LNA: Difference between revisions

From Class Wiki
Jump to navigation Jump to search
No edit summary
No edit summary
Line 9: Line 9:
[[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> -> -
Line 16: Line 18:
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}}
Line 24: Line 30:


</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 10:21, 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 (syntax error): {\displaystyle r = 40 Ω}