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ELECTRICAL CIRCUITS 1 LECTURE
LESSON 2
Ohmโ€™s Law and Resistive Circuit
๏ƒ˜ State and apply Ohmโ€™s Law.
๏ƒ˜ Define power and energy including their units.
๏ƒ˜ Calculate energy and power.
๏ƒ˜ Recognizes series, parallel, series-parallel, wye and delta
connections.
๏ƒ˜ Solve circuits (i.e. find currents and voltages of interest) by combining
resistances in series and parallel.
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Learning Objectives
At the end of the lesson, the learner is expected to:
โ€ข This law applies to electric to electric conduction
through good conductors and may be stated as
follows :
โ€ข โ€œThe ratio of potential difference (V) between any two
points on a conductor to the current (I) flowing
between them, is constant, provided the temperature
of the conductor does not change.โ€
After George Simon
Ohm (1787-1854), a
German
mathematician who
in about 1827
formulated the law
known after his
name as Ohmโ€™s
Law.
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Ohmโ€™s Law
where R is the resistance of the conductor between the two points
considered.
โ€ข Put in another way, it simply means that provided R is kept constant,
current is directly proportional to the potential difference across the
ends of a conductor. However, this linear relationship between V and I
does not apply to all non-metallic conductors. For example, for silicon
carbide, the relationship is given by V = KI^m where K and m are
constants and m is less than unity. It also does not apply to non-linear
devices such as Zener diodes and voltage-regulator (VR) tubes.
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Ohmโ€™s Law
1. A coil of copper wire has resistance of 90 ฮฉ at 20ยฐC and is connected
to a 230-V supply. By how much must the voltage be increased in order
to maintain the current constant if the temperature of the coil rises to
60ยฐC ? Take the temperature coefficient of resistance of copper as
0.00428 from 0ยฐC.
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Illustrative Problems: ( Instructor actual discussion)
-
2. Three resistors are connected in series across a 12-V battery. The first resistor has a
value of 1 ฮฉ, second has a voltage drop of 4 V and the third has a power dissipation of 12
W. Calculate the value of the circuit current.
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Illustrative Problems: ( Instructor actual discussion)
โ€ข Power (P) - it is the rate of doing work. Its units is watt
(W) which represents 1 joule per second.
1 W = 1 J/s
โ€ข If a force of F newton moves a body with a velocity of ฮฝ
m./s then
Power = F ร— ฮฝ , watt
โ€ข If the velocity ฮฝ is in km/s, then
Power = F ร— ฮฝ, kilowatt
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Power and Energy
Also, in Calculus Based Physics:
, Watts
At any instant:
, Joules
and
, watt-sec or Joules
Note : W is the energy: t is in seconds and P is in watts.
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Power and Energy
โ€ข Energy (W) - ability of doing electrical work. It is the product of power
obtained and time.
In Electric Circuit,
, watt-sec
Note: P is power, E or V is voltage, I is current, R is resistance and t is time
in sec.
FUNDAMENTALS OF ELECTRICAL CIRCUITS
Ohmโ€™s Law and Resistive Circuit
Power and Energy
Important SI Units:
(i) Kilowatt-hour (kWh) and kilocalorie (kcal)
(ii) Miscellaneous Units
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Power and Energy
1. A de-icing equipment fitted to a radio aerial consists of a length of a
resistance wire so arranged that when a current is passed through it,
parts of the aerial become warm. The resistance wire dissipates 1250
W when 50 V is maintained across its ends. It is connected to a d.c.
supply by 100 metres of this copper wire, each conductor of which has
resistance of 0.006 ฮฉ/m.
Calculate:
(a) the current in the resistance wire
(b) the power lost in the copper connecting wire
(c) the supply voltage required to maintain 50 V across the heater itself.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
2. A factory has a 240-V supply from which the following loads are taken :
Lighting : Three hundred 150-W, four hundred 100 W and five hundred
60-W lamps
Heating : 100 kW
Motors : A total of 44.76 kW (60 b.h.p.) with an average efficiency of 75
percent
Misc. : Various load taking a current of 40 A.
Assuming that the lighting load is on for a period of 4 hours/day, the
heating for 10 hours per day and the remainder for 2 hours/day, calculate
the weekly consumption of the factory in kWh when working on a 5-day
week. What current is taken when the lighting load only is switched on ?
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข When some conductors having resistances R1, R2 and R3 etc. are
joined end-on-end as in figure below, they are said to be connected in
series.
โ€ข Being a series circuit, it should be remembered that:
(i) current is the same through all the three conductors.
