Torque Equilibrium to find center of mass.

In summary, a non-uniform beam with a mass of 85kg and a length of 6.2m is attached to a wall and supported at an angle of 28 degrees by a horizontal rope. The tension in the rope is 310N and the center of mass of the beam is being sought. Using the equations Fg= m x g and Trigonometry (sin=o/h, cos=a/h, tan=o/a), the center of mass is found to be at a distance of approximately 727.88m from the pivot point. However, in order to solve this problem accurately, a free body diagram and proper execution of the equations is necessary.
  • #1
MedChill
1
0

Homework Statement


1. A non-uniform beam with a mass of 85kg has a length of 6.2m and is attached to a wall and supported at an angle of 28 degrees from the wall by a horizontal rope which is attached to the wall above the beam . The tension in the rope is found to be 310N. How far from the pivot point is the center of mass of the beam?

Homework Equations


T= d x F
Trigonometry (sin=o/h, cos=a/h, tan=o/a)
Fg= m x g

The Attempt at a Solution


Well I am pretty lost in the question but I gave it a shot anyways.
Fg= 85 x 9.8= 833 N
Fg(perpendicular)= 833sin28= 391.1 N
Ft= 310 N
Ft(perpendicular)= 310cos28= 273.7 N
∑= 391.1-273.7= 117.4 N
T= 117.4 x 6.2= 727.88

This is where I think I messed up but don't know where else to go from here.
 
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  • #2
Welcome to PF;
The trick with this sort of question is to sketch it out and draw in the forces, and label points.

So call the pivot O, the other end A and the point the rope joins the wall is B ... pick an arbitrary point off-center on the beam to represent the center of mass and call it C.

OC=x (which you want to find).
I don't see any reference to an unknown distance in your analysis.
Sketch in the forces at O, A, B, and C, don't forget the directions.

Now you should be in a position to write the expression for the total torque about O, which will include the unknown x. Solve for x.

Note - torque is usually given as a cross product as in T = d x F, but the weight is just a scalar product Fg=mg.
Formally: ##\vec \tau = \vec r \times \vec F## and ##\vec F\!_g=m\vec g##
 
  • #3
Maybe a free body diagram would help us follow what you are trying to do.

But you got the right equations, just need to execute them properly.
 

Related to Torque Equilibrium to find center of mass.

What is torque equilibrium?

Torque equilibrium is a state in which an object is not rotating, meaning the net torque acting on the object is zero. This occurs when the sum of all the clockwise torques is equal to the sum of all the counterclockwise torques.

How is torque equilibrium used to find the center of mass?

Torque equilibrium can be used to find the center of mass by using the principle of moments. This involves balancing the torques acting on the object around a pivot point and using the perpendicular distance from the pivot point to each force to calculate the net torque. By setting this net torque equal to zero, the position of the center of mass can be determined.

What is the significance of finding the center of mass?

The center of mass is an important physical property of an object as it represents the point at which an object's mass can be considered to be concentrated. It is also the point around which an object will rotate if subjected to an external force, making it a key factor in understanding the behavior of objects in motion.

Can torque equilibrium only be used for simple shapes?

No, torque equilibrium can be used for objects of any shape as long as the forces acting on the object are known. The principle of moments can be applied to any object, and the position of the center of mass can be found regardless of the object's shape or size.

How does the location of the center of mass affect an object's stability?

The location of the center of mass is directly related to an object's stability. If the center of mass is located over the base of support, the object is stable and will remain in equilibrium. However, if the center of mass falls outside of the base of support, the object will become unstable and may topple over.

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