ELECTRIC FIELD

Concept of Electric Field

Capacitors may be defined as a two metal plates separated by an insulator the thin insulated materials are paper, mica, air, glass, oil etc. capacitor stores electric charge.


Concept of Electric Field


Capacitance is the property exhibited by a capacitor when two metal plates are connected to a source voltage. The unit of capacitance is the Farad (F) or microfarad (µF) – 10-6F. Farad is the capacitance of a capacitor which has a pd of 1V when maintain a charge of 1C.

 

Electric Field Strength (E)

Electric field strength is defined as the potential drop per unit length. Electric field strength is also called electric field intensity or potential gradient.

E = V v/m  

       D


Electric Flux Density (D)

Electric flux density is the ratio of charge to the cross – sectional area of the plate. 

Electric Flux Density formula

 If the dielectric has a relative permittivity, then

Electric Flux Density equation

Electric Charge (Q)

Electric Charge is the current that flows through the plates of a capacitor.

Q = CV

Coulombs (C)


Dielectric

Dielectric is the medium separating the plates of an insulator.

 

Permittivity of free space (𝜀𝑜)

(Electric Consonants)

It is the ratio of ratio of the electric flux density in vacuum (air) to the electric field strength.

𝜀𝑜 = electric flux density      = D

       electric field strength      E

 

D = Q/A = Q x d = Q x d

E     v/d      A    v     v   A

 

But Q = C

         v

 

𝜀𝑜 = C x 𝑑

              A

𝜀𝑜 = 8.55x10-12 F/m

𝜀𝑜 = 8.85p F/m


For a given value of applied voltage a material with a higher value of permittivity produces a greater electric flux than a material with a lower value of permittivity.

 

Relative Permittivity (er )

It is defined as the ratio of absolute permittivity to the permittivity of free space.

𝜀𝑟 =      𝑎𝑏𝑠𝑜𝑙𝑢𝑡𝑒 𝑝𝑒𝑟𝑚𝑖𝑡t𝑖𝑣𝑖𝑡y        =  𝜀

         𝑝𝑒𝑟𝑚𝑖𝑡𝑡𝑖𝑣𝑖𝑡𝑦 𝑜𝑓 𝑓𝑟𝑒𝑒 𝑠𝑝𝑎𝑐y      𝜀𝑜 

 

(Dimensionless)

 

Terminologies

1)      Capacitance is the measure of the ability to store electric charge.

2)      Charging is the process of increasing the charge held in a capacitor

3)      Discharging is the process of reducing the charge held in a capacitor.

Leakage current is the role of movement of charge through a dielectric


TYPES OF CAPACITORS

Capacitors are classified by the type of dielectric material used in their construction.

1.   Paper capacitors: They consist of thin aluminium foils separated by a layer of waxed paper. Paper capacitors are used in household appliances (e.g. fluorescent lighting fittings) and power circuits (e.g. motors).  

2.      Electrolytic capacitors: They consist of two aluminium foils, one with an oxide film/skin and one without. Electrolytic capacitors must be connected to the correct voltage polarity to prevent damage to the oxide film/skin. The main disadvantages of this type of capacitor are (a) the insulation resistance is comparatively low (b) it is only suitable for circuits where the voltage applied to the capacitor never reverses its direction. They are used where a large capacitance is required and where the terminal voltage never reverses polarity.

3.      Mica capacitors: They are constructed of thin aluminium foils separated by a layer of mica. With low dielectric loss. The main disadvantage of this type of capacitor is that it is relatively expensive. They are often used in high-frequency electronic circuits.

4.      Ceramic capacitors: A thin ceramic dielectric is coated on both sides with a metal. The capacitor is made up by making a stack of these ceramic. Ceramic capacitors are used in high-temperature situations.

5.      Air capacitors: They are usually constructed of multiple aluminium vanes of which one section moves to make the capacitance variable. They are often used for radio tuning circuits.

6.   Polyester capacitors: They are manufactured in a very thin film of thickness as little as 2μm and metallized on one side. They can operate at high voltage.

 

Application

      Power circuit of household appliances

      Reduce ripple in the voltage wave

      High frequency circuits

      High temperature situations

 

Parallel – Plate Capacitors

The capacitance of a parallel – plate capacitor (neglecting the effect of electrostatic fringing) is given by

C =  𝜀𝑜𝜀𝑟𝐴  (F)

            𝑑  

In case of an n – plate capacitor (multi-plate) capacitor the capacitor is (n – 1) times greater than between one pair of plates.