Resistances in Series
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
(ii) but voltage drop across each is different due to its different
resistance and is given by Ohmโ€™s Law.
(iii) sum of the three voltage drops is equal to the voltage applied across
the three conductors.
where R is the equivalent resistance of the series combination. Also,
Resistances in Series
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข The main characteristics of a series circuit are :
1. same current flows through all parts of the circuit.
2. different resistors have their individual voltage drops.
3. voltage drops are additive.
4. applied voltage equals the sum of different voltage drops.
5. resistances are additive.
6. powers are additive.
Resistances in Series
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Voltage Divider Rule
โ€ข Since in a series circuit, same current flows through each of the given
resistors, voltage drop varies directly with its resistance.
Total resistance R = R1 + R2 + R3 = 12 ฮฉ
According to Voltage Divider Rule, various
voltage drops are :
Figure of series network
Resistances in Series
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
1. A series circuit consists of three resistors A, B, and C connected to a
120 V source. If the voltage drop across resistor A is 30 volts when
the circuit current is 2A, and Rb = 1.5Rc, Calculate the values of Ra,
Rb, and Rc.
2. The resistors in the voltage-divider circuit shown have a tolerance of ๏‚ฑ
10%. Find the maximum and minimum value of Vo.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
3. A source supplies 120V to the series combination of a 10 ohm
resistance, an 8 ohm resistance and an unknown resistance Rx. The
voltage across the 8 ohm resistance is 20V. Determine the value of the
unknown resistance.
4. Find the voltage Vo for the circuit shown below: Calculate the power at
380V source. Is the power delivering or absorbed?
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION for NUMBER 4 : By voltage division :
๐‘‰25 ๐‘˜ = 380 ๐‘‰ (
25 ๐‘˜๐‘œโ„Ž๐‘š
25๐‘˜๐‘œโ„Ž๐‘š+75 ๐‘˜๐‘œโ„Ž๐‘š
)= 95 V
๐‘– =
95๐‘‰
25 ๐‘˜๐‘œโ„Ž๐‘š
= 0.0038 A
By voltage division to get Vo:
๐ท๐‘’๐‘๐‘’๐‘›๐‘‘๐‘’๐‘›๐‘ก ๐‘‰๐‘œ๐‘™๐‘ก๐‘Ž๐‘”๐‘’ ๐‘†๐‘œ๐‘ข๐‘Ÿ๐‘๐‘’ = 25,000 ๐‘ฅ ๐‘– = 25,000 ๐‘ฅ 0.0038 ๐ด = 95๐‘‰
๐‘‰๐‘‚ = 95 ๐‘‰ (
60๐พ๐‘œโ„Ž๐‘š
60 ๐‘˜๐‘œโ„Ž๐‘š+40 ๐‘˜๐‘œโ„Ž๐‘š
) = 57 volts
โ€ข Three resistances, as joined in figure below are said to be connected in
parallel.
(i) potential drop across all resistances is the same
(ii) current in each resistor is different and is given by Ohmโ€™s Law.
(iii) the total current is the sum of the three separate currents.
Figure of parallel network
Resistances in Parallel
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข Now,
โ€ข The main characteristics of a parallel circuit are :
1. same voltage acts across all parts of the circuit
2. different resistors have their individual current.
3. branch currents are additive.
4. conductance's are additive.
5. powers are additive.
Resistances in Parallel
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Division of Current in Parallel Circuit
โ€ข In the figure below, two resistances are joined in parallel across a
voltage V. The current in each branch, as given in Ohmโ€™s law, is :
Figure of parallel network
Resistances in Parallel
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข Hence, the division of current in the branches of a parallel circuit is
directly proportional to the conductance of the branches or inversely
proportional to their resistances. We may also express the branch
currents in terms of the total circuit current thus :
โ€ข The same approach for 3 or more resistances connected in parallel.
Resistances in Parallel
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
1. Three loads A, B, and C are connected in parallel to a 230 volt source.
Load A takes 9.2 kw. load B takes a current of 60 amp. and load C is a
resistance of 4.6 ohms. Calculate:
(a) the resistances of load A and B,
(b) the total equivalent resistance of the three paralleled loads.
(c) the total current
(d) the total power.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
2. A coil wire having a resistance of 3.84 ohms and carrying a current of
0.15 amp. is in parallel with an unknown resistance through which
there is a current of 1.44 amp. Calculate (a) the unknown resistance
(b) the total equivalent resistance.
