it similar to assigning force vectors in an inclined plane diagram?

Thanks!
 
Tybstar said:
My book says that the equation for torque is \tau=Frsin\theta where \theta is the angle between the force and position vector.

This equation sums it up pretty nicely. Where's the force vector (hint: the force is gravity)? Where's the position vector (hint: it's the vector from the pivot to the object)? Which angle is the angle between them?
 
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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