Laplace Step Response Circuit Analysis

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Discussion Overview

The discussion revolves around the analysis of a step response circuit with a 3V input, focusing on the conversion of circuit components to the s-domain, the calculation of voltage across a resistor, and the comparison of theoretical results with empirical data. The scope includes theoretical analysis, mathematical reasoning, and practical application in circuit analysis.

Discussion Character

  • Homework-related
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning
  • Experimental/applied

Main Points Raised

  • One participant outlines their method for analyzing the circuit, including converting components to the s-domain and calculating the voltage across the resistor using a voltage divider formula.
  • Another participant questions the clarity of the LaTeX formatting and suggests that the expression for the parallel impedance of the capacitor and inductor may be incorrect.
  • Some participants note that while the capacitor behaves close to ideal, the inductor has significant equivalent resistance that varies with frequency, which may affect the expected results.
  • Concerns are raised about the tolerance variations of capacitors, with some suggesting that inexpensive capacitors can deviate significantly from their marked values, which could impact measurements.
  • Participants discuss the potential impact of inductor saturation and the importance of varying input voltage to avoid this issue.
  • There is a mention of the DC resistance of the inductor, suggesting it could be in the range of 200 to 300 Ohms, which may influence the circuit's performance.

Areas of Agreement / Disagreement

Participants express differing views on the accuracy of the theoretical model compared to empirical results, with some agreeing on the potential issues related to the inductor's behavior and capacitor tolerances, while others emphasize the need for further verification of component values and circuit behavior.

Contextual Notes

Participants highlight limitations related to the assumptions made in the analysis, such as the ideal behavior of components and the effects of frequency on inductor resistance. There is also mention of the need for error analysis in practical measurements.

Meadman23
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Homework Statement



Shown in attachment

Homework Equations


The Attempt at a Solution



I'm trying to analyze the circuit in the attached picture. This is a step response with a 3V input or 3u(t).

What I've done so far is:

1. convert all of the components to the s-domain.

R = R, L = sL, C = 1/sC

2. Combine the L and C into one impedence

[sL*(1/sC)]/[sL + (1/sC)] = Z

\[\frac{7.4999999999999985\,{10}^{7}}{0.15\,s+\frac{4.9999999999999994\,{10}^{8}}{s}}\]

3. Using voltage divider formula, solve for the voltage across R

Vout = (R*Vin)/(R+Z)

Vout = [R*(3/s)]/(R+Z)4. Simplified all calculations

Vout = (3R/s)/R+Z

\[\frac{9000.0}{\left( \frac{7.4999999999999985\,{10}^{7}}{0.15\,s+\frac{4.9999999999999994\,{10}^{8}}{s}}+3000.0\right) \,s}\]

5. Evaluated inverse laplace transform of Vout using Maxima

\[3-\frac{30\,{e}^{-\frac{250000\,t}{3}}\,\mathrm{sinh}\left( \frac{50000\,\sqrt{13}\,t}{3}\right) }{\sqrt{13}}\]

After plugging in certain times and comparing them to actual measured values this circuit provides at the same times, I get step responses with percent differences ranging from 4-30%.

I feel like this is wrong since most formulas I've derived for earlier types of circuits resemble the real life results quite closely.
 

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Meadman23 said:

Homework Statement



Shown in attachment

Homework Equations





The Attempt at a Solution



I'm trying to analyze the circuit in the attached picture. This is a step response with a 3V input or 3u(t).

What I've done so far is:

1. convert all of the components to the s-domain.

R = R, L = sL, C = 1/sC

2. Combine the L and C into one impedence

[sL*(1/sC)]/[sL + (1/sC)] = Z

\[\frac{7.4999999999999985\,{10}^{7}}{0.15\,s+\frac{4.9999999999999994\,{10}^{8}}{s}}\]

3. Using voltage divider formula, solve for the voltage across R

Vout = (R*Vin)/(R+Z)

Vout = [R*(3/s)]/(R+Z)


4. Simplified all calculations

Vout = (3R/s)/R+Z

\[\frac{9000.0}{\left( \frac{7.4999999999999985\,{10}^{7}}{0.15\,s+\frac{4.9999999999999994\,{10}^{8}}{s}}+3000.0\right) \,s}\]

5. Evaluated inverse laplace transform of Vout using Maxima

\[3-\frac{30\,{e}^{-\frac{250000\,t}{3}}\,\mathrm{sinh}\left( \frac{50000\,\sqrt{13}\,t}{3}\right) }{\sqrt{13}}\]

After plugging in certain times and comparing them to actual measured values this circuit provides at the same times, I get step responses with percent differences ranging from 4-30%.

I feel like this is wrong since most formulas I've derived for earlier types of circuits resemble the real life results quite closely.

Can you fix your LaTex? It's hard to follow what you've done with the equations so battered looking :smile:

Even so, It doesn't appear to me that your resulting expression for the parallel impedance of the cap and coil looks right. C1 is 0.002 μF, right?
 
Your basic math looks good.
As gneill says, hard if not impossible to check the details.

As far as corroborating your empirical data with your analysis I would point out that, while the capacitor probably acts very close to an ideal capacitor, such is not true of the inductor, which has very appreciable equivalent resistance in series with it. Actually, that resistance is a function of frequency, and since your step input spans a large frequency range (|1/jw|) it is wishful thinking for you to hope that you will get the exact results you expect.

As an example: set your input sine generator to about 9.2 KHz. You should see a dip in the output around that frequency. The fact that you can't attain zero output is ascribable almost entirely to the finite "Q" of the inductor.

P.S. also vary the input voltage to make sure you're not saturating the inductor which at that value most probably has a high-permeability core.
 
Also following along the lines of what Rude Man has stated about the inductor, capacitors can have a rather large tolerance variations in their values. Some inexpensive capacitors can have values that stray -20% to +80% of their marked values. You may be able to locate a Tolerance Code on your capacitor to give you an idea of what range the actual capacitance will lie. Failing that, find a capacitance meter and measure it.
 
gneill said:
Also following along the lines of what Rude Man has stated about the inductor, capacitors can have a rather large tolerance variations in their values. Some inexpensive capacitors can have values that stray -20% to +80% of their marked values. You may be able to locate a Tolerance Code on your capacitor to give you an idea of what range the actual capacitance will lie. Failing that, find a capacitance meter and measure it.

Sure, but a 0.002uF capacitor is 2000 pF which will probably be a good-quality ceramic or something equally free from those problems. Totally ignorable compared to the inductor IMO.
 
rude man said:
Sure, but a 0.002uF capacitor is 2000 pF which will probably be a good-quality ceramic or something equally free from those problems. Totally ignorable compared to the inductor IMO.

True, it depends upon the type of capacitor. Still, there will be some variance from the stated value. For a lab where one should do error analysis, it would make sense to check.

I would think that an inductor as large as 150 mH would have a DC resistance on the order of 200 to 300 Ohms.
 

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