Determine Voltage vk(t) across Switch K After Opening

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Discussion Overview

The discussion revolves around determining the voltage vk(t) across a switch K in a circuit after the switch is opened at time t=0. Participants explore the implications of the switch's operation on the circuit's behavior, particularly focusing on the initial conditions and the subsequent oscillations in a serial RLC circuit.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant attempts to derive equations for the circuit after the switch is opened but expresses uncertainty about their correctness.
  • Another participant suggests that the switch K disconnects the battery, allowing the circuit to oscillate until energy is dissipated, leading to equal currents in the branches.
  • There is a discussion about the initial current in the new loop being V0/R1, with acknowledgment of the inductor's influence on maintaining this current.
  • Concerns are raised about the complexity of the circuit's response, which may involve underdamped, overdamped, or critically damped behaviors, complicating the inverse Laplace transform process.
  • Participants discuss the need to consider the polarity of the initial voltage source related to the inductor current and how it affects calculations.
  • One participant mentions performing a source transformation and seeks confirmation on the correctness of their approach before applying nodal analysis.
  • Another participant affirms that nodal analysis is a valid method to proceed with the calculations.

Areas of Agreement / Disagreement

Participants express various viewpoints on the circuit's behavior and the methods to analyze it, indicating that multiple competing views remain. There is no consensus on the correctness of specific equations or approaches yet.

Contextual Notes

Participants note the potential complexity of the circuit's response and the need for careful consideration of initial conditions and component values, which may affect the analysis outcomes.

magnifik
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The circuit below operates with the switch K closed until steady state is reached. At t = 0 the switch K is opened. Determine the voltage vk(t) across the switch after it is opened. (> 0)
i3vts2.png



What I attempted to do first was redraw the circuit when the switch is opened:
r6ztar.png


I am unsure of what the next steps should be. But this is my attempt:
V0 + Vk + LI1 = R1(I1 - I2) + Ls(I1 - I2)
LI1 + V1/s = R1(I2 - I1) + Ls(I2 - I1) + R2I2 + I2/Cs

I'm not sure if these equations are correct and do not want to go on if they aren't since everything would be wrong. Thanks in advance.
 
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Perhaps it is intended that K impose the initial conditions on the system, then at t=0 K disconnects the battery from the circuit and leaves the circuit to oscillate until its energy is dissipated? The currents in the two branches therefore become equal; the current now being a loop current.
 
NascentOxygen said:
Perhaps it is intended that K impose the initial conditions on the system, then at t=0 K disconnects the battery from the circuit and leaves the circuit to oscillate until its energy is dissipated? The currents in the two branches therefore become equal; the current now being a loop current.

so i(0) = V0/R1?
 
magnifik said:
so i(0) = V0/R1?

Yes, that would be the initial current in the "new" loop -- the inductor will "insist" that it be so!

But the problem is going to be that this is a serial RLC circuit. As such it can have three distinct solution forms depending upon the particular values of the components; The circuit can be underdamped, overdamped, or critically damped.

A straight inverse Laplace transform of the circuit's Laplace domain equation for the voltage at the top node (top horizontal rail), containing all the individual circuit component values, will be a real "dog's breakfast"! Loads of sine and cosine terms, exponentials, and so on.

It might be worthwhile trying to batter it into a more familiar form by converting the terms that represent the natural frequency ωo, the damping ratio [itex]\alpha[/itex] and any time constants [itex]\tau[/itex] into those symbols.
 
gneill said:
Yes, that would be the initial current in the "new" loop -- the inductor will "insist" that it be so!

But the problem is going to be that this is a serial RLC circuit. As such it can have three distinct solution forms depending upon the particular values of the components; The circuit can be underdamped, overdamped, or critically damped.

A straight inverse Laplace transform of the circuit's Laplace domain equation for the voltage at the top node (top horizontal rail), containing all the individual circuit component values, will be a real "dog's breakfast"! Loads of sine and cosine terms, exponentials, and so on.

It might be worthwhile trying to batter it into a more familiar form by converting the terms that represent the natural frequency ωo, the damping ratio [itex]\alpha[/itex] and any time constants [itex]\tau[/itex] into those symbols.

unfortunately we have to do Laplace transform and then convert back to the time domain. i just realized that shouldn't it simplify to the circuit below with the switch open?
vwxzx4.png


Then I can do I(s) = V(s)/Z(s) where V(s) is the sum of the transform voltages and Z(s) is the sum of the transform impedances so...
I(s) = [LI1 - V1/s]/[Ls + R1 + R2 + 1/Cs]

err I suppose I should do V(s) = I(s)/Y(s)
 
Sure, you can do that (Be careful about the polarity of the initial voltage source associated with the initial inductor current. Its polarity should be in the same direction as the initial current).

Once you have the current in the time domain, presumably you can use it to work out an expression for the voltage at the top. It may involve some calculus.
 
gneill said:
Sure, you can do that (Be careful about the polarity of the initial voltage source associated with the initial inductor current. Its polarity should be in the same direction as the initial current).

Once you have the current in the time domain, presumably you can use it to work out an expression for the voltage at the top. It may involve some calculus.

is my polarity incorrect? I know usually it's the other way around, but in this case I1 is defined as going up so shouldn't the voltage source be - to + ?
 
magnifik said:
is my polarity incorrect? I know usually it's the other way around, but in this case I1 is defined as going up so shouldn't the voltage source be - to + ?

Disregard the labelled current and determine the actual direction of the initial current flow. The true polarity of the model source will be determined by that.

Otherwise, calculate the value of your I1 according to the label and you'll find it to be negative. Again, set your model voltage source accordingly. :smile:
 
So after combining impedances I have
2z86iz9.png


Then I did a source transformation
smzwp3.png


is what i have done so far correct?? can i now apply nodal analysis to get Vk?
 
  • #10
Looks okay. Sure, you can do nodal analysis, or you could continue to simplify the circuit; the current sources and impedances are in parallel...
 
  • #11
gneill said:
Looks okay. Sure, you can do nodal analysis, or you could continue to simplify the circuit; the current sources and impedances are in parallel...

awesome. thanks!
 

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