 

Energy stored in a capacitor


W = ½ CV2 


Capacitors

Multi-plate – plate capacitor

 C =  𝜀𝑜𝜀𝑟𝐴(n-1)  (F)

            𝑑   

 

Numerical Examples

1) A parallel plate capacitor consists of 5 metal plates each of area 40cm2 separated by a dielectric of thickness 0.25mm, whose relative permittivity is 5. Calculate the capacitance of the capacitor [𝜀𝑜  = 8.85 x 10-12F/m]

 

Solution

Number of plate (n) = 5

Area  (A) = 40cm2 = 40x10-2

            A = 40 (10-2)2 = 40 x 10-4

Area (A) = 40 x 10-4 =     40        = 0.004𝑚2

                                     10000  

Relative Permittivity (er) = 5

Dielectric thickness (d) = 0.25mm = 0.25/1000

                                 (d) = 0.00025m

Permittivity of free space = (eo) = 8.85x10-12F/m

C =  𝜀𝑜𝜀𝑟𝐴(n-1)  (F)

            𝑑   

 C  =  85 x 10-12 x 5 x 0.004 x (5- 1) (F)

                      0.00025

C =  85 x 10-12 x 5 x 0.004 x 4 (F)

                      0.00025

C =   7.08 x 10-12

         0.00025

   = 28320 x 10-12 F = 28320pF

   = 28.32 x 10-9

   = 28.32nF 


2) A capacitor is made with 7metal and separated by sheets of mica having a thickness of 0.3mm and a relative permittivity of 6. The area of one side of each plate is 500cm2 and a Pd of 400V is maintained across its terminals. Calculate

a.       The capacitance in micro farads

b.      The charge

c.       The potential gradient

d.      The energy stored

[𝜀𝑜 = 8.85x10-12F/m]

Solution

Number of plates         (n) = 7

Thickness   (d) 0.3mm = 0.3/1000 = 0.3mm   

Relative permittivity (𝜀𝑟) = 6  

Area (A) = 500cm2 = 500(10-2)2 = 5000cm

Voltage (V) = 400V

(a)   C =  𝜀𝑜𝜀𝑟𝐴(n-1)  (F)

                   𝑑   

        C  =  8.85 x 10-12 x 6 x 500x10-4 x (7 - 1) (F)

                             0.3 x 10-3

        C  =  15.93 x 10-12   = 53100x10-12

                       0.003

= 0.0531x10-6

= 0.0531µF

(b) Q = CV

         = 0.0531x10-6 X 400  = 21.24µC.

 

(c) E = v 400

            d     0.0003

E = 1333333.3V/m

E = 1333.3KV/m

 

(d)  W = ½ CV2  

     = ½ x 0.0531x10-6 x (400)2

     = ½ x 0.0531x10-6 x160000

     = 0.0531x10-6 x80000

     = 4248x10-6J

     = 4248µJ

 

3) A capacitor has seven parallel plates separated by sheets of mica, 0.5mm thick and a relative permittivity of 6. The capacitor whose area of each plate is 500cm2 is connected to a 400V supply. Calculate the 

a.       Electric field strength

b.      Capacitance of the capacitor

c.       Electric flux density.

[eo =8.85x10-12F/m]

Solution

Number of plates         (n) = 7

Dielectric thickness (d) 0.5mm = 0.5𝑥102𝑚𝑚

Relative permittivity (er) = 6

Area (A) = 500cm2 = 500(10-2)2 = 5000cm

Voltage (V) = 400V


a. Electric field strength (E)

E = v =        400v        =   800000v/m

    d       0.5 x 10-3m

E = 800000v/m 


c. Capacitance of the capacitor

C =  𝜀𝑜𝜀𝑟𝐴(n-1)  (F)
               𝑑   
C  =  8.85 x 10-12 x 6 x 500 x10-4 x (7 - 1) (F)
                                 0.5 x 10-3 
C  =  15.93 x 10-12   = 31860x10-12 F 
              0.0005
C = 31860pF
C = 0.03186µF


d.      Electric flux density (D)

D =  Q   =

        𝜀𝑟𝐴

 

But Q = CV

                 = 31860x10-12 X 400

       = 12744000 x10-12 C

                 = 12.744µC

 

D =  Q   =  12.7 x 10-6   

       𝜀𝑟𝐴       6 x 500 x10-6 

    = 42.48 x10-6 c/m2

 

