DIRECT CURRENT CIRCUIT THEORY

electric current


DIRECT CURRENT (DC) CIRCUIT 

In direct current circuits, current flows in one direction only. Such current is said to be unidirectional. An electrical circuit is a symbolic representation showing all the components forming the circuit. 

DEFINITIONS 

Electric Current (I) 

Electric current is a measure of the rate of movement of charged particles along an electrical conductor. It is measured in ampere (A) using an ammeter. 

Electromotive Force (E)  

Electromotive force (emf) is the force which drives electrons round the circuit. It is measured in volts (V) using a voltmeter. 

Resistance (R) 

Resistance is the opposition offered to the flow of electric current in a circuit. It is measured in ohms (Ω) using an ohmmeter. 

Conductor 

A conductor is a material that readily allows the flow of electric current (charge) through it. Conductors have very low resistance to the flow of electric current. Examples are copper, aluminum, iron, silver etc.  

Electrolyte 

It is a substance whose aqueous solution conducts electric current. Examples are salts (sodium chloride), Potassium Carbonate acids (hydrochloric acid, tetraoxosulphate (v) acid and bases (copper oxide, sodium hydroxide).  

Insulator 

An insulator is a material that does not allow the flow of electric current through them. Insulators have high resistance to the flow of electric current. Examples are glass, plastics, porcelain, dry wood, polythene, ebonite, etc.  

Semiconductor 

A semiconductor is a material whose resistively lies between a good conductors and a good insulator. Examples are silicon, germanium, arsenic, indium, phosphorus etc.  
 

Sources of Energy 

Battery: A battery is the combination of two or more cells connected in series. 

Cell: A cell is a device that converts chemical energy into electrical energy. There are two basic sources of electrical energy.  

Primary Cells: They produce direct current and voltage and cannot be recharged when discharged. Examples are torchlight battery, watch battery etc.  

Secondary Cells: They produce direct current and voltage and can be recharged when discharged. Examples are lead acid accumulator, electric bell etc.  

 

Resistors 

A resistor is a device used to oppose/regulate the flow of electric current in a conductor. The magnitude/size of the resistor is referred to as resistance. 

electric current

TYPES OF RESISTORS 

(1) Carbon 

(2) Wire wound 

(3) Variable 

 

THE STANDARD COLOR CODE 

Resistor values are often indicated with color codes. The code is given by several bands. Together they specify the resistance value, the tolerance and sometimes the reliability or failure rate. 

Resistors color code is a system of identifying resistors by painting or coloring its bands. The resistance value, tolerance and wattage rating are generally printed on the resistors as numbers or letters. But when the resistors are small (e.g. 1/4W, 1/2W etc.), these specifications must be shown in some manner as the print would be small to read. Therefore, small resistors use color printed bands to indicate both their resistive value and their tolerance with the physical size of the resistor indicating its wattage rating. 


THE STANDARD COLOR CODE 

COLOR

BAND A 1ST NUMBER

BAND B 2ND NUMBER

BAND C NUMBER OF NOUGHT

BAND D TOLERANCE

BLACK

0

0

0

-

BROWN

1

1

1

1%

RED

2

2

2

2%

ORANGE

3

3

3

-

YELLOW

4

4

4

-

GREEN

5

5

5

-

BLUE

6

6

6

-

VIOLET

7

7

7

-

GREY

8

8

-

-

WHITE

9

9

-

-

SILVER

-

-

÷100

10%

NON

-

-

-

20%

PINK

-

-

-

 

GOLD

-

-

÷10

5%


Numerical Example

1. A resistor is coded, yellow, violet, red and gold. Determine the value of the resistor.

 

Solution

Yellow = 4, Violet = 7, R = 2, Gold = 5%

= 4700 + 5%

= 4700 × 5100

= 235Ω


Upper value = 4700 + 235 = 4935Ω  = 4.935KΩ

Lower value = 4700 – 235 = 4465Ω  = 4.465KΩ

Tolerance ranges from 4.465KΩ - 4.935kΩ

 

2. A resistor is coded green, blue, brown and silver. Determine the value of the resistor. 

 

Solution

Green = 5, Blue = 6, Brown = 1

Silver = 10%

560 ± 10%

560 × 10⁄100

= 56Ω 

Upper limit = 560 + 56 = 618Ω

                    = 0.616KΩ

Lower limit = 560 – 56 = 504Ω

                    = 0.504KΩ

Ranges from 504Ω - 616Ω.

