Static equilibrium involving toque

In summary: So, the components can be thought of as rotated from your diagram by an angle of 90 degrees, and the same values of force will be maintained. This is why in the solution I gave you, Tcos(24.5 deg) is used instead of Tsin(24.5 deg).In summary, a knight and his horse are stuck on a bridge because the drawbridge was not lowered properly. The problem asks to determine the tension in the cable supporting the bridge. Using the given information and applying torque calculations, the tension in the cable is found to be 27.7 kN. There was some confusion about the symbols and numbers in the problem, but ultimately, the solution was found by using the horizontal and vertical
  • #1
Zynoakib
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Homework Statement


Sir Lost-a-Lot dons his armor and sets out from the
castle on his trusty steed (Fig. P12.19). Usually, the
drawbridge is lowered to a horizontal position so that
the end of the bridge rests on the stone ledge. Unfortunately,
Lost-a-Lot’s squire didn’t lower the drawbridge
far enough and stopped it at 20 degree above
the horizontal. The knight and his horse stop when
their combined center of mass is 1.00 m from the
end of the bridge. The uniform bridge is 8.00 m
long and has mass 2 000 kg. The lift cable is attached
to the bridge 5.00 m from the hinge at the castle end
and to a point on the castle wall 12.0 m above the
bridge. Lost-a-Lot’s mass combined with his armor
and steed is 1 000 kg. Determine the tension in the
cable

Homework Equations

The Attempt at a Solution


Actually I have the answer, but I just don't understand why you have to take the horizontal component of tension and the force from the hinge because it is perpendicular to surface of the bridge

The angle between the wall and the cable is 24.5 degrees

Take torques about the hinge end of the bridge:
Hx (0)+ Hy (0)− Mg(4.00 m)cos20.0°
(T sin 24.5°)(1.71 m)+ (T cos24.5°)(4.70 m)
− mg(7.00 m)cos20.0° = 0
T = 27.7 kN

Thanks
 
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  • #2
What makes you conclude that ?
Could you explain some of the symbols and the funny numbers, or perhaps even all of them, instead of letting us find out the hard way that M is the bridge and m is man + horse ?
MAke a drawing (you probably did that already). Did you discover the error in the problem statement (or rather the unmentioned assumption) ?
 
  • #3
BvU said:
What makes you conclude that ?
Could you explain some of the symbols and the funny numbers, or perhaps even all of them, instead of letting us find out the hard way that M is the bridge and m is man + horse ?
MAke a drawing (you probably did that already). Did you discover the error in the problem statement (or rather the unmentioned assumption) ?

That's the diagram according to the answer's calculation. Any better?
20150911_230557.jpg


I don't understand how you can get the answer because you can see Tx is not perpendicular to the bridge. So how can you calculate torque of Tx by using (T sin 24.5°)(1.71 m)?
 
Last edited:
  • #4
The picture at least explains where the 24.5 degrees comes from.
Doesn't look as nice as most of the official solutions (such as in books) I've seen, but it looks OK.

This way the problem solver avoids having to work out the angle between T and the bridge (85.5 degrees, I would say :smile:). T is the sum of Tx and Ty and the torque of T about the hinge is the sum of the torques about the hinge from Tx and from Ty.

If you know about cross products and their linearity: $$
\vec \tau = \vec r \times \vec T = \vec r \times (\vec T_x + \vec T_y) = \vec r \times \vec T_x + \vec r \times \vec T_y$$​
Something seems to go wrong, though: one has a minus sign and the other a plus sign, but both torques are in the same direction. Brackets missing ?

My ironic criticism on the problem statement was that the center of mass for man+horse is more than 1 m away from the end of the bridge (unless very small horse). What the problem composer (is that also the solver? hmmm...) means is that the center of mass is straight above a point on the bridge that is 1 m from the end. This isn't clear from the problem statement at all. Apart from my corny height, it could well be meant that its 1 m / cos 20 degrees from the end...
Now what's this about the force from the hinge ?
 
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  • #5
Zynoakib said:
That's the diagram according to the answer's calculation. Any better?
20150911_230557.jpg


I don't understand how you can get the answer because you can see Tx is not perpendicular to the bridge. So how can you calculate torque of Tx by using (T sin 24.5°)(1.71 m)?
The components of the tension which you have drawn in your diagram are oriented so that they are parallel and vertical to the ground. You can just as easily find different components which are parallel and vertical w.r.t. the bridge.
 
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Related to Static equilibrium involving toque

1. What is static equilibrium involving torque?

Static equilibrium involving torque is a state in which an object is at rest and the forces acting on it are balanced, causing no net acceleration. Torque is the measure of the tendency of a force to rotate an object around an axis.

2. How is torque calculated?

To calculate torque, you multiply the force applied to an object by the distance from the axis of rotation to the point where the force is applied. This distance is known as the lever arm or moment arm. The formula for torque is T = F x r, where T is torque, F is force, and r is the lever arm.

3. What is the difference between static equilibrium and dynamic equilibrium?

Static equilibrium involves a balanced state where an object is at rest and not moving. Dynamic equilibrium involves a balanced state where an object is moving at a constant speed in a straight line.

4. How does the center of mass affect static equilibrium involving torque?

The center of mass is the point at which an object's mass is evenly distributed. In static equilibrium involving torque, the center of mass must be directly above the axis of rotation in order for the object to remain balanced. If the center of mass is not directly above the axis of rotation, the object will experience a rotational force and will not be in static equilibrium.

5. What are some real-life examples of static equilibrium involving torque?

Some real-life examples of static equilibrium involving torque include a see-saw in a playground, a balance scale, a door on its hinges, and a lever used to lift heavy objects. In each of these examples, the forces acting on the object are balanced, causing it to remain at rest.

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