Solving Car Suspension Modeling: Understanding Input Forces and Movement Types

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Discussion Overview

The discussion revolves around modeling car suspension systems, specifically focusing on the input forces and types of movement involved. Participants explore the roles of torque, damping forces, and the interpretation of components like the torsional spring within the system.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the system has two input forces: torque and an external force u(t), while others suggest that only u(t) is the primary input force affecting the system.
  • There is a contention regarding the types of movement in the system, with some asserting that both linear and rotational movements are present, while others argue that only rotational movement is relevant, with linear movement being a consequence of rotation.
  • The interpretation of the KT spring as a torsional spring is discussed, with some participants noting that it links torque and angular displacement.
  • Concerns are raised about the effect of the damper and its distance from the pivot, suggesting that its influence on the mass may be reduced compared to a classical spring-damper system.
  • Participants discuss the relationship between the input force u and the torque, highlighting the need for proper calculation involving perpendicular directions for accurate modeling.

Areas of Agreement / Disagreement

There is no consensus on the number of input forces or the nature of movements in the system. Multiple competing views remain regarding the roles of torque and the interpretation of the system's dynamics.

Contextual Notes

Participants express uncertainty about the interactions between various forces and components, including the torsional spring and damping effects, indicating a need for further clarification on these relationships.

Lord Doppler
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Homework Statement
Find the mathematic model of car suspension, express the movement equations in differential equations U(t)
Relevant Equations
F = ma
T = Ja
Hello, I'm trying to solve this problem but I'm confused with some things, is correct that in the system there are two input forces, the torque and u(t)? I assumed that the system has two free levels, which are the z displacement and theta (rotational movement), so the system has a linear movement and a rotational movement? Besides the KT spring inside of the arm how I can intepret it? I'm not sure how to board this problem
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Lord Doppler said:
is correct that in the system there are two input forces, the torque and u(t)?
There is also the damping force from element ##b##.
Lord Doppler said:
I assumed that the system has two free levels, which are the z displacement and theta (rotational movement), so the system has a linear movement and a rotational movement?
Just the rotational movement. The linear movement you are referring to is a direct consequence of the rotation.
Lord Doppler said:
Besides the KT spring inside of the arm how I can intepret it?
It is a torsional spring. ##K_T## would be the torsional stiffness which links the torque and the angular displacement.
 
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It seems to me that the only input force to the system is U.
That input makes the two parts of the system oscilate:
1) The mass-less pivoting arm with the mass m, onto which U is acting vertically.
2) The torsion bar, which acts as a spring and having rotational inertia.

You can consider the points represented by a cross to be common fixed points, all interconnected via chassis of the car.

The damper is located at distance r1 from the pivot, so its effect on stopping m should be reduced (respect to a classical oscillating spring-damper system).
The given angle also reduces the effect of U about the pivot and torsion bar.

The effect of the torsional and linear resistances or springs should be added up, as they seem to be working in series rather than in parallel.
 
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Lnewqban said:
It seems to me that the only input force to the system is U.
That input makes the two parts of the system oscilate:
1) The mass-less pivoting arm with the mass m, onto which U is acting vertically.
2) The torsion bar, which acts as a spring and having rotational inertia.

You can consider the points represented by a cross to be common fixed points, all interconnected via chassis of the car.

The damper is located at distance r1 from the pivot, so its effect on stopping m should be reduced (respect to a classical oscillating spring-damper system).
The given angle also reduces the effect of U about the pivot and torsion bar.

The effect of the torsional and linear resistances or springs should be added up, as they seem to be working in series rather than in parallel.
I agree when you say that U is the only input force, but there is no a torque T also? Like input force I mean
 
Yes, the torsional bar will never see what is causing the torque that it has to resist.
That torque is the combination of U and horizontal projection of the arm’s length r2.
Note that directions of U and distance about the torsion bar must be perpendicular for proper calculation.
Same applies for resistive force of damper b.
 
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Lnewqban said:
Yes, the torsional bar will never see what is causing the torque that it has to resist.
That torque is the combination of U and horizontal projection of the arm’s length r2.
Note that directions of U and distance about the torsion bar must be perpendicular for proper calculation.
Same applies for resistive force of damper b.
Thanks!
 
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