 

3. A resistor marked with color bands red, violet, orange and gold has the value of? (NOVDEC. 2005 Objective Question 30)

 

Solution  

R = 2, Violet = 7, Orange = 3, Gold = 5% = 27000 ± 5%

 

= 27000 ×5⁄100 = 2,70k KΩ    

 

4. The resistance of 650 resistor of a tolerance of 10% ranges from? (SSCE May/June 2011 Objective Question 57)

 

Solution

Blue = 6, Green = 5, Brown = 0

= 650 ± 10%

650 ×10⁄100= 65  


Upper limit = 650 + 65 = 715Ω

Lower limit = 650 – 65 = 585Ω

Ranges from 585Ω - 715Ω  

Types of Resistors Connections 

1. Series connection  

2. Parallel connection  

3. Series-Parallel Connection  


Series Connection  

A resistor is said to be connected in series when the same current flows through each resistor. It implies that the resistors are connected on the same wire (conductor).  

The total (equivalent or effective) resistance is greater than the value of the highest individual resistance in the circuit.  

Series connection resistor

In series resistors, current is the same

I = I1 + I2 + I3

Sum of Voltage drops equal the supply Voltage

V = V1 +V2 +V3

V1  =  IR1,  V2  =  IR2,  V3  =  IR3

From Ohm’s Law

V  =  IR

V  =  IR1  + IR2  +  IR3

IR =  IR1  + IR2  +  IR3

Dividing through by I

R  =  R1  +  R2  +  R3


Example 

series resistors

Calculate the total resistance in the circuit above.  

Solution

RT = R1 + R2 +R3 + R4

     = (2+1+3+4) Ω

     = 10 Ω 


Parallel Connection  

A resistor is said to be connected in parallel with one another when the same voltage appears across each resistor.  

The total (equivalent or effective) resistance is less than the value of lowest individual resistance in the circuit. 


resistor


In parallel circuit, Voltage is the same

V  =  V1  =  V 2 =  V3

Sum of currents through each component equal the supply current

I  =  I1  +  I2  +  I3

 

From Ohm’s Law 

I  =  V/R

I1 =  V/R1,  I=  V/R2,  I3  =  V/R3

I  =  V/R1  +  V/R2  +  V/R3

V/R  =  V/R1  +  V/R2  +  V/R3

Multiplying through by 1/V 

 1/R   =   1/R1   +   1/R +   1/R3

resistors

  

Example
Calculate the total resistance in the diagram above.

Solution

1/RT   =   1/R1   +   1/R +   1/R3

= 1/2 + 2/4 + 3/6

 = (6 + 3 + 1)/12

1/RT  = 10/12

 RT = 12/10 = 1.2


Series – Parallel Connection  

Resistors are said to be connected in series-parallel when the same current flows through the series resistors and the same voltage appears across the parallel resistor.  


Resistors

Calculate the total resistance in the diagram above.  


Solution 

Solve parallel connection first  

1/RT   =   1/R1   +   1/R 

= 1/2 + 1/4

 = (2 + 1)/4 = 3/4

1/RT  = 3/4

 RT = 4/3 = 1.3

Alternatively

Rp = (R3 x R4) / (R3 + R4)

 2 X 4

         2 + 4

      = 8/6 = 1.3

Then the circuit becomes  
resistance

𝑅𝑇 = 𝑅1 + 𝑅2 + 𝑅𝑃

= 2 + 3 + 1.3 

= 6.3Ω 


Quantity of Electricity 

Quantity of electricity is defined as the quantity of electric current passing through a given point in a circuit in a length of time. It is measured in coulombs (c). 

Quantity of electricity = Current x time  

Q = It 

Q = Quantity of electricity (coulombs)  

I = Current (Ampere) 

T= Time interval (Seconds)  


Numerical Example 

1. The current flowing in a circuit is 2A. Calculate the quantity of electricity in the circuit in a time interval of 40 seconds.  


Solution 

Current (I) = 2A  

Time (t) = 40 seconds  

Quantity of electricity (Q) = ? 

Q= It  

   = 2 × 40 

   = 80c  

 

2. A current of 20mA flows for 2hrs through a circuit. Calculate the quantity of electricity passing through the circuit. 


