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AC i-V relationship for R, L, and C
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AC i-V relationship for R, L, and C Resistive Load Source v S (t) Asint t R A R v R i t A t v v R S R sin sin V R and i R are in phase or representation: v S (t) =Asint = Acos(t-90°)= A -90°=V I S (jw) =(A / R)-90° Impendence: complex number of resistance Z=V S (j)/ I S (j)=R Generalized Ohm’s law V S (j) = Z I S (j) Everything we learnt before applies for phasors with generalized ohm’s law
description
AC i-V relationship for R, L, and C. Source v S (t) = Asin w t. Resistive Load. V R and i R are in phase. Phasor representation: v S (t) =Asin w t = Acos( w t-90 ° )= A -90 °= V S (j w ). I S (j w ) =(A / R) -90 °. - PowerPoint PPT Presentation
Transcript of AC i-V relationship for R, L, and C
AC i-V relationship for R, L, and C
Resistive Load Source vS(t) Asint
tR
A
R
vRi
tAtvv
R
SR
sin
sin
VR and iR are in phase
Phasor representation: vS(t) =Asint = Acos(t-90°)= A -90°=VS(j)
IS(jw) =(A / R)-90°
Impendence: complex number of resistance Z=VS(j)/ IS(j)=R
Generalized Ohm’s law VS(j) = Z IS(j)
Everything we learnt before applies for phasors with generalized ohm’s law
Capacitor Load
CjCj
jj
C
j
XjI
jVZ o
CC
CC
1
90
tCAdt
dqi
Cvq
ttAv
CC
CC
C
cos
sin
90sin1
tC
AiC
ICE
VC(j)= A -90°
Notice the impedance of a capacitance decreases with increasing frequency
o
cC X
AjI 0
Inductive Load
tL
Adt
L
Ai
dt
diLv
tAv
L
LL
L
cossin
sin
90sin tL
AiL
Phasor: VL(j-90°IL(j)=(A/L) -180°
ZL=jL
ELI
Opposite to ZC, ZL increases with frequency
AC circuit analysis
• Effective impedance: example
• Procedure to solve a problem– Identify the sinusoidal and note the excitation frequency.
– Covert the source(s) to phasor form
– Represent each circuit element by its impedance
– Solve the resulting phasor circuit using previous learnt analysis tools
– Convert the (phasor form) answer to its time domain equivalent.
Ex. 4.16, p180
