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[[Image:Circuitben.jpg]]
[[Image:Circuitben.jpg]]


----
First, lets write each of the components into their Laplace form, go from the "t" to the "s" domain. Using KVL and assuming the current from ground through the voltage source>resister>capacitor>back to ground.
=====Write Each Components in Laplace Form=====
Go from the "t" to the "s" domain right off the bat. Using KVL and assuming the current from ground through the voltage source>resister>capacitor>back to ground.


Voltage Source in Volts: <math>v(t)</math> -> -
Voltage Source in Volts: <math>v(t)</math> -> -
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Resister in OHMs: r -> R
Resister in OHMs: r -> R


Capacitor in Farads: c -> 1/(C*S) - <math>V_c</math>(0) Where <math>V_c</math> is the initial voltage of the cap.
Capacitor in Farads: c -> 1/(CS) - <math>V_c</math>(0) Where <math>V_c</math> is the initial voltage of the cap.

=====Combining to portray the circuit B above using KVL gives:=====
----
-<math>V-t</math>(0)+I(s)(R+1/(CS))-<math>V_c</math>(0)=0
=====Apply KVL to Circuit B in S Domain=====
-<math>\tfrac{V_t(0)}{S}</math>+I(s)(R+<math>\tfrac{1}{CS}</math>)-<math>V_c</math>(0)=0

----
=====Solving for I(S)=====
=====Solving for I(S)=====
<math>I(S)=\cfrac{V_t(0)+V_c(0)}{S(R+\tfrac{1}{CS})}=\cfrac{(V_t(0)+V_c(0))}{SR+\tfrac{1}{C}}\frac{\tfrac{1}{R}}{\tfrac{1}{R}}=\cfrac{\tfrac{V_t(0)+V_c(0)}{R}}{S+\tfrac{1}{RC}}
<math>I(S)=\cfrac{V_t(0)+V_c(0)}{S(R+\tfrac{1}{CS})}=\cfrac{(V_t(0)+V_c(0))}{SR+\tfrac{1}{C}}\frac{\tfrac{1}{R}}{\tfrac{1}{R}}=\cfrac{\tfrac{V_t(0)+V_c(0)}{R}}{S+\tfrac{1}{RC}}
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</math>
</math>

----


=====Performing the inverse Laplace=====
=====Performing the inverse Laplace=====
<math>
<math>
L^{-1}(I(S))=L^{-1}(\cfrac{\tfrac{V_t(0)+V_c(0)}{R}}{S+\tfrac{1}{RC}})=i(t)=\frac{V_t(0)+V_c(0)}{R}e^{(-\tfrac{1}{RC}t)}
L^{-1}(I(S))=L^{-1}(\cfrac{\tfrac{V_t(0)+V_c(0)}{R}}{S+\tfrac{1}{RC}})=i(t)=\frac{V_t(0)+V_c(0)}{r}e^{(-\tfrac{1}{rC}t)}

</math>

----

=====Apply Initial Conditions=====
<math>V_t(0) = 7v</math>

<math>r = 40 Ω</math>

<math>c = 2 F</math>

<math>V_c(0) = 3v</math>

<math>

i(t)=\frac{V_t(0)+V_c(0)}{r}e^{(-\tfrac{1}{rC}t)}=\frac{7+3}{40}e^{(-\tfrac{1}{40*2}t)}=\tfrac{1}{4}e^{-\tfrac{1}{40}t}


</math>
</math>

Revision as of 11:21, 10 November 2009

Ben Henry LNA Homework

HW#5

The below problem, although simple, is done with variables so that values can be plugged in afterwords. Thus one can see how the problem progresses and see where the initial conditions end up at the end. PROBLEM STATEMENT: Solve for current i(t) in CIRCUIT A below using Laplace Transforms. The two circuits (A and B below) are the same circuit. B is the same as A, only it shows are current when we use KVL and after we have moved the circuit into the "S" domain.

Circuitben.jpg


Write Each Components in Laplace Form

Go from the "t" to the "s" domain right off the bat. Using KVL and assuming the current from ground through the voltage source>resister>capacitor>back to ground.

Voltage Source in Volts: -> - (0)/S

Resister in OHMs: r -> R

Capacitor in Farads: c -> 1/(CS) - (0) Where is the initial voltage of the cap.


Apply KVL to Circuit B in S Domain

-+I(s)(R+)-(0)=0


Solving for I(S)


Performing the inverse Laplace


Apply Initial Conditions

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle r = 40 Ω}