Parallel Circuit

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VFP2
Parallel Circuit
TTC
Dr. Frank Neumann
Rayan Ateeq 308
202333308
Table of content
1.Didactic Reflection ............................................................................... 2
1.1.Curriculum Analysis .......................................................................... 2
1.2.Content Analysis ............................................................................... 4
1.2.1The TVTC Curriculum RCT ............................................................. 4
1.2.2The Internet Web- Research ........................................................... 6
1.2.3Comparison between TVTC and web- research ............................ 9
1.2.4The content : ................................................................................... 9
1.3.Didactic Analysis ............................................................................. 13
2.Lesson Plan ....................................................................................... 14
3.References ........................................................................................ 16
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1. Didactic Reflection
1.1. Curriculum Analysis
The name of this module is electrical circuit 1, which is in trimester 2. The unit has
four contact hours a week three hours Theoretical and one hour for tutorial. The
subject of the lesson is Methods of connecting resistors. It gives the students basic
knowledge of electrostatic, batteries, and fundamentals of DC current. The unit code
is (ELT 106 ) . The contact hours for this Module is 52. the students are having
passed through this course. the students will study Electrical Circuits- 2
.
Electrical
Power
&
Specialization:
Machinery
& Equipment
Department:
Electrical Technology
Module Name:
Methods of connecting
resistors
Course code:
ELT 106
Prerequisites:
None
Trimester
2
Credit
Hours
3
The Module contains an explanation of electrostatics
laws, batteries, DC circuit analysis, electromagnetism
and magnetic circuits. The unit contents include:
capacitors, Ohm's law, Kirchhoff's laws, series &
parallel circuits, power, and DC bridges.
Contact
Hours
(h/w)
L
P
3
0
T
1
Source : Curriculum of Electrical
Technology in RCT
1.1.1. The trainee should study before the lesson :
Unit-1 Electrostatics:
A. Electric charge:
 Electric charge
 Coulomb's law
 Force between two charges
 Electric field
 Electric potential
 Potential difference
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B. Capacitors:
 Capacitance of an isolated ball
 Capacitance of an earthed ball capacitor
 Capacitance of a parallel plate capacitor
 Series and parallel connections of capacitors
 Energy stored in capacitors
Unit-2 DC circuits:
Electrical Quantities:
 Quantity of charge
 Current and current intensity
 DC voltage and current
 Resistance and resistors
 Ohm's law
Unit-3 Methods of connecting resistors:
 Series connection of resistors.
Unit- 4 Kirchhoff's laws:
 Kirchhoff's voltage laws.
1.1.2. The trainees studying.
Unit-3 Methods of connecting resistors:
 Parallel connection of resistors.
Unit- 4 Kirchhoff's laws:
 Kirchhoff's current laws.
1.1.3. The trainees studying after the lesson :
Unit-3 Methods of connecting resistors:
 Calculation of resistances connected in series-parallel connections.
Unit-5 Simple circuit calculations:
 Series connection.
 Voltage divider rule.
 Parallel connection.
 Current divider rule.
 Series parallel connection.
 Star or delta connection.
 Star or delta transformations.
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1.2. Content Analysis
1.2.1 The TVTC Curriculum RCT:
If two or more components are connected in parallel they have the same potential
difference (voltage) across their ends. The potential differences across the
components are the same in magnitude, and they also have identical polarities. The
same voltage is applicable to all circuit components connected in parallel. The total
current is the sum of the currents through the individual components, in accordance
with Kirchhoff’s current law.
Fig 1 of parallel circuit
Source: Principles of Electric circuits, Thomas L. Floyd, 1999,
page 189
To calculate total resistance.
RT =
To
find
the
resistances
1
1
1
1
1
R1 + R 2 + R 3 + … … … … … … . R N
total resistance of
all
components,
add
the reciprocals of
the
of each component and take the reciprocal of the sum. Total
resistance will always be less than the value of the smallest resistance:
To calculate total current.
IT = I1 + I2 + I3 … … … … … … IN
Each voltage are equal.
E=V1 = V2 = V3 = VN
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To calculate the power
V2
2
PN = V × IN or PN = IN
× R N or PN = R
N
The power is hasn't change we for each circuit in parallel and series circuit.
To calculate total power
PT = P1 + P2 + P3 … … … … … … PN
Example 1 : Find out the following if R1 = 9 Ω , R 2 = 18 Ω and E = 27v
1. R T
2. IT
Fig 2 of Parallel circuit
3. I1 , I2
4. P1 , P2
5. Pin
1. R T =
1
1
1
+
R1 R2
or we use in this
situation this furmala 𝑅𝑇=
Source :Handout of Eng, Kahaled , in RCT
R1 ×R2
R1 +R2
To calculate the total Resistors R T , we use this formula only in parallel circuit
RT =
1
1 1
9 + 18
V
IT =
RT
= 6Ω
You have taken already ohm's law to find out the current we use it.
