Using Triple integrals to solve torque around a point.

AI Thread Summary
The discussion focuses on calculating the torque around the handle of a cylindrical coffee cup filled with water using triple integrals. The setup involves defining a coordinate system with the origin at the center of the cup and applying the torque formula T = r x F, where F is the gravitational force. Participants express challenges in determining the vector r for each differential mass element dm and integrating the resulting vector field. The conversation emphasizes the importance of obtaining the torque vector's components before calculating its magnitude, which is essential for finding the final torque value. The final answer for the torque is suggested to be 0.296 N*m, but the method to arrive at this result requires clarification on integration and coordinate setup.
BSJ90
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Homework Statement


A cylindrical coffee cup (8 cm in diameter and 10 cm tall) is filled to the brim
with coffee. Neglecting the weight of the cup, determine the torque at the handle
(2 cm from edge of cup 5 cm up from bottom of cup).

The easy way would be to just use the center of mass of the cup but that isn't the way its told to be done. So triple integrals it is.

density of water(ρ) = 1g/cm3

Homework Equations


T = r x F

if R is from

The Attempt at a Solution


So to set up my coordinate's I put the origin in the center of the cylinder with x going out of the page y to the right and z up.T = r x F
= r x mFg (Fg = force of gravity)
dT = r x dmFg (dm = ρdxdydz)

\int \int\int |r|ρgdzdydx

I think (tell me if I'm wrong) the bounds of the first integral (from left to right):
-4 to 4, -\sqrt{}4-x2 to \sqrt{}4-x2, -5 to 5.

but where I'm having problem is finding an equation that relates r ( the vector from the handle to the cup) for each dm. If someone could help me out that would be great.
 
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I don't think you have to integrate anything (but then I have been drinking). You are told to ignore the mass of the cup. Assume the total mass of the water acts at it geometric center.

Torque = r X F = [8/2 +2]*m*g where m = ρ*V

??
 
BSJ90 said:
T = r x F
= r x mFg (Fg = force of gravity)
dT = r x dmFg (dm = ρdxdydz)

The force of gravity is mg. Do not multiply with the mass again.

BSJ90 said:
\int \int\int |r|ρgdzdydx

As g is vertical (parallel to the z axis), the vector product \vec r \times dm \vec{g} = -g (y \hat x -x \hat y)dm

ehild
 
Now how am I supposed to work with that. It makes sense but now I'm integrating a vector field and the only thing i can think to do is take the magnitude of that. Shouldn't it be different because the of symmetry.

Plus i tried taking the magnitude of that field and it was not fun by the time i had to do the second integral.
 
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The torque is a vector, has both x and y components, depending on the orientation of the coordinate system. You can find its magnitude after having the components, but the magnitudes do not add.

ehild
 
So how would i go about solving the problem from this point on. I mean i get a torque vector and obviously there is an answer (0.296 N * m) but I don't see how we can get from the vector field to this answer.
 
How do you set up your coordinate system? Show a picture. How do you calculate the torque vector and what is the result? If you have the torgue vector with components Tx, Ty, the magnitude is sqrt(Tx2+Ty2).

ehild
 
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