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Chapter 6

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Title: Chapter 6


1
Chapter 6 Parallel dc Circuits
  • Introductory Circuit Analysis
  • Robert L. Boylestad

2
6.1 - Introduction
  • There are two network configurations series and
    parallel.
  • In Chapter 5 we covered a series network. In
    this chapter we will cover the parallel circuit
    and all the methods and laws associated with it.

3
6.2 Parallel Resistors
  • Two elements, branches, or circuits are in
    parallel if they have two points in common as in
    the figure below

Insert Fig 6.2
4
Parallel Resistors
  • For resistors in parallel, the total resistance
    is determined from
  • Note that the equation is for the reciprocal of
    RT rather than for RT.
  • Once the right side of the equation has been
    determined, it is necessary to divide the result
    into 1 to determine the total resistance

5
Parallel Resistors
  • For parallel elements, the total conductance is
    the sum of the individual conductance values.
  • As the number of resistors in parallel increases,
    the input current level will increase for the
    same applied voltage.
  • This is the opposite effect of increasing the
    number of resistors in a series circuit.

6
Parallel Resistors
  • The total resistance of any number of parallel
    resistors can be determined using
  • The total resistance of parallel resistors is
    always less than the value of the smallest
    resistor.

7
Parallel Resistors
  • For equal resistors in parallel
  • Where N the number of parallel resistors.

8
(No Transcript)
9
1/RT 1/1 ¼ 1/5 1 0.25 0.2 1.45 ?RT
1/1.45 0.69?
10
Parallel Resistors
  • A special case The total resistance of two
    resistors is the product of the two divided by
    their sum.
  • The equation was developed to reduce the effects
    of the inverse relationship when determining RT

RT PRODUCT/SUM
11
RT (3 x 6)/(3 6) 18/9 2?
12
Parallel Resistors
  • Parallel resistors can be interchanged without
    changing the total resistance or input current.
  • For parallel resistors, the total resistance
    will always decrease as additional parallel
    elements are added.

13
Using a protoboard to set up the circuit
14
6.3 Parallel Circuits
  • Voltage is always the same across parallel
    elements.
  • V1 V2 E
  • The voltage across resistor 1 equals the voltage
    across resistor 2, and both equal the voltage
    supplies by the source.

15
Measuring the voltages of a parallel dc
network.
16
Parallel Circuits
  • For single-source parallel networks, the source
    current (Is) is equal to the sum of the
    individual branch currents.
  • For a parallel circuit, source current equals
    the sum of the branch currents. For a series
    circuit, the applied voltage equals the sum of
    the voltage drops.

17
Parallel Circuits
  • For parallel circuits, the greatest current will
    exist in the branch with the lowest resistance.

18
6.4 Power Distribution in a Parallel Circuit
  • For any resistive circuit, the power applied by
    the battery will equal that dissipated by the
    resistive elements.
  • The power relationship for parallel resistive
    circuits is identical to that for series
    resistive circuits.

19
Measuring the source current of a parallel
network.
20
Measuring the current through resistor R1.
21
6.5 - Kirchhoffs Current Law
  • Kirchhoffs voltage law provides an important
    relationship among voltage levels around any
    closed loop of a network.
  • Kirchhoffs current law (KCL) states that the
    algebraic sum of the currents entering and
    leaving an area, system, or junction is zero.
  • The sum of the current entering an area, system
    or junction must equal the sum of the current
    leaving the area, system, or junction.

22
Kirchhoffs Current Law
  • Most common application of the law will be at
    the junction of two or more paths of current.
  • Determining whether a current is entering or
    leaving a junction is sometimes the most
    difficult task.
  • If the current arrow points toward the junction,
    the current is entering the junction.
  • If the current arrow points away from the
    junction, the current is leaving the junction.