2. IT =
27V
6A
= 4.5 A
V
3. A. I1 = R
I1 =
1
27v
= 3A
9
V
B. I2 = R
I2 =
2
27 v
= 1.5A
18
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4. A. P1 = V × I1
The power is hasn't change we for each circuit in parallel and series circuit.
P1 = 27v × 3A = 81 w
B. P2 = V × I2
P2 = 27 v × 1.5 A = 40.5 w
5. A . Pin = P1 + P2
Pin = 81w + 40.5 w = 121.5w
other method to solve Pin
B. Pin = E × IT
1.2.2 The Internet Web- Research:
1.2.2.1 Properties of a Parallel Circuit
Fig.3 of Parallel circuit
of
The same voltage is effective across each
individual resistor in a parallel circuit as in
Fig. 3. All upper ends of the resistors are
connected to plus and all lower ends, to the
negative pole of the input voltage.
Source: Direct Current Technology, Elabot
Trainings systems page 34
Therefore, it applies:
U = U1 = U2 = U3 = UN
If there is a voltage difference between the ends of a resistor or consumer, a current
flows through the component. In a parallel circuit, the current in each branch is given
by:
I1 =
U
R!
, I2 =
U
R2
, I3 =
U
R3
,In =
U
Rn
The branch currents in a parallel circuit are added to give the total current flow, IT :
The current, It flowing from the plus pole of the input voltage is divided through the
individual resistors. Thus the term, 'voltage divider'. If a resistor is connected in
parallel to an existing resistor, the current finds an extra path for a charge carrier
balance between the poles of the voltage source.
It = I1 + I2 + I3 … … … IN
A total resistance Rtot, has an effect on the voltage that is smaller than the smallest
individual resistor. This is given by the formula:
The relatively complicated formula for a parallel circuit can be simplified for 2 special
cases. With only 2 resistors in parallel, the formula becomes:
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Easier still, is the calculation of the total resistance if all parallel connected resistors
have the same value:
RT =
1
1
1
1
1
+ + + ……………….
R1 R2 R3
RN
𝑅𝑔𝑒𝑠 =
RT =
R
N
𝑅1 × 𝑅2
𝑅1 + 𝑅2
n = Number of equal-value resistors
Fig 4 of Kirchhoff's law
1.2.2.2 Kirchhoff’s Current Law:
The sum of the currents into a node ( total current ) is
equal to the sum the currents.
A node is any point or junction in a circuit where two or
more components are connected .In a parallel circuit , a
node or junction is a point where the parallel come
together . For example in the circuit of Fig 4of Kirchhoff's
Source: Principles of Electric circuits,
Thomas L. Floyd, 1999, page 185
current law point A is one node and point B is another .
Let's start at the positive terminal of the source and follow the current .the total
current It from the source is into is node A. At point, the current splits the
(I1 , I2 and I3 ) is out of node A. Kirchhoff's current law says that total current into node
A is equal to the total current out of node A; that is,
It = I1 + I2 + I3
Now, following the current in Fig 1 of Kirchhoff's current law though the branches
,you see that they come back together at node B.
Fig.5 of kirchhoff's law
Currents I1 , I2 and I3 are node B, and It is out of
node B. Kirchhoff's current law formula at node B is
therefore the same as at node A.
It = I1 + I2 + I3
Fig 5 of Kirchhoff's current law illustrates the
general case of Kirchhoff's current be written as
IIN(1) + IIN(2) + IIN(3) + ⋯ + IIN(n) = IOUT(1) + IOUT(2) + IOUT(3) + ⋯ + IOUT(m) = 0
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This equation shows that all current into and out of the junction sums to zero and can be
stated as:
The algebraic sum of all the current entering and leaving a node is equal to zero
An equivalent way of writing Kirchhoff's current law can be expressed using the mathematical
summation shorthand as was done for Kirchhoff's voltage law :
∑𝑛𝑖=1 𝐼𝐼 =0
Fig 6 of example use Kirchhoff's
Source: Principles of Electric circuits, Thomas L. Floyd, 1999,
page 187
Example 2 : Use Kirchhoff's current law to find the current measured by ammeters
A3 and A5 in figure of example 2
Solution , The Total current into node X is mA. Two currents are out of node X:
1.5mA through resistor 𝑅1 and the current thoughA3 Kirchhoff's current law applied
node X gives
5mA - 1.5mA -IA3 = 0
The total current into node Y is IA3 = 3.5mA two currents are out of node Y: 1 mA
though resistor 𝑅2 and the current though A5 and 𝑅3 . Kirchhoff's current law applied
at node Y gives
3.5mA - 1mA - IA5 = 0
solving forIA5 yields
-IA5 = 3.5mA - 1mA = 2.5mA
How much current will an ammeter measure when it placed in the circuit be low 𝑅3 in
figure 6? Below the negative battery terminal ?