Solution  

Current (I) = 20mA = 20X10-3 = 20/1000 = 0.02 

Time (t) = 2hs = 60s = 1m, 60m = 1hr, 120m = 2hrs, 

therefore 120X60 = 7200s 

Q = It  

   = 0.02 X7200 

  = 144c 


1. A current of 120mA flows for 3hrs through a circuit. Calculate the frequency of electricity passing through the circuit.  

2. The current flowing in a circuit is 6A. Calculate the time intervals in seconds if the quantity of electricity in the circuit is 240c.  

3. Calculate the current flowing in a circuit if the quantity of electricity in the circuit is 80c in a time interval of 40 seconds.  


OHM’S LAW 

Ohm’s law states that the current flowing through a metallic conductor is directly proportional to the potential difference (voltage) provided temperature is kept constant.  

 

I α V/R    →  I = KV/R

I = V/R

V = IR

 

NUMERICAL EXAMPLE 

A torch has 6V battery and a bulb of resistance of 12Ω. Calculate the current flowing through the bulb when the switch is closed.  

Solution 

Voltage (V) = 6V 

Resistance (R) = 12Ω Current (I) =?  

From ohm’s law, I = V

                       𝑅

I  = 5/12

 

I  =  0.5A  


Power and Energy

Electrical Power 

Power is defined as the rate of dissipating energy. The unit of power is the watts (W) and measured using a wattmeter. 

Power  =    Energy

                    Time

P = I2 R,           P = I V ,     

P = V2/R

 

Electrical Energy

Electrical energy is defined as the consumption of power in a length of time. It is measured in joules (J). 

E  =  Power × Time

E  =  I2Rt,   E  =  IVt    ,  E  = V2t/R

 

Numerical Example

(1) A cell of emf 5V is connected to a circuit of resistance 8Ω. Calculate; 

(a)  The current in the circuit 

(b)  The power consumed by the circuit 

(c)The energy consumed if the emf is connected for 22min 

Solution

Voltage (V) = 5V 

Resistance (R) = 8Ω

Time (t) = 22min 


(a) Current (I) = V = 5        

                           R    8

I = 0.625A

(b) P = IV = 0.625 X 5 

      P = 3.125 W 

(c) Energy (E) = 𝑃𝑜𝑤𝑒𝑟 × 𝑡𝑖𝑚𝑒  

E = I2Rt,  

But 1minute = 60seconds, 22minutes = 22x60 = 1320s

                                                                     1

     = 0.625 × 0.625 × 8 × 1320

     = 41255J

 

(2) A student leaves an electric iron on for a period of 8hours. If the iron has 2KW element, calculate the energy consumed in;

(a) Joules

(b) KJ

(c) KWh

Solution

Power (P) = 2KW =2000W

Time (t)    = 8H = 8 × 3600s = 28800s

Energy (E) =?


(a) E = Power × time

      E = 2000  × 28800

      E = 57600000J 

 

(b) E = 57600000/1000

      E = 57600KJ 

(c) E    = Power (KW) × time (h)

E = 2KW × 8h

      E = 16KWh


resistance


From the circuit above, calculate the; 

(a) Effective resistance in the circuit  

(b) Total current in the circuit  

(c)Current in the 6Ω resistor  

(d) Current in the 3Ω resistor

(e) Power in the 2Ω resistor  

(f) Energy consumed by 4Ω resistor  

If the circuit was on for 10 minutes  


Solution

Parallel 

(a)   1  =  1   +    1

       Rp    R3       R4

1  +   1   =  2 + 1  = 3

3       6            6       6

 Rp = 6  = 2

          3      

 

In Series connection 

(a) 𝑅𝑇 = R1 + R2 + RP

            = 2 + 4 + 2 = 8Ω

      𝑅𝑇 = 8

Total current 

IT =   V  =  12 = 1.5A

         RT      6

 

 

(b) Current in the 6Ω resistor Using current divides rule

 

    IR4 =   IT  x  R3  =  1.5 x 3  =   4.5  = 0.5A

              R3 +  R4          3 +  6          9 

  

(c)    Current in the 3Ω resistor  

 IR3 = IT  x  R4  =  1.5 x 6  =   9 = 1A

         R3 +  R4          3 +  6        9 

 

(d)    P𝑅2 = (𝐼𝑇)2  ×𝑅2  

              = (1.5)2 × 2

             = 2.5 × 2 = 4.5𝑊

 

