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jbriggs444
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I am having trouble following your logic.Specter said:You said that the normal component of the gravitational force plus the normal component of the contact force will total to give you the net force in the normal direction.
I now see that the normal component of the contact force is ##F_N##. I don't know what the normal component of gravitational force would be. I thought it would be ##mg\sin \theta## because it is perpendicular to ##mg\cos \theta## and ##F_N=mg\cos \theta##. If that's not the case, would the normal component of gravitational force be ##mg## then?
The point of this little exercise is to determine ##F_N##. If you've already decided that ##F_N=mg\cos \theta## then you are done.
The appropriate reasoning would be as follows:
Write down a force balance for the object in the normal direction. There are two relevant forces in this direction. One is the normal component of the gravitational force. That component is ##F_{gy}##. It is directed negative (into the surface) and has a magnitude of ##mg \cos \theta##. The other is the normal force (aka the normal component of the total contact force). It is directed positive (out of the surface). Its magnitude is unknown. The whole point of this little sub-exercise is to determine ##F_N##.
We can write down the force balance equation. ΣF=ma: ##-mg \cos \theta + F_N = ma_N##
The object is not accelerating perpendicular to the surface. It is simply sitting there or sliding. So ##a_N = 0##.
Solve for ##F_N##. What do you get?
Nowhere in this line of reasoning does ##mg \sin \theta## come in. It is irrelevant to the normal direction. It might have some relevance if we were doing a force balance in the tangential direction. But we are not doing any such thing at this point. Put it right out of your head.
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