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1.2.3 Comparison between TVTC and lesson of the internet web- research
The lesson for the RCT
Lesson of The Internet WebResearch: by , Direct Current
Technology Elabot Trainings systems
and Principles of Electric circuits,
Thomas L. Floyd, 1999
Less information about parallel
connection. the teacher can
explain it in one class . The RCT
has a few details and important
laws for use to calculate the
voltage drop, power and current.
Only theory hasn't practice .
More information about parallel
connection . it is not enough to teach
the student these information in one
time . the parallel circuit has more
details .the lesson from website clear
information.
Has a few example and it is more
easy .
It has practice and theory
Has more example and it is more
complicated .
1.2.4 The content :
Step 1 :
In series connection the amperes doesn't change in each loads. as you see in this
circuit we have 2A only for each loads in this circuit . you have taken this already .
But now we will take parallel connection . have a look to this circuit we have three
situations of amperes who can tell me what these situations, the total amperes is 2A
but in some point divided in two one 1A for each branches .
fig 7 of the parallel circuit
Source: Own Development
Rayyan Ateeq 308
fig 8 parallel circuit
Source: Own Development
Page 9
fig 9 of Parallel circuit
Step 2 :
These are shapes of parallel
connection , each shape has
different connection but the
result hasn't change .
Source: Principles of Electric circuits,
Thomas L. Floyd, 1999, page 182
Step 3 :
If two or more components are connected in parallel they have the same potential
difference (voltage) across their ends. The potential differences across the
components are the same in magnitude, and they also have identical polarities. The
same voltage is applicable to all circuit components connected in parallel. The total
current is the sum of the currents through the individual components, in accordance
with Kirchhoff’s current law.
fig 10 of the content
To calculate total resistance.
RT =
1
1
1
1
+ + +
R1 R2 R3
……………….
source : Principles of Electric circuits, Thomas L. Floyd, 1999,
page 189
1
RN
To find the total resistance of all components, add the reciprocals of the
resistances
of each component and take the reciprocal of the sum. Total
resistance will always be less than the value of the smallest resistance:
To calculate total current.
IT = I1 + I2 + I3 … … … … … … IN
The current, It flowing from the plus pole of the input voltage is divided through the
individual resistors. Thus the term, 'voltage divider'. If a resistor is connected in
parallel to an existing resistor, the current finds an extra path for a charge carrier
balance between the poles of the voltage source.
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Each voltage are equal.
E=V1 = V2 = V3 = VN
To calculate the power
PN = V × IN or
V2
2
PN = IN
× R N or PN = R
N
The power is hasn't change we use it for each circuit in parallel and series circuit.
To calculate total power
PT = P1 + P2 + P3 … … … … … … PN
Step 4 :
Example 1 : Find out the following if 𝑅1 = 9 𝛺 , 𝑅2 = 18 𝛺 and
𝐸 = 27v
Fig 11. of example
1. R T
Source: Handout of Eng, Kahaled , in RCT
2. IT
3. I1 , I2
4. P1 , P2
5. Pin
solution
1. R T =
RT =
1
or we use in this situation this formula R T=
1
1
+
R1 R2
1
1 1
9 + 18
R1 ×R2
R1 +R2
=6 Ω
V
2. IT = R
T
You have taken already ohm's law to find out the current we use it.
IT =
27V
= 4.5 A
6A
V
3. A. I1 = R
I1 =
1
27v
= 3A
9
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V
B. I2 = R
I2 =
2
27 v
= 1.5A
18
4. A. P1 = V × I1
to calculate the power 1 most be multiplied
the voltage with the current of the
resistor one
P1 = 27v × 3A = 81 w
B. P2 = V × I2
P2 = 27 v × 1.5 A = 40.5 w
5. A . Pin = P1 + P2
Indicated in step 3 (page10) the power sum of power will lead to the total .
Pin = 81w + 40.5 w = 121.5w
other way to solve Pin if you don't like to sum the power you can slove it by m
multiplication the voltage with total current .
