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Physics 202
Thursday, February 18, 1999
Announcements: No recitation quiz next
week
Lab Quiz next week on the concepts covered in labs 3 and 4
Recitation quiz for February 26 or March 1 will cover chapter 25.
Lecture notes:
Capacitors, Capacitance, and Dielectrics
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A capacitor is a device to store charges ( and hence
store electrical energy). Capacitance is a measure of how effective a capacitor
is.
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Let's consider of simple circuit:

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A battery is connected to a pair a parallel plates.
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This can be shown as the following diagram:
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A battery is a device that through chemical reactions maintains a
potential difference (V) between its positive and negative terminals.
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When the battery is connected to the pair of parallel conducting plates,
( some of the) electrons in the red plate are driven to the positive terminal
and an equal amount of electrons are driven from the negative terminal
to the black plate.
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The set of parallel plates acts as a capacitor.
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The amount of charge the plate can hold is proportional to the potential
applied ( by the battery) on the plate
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Q = CV
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Q is charge measured in coulombs
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V is potential measured in volts
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C is Capacitance and its unites are coulomb/ volt
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A coulomb/ volt is equal to one Farad
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On Farad is a huge amount; we will usually deal with mF
( 10-6 F) or pF ( 10-12)
Geometry of Capacitors
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The capacitance depends on the physical characteristics
of the capacitor (i.e. the geometry)
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Parallel plate capacitor:
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The potential (or voltage) difference between the positive and negative
plates is V.
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We know that E = s /eo = Q / Aeo
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V = - I (integral) E (dot product) ds = Ed = Qd/ Aeo
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Q = CV or V= Q/C ; therefore C = Aeo
/d
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The larger the area of the plate, the more charge the plate can hold
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As d gets smaller, the capacitance increases
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Cylindrical Capacitor
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What is the electric field in the gap?
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I (Integral) E (dot product) dA = Qenclosed
/ eo
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E ( 2pr L) = Qenclosed / eo
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E = Qenclosed /( 2prL eo
)
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What is the potential in the gap?
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Vb -Va = - I (Integral from a to b)
E (dot product) ds = - I (Integral from a to b) Er dr
= - [Qenclosed /( 2prL eo
)] I (Integral from a to b) dr/r = - [Qenclosed
/( 2prL eo )]
ln (b/a)
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C= Q/V ; therefore C = ( 2prL eo
)/ ln (b/a)
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To make the capacitance very large, decrease the distance between a and
b
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What is the electric field in the gap?
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I (Integral) E (dot product) dA = Qenclosed
/ eo
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E = Qenclosed / ( 4pr2
eo )
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What is the potential in the gap?
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Vb -Va = - I (Integral from a to b)
E (dot product) ds = - I (Integral from a to b) Er dr
= - [Qenclosed /( 4peo
)] I (Integral from a to b) dr/r2 = + [Qenclosed
/( 4peo )] [ 1/r ] evaluated
from a to b
= [Q /( 4peo )]
[ (1/b) - (1/a) ] = [Q /( 4peo
)] [ (a-b)/(ab)]
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So if V = Va - Vb = [Q /( 4peo
)] [ (b-a)/(ab)]
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Then C= Q/V = ( 4peo )/
[ (ab)/(b-a)]
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To make capacitance large, a-b needs to be very small
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If we let b go to infinity, what happens?
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C = ( 4peo )/
[ (ab)/(b-a)] goes to C = ( 4peo
)/ (a)
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Therefore the Capacitance of an isolated sphere of radius a is (
4peo )/ (a)
Combination of Capacitors
A) Capacitors in parallel
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The potential difference across each of the three capacitors is the same;
it is V and it is maintained by the battery
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The changes in each capacitor are:
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q1 = C1V
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q2 = C2V
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q3 = C3V
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The total charge on all three capacitors is :
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qtotal = q1 + q2 + q3
= ( C1+ C2+ C3)V
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This process is the some for any number of capacitors in parallel
B) Capacitor in series
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V = voltage through C1 (V1) + voltage through C2 (V2)
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When the battery is connected, some electrons from the top plate of C1
are transferred to the bottom plate of C2 (through the battery). As the
negative charges accumulate at the bottom plate of C2, an equivalent amount
of negative charges are driven away from the top plate of C2 to the bottom
plate of C1.
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Summary: The amount of charges "stored" in both C1 and C2 are equal to
Q
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Notice that the amount of charges "transferred" by the battery is not the
sum of the charges on C1 and C2, but only Q.
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For an equivalent circuit, C = Q/V
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V = V1 + V2
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V1 = Q/ C1 and V2 = Q/ C2
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Therefore, V = (Q/C1) + (Q/C2) = (Q/ Cequivalent)
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Hence, (1/ Cequivalent) = (1/ C1) + (1/C2)
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The process is the same if there are more capacitors in series
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In general, when capacitors are in parallel, the capacitance increases
and when the capacitor are in parallel, the capacitance decreases.
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