Mechanical problems converted into electrical circuits.

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Discussion Overview

The discussion revolves around the conversion of mechanical systems into analogous electrical circuits, specifically focusing on two mechanical problems presented in a homework assignment. Participants are analyzing the correctness of their conversions and the relationships between the mechanical and electrical components.

Discussion Character

  • Homework-related
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the direction of the gravitational force in the first analog and the arrangement of components, suggesting that they should be in series rather than parallel.
  • Another participant seeks clarification on the definition of B4, which represents friction, and whether it should be the same for all three masses.
  • There is a discussion about the steady state of the second analog, with one participant proposing a relationship between voltages and friction, while another challenges this by stating that the shorted inductors would tie all nodes together.
  • Participants explore the number of velocity nodes in the first analog, with one suggesting there are only two, while another indicates the possibility of defining additional nodes at junctions.
  • A participant raises a concern about the apparent discrepancy in the arrangement of masses in the analog compared to the mechanical system, questioning the direction of gravitational forces and the modeling of inertial mass.
  • One participant acknowledges a previous error regarding the direction of forces in the pulley system, correcting their earlier statement about the direction of currents.

Areas of Agreement / Disagreement

Participants express differing views on the correctness of the analogs and the relationships between components, indicating that multiple competing interpretations exist. The discussion remains unresolved regarding some aspects of the analogs and their representations.

Contextual Notes

Some assumptions regarding the definitions of components and the conditions of the systems are not fully clarified, leading to varying interpretations of the analogs. The discussion includes unresolved mathematical steps related to the steady state analysis.

peripatein
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Hi,

Homework Statement


Attached (Q1,Q2) are two mechanical systems I am asked to convert into analogous electrical circuits. In Q2, it was stated that B4 is the friction between each of the three masses and the surface.

Homework Equations





The Attempt at a Solution


Attached (Q1 - Converted, Q2 - Converted) are my conversions, which I am not sure are correct. I'd sincerely appreciate some feedback on these two conversions.
 

Attachments

  • Q1 - Converted.jpg
    Q1 - Converted.jpg
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  • Q1.JPG
    Q1.JPG
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  • Q2.JPG
    Q2.JPG
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  • Q2 - Converted.jpg
    Q2 - Converted.jpg
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In your first analog, shouldn't the force due to gravity be working in the same direction for both masses? How did you end up with the inductor and resistor in parallel between the two nodes? Surely the mechanical versions are in series in the "light inextensible string" that winds through the pulleys.

In the second analog I don't see where B4 is defined in the mechanical version, but I presume it's meant to represent friction between the masses and the "ground" surface. Should they be the same value for all three masses?
 
I referred to B4 in my statement above. Is my analog correct then?
Please see new attachment for the corrected analog of Q1. Is it indeed correct now?
 

Attachments

  • Q1 - Converted1.jpg
    Q1 - Converted1.jpg
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peripatein said:
I referred to B4 in my statement above. Is my analog correct then?
Please see new attachment for the corrected analog of Q1. Is it indeed correct now?

It looks fine to me, provided that "down" is defined to be positive in your mechanical system.
 
Thanks :). By the way, would it be correct to say that in Q2, in the steady state (i.e. capacitors are open, inductors are short), V1 would be equal to f/(3B4) whereas V2 and V3 would be zero?
 
peripatein said:
Thanks :). By the way, would it be correct to say that in Q2, in the steady state (i.e. capacitors are open, inductors are short), V1 would be equal to f/(3B4) whereas V2 and V3 would be zero?

Nope. The shorted inductors tie all three nodes together, so they must all have the same potential.

If you consider the "original", the dampers between the masses will cause any initial oscillations to die away, but the whole ensemble will continue to move at some constant velocity limited by friction.
 
I see. So is V1=V2=V3=f/(3B4)?
 
peripatein said:
I see. So is V1=V2=V3=f/(3B4)?

You should be able to answer that by redrawing the circuit with the reactive components suppressed as you've stated. What does the steady state circuit look like?
 
Please see attachment. Each branch gets f/3 so Vi should be equal to f/3B4. Unless I am mistaken. Am I?
 

Attachments

  • Q2 - Converted1.jpg
    Q2 - Converted1.jpg
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  • #10
peripatein said:
Please see attachment. Each branch gets f/3 so Vi should be equal to f/3B4. Unless I am mistaken. Am I?

You are not mistaken :smile:
 
  • #11
In analog 1, are there only 2 velocity nodes/points? My guess is that there are only two, viz. V1 and V2, since the other potential nodes/points are in parallel. Am I right?
 
  • #12
peripatein said:
In analog 1, are there only 2 velocity nodes/points? My guess is that there are only two, viz. V1 and V2, since the other potential nodes/points are in parallel. Am I right?

You could define a node at the junction of the resistor and inductor in order to determine the velocity of the spring end. But this would not be an "essential node", as it occurs in the middle of a branch.
 
  • #13
Hi,
In your first reply to my question yesterday, you wrote "surely the mechanical versions are in series in the 'light inextensible string' that winds through the pulleys." However, when you take a look at the analog (attachment '2') of the system shown in the recently added attachment '1', the masses are drawn in parallel whereas here too a light inextensible string winds through the pulleys and connects the two masses. Why the seeming discrepancy?
Furthermore, why are the forces due to gravity now in opposite directions?
 

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  • 2.JPG
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Last edited:
  • #14
peripatein said:
Hi,
In your first reply to my question yesterday, you wrote "surely the mechanical versions are in series in the 'light inextensible string' that winds through the pulleys." However, when you take a look at the analog (attachment '2') of the system shown in the recently added attachment '1', the masses are drawn in parallel whereas here too a light inextensible string winds through the pulleys and connects the two masses. Why the seeming discrepancy?
For masses, what is being modeled is their inertial mass. This is always referenced to the rest frame, so one leg of the analogous capacitor is always tied to ground. This is true even for masses suspended in the air by ropes.

In this new system, note that the string ties the masses together so their movements (positions, velocities, accelerations) are linked. While the ground "leg" of both capacitors are automatically tied together simply because all masses are tied to ground, in this case the "free" legs are tied together too by the inextensible string. That's why they end up in parallel.

Furthermore, why are the forces due to gravity now in opposite directions?

Ah. I think I have an apology to deliver :blushing: Upon reflection I realize that I made an error before when I suggested that the currents ("Forces") should be in the same direction. Of course they should be opposite as you had them. If the pulley system is redrawn, stretched out horizontally and the acting forces reoriented accordingly, the correct directions for the motions and forces becomes obvious:

attachment.php?attachmentid=63672&stc=1&d=1383653816.gif


Here Fg is pulling "left" on M1 and "right" on M2. Opposite directions. I should have spotted that, sorry.
 

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  • Fig1.gif
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  • attachment.php?attachmentid=63672&stc=1&d=1383653816.gif
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