(e)    Energy in 4Ω resistor in 10 minutes 

       10 minutes = 10 x 60 = 600s

       𝐸 = 𝐼2𝑅4 × 𝑅4 × 𝑡  

            = (1.5)2 × 6 × 600

          = 2.25 × 4 × 600 

          = 900J


Resistivity and Conductivity 

Resistivity: Resistivity of a material is the ability of the material to oppose/regulate the amount of current flowing through the material. Resistivity is the reciprocal of conductivity. Low resistivity relates the materials having low opposition to the flow of current.  The resistance of a material depends on;

(a) The resistivity of the material (p) (Ωm) 

(b) The length of the material (l) (m)  

(c) The cross – sectional area of the material (𝑚2) 

 

Numerical Example 

(1)A copper wire has a length of 200m and a cross – sectional area of 0.2 × 10−6𝑚2. Calculate the;  

Resistance of the material if the resistivity of copper is 1.73 × 10−8Ω𝑚. 

Solution

Length (L) = 200m 

Area (a) = 0.2 × 10−6𝑚2

Resistivity (p) = 1.73 × 10−8Ω𝑚

Resistance (R) = ?

R   =   𝓅𝑙 /𝑎 

      = 1.73 × 108 x 200

                 0.2 x 10-6

 

     = 1730 × 10−2 = 17.3Ω

 

(2) Calculate the resistance of 300m length of copper wire of diameter 1 mm whose resistivity is

1.73 × 108 m

 

Solution

Length (l) = 300m

Resistivity ( = 1.73 × 108 m  

Diameter (d) = 1mm = 1 × 103   

Area of conductor (a) = ?

𝑎 = πd2 = 3.142 x (1 x 10-3)2

         4                        4

    = 3.142 x 10-6

               4

𝑎 = 0.7855 x 10-6 m2

 

R   =   𝓅𝑙 /𝑎 

     = 1.73 × 108 x 300 =   51.9   x  10-8

          0.7855 x 10-6             0.7855 x 10-6

     = 660.726 x 10-2

    = 6.61Ω

 

Conductivity: Conductivity is the ability of a material to allow the free passing of electric current through it. The symbol for conductivity is (ϭ) sigma.

ϭ = 1/𝓅(Ωm)-1

Conductance: Conductance is the reciprocal of resistance of a material. The symbol is G.

G = 1/R Siemens (S)

 

Numerical Example

(1)  A copper wire has a resistance of 10Ω. Determine its conductance.

 

Solution

Resistance (R) = 10Ω

Conductance (G) =? 

  G =1/R = 1/10 = 0.15S

 

(2)  A copper wire has a conductance of 0.2 Siemens.  What is the resistance of the wire? 

 

Solution

Conductance (G) = 0.2S

Resistance (R) =? 

 R =1/G = 1/0.2 = 5   

 

(3) A copper wire of length 50m has a conductance of 5 Siemens. Calculate the area of the conductor if the resistivity of copper is 0.0173Ωm. (Take 𝓅 = 0.0173µm)


Solution

Length (l) = 50m 

G = 5S

𝓅 = 0.0173µm = 0.0173 x 10-6m

 

G = ϭ𝑎  ,  𝑎 = G𝑙     
        𝑙              ϭ

 But ϭ = 1/ 𝓅 = 1/(0.0173 x 10-6) = 57.8 x 10-6m

𝑎 = (5 x 50)/( 57.8 x 10-6) = 4.33 x 10-6m2

  𝑎 = 0.00000433 m2


TEMPERATURE COEFFICIENT 

A temperature coefficient describes the relative change of a physical property that is associated with a given change in temperature.  

The resistance of most materials changes with temperature. In general, conductors increase their resistance as the temperature increases and insulators decrease their resistance with a temperature increase. 

Therefore, an increase in temperature has a bad effect upon the electrical properties of a material. Each material responds to temperature change in a different way, and constants have been calculated for each material (temperature coefficient of resistance ∝). 

 

Temperature coefficient values

Material

Temperature coefficient ( Ω/ Ω oС)

Silver

 0.004

Copper

 0.004

Aluminium

 0.004

Brass

 0.001

Iron

 0.006

Carbon

-0.00048

Tin

 0.0044

 

For a temperature increase from 0 oС

Rt = Ro (1 + t) (Ω)

Where

Rt =  the resistance at the new temperature t oС

Ro = the resistance at  0 oС

  = the temperature coefficient for a particular material

For a temperature increase between two intermediate temperatures above 0 oС

R1/R2 = (1 + t1)/(1 + t2

Numerical Example

(1) The field winding of a D.C. motor has a resistance of 100Ω at 0 oС. Determine the resistance of the coil at 20 oС if the temperature coefficient is 0.004 Ω/ Ω oС.

