Capacitors in Electrical Circuits, Study notes of Physics

A comprehensive overview of capacitors and their role in electrical circuits. It covers the fundamental principles of capacitance, including how capacitors store electrical energy, the factors affecting capacitance, and the behavior of capacitors in series and parallel configurations. The document also discusses the concept of time constant and the discharging process of capacitors. With detailed explanations, formulas, and illustrative examples, this document serves as a valuable resource for understanding the practical applications of capacitors in various electronic circuits and systems.

Typology: Study notes

2022/2023

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Capacitor
Hence
capacitors
are
always
attached
in
parallel
to
circuit
so
that
An
electronic
component
that
is
used
the
circuit
keeps
on
working
even
to
store
electrical
energy
and
supply
when
capacitor
is
fully
charged
.
current
to
the
circuit
when
need
be
.
metal
plates
Explain
why
capacitor
stores
energy
,
not
charge
.
Symbol
:
For
a
parallel
plate
capacitor
,
both
plates
have
equal
and
opposite
charge
,
hence
net
charge
is
zero
.
I
Parallel
plate
capacitor
Work
is
done
in
separating
those
insulator
charges
therefore
energy
is
1
dielectric
material
)
stored
.
Uses
of
capacitor
1
Functions
)
Capacitance
1.
Stores
energy
2.
Time
delay
circuits
It
is
the
charge
stored
on
one
3.
smoothing
in
rectifier
plate
of
a
capacitor
per
unit
4.
Power
supplies
5.
Tuni ng
circuits
potential
difference
.
Charging
a
capacitor
C
=
9
or
q=CV
pod
.
v
t
I
Positive
terminal
pulls
charge
capacitance
electrons
from
one
plate
and
negative
SI
Unit
:
Farad
11=1
¥
terminal
deposits
them
on
the
other
.
Define
the
Farad
111=1
:
It
is
the
capacitance
of
a
capacitor
when
>
+
-
Both
plates
begin
to
1C
of
charge
is
stored
across
a
achieve
equal
&
opp
.
p.d.
Of
IV.
charge
.
Charging
process
stops
when
the
Factors
affecting
capacitance
p.cl
.
across
the
capacitor
is
equal
to
EMF
of
the
battery
.
1.
*
surface
Area
of
plates
Bigger
SA
of
plate
>
more
capacitance
+
-
I
=
+
-
"
I
=
2.
Insulation
-
better
insulators
more
capacitance
I
-
i
'
II
+
-
+
-
3
.
Distance
between
plates
lamp
off
after
Lamp
still
on
!
more
capacitor
charges
less
distance
stronger
field
capacitance
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Physics by Kashan Rashid
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Capacitor Hence^ capacitors are^ always attached

in parallel to^ circuit^ so that

An electronic component that^ is^ used the circuit keeps on working even

to (^) store electrical (^) energy and^ supply when (^) capacitor is fully charged.

current to^ the circuit^ when^ need

be. →

metal plates Explain why capacitor stores energy ,

not (^) charge.

Symbol : • For a

parallel plate (^) capacitor,^ both

plates have^ equal^ and^ opposite

charge,^ hence^ net^ charge^ is^ zero^.

I ←^ Parallel^ plate capacitor • Work is^ done in separating those

insulator charges

therefore energy^ 1 is dielectric material (^) ) (^) stored. Uses (^) of capacitor 1 Functions (^) ) (^) Capacitance

  1. (^) Stores (^) energy 2. (^) Time (^) delay circuits It is the (^) charge stored on one
    1. (^) smoothing in (^) rectifier plate (^) of a (^) capacitor per unit
      1. (^) Power (^) supplies 5.^ Tuning circuits (^) potential (^) difference.

Charging a^ capacitor C^ =^9 v^ or^ q=CV→^ pod^.

  • t^ I

Positive terminal^ pulls charge capacitance

electrons (^) from one ¥ (^) terminal plate and negative SI Unit :^ Farad 11= deposits them ⑦ on^ the^ other^.^ Define^

the (^) Farad 111=1 :^ It is the > (^) + - • Both capacitance^ of^ a^ capacitor^ when achieveplates begin^ to^ 1C^ of^ charge^ is^ stored^ across^ a

equal &^ opp.^ p.d.^ Of IV.

charge.