3. Given the circuit below. Calculate the following:
(a) total equivalent resistance.
(b) total current.
(c) voltage drop across each section.
(d) current through each resistor.
(e) total power taken by the entire circuit.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
Figure for problem 3:
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
4. Use current division to find the current io and use voltage division to
find the voltage vo, for the circuit shown below.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SIMPLIFY THESE RESISTANCES FIRST
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION :
6.485
1
๐‘…๐‘‡
=
1
10
+
1
80
+
1
24
๐‘…๐‘‡ =
1
0.1542
๐‘…๐‘‡ = 6.485 ๐‘œโ„Ž๐‘š๐‘ 
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION :
6.485
I1
๐ผ1 = 8
80
80 + 6.485
= 7.40 ๐ด
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION :
I1= 7.40 A
1
๐‘…๐‘‡
=
1
80
+
1
24
๐‘…๐‘‡ =
1
0.054167
๐‘…๐‘‡ = 18.461
18.861
ohms
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION :
I1= 7.40 A
Type equation
here.
๐ผ2 =7.40(
10
10+18.861
)
18.861
ohms
I2= 2.564 A
๐ผ2 = 2.564 ๐ด
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION :
I1= 7.40 A I2= 2.564 A
IO =1.972 A ๐‘–๐‘œ=2.564(
80
80+24
) = ๐Ÿ. ๐Ÿ—๐Ÿ•๐Ÿ ๐‘จ
๐‘ฃ๐‘œ = 2.564 โˆ’ 1.972 โˆ— 30 ๐‘œโ„Ž๐‘š๐‘ 
๐‘ฃ๐‘œ = 17.76 ๐‘‰๐‘œ๐‘™๐‘ก๐‘ 
โ€ข Circuits combining series and parallel sections with one source of
supply are treated in as much the same way as simple circuits
arrangements.
Figure of series - parallel network
Series-Parallel
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
1. What is the value of the unknown resistor R in figure below if the voltage
drop across the 500 ฮฉ resistor is 2.5 volts ? All resistances are in ohm.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
2. Calculate the effective resistance of the following combination of
resistances and the voltage drop across each resistance when a P.D. of
60 V is applied between points A and B.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
3. The equivalent resistance between terminals a and b in the figure
below is Rab = 23 ohms. Determine the value of R2.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION for NUMBER 3 :
23 =(
12โˆ—6
12+6
+ ๐‘…2) * 80
12 โˆ— 6
12 + 6
+ ๐‘…2 + 80
+ 7
R2 = 16 ohms
4. Refer to the circuit shown below. With the switch open, we have v2 =
8V. On the other hand, with the switch closed, we have v2 = 6V.
Determine the values of R2 and RL.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข Resistors are sometimes interconnected to form rather complex
networks. Due to this, some common rules applicable to simple series
and parallel circuits cannot be used for the calculation of equivalent
resistances, branch currents, and voltage drops.
โˆ† - Y and Y - โˆ† Transformation
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข Considering the connections of resistors below:
โ€ข โˆ† - Y Transformation:
โˆ† - Y and Y - โˆ† Transformation
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข For โˆ† - Y Transformation : Each of the resistances in the star is equal
to the product of the resistances of the adjacent arms of the delta
divided by the sum of the three delta resistances.
Y-โˆ† Transformation:
For Y-โˆ† Transformation : Each of the resistances in delta is equal to the
sum of the products of the resistances in the star, taken two at a time,
divided by the resistance in the opposite leg.
โˆ† - Y and Y - โˆ† Transformation
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข Drawn as a 4 terminal arrangement of components
T and ( Tee and Pi )
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
โ€ข 2 of the terminals are connects at one node. The node is a
distributed node in the case of the P network.
T and ( Tee and Pi )
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
1. Referring to the figure in our lecture, the three resistances in a delta-
connected group of resistors are X= 35 ohms, Y = 25 ohms, Z = 40
ohms. Calculate the resistances A, B, and C of the equivalent star.
