Analogous electric circuit for mass-spring-damper system

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Homework Statement



Find the analogous electrical circuit for the following mass spring damper system.

Diagram of a two-mass spring-damper system: a fixed top support with spring k1 to mass m1, which has force p(t) applied; m1 connects to m2 via spring k2 in parallel with spring k3 in series with damper b; displacements x1 and x2 are marked downward.


Homework Equations

The Attempt at a Solution



I am rusty with writing equations of motion. I wanted to see if someone could check my work.

Looking at the diagram, there are three equations to write. Also there should be a third displacement variable, call it ##x_3##, between ##k_3## and ##b##. Assume down is positive.

For mass ##m_1##:

$$m_1x'' = -k_1x_1 + k_2(x_2 - x_1) + k_3(x_3 - x_1) + b(x_2' - x_3') + p(t)$$

For mass ##m_2##:

$$m_2x'' = -k_2(x_2 - x_1) - b(x_2' - x_3') - k_3(x_3 - x_1)$$

At the node in between the damper and spring:

$$0 = -k_3(x_3 - x_1) + b(x_2' - x_3')$$

Do these look okay?
 
You do realize that you can draw an analogous electrical circuit for the mechanical system without writing and solving the differential equations, right?
 
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gneill said:
You do realize that you can draw an analogous electrical circuit for the mechanical system without writing and solving the differential equations, right?

Yes this is possible, but I was hoping to understand how to write the equations of motion anyway. It would be nice to know how to write them for a more complicated system, so I would still like to know if I've done that properly.

I'll give your idea a try though. Here is my attempt:

Hand-drawn electrical circuit schematic on lined paper with capacitors C1, C2 and C3, inductors L1 and L2, a resistor R, and sources labelled m3, m2 and p(t) at the right.


The battery on the far right corresponds to ##p(t)##.
 
Yes, your figure looks okay to me. You've chosen the Force ⇒ Voltage paradigm. You could also have used the Force ⇒ Current paradigm where masses become capacitors rather than inductors.

For your equations, at a glance they look fine except I don't see where you've accounted for gravity acting on the masses.
 
gneill said:
Yes, your figure looks okay to me. You've chosen the Force ⇒ Voltage paradigm. You could also have used the Force ⇒ Current paradigm where masses become capacitors rather than inductors.

Okay.

gneill said:
For your equations, at a glance they look fine except I don't see where you've accounted for gravity acting on the masses.

Yeah I find this weird because in my textbook they never seem to account for the force of gravity on a mass.

They compensate for this by making a substitution like so:

Two-panel diagram of a spring-mass system: left, a dashed outline of mass m hanging from spring k before attachment, with y = x + δ marked; right, mass m resting on the spring k after attachment, with δ shown as the static deflection between the two positions.

Printed textbook page deriving the equation of motion for a mass on a spring, covering forces ky and mg, Equations 3-11 to 3-13, and the substitution y = x + δ removing gravity.
 
Ah, I see. Yes, that substitution works and makes the math simpler. Of course, to match the model's predicted position to a real-world position one would need to know the equilibrium position's offset in real-world coordinates.