23
Kirchhoffs current law.
24
(a) Demonstrating Kirchhoffs current law (b)
the water analogy for the junction in (a).
25
I3 5A and I4 4A
26
I1 1A I3 I1 1A I4 I2 4A I5 I3 I4
5A
27
6.6 Current Divider Rule
  • The current divider rule (CDR) is used to find
    the current through a resistor in a parallel
    circuit.
  • General points
  • For two parallel elements of equal value, the
    current will divide equally.
  • For parallel elements with different values, the
    smaller the resistance, the greater the share of
    input current.
  • For parallel elements of different values, the
    current will split with a ratio equal to the
    inverse of their resistor values.

28
Current Divider Rule
29
Using the current divider rule to calculate
current I1
1/RT 1/1k 1/10k 1/22k ?RT 873? I1
(RT/R1)IT (873/1000)(12 mA) 10.5 mA
30
6.7 - Voltage Sources in Parallel
  • Voltage sources are placed in parallel only if
    they have the same voltage rating.
  • The purpose for placing two or more batteries in
    parallel is to increase the current rating.
  • The formula to determine the total current is
  • at the same terminal voltage.

31
Voltage Sources in Parallel
  • Two batteries of different terminal voltages
    placed in parallel
  • When two batteries of different terminal
    voltages are placed in parallel, the larger
    battery tries to drop rapidly to the lower supply
  • The result is the larger battery quickly
    discharges to the lower voltage battery, causing
    the damage to both batteries

32
Examining the impact of placing two lead-acid
batteries of different terminal voltages in
parallel.
I (12 6)/(0.03 0.02) 120A
33
6.8 - Open and Short Circuits
  • An open circuit can have a potential difference
    (voltage) across its terminal, but the current is
    always zero amperes.

34
Open and Short Circuits
  • A short circuit can carry a current of a level
    determined by the external circuit, but the
    potential difference (voltage) across its
    terminals is always zero volts.

Insert Fig 6.44
35
I (6V)/(12?) 0.5A and V (0.5A)(10?) 5V
36
I (6V)/(2?) 3A and V 0
37
6.9 Voltmeter Loading Effects
  • Voltmeters are always placed across an element
    to measure the potential difference.
  • The resistance of parallel resistors will always
    be less than the resistance of the smallest
    resistor.
  • A DMM has internal resistance which may alter
    the resistance of the network under test.
  • The loading of a network by the insertion of a
    meter is not to be taken lightly, especially if
    accuracy is a primary consideration.

38
Voltmeter Loading Effects
  • A good practice is to always check the meter
    resistance against the resistive elements of the
    network before making a measurement.
  • Most DMMs have internal resistance levels in
    excess of 10 MW on all voltage scales.
  • The internal resistance of a VOM depends on the
    scale chosen.
  • Internal resistance is determined by
    multiplying the maximum voltage of the scale
    setting by the ohm/volt (? / V) rating of the
    meter, normally found at the bottom of the face
    of the meter.

39
Vab 20V
Vab (11M?)/(12M?)(20V)
18.33V
40
6.11 Troubleshooting Techniques
  • Troubleshooting is a process by which acquired
    knowledge and experience are employed to localize
    a problem and offer or implement a solution.
  • Experience and a clear understanding of the basic
    laws of electrical circuits is vital.
  • First step should always be knowing what to
    expect

41
6.13 Applications
  • Car system
  • The electrical system on a car is essentially a
    parallel system.
  • Parallel computer bus connections
  • The bus connectors are connected in parallel
    with common connections to the power supply,
    address and data buses, control signals, and
    ground.

42
Expanded view of an automobiles electrical
system.
43
Applications
  • House wiring
  • Except in some very special circumstances the
    basic wiring of a house is done in a parallel
    configuration.
  • Each parallel branch, however, can have a
    combination of parallel and series elements.
  • Each branch receives a full 120 V or 208 V, with
    the current determined by the applied load.

44
Single phase of house wiring (a) physical
details (b) schematic representation.
45
Continuous ground connection in a duplex outlet.
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