Door torque problem

ninguen

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Jan 1, 2012
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I've got a really good torque question from Schaum's College Physics.

This one has me totally stumped. I don't quite understand the explanation they're giving here. Anyone have experience with this one?

doorproblem.JPG

How are they getting (h/4)(400N)(sin90)?
 
How are they getting (h/4)(400N)(sin90)

T = r x F sin(theta)

r = (h/4) is the distance of the cg of the door from the hinge line. F = 400N is the applied force. Theta is 90 degrees in this case.
 
T = r x F sin(theta)

r = (h/4) is the distance of the cg of the door from the hinge line. F = 400N is the applied force. Theta is 90 degrees in this case.

I still don't get it.

The way I see it, there is a virtual bar of length h/4 which sticks out perpendicular to the line between the hinges at a distance of h/2. And the 400N force being applied to the end of this bar is parallel to the line between the hinges.

So it seems that the 400N force must be applied at a diagonal angle of some sort.... with some force going downwards and some force going to the left.

How is this not the case?
 
Here's how I visualize the problem. If it were a L-shape with the h/4 bar at the top hinge, I'd understand how to work this out. But this T-shape adds a level of complexity for me.

Am I looking at this the right way?

myview.JPG

EDIT: So working around a bit, and I got the same answer as the book by treating it as an L-shaped lever. But it seems odd to me since the 100N horizontal force is being applied halfway down the door instead of at the top. So it seems to me that the torque should be different as you move downwards.

tldr; I got the right answer, but I'm still confused.
 
Last edited:
The way I see it, there is a virtual bar of length h/4 which sticks out perpendicular to the line between the hinges at a distance of h/2. And the 400N force being applied to the end of this bar is parallel to the line between the hinges.

So it seems that the 400N force must be applied at a diagonal angle of some sort.... with some force going downwards and some force going to the left.

How is this not the case?

The 400N force is *downward only* -- there is no component going to the left. It is due strictly to gravity.

Consider your drawing with the conceptual bars. The horizontal bar (h/4 in length) could be attached at the top, middle (where you have drawn it), or bottom -- and the torque it applies to point A would not change. The resultant force F would not change either. It will always be 1/4 of the vertical force, simply because its moment arm, h, is four times greater than the horizontal moment arm, h/4.
 
The 400N force is *downward only* -- there is no component going to the left. It is due strictly to gravity.

Consider your drawing with the conceptual bars. The horizontal bar (h/4 in length) could be attached at the top, middle (where you have drawn it), or bottom -- and the torque it applies to point A would not change. The resultant force F would not change either. It will always be 1/4 of the vertical force, simply because its moment arm, h, is four times greater than the horizontal moment arm, h/4.

This seems very counter-intuitive to me. But I'm going to believe you. This sounds like a great idea for an experiment later.
 
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