 

Solution

Ro = 100Ω , t = 20 oС , =  0.004 Ω/ Ω oС

Rt = Ro (1 + t)(Ω)

Rt = 100 Ω (1 + 0.004 Ω/ Ω oС × 20 oС)

Rt =  100 Ω (1 + 0.08)

Rt =  108Ω  


(2) The field winding of a generator has a resistance of 150Ω at an ambient temperature of 20 oС. After running for some time, the mean temperature of the generator rises to 45 oС. Calculate the resistance of the winding at the higher temperature if the temperature coefficient of resistance is 0.004 Ω/ Ω oС.

 

Solution

R1 = 150 Ω , 

t1 = 20 oС , t2 = 45 oС , 

= 0.004 Ω/ Ω oС ,  

R2 = ?

R1/ R2 = (1 + t1)/(1 + t2)

150    = (1+ 0.004 Ω/ Ω oС  × 20 oС)
  R2       (1+ 0.004 Ω/ Ω oС  × 45 oС)
150Ω/R2 = 1.08/1.18
R2 = (150Ω × 1.18)/1.08
R2 = 164Ω 


APPLICATIONS OF TEMPERATURE COEFFICIENT OF RESISTANCE 

(1) Positive Temperature Coefficient (PTC) Thermistors 

(2) Negative Temperature Coefficient (PTC) Thermistors 

(3) Heaters 

 

KIRCHHOFF’S LAWS 

The laws were proposed by a German physicist called Gustav Robert Kirchhoff (1824-1887) Junction/Node: A junction or node is point at which two or more conductors meet.  

 

Kirchhoff’s First Law (Current Law)  

Kirchhoff’s first law states that the total current flowing towards a junction (node) in a circuit is equal to the total current flowing away from it.  

 

Implication of the First Law  

Current cannot accumulate within a circuit. 

Total current flowing towards the node N = 𝐼3 + I4

Total current flowing away from the node 

𝑁 =𝐼1 +𝐼2

 Therefore;  𝐼1 + 𝐼2 = 𝐼3 + 𝐼4

∑ 𝐼1 +I2   =   ∑ 𝐼3 + 𝐼4

(∑ 𝐼1 + I2) – (∑ 𝐼3 + 𝐼4) = 0

Algebraic sum of currents is zero.  



Kirchhoff’s Second Law (Voltage Law) 

Kirchhoff’s second law states that in any closed circuit, the algebraic sum of the potential drops and emf’s is zero. 

 

 Voltage Law


Implication of the   Second Law  

The sum of emfs + sum of pds = 0 

∑(𝑒𝑚𝑓𝑠) + ∑(𝑝𝑑𝑠) = 0  

𝐸1 − 𝐸2 = 𝐼𝑅1 + 𝐼𝑅2 + 𝐼𝑅3

 

Numerical Example

(1) Use Kirchhoff’s laws to calculate for; 

(a) The current through each battery 

(b)  The power dissipated in the 20Ω resistor 

(c)   The terminal voltage.  


Kirchhoff’s laws


6 = 1.2𝐼1 + 20(𝐼1 + 𝐼2)

6 = 1.2𝐼1 + 20𝐼1 + 20𝐼2

6 = 21.2𝐼1 + 20𝐼2           → (1)


Moving clockwise  


Kirchhoff’s laws

Consider loop ABDEA

6 − 4 = 1.2𝐼1 − 0.5𝐼2

2 = 1.2𝐼1 − 0.5𝐼2           → (1)

Matching both equation

6 = 21.2𝐼1 + 20𝐼2               → (1)

2 = 1.2𝐼1 − 0.5𝐼2           → (2)


Equation  (1) × 0.5 and Equation  (2) × 20  

3 = 10.6𝐼1 + 10𝐼2             → (3)

40 = 24𝐼1 + 10𝐼2             → (4)


Add equation  (3) and (4)


43   =   34.6𝐼1

34.6      34.6

𝐼1 = 1.243𝐴

𝑃𝑢𝑡 𝐼1 = 1.243 𝑖𝑛𝑡𝑜 Equation  (1)

6 = 21.2𝐼1 + 20𝐼2       Equation  (1)

