Inverted pendulum -- What force is applied at the center of mass?

In summary, the conversation explores the concept of keeping an inverted pendulum balanced by accelerating the bottom and the force applied to its center of mass. It discusses the possibility of a torque due to gravity and the use of a fictitious inertial force or a real compression/tension force. The conversation also mentions the use of fuzzy logic in designing the inverted pendulum system.
  • #1
fizzyfiz
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Summary: I know that in order to keep inverted pendulum balanced when it leans forward, I should accelerate the bottom of it, but what is the force which is applied to center of mass of the pendulum with balances torque due to gravity? Is it inertial force? We assume that our inverted pendulum is massles rod with a center of mass at its top. As a Radius of rotation we denote "L"as angle between vertical and pendulum "a"

M*g*sin(a)*L= F*L
 
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  • #2
fizzyfiz said:
what is the force which is applied to center of mass of the pendulum with balances torque due to gravity? Is it inertial force?
If you imagine that there is a torque due to gravity, you must imagine that there is an axis about which the torque applies. Let us choose the point where the pendulum is attached to the ground.

If you move the point where the pendulum is attached to the ground, you adjust the torque due to gravity by redefining your coordinate system. If you insist on viewing this as an applied force then yes, it would be a fictitious inertial force (the D'Alembert force) associated with the acceleration of the coordinate system.

If you prefer to stick to a single inertial frame then the relevant force is real and is, instead, the compression or tension force on the pendulum arm. When the pendulum's bottom end moves, this compression or tension force no longer produces zero torque about a reference axis at the original attachment point.
 
  • #3
Thank you for reply! Could you draw the second case?
 
  • #4
fizzyfiz said:
Thank you for reply! Could you draw the second case?
The star is the axis of rotation, the thin line is the downward force from gravity, the rectangle is where the support point was moved, the pendulum arm is the bold line and the circle is the pendulum bob. You can see that the compression force of arm on bob amounts to a clockwise torque while gravity amounts to a counter-clockwise torque.

My skills with mspaint are of questionable value.
inverted.png
 
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  • #5
Check out this paper. It should be helpful with the equations, and the design.

https://link.springer.com/content/pdf/10.1007/0-387-29295-0_7.pdf
This thread triggered a memory. The inverted pendulum was the earliest and only? clear victory for fuzzy logic. So I searched for inverted pendulum fuzzy logic, and found many hits.
 

FAQ: Inverted pendulum -- What force is applied at the center of mass?

1. What is an inverted pendulum?

An inverted pendulum is a physical system where a rigid body is balanced in an unstable equilibrium position, with its center of mass directly above its pivot point.

2. What is the center of mass?

The center of mass is the point in a system where the mass is evenly distributed and the object will be balanced if supported at that point.

3. What force is applied at the center of mass of an inverted pendulum?

The force applied at the center of mass of an inverted pendulum is the gravitational force acting on the mass of the pendulum.

4. How does the force at the center of mass affect the stability of an inverted pendulum?

The force at the center of mass is what keeps the inverted pendulum balanced. If the force is not strong enough, the pendulum will fall over. If the force is too strong, the pendulum will swing too far in the opposite direction and also fall over.

5. What factors can affect the force at the center of mass of an inverted pendulum?

The force at the center of mass can be affected by the mass of the pendulum, the length of the pendulum, and the angle at which it is balanced. Additionally, external forces such as air resistance or friction can also affect the force at the center of mass.

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