lecture 03_parallel circuit
TRANSCRIPT
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Parallel Circuit
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Series or Parallel???
Comment on whether R1, R2 and R3 are in series/parallel/series-parallel
combination. Signify your answer.
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Parallel elementsTwo elements, branches, or networks are in parallel if they have
two points in common.
FIG. 1 Different ways in which three parallel elements may appear.
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Total conductance & resistance
Recall that for series resistors, the total resistance is the sum of the
resistor values. What about conductance???
Can you work it out?????
For parallel elements, the total conductance is the sum of the individual
conductances.
That is, for the parallel network
of Fig. 2, we write
FIG. 2 Determining the total conductance of
parallel conductances.
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Total conductance & resistance
Substituting resistor values for the network of Fig. 2 will result inthe network of Fig. 3. Since G =1/R , the total resistance for the network
can be determined by direct substitution into the equation of GT ,
FIG. 3 Determining the total resistance of
parallel resistors
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Example problemsQ.1 Find the total resistance for the circuit shown in fig 4.
Also find the total conductance.
FIG. 4 Circuit diagram for example problem#1
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Resistors in parallel…….
The total resistance of parallel resistors is always less than the value
of the smallest resistor. (check it out with Q.1 u just did!!!)
For equal resistors in parallel, the equation becomes significantly easier
to apply. In other words, the total resistance of N parallel resistors of
equal value is the resistance of one resistor divided by the number (N)
of parallel elements.
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Resistors in parallel……. The total resistance of two parallel resistors is the product of the two
divided by their sum.
Parallel elements can be interchanged without changing the
total resistance or input current.
For parallel resistors, the total resistance will always decrease as
additional elements are added in parallel.
For 3 parallel resistors
Q.2 Find the RT for the circuit in fig. 5.
FIG. 5 Circuit diagram for
example problem#2 8M.S.Muhit
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Resistors in parallel…….
The voltage across parallel elements is the same.
FIG. 6 Parallel network.
For single-source parallel networks, the source current (I s ) is equal
to the sum of the individual branch currents.
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Example problemsQ.3 For the parallel network of Fig. 7
a. Calculate RT .b. Determine Is.
c. Calculate I1 and I2, and demonstrate that Is = I1+I2.
d. Determine the power to each resistive load.
e. Determine the power delivered by the source, and compare it to the
total power dissipated by the resistive elements.
FIG. 7 Circuit diagram for example problem#3
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Example problemsQ.4 Given the information provided in Fig. 8,
a. Determine R3.b. Calculate E.
c. Find Is.
d. Find I2.
e. Determine P2.
FIG. 8 Circuit diagram for example problem#4
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Don’t use calculator……… Q.5 Determine the currents I1 ,I3 ,I4 & I5 of Fig. 9 using Kirchhoff’s
current law.
FIG. 9 Circuit diagram for example problem#5
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Don’t use calculator………
Q.6 Find the magnitude and direction of the currents I3 , I4 , I6 , and I7 for
the network of Fig. 10. Even though the elements are not in series or
parallel, Kirchhoff’s current law can be applied to determine all the
unknown currents.
FIG. 10 Circuit diagram for example problem#6
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Current divider ruleFor two parallel elements of equal value, the current will divide equally.
For parallel elements with different values, the smaller the resistance, thegreater 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.
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Current divider rule
Technique #2
Current seeks the path of least resistance. 16M.S.Muhit
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Voltage sources in parallel
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Open circuit
An open circuit can have a potential difference ( voltage ) across its
terminals, but the current is always zero amperes.
FIG. 11 Demonstrating the characteristics of an
open circuit.
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Short circuit 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.
Net resistance = 0; V=10 V, hence, I=infinite.
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FIG. 12 Single phase of house wiring:
physical details ;
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Reference
1. Introductory Circuit Analysis by Robert . L. Boylestad
2. http://www.electronics-tutorials.ws/dccircuits/dcp_1.html
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http://www.electronics-tutorials.ws/dccircuits/dcp_1.htmlhttp://www.electronics-tutorials.ws/dccircuits/dcp_1.htmlhttp://www.electronics-tutorials.ws/dccircuits/dcp_1.htmlhttp://www.electronics-tutorials.ws/dccircuits/dcp_1.html