  • Charging (^) process (^) stops when (^) the Factors (^) affecting capacitance

p.cl. across^ the^ capacitor is^ equal^ to

EMF of the^ battery. 1.* surface Area^ of plates

I =^ +^ -^ Bigger^ SA^ of^ plate^ >^ more^ capacitance

"

I =^ 2.^ Insulation

  • I - i^ ' II better^ insulators^ →^ more^ capacitance
        • (^3). Distance between (^) plates lamp (^) off after Lamp^ still^ on^!^ more

capacitor charges^ less^ distance^ →^ stronger^ field^ →^ capacitance

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Energy stored^ in^ a^ capacitor capacitors^ in^ series

g-^ -^ CV Tc=qgt (^) ±, = I = ++ =

✓μ ^^ Cz^ + - +

c. (^) ,

° For the same V (^) , C (^) , stores more > V '^ '^ '^ '='^ '^ '^ '^ '^ '^ ': (^) charge than Cz (^). + -

= = VT 19T^ )

o =^ I^ > ° As^ q ✗^ C^ , C^ , > Cz .

(^092 9) , (^) qlc Charge :^ Each (^) capacitor gains the

same magnitude of charge

on one of its^ plates. VIV (^) As V= (^) Energy go (^9) , = 92=93 = (^) 9T ^ (^) R (^) charge i (^) E-- Vxq Voltage : (^) Each (^) capacitor achieves " (^) a different p.cl. based

to

' under^ = Energy on^ their^ capacitance^. "^ graph^ stored^ in ° 0 : (^) capacitor 9=95-9^ q=cv^ Text

>qk 44=44 Tt

Aof A-- lzbh (^) or smallermore capacitors^ achieve pd and^ vice^ versa^. =tzqV so^ Ecap^

: Izvq Lil, --^ 4-^ Vt

sum of all^ P.d. is^ equal

v v^ to^ EMF^ of source^.

if g--^ CV^ so^ if V^ - - Eso (^) Vi 1- (^) V2 -1 (^) V3 = (^) Vt Ecap (^) :{V44^ Ecap - -1-21% **E cap : Izu Ecap -.^ 1- 2C^ Ñ Capacitance :^ V1^ +^ V2^ +^ V3^ =^ Vt

* * as^ g--^ CV^ so^ V=^9

BE (^) cap z -1244?^

  • (^) V (^) ;) T II. +^ %: %: %. VIV ^ As (^9) , =^ 92=93^ =^ Ut V - = -1 Area =^ W^ -^ D^ by battery

÷ iv.^ ☐^ by^ battery^

: (^) Va ✗ (^) ( E. + IgE,^ )^

  • -41¥ ) =. During (^) charging (^) process o = > (^) way of the (^) workdone (^) = I (^0) or 91C (^) by the (^) source is , +^ {at^ É, cell (^) / (^) Battery stored in (^) capacitor and the^ other (^) half (^) for identical (^) capacitors , G-^ = En

lost as heat^ in capacitance <

connecting wires^!^ of each^ no. -

-9 cap.

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Discharging of a^ capacitor Time^ Constant^ :^ The^ time^ taken

C forits^ the^ capacitor^ to^ decrease

±,^ I^ • the rate charge^ /voltage/^ current^ in

of discharge^ circuit^ ,^ to^ § of its^ initial

+^

of (^) directlya^ capacitor is

proportional value^.

to the^ chaise on q =^ g.^ e-^ that Éc

capacitor.

if t^

    • RC (^) so II. ✗^ x^ > (^) x= Koe
  • " t g = g. e-^7 ¥ such relations^ follow exponential functions!^ q=%e^

q = 9oz or^9 = Lego 9 ¥ ✗^9 >^ q=^ g.^ e-^

Éc

e e' so 1g =^00368 (^ 36.8%^ ) 1 ¥.^ ✗^

V >^ V^ =^ V.^ e-^ Éc

After t=T^ ,^ remaining^ charge^ is 1 ¥,^ ✗^

I >^ I^ =^ Ioe

  • ¥' 36.8% (^) of its^ initial^ charge.
  • go^ :^ initial^ charge^ It^ :o) Vo :^ initial^ voltage^ It^ :o)

Io :^ initial^ current^ It^ :o)

  • (^9) , V (^) ,^ I^ : quantities at^ time^ t^.
    • R :^ resistance •^ C : capacitance 91C ^ - (^) T, > T, as^ graph 2 No • reduces (^) charge at a

faster rate.

Of (^) , -^ l^ l^ l^ l^ l^ l--l^ l^ l^ l^ l^ l-- O ==^ =-^ T,

0 Tz T,

% (^) >

t /s

T =^ RC , where T is^ Time Constant

Larger Time^ constant^ >^ dischargeslower.

