Capacitor and Inductor - upload.wikimedia.org · Version 1.2 or any later version published by the...
Transcript of Capacitor and Inductor - upload.wikimedia.org · Version 1.2 or any later version published by the...
![Page 1: Capacitor and Inductor - upload.wikimedia.org · Version 1.2 or any later version published by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and](https://reader030.fdocuments.in/reader030/viewer/2022041122/5d1ebb7388c99335368df2ae/html5/thumbnails/1.jpg)
Young Won Lim05/18/2017
Capacitor and Inductor
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Young Won Lim05/18/2017
Copyright (c) 2015 – 2017 Young W. Lim.
Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and no Back-Cover Texts. A copy of the license is included in the section entitled "GNU Free Documentation License".
Please send corrections (or suggestions) to [email protected].
This document was produced by using OpenOffice and Octave.
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Capacitor 3 Young Won Lim05/18/2017
Energy Storage
+
−
+
−
+
−
+
−
+
−−
+
Final
energy stored in electric field
+
−
Final
energy stored in magnetic field
potential energy of accumulated electrons
kinetic energy of moving electrons
f (v c) f (iL)
Q Φ
Q = CV N Φ = LI
W =12CV 2
W =12L I2
Φ = BA
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Capacitor 4 Young Won Lim05/18/2017
Newton's First Law of Motion
tendency to try to maintain voltage at a constant level
a capacitor resists changes in voltage drop vc
tendency to try to maintain current at a constant level
an inductor resists changes in current flow iL
iC
iC
iL
iL
vC
vC
vL
vL
f (v c) f (iL)potential energy kinetic energy
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Capacitor 5 Young Won Lim05/18/2017
Inertia
when vc is increasedthe capacitor resists the increase
by drawing current ic
from the source of the voltage change
in opposition to the change
when iL is increasedthe inductor resists the increase
by dropping voltage vL
from the source of the current change
in opposition to the change
Δ v s
Δ iC
Δ is
Δ vC = 0 → Δ v s
Δ iL = 0 → Δ is
0+∞
0+∞
+
−
Δ v L
sc oc
oc sc
temporarily short circuit temporarily open circuit
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Capacitor 6 Young Won Lim05/18/2017
Resisting changes
resists the change of voltage
increasing vc =
increasing electric field : opposing current → back voltage drop acting as reducing the voltage drop :resists the change of voltage
resists the change of current
increasing iL =
increasing magnetic field : opposing emf → back current acting as reducing the current :resists the change of current
v s
Δ v s
is
Δ is
tries to cancel
+
−
−Δ v s
Δ v s tries to cancel Δ is
−Δ is +
−
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Capacitor 7 Young Won Lim05/18/2017
Opposition to the change
temporarily short circuit temporarily open circuit
Δ is
Δ v s change at t = 0 Δ is change at t = 0
+
−
Δ vC = 0
Δ v s
−Δ v s −Δ is
Δ iL = 0
Δ isΔ v s
by drawing current Δ iC by inducing voltage Δ vL
+
−
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Capacitor 8 Young Won Lim05/18/2017
Opposition to the change
Δ v s change at t = 0
Δ v s
−Δ v s
Δ is change at t = 0
initial t = 0
Δ v s
initial t = 0
final t = ∞
Δ v s
final t = ∞
Δ is Δ is Δ is
Δ vC = 0 Δ vC = Δ v s
Δ iC peak Δ iC = 0
Δ iL = 0 Δ iL = Δ is
Δ v L peak Δ v L = 0
sc
oc
sc
oc
−Δ is
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Capacitor 9 Young Won Lim05/18/2017
Charging
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+
−
+
−
+
−
+
−−
+
v s is
+
−
+
−
+
−
+
−−
+
iC = 0
v s
Δ v s++
− −
is
Δ is
Δ iC → 0
+
−
Δ v L → 0
vL = 0
power load power load
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Capacitor 10 Young Won Lim05/18/2017
Discharging
+
−
+
−
+
−
+
−
+
−−
+
v s is
+
−
+
− −
+
iC = 0
v s
Δ v s
is
Δ is
Δ iC → 0
+
−
Δ v L → 0
vL = 0
power source power source
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Capacitor 11 Young Won Lim05/18/2017
Dissipating Energy
when vc is decreasedthe capacitor resists the decrease
by supplying current ic
to the source of the voltage change
in opposition to the change
when iL is decreasedthe inductor resists the decrease
by producing voltage vL
to the source of the current change
in opposition to the change
Δ v s
Δ iC
Δ is
+
−
Δ v L