SOLUTION:
๐ด =
๐‘Œ๐‘
100
=
25 ๐‘ฅ 40
100
= 10 ๐‘œโ„Ž๐‘š๐‘ 
๐ต =
๐‘‹๐‘
100
=
35 ๐‘‹ 40
100
= 14 ๐‘œโ„Ž๐‘š๐‘ 
๐ถ =
๐‘‹๐‘Œ
100
=
35 ๐‘‹ 25
100
= 8.75 ohms
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
2. The wiring diagram shown below is known as the Wheatstone Bridge
circuit; when the potential difference between points a and b is zero
the bridge is said to be balanced. For the resistance values given, the
bridge is unbalanced. (a) Calculate the total resistance (b) total current
(c) the current at 110 ๏— resistance.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
๐ด =
60 ๐‘‹ 80
250
= 19.2 ๐‘œโ„Ž๐‘š๐‘ 
SOLUTION:
๐ต =
60 ๐‘ฅ 110
250
= 26.4 ๐‘œโ„Ž๐‘š๐‘ 
๐ถ =
80 ๐‘‹ 110
250
= 35.2 ๐‘œโ„Ž๐‘š๐‘ 
Get the equivalent resistance:
๐‘…๐‘’๐‘ž = 19.2 +
35.2+84.8 ๐‘ฅ (26.4+33.6)
(120+60)
= 59.2 ohms
(a)
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION:
(b) ๐‘‡โ„Ž๐‘’ ๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ ๐ถ๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘ก ๐‘–๐‘  ๐ผ =
177.6
59.2
= 3 ๐‘Ž๐‘š๐‘
(c) ๐‘‡๐‘œ ๐‘๐‘œ๐‘š๐‘๐‘ข๐‘ก๐‘’ ๐‘กโ„Ž๐‘’ ๐‘๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘ก ๐‘กโ„Ž๐‘Ÿ๐‘œ๐‘ข๐‘”โ„Ž ๐‘กโ„Ž๐‘’ 110 โˆ’ ๐‘œโ„Ž๐‘š ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘œ๐‘Ÿ ๐‘–๐‘ก ๐‘ค๐‘–๐‘™๐‘™ ๐‘๐‘’ ๐‘“๐‘–๐‘Ÿ๐‘ ๐‘ก ๐‘๐‘’ ๐‘›๐‘’๐‘๐‘’๐‘ ๐‘ ๐‘Ž๐‘Ÿ๐‘ฆ ๐‘ก๐‘œ ๐‘“๐‘–๐‘›๐‘‘ ๐‘กโ„Ž๐‘’
potential difference between points a and b. To do this, the currents through the branches of the parallel
Circuit of the figure in (a) must be found. These are:
๐ผ120 ๐‘™๐‘’๐‘“๐‘ก ๐‘๐‘Ÿ๐‘Ž๐‘›๐‘โ„Ž =
60
120+60
๐‘ฅ 3 = 1 amp
๐ผ110 ๐‘Ÿ๐‘–๐‘”โ„Ž๐‘ก ๐‘๐‘Ÿ๐‘Ž๐‘›๐‘โ„Ž =
120
120 + 60
๐‘ฅ 3 = 2 ๐‘Ž๐‘š๐‘
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
SOLUTION:
The voltage drop across M is 84.8 x 1 = 84.8 volts, and the voltage drop across N is 33.6 x 2 = 67.2 volts. Therefore,
