- #1
erfz
Homework Statement
In this diagram,
I wondered if there is any torque due to the normal force from the hinge, once the support stick is removed. I also want to know what the normal force would be at the hinge. The cup and ball are to be ignored here (essentially massless).
Homework Equations
##F_{net} = ma##
##\tau_{net} = I\alpha##
##\tau = Frsin(\phi)##, where ##\phi## is the angle between F and r
The Attempt at a Solution
My assumption would be yes: there is a torque due to the normal force acting straight up from the hinge on the point touching the table. However, the solution to the problem measures torque from the hinge axis (going in and out of the page), and states that the torque is ##\tau_{net} = Mgcos(\theta)\frac{L}{2}##.
I'm confused by this, but I feel that there are two possibilities here:
- The torque due to the hinge is somehow 0
- The "net" in the expression ##\tau_{net} = I\alpha## depends on the axis it is measured with respect to, just like ##\tau = Frsin(\phi)##. That is to say that the only torques that contribute to the net are those not acting at the axis of choice.
As for the normal force at the hinge, I was thinking that I could say that ##F_{net, ~vertical} = Mg - N## at the center of mass? This happening at only the center of mass is just a guess. So then, if I go through ##\tau = I\alpha = \frac{1}{3}ML^2 \alpha = Mgcos(\theta)\frac{L}{2}##, I can derive that ##\alpha = \frac{3g}{2L}cos(\theta)## and that the linear acceleration down from this is ##a_{down} = \alpha cos(\theta) \frac{L}{2}##. Using this for the ##F_{net}##, I get that ##a_{down} = g - N##, so ##N = g - a_{down}##.
Is this reasoning correct here?
Thanks!
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