Recommended problems for Lecture 12: 26.6, 26.26, 26.37 26.45
Recommended reading for Lecture 13: Chap. 26
Now that we have the defined what a capacitor is,
we can begin our study of circuits. We have seen
that to make a capacitor all we need is two pieces of
metal. In power circuits we need large capacitors so
parallel plates are used (they are often
wrapped into cylinders), with a good dielectric material
between them. In integrated circuits metal films
are separated by insulating layers in the fabrication
process. In addition to the capacitors that we want,
circuit designers often have to deal with stray
capacitance, that is capacitors that we don't want
and can't get rid off. In circuit analysis
it is often possible to reduce a complicated
looking circuit to a simpler form. We will
learn how to do this for capacitors.
Many complicated circuits can be reduced if
we know how to reduced combinations which
are in series or in parallel.
Capacitors in series and parallel
Series combination
When capacitors are combined in series, the charge
on each plate(piece of metal) has the same magnitude. If there are
n capacitors in series, each may have a different voltage
across its plates. Let's call the voltage across the
ith capacitor Vi. We want to combine the n
capacitors which are connected in series into one
capacitor which has capacitance
Cseries. If this
is possible, this ``effective capacitor'' also has charge magnitude
Q on its places. The voltage, V, across the plates
of this effective capacitor then should satisfy,
Q = Cseries V = Cseries(V1+V2 +....Vn) | (1) |
(2) |
(3) |
Parallel combination
When capacitors are combined in parallel they have the
same voltage across each capacitor. Thus we can write
Q = Cparallel V = Q1+Q2+...Qn | (4) |
Q = Cparallel V = C1V+C2V+...CnV | (5) |
Cparallel = C1+C2+...Cn | (6) |
Example
Consider a parallel combination of
and
which
is in series with two capacitors
and
.
Parallel combination
(7) |
Series combination
(8) |
(9) |
Dielectric materials
So far, we have discussed the electric field
in vacuum. That is, we have not even included
the effect of air. However air does not alter
the electric field much, so our previous
conclusions apply almost unaltered to air. However
if we place charges inside a material, either
a liquid like water or a solid material then
there can be important changes in the electric
field and capacitance as compared to the
same charges in air. Actually we have already
seen this. The behavior of conductors is
very different than the behavior of air. However
we now want to consider insulating materials, which
we now call "dielectrics'' when they are used to
modify electric fields or when they are used inside
a capacitor. For the purposes of this course we shall
only need one formula to describe how to treat the
effect of a dielectric material on electric fields and
capacitance. We make the replacement,
(10) |
(11) |