Type of Capacitor Connections


Series Connection

If V1 and V2 are the corresponding p.ds across C1 and C2 respectively

Q = C1V1                                 Q = C2V2

V1 = Q/C1                               V2 = Q/C2


But Q = CV    or  V = Q/C 

capacitors

V = V1 + V2

V1 + V2 = 𝑄/𝐶 

𝑄/𝐶 = V1 + V2

 𝑄/𝐶 = 𝑄/𝐶1 + 𝑄/𝐶2

Q (1/𝐶) = Q(1/𝐶1 + 1/𝐶2 )

Dividing through by Q

𝟏/𝑪𝑻 = 𝟏/𝑪𝟏 + 𝟏 𝑪𝟐 + + 𝟏/𝑪𝒏          

 

Numerical Example

1) If two capacitors having capacitance of 6µF and 12µF respectively are connected in series across a 200V supply, find the 

a.       Total capacitance of the capacitor

b.      The pd (voltage) across each capacitor

c.       The charge on each capacitor


Solution

For series connection

a)      Total capacitance

𝟏/𝑪𝑻 = 𝟏/𝑪𝟏 + 𝟏 𝑪𝟐 = 1/6 + 1/10

       𝟏/𝑪𝑻 = 10 +  6  = 16

           60          60

 

CT = 60/16 = 3.75µF

CT = 3.75µF

 

b)     The charge on each capacitor

Q = CV

    = 3.75x10-6 X 200

   = 750 x10-6 C

    = 750µC


Charge is common to all series capacitors

c)      Pd across each capacitor

V1 = 𝑄 750𝑥10 6

         𝐶1     6𝑥10−6

 

 V1 = 750 = 125V

            6

 

V2 = 𝑄 750𝑥10 6

         𝐶2     10𝑥10−6

 

V2 750 = 75V

            10


Note

In series connection

V1 = 𝑄    V2 = 𝑄      

        𝐶1              𝐶2


Parallel Connection

If Q1 and Q2 are the corresponding charges in capacitance C1 and C2 respectively

Q1 = C1V             Q2 = C2V

Q = CV 

capacitor

But Q = Q1 + Q2

Q1 + Q2= CV

CV = Q1 + Q2

CV= C1V + C2

CV= C1V + C2V

V(C) = V (C1 + C2)


Dividing through by V

𝐶𝑉 = 𝑉(𝐶1+𝐶2) 
𝑉             𝑉
C = C1 + C2
CT =C1 + C2

In parallel connection

𝑉1 = 𝑉𝐶2

       C1 + C2

𝑉2 = 𝑉𝐶1

       C1 + C2 


Numerical Example
(1) Three capacitors have capacitances 2µF, 4µF and 8µF respectively are connected in parallel across a 40V supply. Calculate the 
a)      Total capacitance of the capacitor
b)      Charge on each capacitor
c)      Total energy stored

Solution
a)      Total capacitance of the capacitor
For parallel connection
CT = C1 + C2 + C3 
     = 2 + 4 + 8
    = 14µF

(b)      Charge on each capacitor 
Q1 = C1V 
     = 2x10-6 X 40
Q1 = 80x10-6C Q1 = 80µC 
Q2 = C2V
    = 4x10-6 X 40 
    = 160µC

Q3  =  C3V
    = 8x10-6 X 40  = 320µC

c)      Total energy stored

W = ½ CV2

     = ½ X 14x10-6 X (40)2

     = 7x10-6 X 1600

= 11200 x10-6 J

     = 11200µJ 


capacitor5

In the diagram above, calculate the 
(i) Voltage V1 across the 3F capacitor
(ii) Every stored in the 6F capacitor

 

Solution

i) V1 = 𝑄 = Q   = 1Q volts

     𝐶1     3      3

W = ½ C2V22 = ½ x 6 x V22 = 3V22J

 

Trial Test

capacitor


a.       The diagram above is an arrangement of capacitors in a circuit. Calculate the 

(a)      Equivalent capacitance of the two capacitors in series 

(b)      Effective capacitance in the 

(c)      Charge on the 40µF

(d)      Capacitor in the 

(e)      Voltage across C2.


b.      Show that the total capacitance of two capacitors having capacitances C1 and C2 connected in series is  C1C2/(C1+C2)


c.       What factors affect the capacitance that exists between two plates insulated from each other


d.      A capacitor consists of two metal plates, each having an area of 900cm2, spaced 3.0mm apart. The whole of the space between the plates is filled with a dielectric having a relative permittivity of 6.A p.d. of 500V is maintained between the two plates. Calculate the (a) capacitance

(b)  charge

(c)   electric field strength

(d)  electric flux density


e.       What are the factors which determine the capacitance of a parallel-plate capacitor?

 

 





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