Projectile motion of a two-point rigid body

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Discussion Overview

The discussion revolves around the physics of projectile motion for a two-point rigid body, specifically focusing on the transition from single mass point dynamics to rigid body dynamics. Participants explore the effects of various forces, including gravity and air resistance, on the motion of the rigid body, considering both translational and rotational aspects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks guidance on modeling the motion of a rigid body made of two mass points connected by a massless rod, specifically how to account for external forces acting on the masses.
  • Another participant confirms that gravity acts on the center of mass, leading to translation without rotation under certain conditions, such as when a bar is dropped horizontally.
  • There is a discussion about different scenarios for modeling forces, including uniform gravity, air resistance, and non-uniform gravity, with some participants expressing a desire to explore various force models.
  • Participants consider the implications of adding air resistance, questioning how it should be modeled (linear, quadratic, or combined) and acknowledging the complexity it introduces.
  • One participant suggests starting with linear air resistance for simplicity, noting that their goal is to create animations for high-school demonstrations that illustrate qualitative behavior rather than precise outcomes.
  • Another participant mentions that with linear air resistance, calculations for rotation and the trajectory of the center of mass can be separated, leading to exponential decay patterns for rotation and convergence to terminal velocity for linear motion.
  • There is a suggestion to simplify the problem by considering cases such as free fall in a vacuum or a body subjected to a single force not acting through the center of gravity, emphasizing the importance of linear systems and superposition.

Areas of Agreement / Disagreement

Participants express various viewpoints on how to model the motion of the rigid body, particularly regarding the effects of air resistance and the separation of translational and rotational motion. No consensus is reached on the best approach, and multiple competing views remain.

Contextual Notes

Limitations include the potential complexity of modeling air resistance and the assumptions made regarding the nature of forces acting on the rigid body. The discussion does not resolve the mathematical steps involved in the modeling process.

luinthoron
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I would like to patch some gaps in my physics background. For example, I've been trying to come up with the sollution to the following: I have a model rigid body made up of two mass points and a massless rod connecting them. I throw the body with initial velocity under some angle of elevation. My problem is the transfer from single mass point physics to rigid body physics. How do I get the actual movement of the rigid body from knowing the outer forces acting on the two masses? I guess I will have to work with the motion of the center of mass and rotation of the object separately, right?

Could you please at least show me the right direction of thought? Thanks a bunch.
 
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luinthoron said:
How do I get the actual movement of the rigid body from knowing the outer forces acting on the two masses? I guess I will have to work with the motion of the center of mass and rotation of the object separately, right?

Yes. Gravity acts on the centre of mass, so a body under gravity will translate but not rotate. If you drop a horizontal bar with a large mass at one end and a smaller mass at the other, then (ignoring air resistance) the bar remains horizontal as it falls.
 
Modelling uniform gravity? Gravity plus air resistance? Non-uniform gravity? Modeling additional ad hoc forces and torques not necessarily confined to the plane of rotation?
 
jbriggs444 said:
Modelling uniform gravity? Gravity plus air resistance? Non-uniform gravity? Modeling additional ad hoc forces and torques not necessarily confined to the plane of rotation?
Uniform gravity plus air-resistance confined to the plane of rotation, for start. But ultimately, I would like to be able to solve the rigid body motion under any kind of given forces.
 
PeroK said:
Yes. Gravity acts on the centre of mass, so a body under gravity will translate but not rotate. If you drop a horizontal bar with a large mass at one end and a smaller mass at the other, then (ignoring air resistance) the bar remains horizontal as it falls.
Fair point, but if I add air-resistance?
 
luinthoron said:
Fair point, but if I add air-resistance?
How will you model the air resistance? Linear? Quadratic? Combined?

You are quickly approaching the point where a differential equation may not have a closed form solution.
 
jbriggs444 said:
How will you model the air resistance? Linear? Quadratic? Combined?

You are quickly approaching the point where a differential equation may not have a closed form solution.
I see. Since my goal is to practice the method on a simple situation first, I would go with linear air resistance first, regardless of the physical reality. I should also add that I am working with simple numerical solutions, first-order or second-order numerical methods. I could go further in precision if needed. My animations are for high-school class demonstration, so they do not have to be exact, but show the correct qualitative behaviour.
 
luinthoron said:
I see. Since my goal is to practice the method on a simple situation first, I would go with linear air resistance first, regardless of the physical reality. I should also add that I am working with simple numerical solutions, first-order or second-order numerical methods. I could go further in precision if needed. My animations are for high-school class demonstration, so they do not have to be exact, but show the correct qualitative behaviour.
Given linear air resistance, one should be able to separate the calculation for rotation from the calculation for the trajectory of the center of mass. This follows since the added air resistance due to the rotation of one end is equal and opposite to the added air resistance of the other end.

You should be able to solve and see that the rotation will follow a pattern of exponential decay. You should be able to see the same for the linear motion, except that it will converge on a fall at terminal velocity.

In addition to rotational and linear motion being separable, linear drag should allow you to treat movement in the x and y directions independently.

I am very rusty at this stuff (unpracticed for 40 years or so) but may be able to guide you through writing and solving the differential equations of motion. Certainly there are others around here who can.
 
luinthoron said:
My animations are for high-school class demonstration, so they do not have to be exact, but show the correct qualitative behaviour.
Then I would recommend keeping it simpler, and not trying to consider all forces at once.

One simple case is a body in free fall in a vacuum. Only the center of gravity is important.

Another simple case is a body subjected to a single force that is not through the center of gravity. It will start rotating, and maybe moving also, depending on the angle of the force.

Then tell students that for linear systems, solutions can be superimposed. That brings two more important concepts in: linear and superposition.
 

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