B. Pin = E × IT
Pin = 27 v × 4.5 A = 121.5w
step 5 :
Kirchhoff’s Current Law
The sum of the currents into a node ( total current ) is equal to the sum the currents .
fig 12 of Kirchhoff's law
fig 13 of Kirchhoff's law
Source:http://www.xzx4ever.com/vb/s
Source:http://www.physics.uoguelp
howthread.php?t=9946
h.ca/tutorials/ohm/Q.ohm.KCL.html
It = I1 + I2
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step 6 :
Example: Find out the total current by using Kirchhoff's law if the first current equal
1A , and second current equal 2A
solution
fig 14 of example
Source: Principles of Electric circuits, Thomas L. Floyd, 1999, page 186
It = I1 + I2
It = 5mA + 12mA = 17mA
1.3. Didactic Analysis
There have to be expected up to 20 trainees in class and each trainee has at the
General Certificate of Secondary Education in the natural sciences. Most of trainees
are from Riyadh and the range of age is from 19-23. An experience in the electrical
power can't be expected , to perform the lesson in an appropriate way the following
equipment will be necessary , Projector, Whiteboard, Computer, Power Point and
Loudspeaker. The lesson is started on 4 May 2014, 8:50 am in room 12F, building
20 an RCT will take place.
Using video because:
 Visualize information from other methods campus.
 Presenting the students example from the subject.
Using feedback control because:
 The trainees shall reflect video, in order to increase the memorizing video.

Trainee's shall think and build an own opinion.
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Using In step 1 , step 3 , step 4 and step 6 classroom conversation because
the trainees shall be able to :

Discuses about the differences between series and parallel connections .
 Communicate with the others.
 Increase the attention .
 Make the students more active.
Using lecture in step 2 and step 5 because the trainees shall receive:
 Clear information about parallel circuit and Kirchhoff's law .
 An introduction about parallel connection .
 A cover to guidance to appropriate learning.
Using Group work in Task (1) of group 1 and group and homework because:
 Make trainees more active.
 Connect theory example with practice example Horizontal reduction .
 Motivate the trainees to work.
 Presenting difference between parallel and series circuit .
2. Lesson Plan
II. Objectives
General Objectives:
The Trainees:
will increase their social competencies by participating
Specific Learning Objectives:
The Trainees will be able to:
explain Parallel circuit (Reorganization).
explain the voltage and current and resistor (Reorganization).
calculate the voltage, the current and resistor by using the formula of Parallel circuit
(Reorganization).
Learn how to measuring the current in the circuit.
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III. Overview of the Intended Process
Opening / Entrance / Motivation
Time
Methodology
Media
Minutes
Expected Trainer-action
Expected Trainee-action
The trainer welcomes the trainees
-
-
-
-
Projector
Video
5
-
Presentation video
visualization
Control Question
The trainees should answer what
the different between parallel and
series circuit .
Feedback
Control
Explanation what the different
between series and parallel
connection
-
Classroom
conversation
Lecture
Slid 1
-
Slide 2
Body (Information / Elaboration)
2
2
Time
Media
Expected Trainer-action
Expected Trainee-action
Methodology
Explanation what does mean
parallel connection and showing
shapes of parallel connection
-
Lecture
Explanation of the formulas of
parallel connection voltage,
current , power , and resistors
-
Minutes
Slide 3
4
Classroom
conversation
Classroom
conversation
Slide 4
7
Handout 1
Whiteboard
Calculation of the currents ,
resistors and powers and gives
them example.
-
Classroom
conversation
Slide 5
9
Handout 2
The trainer divides the trainees
to two groups
The trainer gives the first group
Task (1) in theory
The trainees of group 1solve the
ask in theory the questions.
9
Task (1)
The trainees of group 2 take the
values of experiment
Group Work
Slide 6
The trainer gives second group
task (1) practical
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The trainees are comparing about
the task1on the whiteboard and
the trainer asks them why you
use these method
One of each groups write and
explain the solution the question
and the values on the whiteboard
Whiteboard
4
Slide 7
3
Explanation of definition of
Kirchhoff’s Current Law
-
Lecture
Calculation of Kirchhoff’s Current
Law
-
Classroom
conversation
Slide 8
3
The trainer gives them Homework
-
-
Homework
Nothing
Close (Reflection, Exercises, Homework, Feedback)
Time
Media
Expected Trainer-action
Expected Trainee-action
Methodology
The trainer ask them questions
about the parallel connection
-
Classroom
conversation
Minutes
Slid 9
2
3. References
Principles of Electric circuits, Thomas L. Floyd, 1999, page 182,184,185,188,189
Electrical circuit The Theory And Technology , JOHN BIRD , Fourth Edition 2010
,Pages , 39, 40,41,42,43
http://books.google.com.sa/books?id=v1elek6nS_sC&q=parallel#v=snippet&q=parall
el&f=false
Electrical circuit 1 Arabic book from TVTC , 2008,Pages 103, 104,105,106,107,108
and 109.
fig 11 of the content
http://www.physics.uoguelph.ca/tutorials/ohm/Q.ohm.KCL.html
fig 12of the content
http://www.xzx4ever.com/vb/showthread.php?t=9946
Direct Current Technology Elabot Trainings systems Page , 34 and 35
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