Force on a rod attached to a pivot.

In summary, the question is to find the horizontal force on the right pivot when a 2 kg weight is 0.4 m from the ground on a 0.5 m long rod with a fixed pivot on the left. According to Feynman, the net force must be parallel to the rod, with the horizontal force on the pivot being equal to W tan ø. This results in a horizontal force of 14.7 N, in contrast to the initial reasoning of 9.4 N based on trigonometry. The reason for this difference is that the perpendicular force exerted by the weight has a horizontal component that cannot be ignored and the rod is not rotating about the pivot.
  • #1
albertrichardf
165
11
<Moderator note: Thread moved from Classical Physics, hence no homework template>

Hello.
Can anyone help me confirm the following from the Feynman tips on physics:
View attachment 111741
The above diagram shows two rods, with a weight attached (the square). Each rod has a pivot attached, though the pivot on the left is fixed and cannot roll. The weight is 2 kg, and the rod is 0.5 m long. The question is to find the horizontal force on the right pivot when the weight is 0.4 m from the ground. Both rods exert a force such that the net vertical component balances the weight but for the following pretend that the rod with the moving pivot bears all the weight.

My reasoning is as follows: the weight exerts a vertical force on the rod. Part of this force is parallel to the rod and part is perpendicular. The rod transfers any parallel force to the pivot, and rotates under the effect of the perpendicular force. For our purposes, the perpendicular force can be ignored. The vertical component of the parallel force can also be ignored because that is balanced by the ground. The horizontal component of the parallel force is thus what is being looked for.

The parallel component is W cos ø, where W is the weight of the mass (2 * 9.8) and ø is the angle. The horizontal component is W cos ø sin ø. All this comes from trigonometry. Therefore the total horizontal force is about 9.4 N.However, Feynman reasons that the net force must be parallel to the rod. Because of the weight pushing onto the rod, the rod feels a vertical force, which it exerts on the pivot. The horizontal force on the pivot is also felt by the rod and must be such that the net force is directed parallel to the rod. In other words, the vertical and horizontal forces form right triangle with the net force as the hypotenuse. The horizontal force is then
W tan ø = 14.7

So I got 9.4 but he got 14.7. Can someone explain to me why I am wrong? Also in his explanation, if the rod feels only a vertical force due to the weight, where does the horizontal force on the pivot come from?

Thanks for answering
 
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  • #2
Albertrichardf said:
My reasoning is as follows: the weight exerts a vertical force on the rod. Part of this force is parallel to the rod and part is perpendicular. The rod transfers any parallel force to the pivot, and rotates under the effect of the perpendicular force. For our purposes, the perpendicular force can be ignored. The vertical component of the parallel force can also be ignored because that is balanced by the ground. The horizontal component of the parallel force is thus what is being looked for.

The "perpendicular" force has a horizontal component, which cannot be ignored. The rod is not rotating about the pivot.
 
  • #3
https://www.physicsforums.com/posts/5668969/like see. Thank you
 

FAQ: Force on a rod attached to a pivot.

What is a force on a rod attached to a pivot?

A force on a rod attached to a pivot is a type of force that is applied to a rod that is attached to a pivot point, causing it to rotate or move in a particular direction.

How is the force on a rod attached to a pivot calculated?

The force on a rod attached to a pivot can be calculated using the formula F = r x sin(theta), where F is the force, r is the distance from the pivot point to the point where the force is applied, and theta is the angle between the force and the lever arm.

What factors affect the force on a rod attached to a pivot?

The force on a rod attached to a pivot is affected by the magnitude and direction of the force, the distance from the pivot point to the point where the force is applied, and the angle between the force and the lever arm.

What are some real-life examples of a force on a rod attached to a pivot?

A common example of a force on a rod attached to a pivot is a seesaw, where the pivot point is the fulcrum and the force is applied by pushing down on one end of the seesaw. Another example is a fishing rod, where the pivot point is the handle and the force is applied by pulling on the fishing line.

How is the force on a rod attached to a pivot used in engineering and physics?

The force on a rod attached to a pivot is an important concept in engineering and physics, as it helps to explain how objects rotate and move. It is used in various applications such as designing structures, analyzing mechanical systems, and understanding the movement of objects in space.

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