The potential difference between a and b will be
๐ธ๐‘Žโˆ’๐‘ = 84.8 โˆ’ 67.2 = 17.6 ๐‘ฃ๐‘œ๐‘™๐‘ก๐‘ 
๐ผ110 =
17.6
110
= 0.16 ๐‘Ž๐‘š๐‘
Hence, the current through the 110-ohm resistor is
3. If Ra = 6 ๏—, Rb = 9๏— and Rc = 3 ๏—. Convert ๏ฐ to tee network.
ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion)
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit
๏ƒ˜Nilsson, James W. 2019. Electric Circuits 11th ed. Amazon [C 621.319 N59
2019(CAL)]
๏ƒ˜Nahvi, Mahmood 2018. Schaum's Outline of Electric Circuits 7th ed. Amazon [C
621.3192 N14 2018(CAL)]
๏ƒ˜Kang, James S. 2018. Electric Circuits (MindTap Course List) 1st ed. Amazon [C
621.3192 K13 2018(CAL)]
๏ƒ˜Bird, John 2014. Electrical Circuit Theory and Technology 6th ed. Amazon [C
621.3192 B53 2014(CAL)]
๏ƒ˜Alexander, Charles 2017. Fundamentals of Electric Circuits 6th ed. Amazon [C
621.3815 A12 2017(CAL)]
References
ELECTRICAL CIRCUITS 1 LECTURE
Ohmโ€™s Law and Resistive Circuit

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Lesson 2 - Ohm's Law and Resisitive Circuits 2.pptx

  • 1. ELECTRICAL CIRCUITS 1 LECTURE LESSON 2 Ohmโ€™s Law and Resistive Circuit
  • 2. ๏ƒ˜ State and apply Ohmโ€™s Law. ๏ƒ˜ Define power and energy including their units. ๏ƒ˜ Calculate energy and power. ๏ƒ˜ Recognizes series, parallel, series-parallel, wye and delta connections. ๏ƒ˜ Solve circuits (i.e. find currents and voltages of interest) by combining resistances in series and parallel. ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Learning Objectives At the end of the lesson, the learner is expected to:
  • 3. โ€ข This law applies to electric to electric conduction through good conductors and may be stated as follows : โ€ข โ€œThe ratio of potential difference (V) between any two points on a conductor to the current (I) flowing between them, is constant, provided the temperature of the conductor does not change.โ€ After George Simon Ohm (1787-1854), a German mathematician who in about 1827 formulated the law known after his name as Ohmโ€™s Law. ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Ohmโ€™s Law
  • 4. where R is the resistance of the conductor between the two points considered. โ€ข Put in another way, it simply means that provided R is kept constant, current is directly proportional to the potential difference across the ends of a conductor. However, this linear relationship between V and I does not apply to all non-metallic conductors. For example, for silicon carbide, the relationship is given by V = KI^m where K and m are constants and m is less than unity. It also does not apply to non-linear devices such as Zener diodes and voltage-regulator (VR) tubes. ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Ohmโ€™s Law
  • 5. 1. A coil of copper wire has resistance of 90 ฮฉ at 20ยฐC and is connected to a 230-V supply. By how much must the voltage be increased in order to maintain the current constant if the temperature of the coil rises to 60ยฐC ? Take the temperature coefficient of resistance of copper as 0.00428 from 0ยฐC. ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Illustrative Problems: ( Instructor actual discussion) -
  • 6. 2. Three resistors are connected in series across a 12-V battery. The first resistor has a value of 1 ฮฉ, second has a voltage drop of 4 V and the third has a power dissipation of 12 W. Calculate the value of the circuit current. ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Illustrative Problems: ( Instructor actual discussion)
  • 7. โ€ข Power (P) - it is the rate of doing work. Its units is watt (W) which represents 1 joule per second. 1 W = 1 J/s โ€ข If a force of F newton moves a body with a velocity of ฮฝ m./s then Power = F ร— ฮฝ , watt โ€ข If the velocity ฮฝ is in km/s, then Power = F ร— ฮฝ, kilowatt ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Power and Energy
  • 8. Also, in Calculus Based Physics: , Watts At any instant: , Joules and , watt-sec or Joules Note : W is the energy: t is in seconds and P is in watts. ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Power and Energy
  • 9. โ€ข Energy (W) - ability of doing electrical work. It is the product of power obtained and time. In Electric Circuit, , watt-sec Note: P is power, E or V is voltage, I is current, R is resistance and t is time in sec. FUNDAMENTALS OF ELECTRICAL CIRCUITS Ohmโ€™s Law and Resistive Circuit Power and Energy