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Examiner’s^ For Use

5 A solid metal sphere, of radius r , is insulated from its surroundings. The sphere has charge + Q. This charge is on the surface of the sphere but it may be considered to be a point charge at its centre, as illustrated in Fig. 5.1.

+ Q

r

Fig. 5. (a) (i) Define capacitance. .................................................................................................................................. ............................................................................................................................ [1] (ii) Show that the capacitance C of the sphere is given by the expression C = 4 πε 0 r.

[1]

(b) The sphere has radius 36 cm. Determine, for this sphere, (i) the capacitance,

capacitance = ............................................ F [1]

Charge stored^ per unit^ potential (^) difference.

C--

g- C=q/^ ✗ 4H§ as V=^ 9-^ C=4lTEor 41T for C=q÷u÷Eor

( =^ UH^ C- or C- UH^ (8.85×10-1410.36)

( =^40 × 10 -^ "^ F

4. 0 × 10 - "

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Examiner’s^ For Use

5 (a) State two functions of capacitors in electrical circuits.

  1. .....................................................................................................................................
  2. ..................................................................................................................................... [2] (b) Three capacitors, each marked ‘30 μF, 6 V max’, are arranged as shown in Fig. 5.1.
A B

Fig. 5. Determine, for the arrangement shown in Fig. 5.1, (i) the total capacitance,

capacitance = ......................................... μF [2] (ii) the maximum potential difference that can safely be applied between points A and B.

potential difference = ........................................... V [2]

stores (^) energy Used in (^) tuning circuits

I

30 μF^30 μF

30 μF

É=ÉiÉ 30 μF 60 μF^ ÷ :-O -1%

Ct - -20μF

20

q, 92 q=CVe.^ we^ assume^ Max^ 6V^ on^ the

  • • q same in^ series^ smallest^ capacitor i.^ e-^ 30mF

9 , =^ 9h^9 ,^ =^ Nt

30 μF 60 μF^ *✗ t.gg (^) qv,=CzVz GV, = CTVT 1 t^ smaller^ " C^ " more (^30) ×6=60 ✗ (^) Vz 30 ×6=20 ✗^ Vt bv?^?^ " v " v. =zv Vt=9V✓✓

maxv =^ 6+3=9^ V

\

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Examiner’s^ For Use

(c) A capacitor of capacitance 4700 μF is charged to a potential difference of 18 V. It is then partially discharged through a resistor. The potential difference is reduced to 12 V. Calculate the energy dissipated in the resistor during the discharge.

energy = ........................................... J [3]

DE = E C (^1) Vi-^ Vi^4

1- I 4 7 00 ✗^10 -^ b)^ (^122 -^184

= - 0.^423 J

O o (^42)

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(b) Switch S is now moved to position Y. State what happens to the potential difference across capacitor P and across capacitor Q. capacitor P: .............................................................................................................................. ................................................................................................................................................... ................................................................................................................................................... capacitor Q: ............................................................................................................................. ................................................................................................................................................... ................................................................................................................................................... [4] [Total: 8]

It (^) discharges (^) from 3V^ to^ ov^ as^ it^ is connected (^) across resistor.

It (^) changes (^) up (^) from bv^ to^ 9V^ and^ battery's

p.cl is^ greater than^ 6N.

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7 (a) Explain what is meant by the capacitance of a parallel plate capacitor. ................................................................................................................................................... ................................................................................................................................................... ................................................................................................................................................... ...............................................................................................................................................[3] (b) A parallel plate capacitor C is connected into the circuit shown in Fig. 7.1.

120 V A
X Y
S
C

Fig. 7. When switch S is at position X, the battery of electromotive force 120 V and negligible internal resistance is connected to capacitor C. When switch S is at position Y, the capacitor C is discharged through the sensitive ammeter. The switch vibrates so that it is first in position X, then moves to position Y and then back to position X fifty times each second. The current recorded on the ammeter is 4.5 μA. Determine (i) the charge, in coulomb, passing through the ammeter in 1.0 s,

charge = ....................................................... C [1]

It is The^ charge stoned^ on^ one^ plate of a^ capacitor

per unit^ potential^ difference across^ the^ plates^. C-- Ig

where (^) or is (^) charge on (^) one (^) plate and^ U^ is the (^) pod. across them.

→.

q =^ It of =^ 4.5×10-6^ ×^1 of =^ 4.5×10-6^ (

4. 5 ×10-

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