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there'll be some α,
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and this thing called torque is I·α.
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Now, I think it's very clear
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that if I had several forces acting on the body,
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then the torque will be ∑ (Fi·Ri),
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and there's just one final caveat to this thing,
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one final qualification,
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which is that, in practice,
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the forces that are used to rotate a body
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may not always be perpendicular.
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You can apply a force in some other direction,
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like that.