  • 10. Important SI Units: (i) Kilowatt-hour (kWh) and kilocalorie (kcal) (ii) Miscellaneous Units ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit Power and Energy
  • 11. 1. A de-icing equipment fitted to a radio aerial consists of a length of a resistance wire so arranged that when a current is passed through it, parts of the aerial become warm. The resistance wire dissipates 1250 W when 50 V is maintained across its ends. It is connected to a d.c. supply by 100 metres of this copper wire, each conductor of which has resistance of 0.006 ฮฉ/m. Calculate: (a) the current in the resistance wire (b) the power lost in the copper connecting wire (c) the supply voltage required to maintain 50 V across the heater itself. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 12. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 13. 2. A factory has a 240-V supply from which the following loads are taken : Lighting : Three hundred 150-W, four hundred 100 W and five hundred 60-W lamps Heating : 100 kW Motors : A total of 44.76 kW (60 b.h.p.) with an average efficiency of 75 percent Misc. : Various load taking a current of 40 A. Assuming that the lighting load is on for a period of 4 hours/day, the heating for 10 hours per day and the remainder for 2 hours/day, calculate the weekly consumption of the factory in kWh when working on a 5-day week. What current is taken when the lighting load only is switched on ? ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 14. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 15. โ€ข When some conductors having resistances R1, R2 and R3 etc. are joined end-on-end as in figure below, they are said to be connected in series. โ€ข Being a series circuit, it should be remembered that: (i) current is the same through all the three conductors. Resistances in Series ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 16. (ii) but voltage drop across each is different due to its different resistance and is given by Ohmโ€™s Law. (iii) sum of the three voltage drops is equal to the voltage applied across the three conductors. where R is the equivalent resistance of the series combination. Also, Resistances in Series ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 17. โ€ข The main characteristics of a series circuit are : 1. same current flows through all parts of the circuit. 2. different resistors have their individual voltage drops. 3. voltage drops are additive. 4. applied voltage equals the sum of different voltage drops. 5. resistances are additive. 6. powers are additive. Resistances in Series ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 18. Voltage Divider Rule โ€ข Since in a series circuit, same current flows through each of the given resistors, voltage drop varies directly with its resistance. Total resistance R = R1 + R2 + R3 = 12 ฮฉ According to Voltage Divider Rule, various voltage drops are : Figure of series network Resistances in Series ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 19. 1. A series circuit consists of three resistors A, B, and C connected to a 120 V source. If the voltage drop across resistor A is 30 volts when the circuit current is 2A, and Rb = 1.5Rc, Calculate the values of Ra, Rb, and Rc. 2. The resistors in the voltage-divider circuit shown have a tolerance of ๏‚ฑ 10%. Find the maximum and minimum value of Vo. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 20. 3. A source supplies 120V to the series combination of a 10 ohm resistance, an 8 ohm resistance and an unknown resistance Rx. The voltage across the 8 ohm resistance is 20V. Determine the value of the unknown resistance. 4. Find the voltage Vo for the circuit shown below: Calculate the power at 380V source. Is the power delivering or absorbed? ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 21. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION for NUMBER 4 : By voltage division : ๐‘‰25 ๐‘˜ = 380 ๐‘‰ ( 25 ๐‘˜๐‘œโ„Ž๐‘š 25๐‘˜๐‘œโ„Ž๐‘š+75 ๐‘˜๐‘œโ„Ž๐‘š )= 95 V ๐‘– = 95๐‘‰ 25 ๐‘˜๐‘œโ„Ž๐‘š = 0.0038 A By voltage division to get Vo: ๐ท๐‘’๐‘๐‘’๐‘›๐‘‘๐‘’๐‘›๐‘ก ๐‘‰๐‘œ๐‘™๐‘ก๐‘Ž๐‘”๐‘’ ๐‘†๐‘œ๐‘ข๐‘Ÿ๐‘๐‘’ = 25,000 ๐‘ฅ ๐‘– = 25,000 ๐‘ฅ 0.0038 ๐ด = 95๐‘‰ ๐‘‰๐‘‚ = 95 ๐‘‰ ( 60๐พ๐‘œโ„Ž๐‘š 60 ๐‘˜๐‘œโ„Ž๐‘š+40 ๐‘˜๐‘œโ„Ž๐‘š ) = 57 volts
