Hschreiber (talk | contribs) Created page with "So far circuits have been driven by a DC source, an AC source and an exponential source. If we can find the current of a circuit generated by a Dirac delta function or impulse..." Tag: 2017 source edit |
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So far circuits have been driven by a DC source, an AC source and an exponential source. If we can find the current of a circuit generated by a Dirac delta function or impulse voltage source δ, then the convolution integral can be used to find the current to any given voltage source! | So far circuits have been driven by a DC source, an AC source and an exponential source. If we can find the current of a circuit generated by a Dirac delta function or impulse voltage source δ, then the convolution integral can be used to find the current to any given voltage source! | ||
==Example Impulse Response== | ==Example Impulse Response== | ||
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:<math>C_1 = 0</math> | :<math>C_1 = 0</math> | ||
[[en:{{FULLPAGENAME}}| | [[en:{{FULLPAGENAME}}|Impulse Response]][[de:Impulsantwort]] | ||
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Latest revision as of 07:59, 6 December 2021
So far circuits have been driven by a DC source, an AC source and an exponential source. If we can find the current of a circuit generated by a Dirac delta function or impulse voltage source δ, then the convolution integral can be used to find the current to any given voltage source!
Example Impulse Response
The current is found by taking the derivative of the current found due to a DC voltage source! Say the goal is to find the δ current of a series LR circuit ... so that in the future the convolution integral can be used to find the current given any arbitrary source.
Choose a DC source of 1 volt (the real Vs then can scale off this). The particular homogeneous solution (steady state) is 0. The homogeneous solution to the non-homogeneous equation has the form:
Assume the current initially in the inductor is zero. The initial voltage is going to be 1 and is going to be across the inductor (since no current is flowing):
- ::
If the current in the inductor is initially zero, then:
- Which implies that:
- So the response to a DC voltage source turning on at t=0 to one volt (called the unit response μ) is:
- Failed to parse (Conversion error. 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Taking the derivative of this, get the impulse (δ) current is:
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Now the current due to any arbitrary VS(t) can be found using the convolution integral:
- Failed to parse (Conversion error. 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Don't think iδ as current. It is really Failed to parse (Conversion error. 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'upper C equals negative upper A equals 1 divided by upper R', ), )"): {\displaystyle {d \over dt}\frac{current}{1 volt}} . VS(τ) turns into a multiplier.
LRC Example
Find the time domain expression for io given that Is = cos(t + π/2)μ(t) amp.
Earlier the step response for this problem was found:
- Failed to parse (Conversion error. 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The impulse response is going to be the derivative of this:
- Failed to parse (Conversion error. 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- Failed to parse (Conversion error. 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- Failed to parse (Conversion error. 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- Failed to parse (Conversion error. 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- Failed to parse (Conversion error. 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The Mupad code to solve the integral (substituting x for τ) is:
f := exp(-(t-x)) *sin(t-x) *(1 + cos(x));<br>S := int(f,x = 0..t)
Finding the integration constant
- Failed to parse (Conversion error. 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This implies:
- Failed to parse (Conversion error. 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