Applying forces to a body, outside it's center of mass.

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Discussion Overview

The discussion revolves around the application of forces to a rigid body outside its center of mass, particularly in the context of a physics engine. Participants explore the implications of such force applications on both linear and rotational motion, using the example of spinning a pen on a finger to illustrate their points. The scope includes theoretical considerations of force, torque, and motion dynamics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant describes a function in a physics engine that applies a force to a rigid body outside its center of mass and questions the resultant linear force, suggesting an alternative formula based on the angle of application.
  • Another participant asserts that the acceleration of the center of mass is determined by the vector sum of all external forces, regardless of their point of application, and acknowledges the role of torques in this context.
  • A participant emphasizes the importance of understanding why a pen can be spun on a finger without a noticeable change in linear velocity, seeking clarification on the mechanics involved.
  • Another participant explains that pure rotation cannot be achieved without a net zero force, introducing the concept of a couple and discussing the implications for spacecraft design, where translation and rotation are often coupled.
  • A follow-up question is raised regarding the source of the other force necessary to achieve a zero net linear force when applying a single force to the pen.

Areas of Agreement / Disagreement

Participants express differing views on the mechanics of force application and its effects on motion. While some agree on the principles of force and torque, the specific scenario involving the pen remains a point of contention, with no consensus reached on the underlying mechanics.

Contextual Notes

The discussion highlights the complexities of force application and motion dynamics, with participants acknowledging the need for further clarification on specific scenarios. Assumptions about force interactions and the definitions of terms like "couple" are not fully explored, leaving some aspects unresolved.

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Hello.
I'm currently coding on a physics engine.

To do so, I looked up some code from open-source engines.

I noted that there is a function where you can apply a force to a rigid body, outside it's center of mass.

It goes something like this:

ApplyForceAPosition(vector force, vector positionWorld);

Where the resultant torque would be
distance(positionWorld,m_centerofmass)*force*sin(theta),
as expected.

However, applying the force outside the center of mass can also cause a linear force.
it would be calculated as follows:
m_Force = force;

But this seems strange to me. If I put balance pen on one finger, and I apply a force to it, so that it would spin, I can do so without visually noticing any change in linear velocity.

So it seems to me that a more appropriate formula to compute the resulting linear force from a force applied outside the center of mass would be:

m_force = |cos(theta)|*force;
Where theta would be the angle between the force vector and [forcepos-COM].

I can't seem to find any articles on this, and I'm most likely wrong, but then how come I can spin a pen on one finger without causing any change in linear velocity?
 
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The physics engines are correct. The acceleration of the center of mass of an object is the the vector sum of all of the external forces acting on the object (regardless of point of application) divided by the object's mass. Those external forces also arise in torques, and here the torques obviously do depend on the point of application.
 
Well my question was not really whether I was correct or not. I even stated that I'm most likely wrong. The question is why. Please read my question.

I can spin a pen on one finger (by pushing it with one finger only), without changing any visually noticeable change in linear velocity. However, if I were to change the position of application of the force, it doesn't spin so much, and does have change in linear velocity. Please explain.
 
You cannot create pure rotation unless the forces cancel, resulting in zero net force, but the torques do not cancel. It's called a couple.Spacecraft designers have to deal with the fact that forces result in translation and rotation *all the time*. It would be really nice if jets designed for translational motion always resulted in pure translation, if the jets designed for rotational motion (when operated in pairs) always resulted in a pure couple. This never happens. Instead there is always some undesired cross coupling between translation and rotation.

Those spacecraft designers have to accommodate for this undesired cross coupling in their control systems. If we had the physics wrong, those guidance and control systems would not get the vehicles where they are supposed to go. Those guidance and control systems *do* get the vehicles where they are supposed to go.

NASA simulates every vehicle that is intended to dock with the Space Station to make sure the vehicle will be safe. It uses something very similar to the physics engines calculations you described in the opening post. If we had the physics wrong, those simulations would yield something different from the true behavior of these vehicles. Those simulations are instead spot on. The vehicles behave pretty much as predicted.
 
Don't worry, I'm not saying physicists are wrong :)
But I still need clarification for the situation with the pen on my finger! In the case where I apply a force with one finger only, where is the other force coming from that would create a zero net linear force?
 

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