  • 22. โ€ข Three resistances, as joined in figure below are said to be connected in parallel. (i) potential drop across all resistances is the same (ii) current in each resistor is different and is given by Ohmโ€™s Law. (iii) the total current is the sum of the three separate currents. Figure of parallel network Resistances in Parallel ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 23. โ€ข Now, โ€ข The main characteristics of a parallel circuit are : 1. same voltage acts across all parts of the circuit 2. different resistors have their individual current. 3. branch currents are additive. 4. conductance's are additive. 5. powers are additive. Resistances in Parallel ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 24. Division of Current in Parallel Circuit โ€ข In the figure below, two resistances are joined in parallel across a voltage V. The current in each branch, as given in Ohmโ€™s law, is : Figure of parallel network Resistances in Parallel ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 25. โ€ข Hence, the division of current in the branches of a parallel circuit is directly proportional to the conductance of the branches or inversely proportional to their resistances. We may also express the branch currents in terms of the total circuit current thus : โ€ข The same approach for 3 or more resistances connected in parallel. Resistances in Parallel ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 26. 1. Three loads A, B, and C are connected in parallel to a 230 volt source. Load A takes 9.2 kw. load B takes a current of 60 amp. and load C is a resistance of 4.6 ohms. Calculate: (a) the resistances of load A and B, (b) the total equivalent resistance of the three paralleled loads. (c) the total current (d) the total power. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 27. 2. A coil wire having a resistance of 3.84 ohms and carrying a current of 0.15 amp. is in parallel with an unknown resistance through which there is a current of 1.44 amp. Calculate (a) the unknown resistance (b) the total equivalent resistance. 3. Given the circuit below. Calculate the following: (a) total equivalent resistance. (b) total current. (c) voltage drop across each section. (d) current through each resistor. (e) total power taken by the entire circuit. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 28. Figure for problem 3: ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 29. 4. Use current division to find the current io and use voltage division to find the voltage vo, for the circuit shown below. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SIMPLIFY THESE RESISTANCES FIRST
  • 30. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION : 6.485 1 ๐‘…๐‘‡ = 1 10 + 1 80 + 1 24 ๐‘…๐‘‡ = 1 0.1542 ๐‘…๐‘‡ = 6.485 ๐‘œโ„Ž๐‘š๐‘ 
  • 31. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION : 6.485 I1 ๐ผ1 = 8 80 80 + 6.485 = 7.40 ๐ด
  • 32. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION : I1= 7.40 A 1 ๐‘…๐‘‡ = 1 80 + 1 24 ๐‘…๐‘‡ = 1 0.054167 ๐‘…๐‘‡ = 18.461 18.861 ohms
  • 33. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION : I1= 7.40 A Type equation here. ๐ผ2 =7.40( 10 10+18.861 ) 18.861 ohms I2= 2.564 A ๐ผ2 = 2.564 ๐ด
  • 34. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION : I1= 7.40 A I2= 2.564 A IO =1.972 A ๐‘–๐‘œ=2.564( 80 80+24 ) = ๐Ÿ. ๐Ÿ—๐Ÿ•๐Ÿ ๐‘จ ๐‘ฃ๐‘œ = 2.564 โˆ’ 1.972 โˆ— 30 ๐‘œโ„Ž๐‘š๐‘  ๐‘ฃ๐‘œ = 17.76 ๐‘‰๐‘œ๐‘™๐‘ก๐‘ 
  • 35. โ€ข Circuits combining series and parallel sections with one source of supply are treated in as much the same way as simple circuits arrangements. Figure of series - parallel network Series-Parallel ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 36. 1. What is the value of the unknown resistor R in figure below if the voltage drop across the 500 ฮฉ resistor is 2.5 volts ? All resistances are in ohm. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 37. 2. Calculate the effective resistance of the following combination of resistances and the voltage drop across each resistance when a P.D. of 60 V is applied between points A and B. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 38. 3. The equivalent resistance between terminals a and b in the figure below is Rab = 23 ohms. Determine the value of R2. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 39. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION for NUMBER 3 : 23 =( 12โˆ—6 12+6 + ๐‘…2) * 80 12 โˆ— 6 12 + 6 + ๐‘…2 + 80 + 7 R2 = 16 ohms