Δ vC = 0
Δ vC → Δ v s
Δ iL = 0
Δ iL → Δ is
Δ iC
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Capacitor 12 Young Won Lim05/18/2017
To store more energy
● static nature ● a function of V
to store more energyv
c must be increased →
increasing charges on both sides produces electron movement :a way of resisting change of V
● dynamic nature● a function of I
to store more energyiL must be increased →
increasing magnetic flux induces emf to prohibit electron movement : a way of resisting change of I
+
−
+
−
+
−
+
−−
+
Q = C⋅V Φ = L⋅I
more charges
more magnetic flux
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Capacitor 13 Young Won Lim05/18/2017
Fast Change
Δ v
+
−
+
−
+
−
+
−−
+
Q = C⋅V Φ = L⋅I
more electron imbalance
more moving electrons
fast change Δ qfast change
Δ vΔ t
large ΔqΔ t
∝ ilarge
Δ ifast change Δϕfast change
Δ iΔ t
largeΔϕ
Δ t∝ elarge
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Capacitor 14 Young Won Lim05/18/2017
Ohm's Law
whenever voltage vC
changes
there is a flowing current ic
the magnitude of the current is proportional to the rate of change
whenever current IL changes
there is an induced voltage vL
the magnitude of the voltage is proportional to the rate of change
iC = C⋅d vCdt
v L = L⋅d iLdt
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Capacitor 15 Young Won Lim05/18/2017
Stored Energy
resists to the change of voltage
to increase vc,
energy should betransferred to capacitors by the flowing current i
c
The stored energy is a function of voltage
resists to the change of current
to increase iL,
energy should betransferred to the inductors by the induced voltage v
L
The stored energy is a function of current
Q = C⋅V Φ = L⋅I
dqdt
= C⋅d vdt
dϕ
dt= L⋅
d idt
iC = C⋅d vCdt
v L = L⋅d iLdt
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Capacitor 16 Young Won Lim05/18/2017
Short term effects
iC → 0
vC → v + Δ v
vL → 0
iL → i + Δ i
the short term effect: a way of resisting
the long term result: voltage change
the short term effect: a way of resisting
the long term result: current change
+
−
+
−
+
−
+
−−
+
v s
Δ v s++
− −
is
Δ is+
−
vs is
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Capacitor 17 Young Won Lim05/18/2017
Some (i,v) signal pair examples
vC
dd t
dd t
iC
vC
iC
iL
vL
iL
vL
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Capacitor 18 Young Won Lim05/18/2017
Everchanging signal pairs
decreasing decreasing decreasingincreasing increasing increasing
negative negative negativepositive positive positive
dd t
vC
iC
iL
vL
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Capacitor 19 Young Won Lim05/18/2017
Current & Voltage Changes
constant v constant id vd t
= 0 i = 0d id t
= 0
increasing v increasing id vd t
> 0 i > 0d id t
> 0
+ −
+ −
v > 0
v = 0
decreasing v increasing id vd t
< 0 i < 0d id t
< 0
− +
v < 0
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Capacitor 20 Young Won Lim05/18/2017
Sinusoidal voltage and current
iC = C⋅d vCdt
v L = L⋅d iLdt
vC = A cos(ω t ) iL = A sin (ω t)
iC =−ωC A sin(ω t )
vL = ωL A cos(ω t)= ωC A cos(ω t + π/2)
vC
iC=
1ωC
cos(ω t)cos(ω t+π/2)
vL
iL= ω L
cos(ω t)cos(ω t−π/2)
= A cos (ω t−π/2)
V C = A 0 I L = A −π/2
IC = ωC A π/2 V L = ω L A 0
ZL =V L
I L
= ω L +π/2ZC =V C
IC
=1
ωC−π/2
= jω L=− jωC
=1
jωC
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Capacitor 21 Young Won Lim05/18/2017
Leading and Lagging Current
iC = C⋅d vCdt
v L = L⋅d iLdt
vC = cos(2 π t ) iL = sin (2π t)
iC =−π sin (2π t)
vL = π cos(2π t)= πcos (2π t + π/2)
= cos(2π t−π/2)
vC
iC v L
iL
C=0.5 L=0.5
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Capacitor 22 Young Won Lim05/18/2017
Ohm's Law
vC
iC v L
iL
V C = A 0 I L = A −π/2
IC = ωC A π/2 V L = ω L A 0
ZL =V L
I L
= ω L +π/2ZC =V C
IC
=1
ωC−π/2
= jω L=− jωC
=1
jωC
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Capacitor 23 Young Won Lim05/18/2017
Phasor and Ohm's Law
V C
IC
V C = A 0 I L = A −π/2
IC = ωC A π/2 V L = ω L A 0
ZL =V L
I L
= ω L +π/2ZC =V C
IC
=1
ωC−π/2
= jω L=− jωC
=1
jωC
I L
V L
− jωC
jω L
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Capacitor 24 Young Won Lim05/18/2017
Phase Lags and Leads
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Young Won Lim05/18/2017
References
[1] http://en.wikipedia.org/[2] J.H. McClellan, et al., Signal Processing First, Pearson Prentice Hall, 2003