Module 1—Introduction to Matter, Energy, and Direct CurrentPages
i  ix, 11 to 110,
111 to 120, 121 to 130,
141 to 150, 151 to 160,
161 to 165, 21 to 210,
211 to 220, 221 to 229,
31 to 310, 311 to 320,
321 to 330, 331 to 340,
341 to 350, 351 to 360,
361 to 370, 371 to 380,
381 to 390, 391 to 3100,
3101 to 110, 3111 to 3120,
3121 to 3126, Appendix I,
II, III,
IV, V,
Index
Figure 345.—Example circuit with unequal parallel resistors.
Given:
Solution:
The equivalent resistance the circuit shown in figure 345 is smaller than either the two resistors (R1,
R2). An important point to remember is that the equivalent resistance a parallel circuit is always less than the
resistance any branch.
Equivalent resistance can be found if you know the individual resistance values and
the source voltage. By calculating each branch current, adding the branch currents to calculate total current, and
dividing the source voltage by the total current, the total can be found. This method, while effective, is
somewhat lengthy. A quicker method finding equivalent resistance is to use the general formula for resistors in
parallel:
If you apply the general formula to the circuit shown in figure 345 you will get the same value for
equivalent resistance (2 ) as was obtained in the previous calculation that used source voltage and total
current.
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Given:
Solution:
Convert the fractions to a common denominator.
Since both sides are reciprocals (divided into one), disregard the reciprocal function.
The formula you were given for equal resistors in parallel
is a simplification the general formula for resistors in parallel
There are other simplifications the general formula for resistors in parallel which can be used to
calculate the total or equivalent resistance in a parallel circuit.
RECIPROCAL METHOD.—This
method is based upon taking the reciprocal each side the equation. This presents the general formula for resistors
in parallel as:
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This formula is used to solve for the equivalent resistance a number unequal parallel resistors. You
must find the lowest common denominator in solving these problems. If you are a little hazy on finding the lowest
common denominator, brush up on it in Mathematics Volume 1, NAVEDTRA 10069 (Series).
Example: Three
resistors are connected in parallel as shown in figure 346. The resistor values are: R1 = 20 ohms, R2 = 30
ohms, R3 = 40 ohms. What is the equivalent resistance? (Use the reciprocal method.)
Figure 346.—Example parallel circuit with unequal branch resistors.
Given:
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Solution:
PRODUCT OVER THE SUM METHOD.—A convenient method for finding the equivalent, or total,
resistance two parallel resistors is by using the following formula.
This equation, called the product over the sum formula, is used so frequently it should be committed to
memory.
Example: What is the equivalent resistance a 20ohm and a 30ohm resistor connected in parallel, as in
figure 347?
Figure 347.—Parallel circuit with two unequal resistors.
364
Given:
Solution:
Q36. Four equal resistors are connected in parallel, each resistor has an ohmic value 100 ohms, what is
the equivalent resistance?
Q37. Three resistors connected in parallel have values 12 k , 20 k , and 30
k What is the equivalent resistance?
Q38. Two resistors connected in parallel have values 10 k and
30 k What is the equivalent resistance?
Power in a Parallel Circuit
Power computations in a parallel circuit are essentially the same as those used for the series circuit.
Since power dissipation in resistors consists a heat loss, power dissipations are additive regardless how the
resistors are connected in the circuit. The total power is equal to the sum the power dissipated by the individual
resistors. Like the series circuit, the total power consumed by the parallel circuit is:
Example: Find the total power consumed by the circuit in figure 348.
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Figure 348.—Example parallel circuit.
Given:
Solution:
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Since the total current and source voltage are known, the total power can also be computed by: Given:
Solution:
Equivalent Circuits
In the study electricity, it is ten necessary to reduce a
complex circuit into a simpler form. Any complex circuit consisting resistances can be redrawn (reduced) to a
basic equivalent circuit containing the voltage source and a single resistor representing total resistance. This
process is called reduction to an EQUIVALENT CIRCUIT.
Figure 349 shows a parallel circuit with three
resistors equal value and the redrawn equivalent circuit. The parallel circuit shown in part A shows the original
circuit. To create the equivalent circuit, you must first calculate the equivalent resistance.
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Figure 349.—Parallel circuit with equivalent circuit.
Given:
Solution:
Once the equivalent resistance is known, a new circuit is drawn consisting a single resistor (to represent
the equivalent resistance) and the voltage source, as shown in part B.
Rules for Parallel DC
Circuits
1. The same voltage exists across each branch a parallel circuit and is equal to the source voltage.
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2. The current through a branch a parallel network is inversely proportional to the amount
resistance the branch.
3. The total current a parallel circuit is equal to the sum the individual branch
currents the circuit.
4. The total resistance a parallel circuit is found by the general formula:
or one the formulas derived from this general formula.
5. The total power consumed in a parallel
circuit is equal to the sum the power consumptions the individual resistances.
SOLVING PARALLEL
CIRCUIT PROBLEMS
Problems involving the determination resistance, voltage, current, and power in
a parallel circuit are solved as simply as in a series circuit. The procedure is the same — (1) draw the circuit
diagram, (2) state the values given and the values to be found, (3) select the equations to be used in solving for
the unknown quantities based upon the known quantities, and (4) substitute the known values in the equation you
have selected and solve for the unknown value.
Example: A parallel circuit consists five resistors. The
value each resistor is known and the current through R1 is known. You are asked to calculate the value for total
resistance, total power, total current, source voltage, the power used by each resistor, and the current through
resistors R2, R3, R4, and R5.
Given:
Find:
This may appear to be a large amount mathematical manipulation. However, if you use the step bystep
approach, the circuit will fall apart quite easily.
The first step in solving this problem is for you to
draw the circuit and indicate the known values as shown in figure 350.
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Figure 350.—Parallel circuit problem.
There are several ways to approach this problem. With the values you have been given, you could first
solve for RT, the power used by R1, or the voltage across R1, which you know is equal to the source voltage and
the voltage across each the other resistors. Solving for RT or the power used by Ri will not help in solving for
the other unknown values.
Once the voltage across R1 is known, this value will help you calculate other
unknowns. Therefore the logical unknown to solve for is the source voltage (the voltage across R1).
Given:
Solution:
Now that source voltage is known, you can solve for current in each branch. Given:
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Introduction to Matter, Energy, and Direct Current, Introduction
to Alternating Current and Transformers, Introduction to Circuit Protection,
Control, and Measurement, Introduction to Electrical Conductors, Wiring Techniques,
and Schematic Reading, Introduction to Generators and Motors,
Introduction to Electronic Emission, Tubes, and Power Supplies,
Introduction to SolidState Devices and Power Supplies,
Introduction to Amplifiers, Introduction to
WaveGeneration and WaveShaping Circuits, Introduction to Wave Propagation, Transmission
Lines, and Antennas, Microwave Principles,
Modulation Principles, Introduction to Number Systems and Logic Circuits, Introduction
to Microelectronics, Principles of Synchros, Servos, and Gyros,
Introduction to Test Equipment, RadioFrequency
Communications Principles, Radar Principles, The Technician's Handbook,
Master Glossary, Test Methods and Practices, Introduction to Digital Computers,
Magnetic Recording, Introduction to Fiber Optics