  • 40. 4. Refer to the circuit shown below. With the switch open, we have v2 = 8V. On the other hand, with the switch closed, we have v2 = 6V. Determine the values of R2 and RL. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 41. โ€ข Resistors are sometimes interconnected to form rather complex networks. Due to this, some common rules applicable to simple series and parallel circuits cannot be used for the calculation of equivalent resistances, branch currents, and voltage drops. โˆ† - Y and Y - โˆ† Transformation ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 42. โ€ข Considering the connections of resistors below: โ€ข โˆ† - Y Transformation: โˆ† - Y and Y - โˆ† Transformation ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 43. โ€ข For โˆ† - Y Transformation : Each of the resistances in the star is equal to the product of the resistances of the adjacent arms of the delta divided by the sum of the three delta resistances. Y-โˆ† Transformation: For Y-โˆ† Transformation : Each of the resistances in delta is equal to the sum of the products of the resistances in the star, taken two at a time, divided by the resistance in the opposite leg. โˆ† - Y and Y - โˆ† Transformation ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 44. โ€ข Drawn as a 4 terminal arrangement of components T and ( Tee and Pi ) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 45. โ€ข 2 of the terminals are connects at one node. The node is a distributed node in the case of the P network. T and ( Tee and Pi ) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 46. 1. Referring to the figure in our lecture, the three resistances in a delta- connected group of resistors are X= 35 ohms, Y = 25 ohms, Z = 40 ohms. Calculate the resistances A, B, and C of the equivalent star. SOLUTION: ๐ด = ๐‘Œ๐‘ 100 = 25 ๐‘ฅ 40 100 = 10 ๐‘œโ„Ž๐‘š๐‘  ๐ต = ๐‘‹๐‘ 100 = 35 ๐‘‹ 40 100 = 14 ๐‘œโ„Ž๐‘š๐‘  ๐ถ = ๐‘‹๐‘Œ 100 = 35 ๐‘‹ 25 100 = 8.75 ohms ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 47. 2. The wiring diagram shown below is known as the Wheatstone Bridge circuit; when the potential difference between points a and b is zero the bridge is said to be balanced. For the resistance values given, the bridge is unbalanced. (a) Calculate the total resistance (b) total current (c) the current at 110 ๏— resistance. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 48. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit ๐ด = 60 ๐‘‹ 80 250 = 19.2 ๐‘œโ„Ž๐‘š๐‘  SOLUTION: ๐ต = 60 ๐‘ฅ 110 250 = 26.4 ๐‘œโ„Ž๐‘š๐‘  ๐ถ = 80 ๐‘‹ 110 250 = 35.2 ๐‘œโ„Ž๐‘š๐‘  Get the equivalent resistance: ๐‘…๐‘’๐‘ž = 19.2 + 35.2+84.8 ๐‘ฅ (26.4+33.6) (120+60) = 59.2 ohms (a)
  • 49. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION: (b) ๐‘‡โ„Ž๐‘’ ๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ ๐ถ๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘ก ๐‘–๐‘  ๐ผ = 177.6 59.2 = 3 ๐‘Ž๐‘š๐‘ (c) ๐‘‡๐‘œ ๐‘๐‘œ๐‘š๐‘๐‘ข๐‘ก๐‘’ ๐‘กโ„Ž๐‘’ ๐‘๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘ก ๐‘กโ„Ž๐‘Ÿ๐‘œ๐‘ข๐‘”โ„Ž ๐‘กโ„Ž๐‘’ 110 โˆ’ ๐‘œโ„Ž๐‘š ๐‘Ÿ๐‘’๐‘ ๐‘–๐‘ ๐‘ก๐‘œ๐‘Ÿ ๐‘–๐‘ก ๐‘ค๐‘–๐‘™๐‘™ ๐‘๐‘’ ๐‘“๐‘–๐‘Ÿ๐‘ ๐‘ก ๐‘๐‘’ ๐‘›๐‘’๐‘๐‘’๐‘ ๐‘ ๐‘Ž๐‘Ÿ๐‘ฆ ๐‘ก๐‘œ ๐‘“๐‘–๐‘›๐‘‘ ๐‘กโ„Ž๐‘’ potential difference between points a and b. To do this, the currents through the branches of the parallel Circuit of the figure in (a) must be found. These are: ๐ผ120 ๐‘™๐‘’๐‘“๐‘ก ๐‘๐‘Ÿ๐‘Ž๐‘›๐‘โ„Ž = 60 120+60 ๐‘ฅ 3 = 1 amp ๐ผ110 ๐‘Ÿ๐‘–๐‘”โ„Ž๐‘ก ๐‘๐‘Ÿ๐‘Ž๐‘›๐‘โ„Ž = 120 120 + 60 ๐‘ฅ 3 = 2 ๐‘Ž๐‘š๐‘
  • 50. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit SOLUTION: The voltage drop across M is 84.8 x 1 = 84.8 volts, and the voltage drop across N is 33.6 x 2 = 67.2 volts. Therefore, The potential difference between a and b will be ๐ธ๐‘Žโˆ’๐‘ = 84.8 โˆ’ 67.2 = 17.6 ๐‘ฃ๐‘œ๐‘™๐‘ก๐‘  ๐ผ110 = 17.6 110 = 0.16 ๐‘Ž๐‘š๐‘ Hence, the current through the 110-ohm resistor is
  • 51. 3. If Ra = 6 ๏—, Rb = 9๏— and Rc = 3 ๏—. Convert ๏ฐ to tee network. ILLUSTRATIVE PROBLEMS: ( Instructor actual discussion) ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit
  • 52. ๏ƒ˜Nilsson, James W. 2019. Electric Circuits 11th ed. Amazon [C 621.319 N59 2019(CAL)] ๏ƒ˜Nahvi, Mahmood 2018. Schaum's Outline of Electric Circuits 7th ed. Amazon [C 621.3192 N14 2018(CAL)] ๏ƒ˜Kang, James S. 2018. Electric Circuits (MindTap Course List) 1st ed. Amazon [C 621.3192 K13 2018(CAL)] ๏ƒ˜Bird, John 2014. Electrical Circuit Theory and Technology 6th ed. Amazon [C 621.3192 B53 2014(CAL)] ๏ƒ˜Alexander, Charles 2017. Fundamentals of Electric Circuits 6th ed. Amazon [C 621.3815 A12 2017(CAL)] References ELECTRICAL CIRCUITS 1 LECTURE Ohmโ€™s Law and Resistive Circuit