6 = 21.2(1.243) + 20𝐼2

6 = 26.378 + 20𝐼2

6 − 26.378 + 20𝐼2

−20.378 = 20𝐼2

     20

𝐼2 =-1.018A (It means the cell should be reversed) 


(a) 𝐼1 + 𝐼2 = (1.243) + (−1.018) = 10.225A


(b) Power dissipated in the 20Ω resistor 

𝑃 = 𝐼2𝑅

𝑃 = (𝐼1 + 𝐼2)2 × 𝑅2

0.2252 × 20

  = 1.013W


(c)The terminal voltage 

𝑉𝑡 = 𝐸1 − 𝐼1𝑅1

= 6 − (1.243 × 1.2)

= 6 − (1.4916)

= 4.51𝑉


Alternatively 

Terminal voltage = (𝐼1 + 𝐼2) × 𝑅(1 + 2)

= 0.225 × 20

= 4.5𝑉


(2) Use Kirchhoff’s laws to calculate for; 

(a) The current flowing through each branch of the network 

(b) The power dissipated in the 5Ω resistor 

(c)The terminal voltage  


Kirchhoff’s laws


Consider loop ABEFA moving clockwise  


Kirchhoff’s laws


6 − 2 = 2𝐼1 − 3𝐼2

4 = 2𝐼1 − 3𝐼………………………… (1)


Consider loop BCDEB moving clockwise  


Kirchhoff’s laws

2 = 3𝐼2 + 5(𝐼1 + 𝐼2)

2 = 3𝐼2 + 5𝐼1 + 5𝐼2

2 = 8𝐼2 + 5𝐼1

2 = +5𝐼1 + 8𝐼2 ………………………… (2)


Matching equation (1) and (2) 


4 = 2𝐼1 + 3𝐼2  ………………………… (1)

2 = 5𝐼1 + 8𝐼2   ………………………… (2)

equation (1) × 8  

equation  (2) × 3  

32 = 216 + 24𝐼2 ………………………… (3)

6 = 215 + 24𝐼2   ………………………… (4)

equation (3) + (4)

38  = 31𝐼1 

31     31

𝐼1 = 1.226 𝐴


𝑃𝑢𝑡𝑡𝑖𝑛𝑔 𝐼 = 1.226 𝑖𝑛𝑡𝑜 equation  ( 2 )


2 = 5 𝐼1 + 8𝐼2

2 = 5(1.226) + 8𝐼2

2 = 6.13 + 8𝐼2

2 − 6.13 = 8𝐼2

4.13 = 8𝐼2

    8           8

𝐼2 = −0.5163𝐴

𝐼1 + 𝐼2 = (1.226) + (−0.513)

= 0.7098A

 

(b) Power dissipated in 5resistor

𝑃 = 𝐼2𝑅

𝑃 = (𝐼1 + 𝐼2 )2 × 5

𝑃 = 0.5038 × 5

𝑃 = 2.19𝑊

 

(c)The terminal voltage

(𝐼1 + 𝐼2 × 𝑅(1 + 2))

= 0.7098 × 5

= 3.549𝑉


Alternatively

𝐸2𝐼2𝑅2

= 2 (0.5163)  × 3

= 2 + 1.5489

= 3.5489V

 

Trial Test

1.      A p.d. of 5V is maintained across a resistance of 0.8Ω. Calculate the current flowing through the resistor.

 

2.      An electric heater has a rating of 2KW at 250V supply. Calculate the 

(a)   current drawn by the heater

(b)  resistance of the heating element

 

3.      Calculate the resistance of 100 metres of aluminium cable of 1.5mm2 cross-sectional area if the resistivity of aluminium is taken as 28.5  10-9 Ωm.

 

4.      A coil of copper wire has a resistance 200Ω when its mean temperature is 0 oС. Calculate the resistance of the coil when its mean temperature is 80 oС.

 

5.      The field winding of a generator has a resistance of 10Ω at an ambient temperature of 20 oС. After running for some time the mean temperature of the generator rises to 33.4

oС. Calculate the resistance of the winding at the higher temperature if the temperature coefficient of resistance is 0.004 Ω/ Ω oС.

 

6.      State Kirchhoff’s laws 


7.      Use Kirchhoff’s laws to calculate for 

(a) The current flowing through each branch of the network 

(b) The power dissipated in resistor. 

(c)The terminal voltage  


Kirchhoff’s laws





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