Slides Unit 5. Electric Networks
Transcript of Slides Unit 5. Electric Networks
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Unit 5: Electrical network analysis.
Introduction: junction, branch, loop, network(multi-loop circuit).
Kirchhoffs Rules: junction and loop rules.
Superposition principle.
Equivalent resistor of a passive network.
Thvenins theorem.
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Introduction: definitions
Electrical network: Set of dipoles (active andpassive elements) interconnected between them.
If all the dipoles show linear rates between V and I,the circuit is a linear network.
R
C R
R
L
L
C
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Junction:point of the net where arejoined threeor more wires being different the electric potential.
Network with three junctions:
R
C R
R
L
L
C
There are the same junction
Introduction: definitions
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Branch: is the path joining two junctions. Electricalnetwork with five branchs:
This is not a branch
R
C R
R
L
L
C
Introduction: definitions
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Loop: closed circuit made with branchs, withoutanyone inside. Electrical network with three loops:
R
C R
R
L
L
C
Introduction: definitions
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Junction Rule: The sum of the currents into thejunction must be equal to the sum of the currents
out of the junction. Algebraic addition = 0. Its an expression of the charge conservation principle.
1I
2I
3I kI
nI
0= kI
Tipler, chapter 25, section 25.5
Kirchhoffs Rules: Junction rule
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Loop rule: Algebraic sum of the changes inpotential around a loop must be equal zero.
Its an expression of energy preservation principle. A point can not havetwo different potentials at the same time.
1 2
kn
V1
V2
Vk
Vn 0= kV
Kirchhoffs Rules: loop rule
Tipler, chapter 25, section 25.5
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To solve a circuit, must be writen:
(Junctions -1) equations of junction rule
Loops equations of loop rule
RC R
R
L
L
C
Kirchoffs rule application
Example: 2 equations of junction rule + 3 equations of loop rule = 5 equations
5 unknown (intensity of currents)
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On a circuit with several generators, the solution ofthe circuit (calculus of currents and potentials) is
the algebraic sum corresponding to each generator(ideal) acting alone.
Superposition principle.
a BR
CR DR
A B
1I
2I
AR b
c
a BR
CR
DR
A
AI1 A
I2
AR b
c
= +
a BR
CR
R
B
BI1
I2
AR
b
c
BABA IIIIII
222111 +=+=
This calculus can be made not only for currents, but for potentials too.
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Is a resistor ( ) such that when applying the samed.d.p., current flowing is the same:
eqR
Passive
network
1I1
2 3
4 ...
... n
A
B
1I
eqR
A
B
Equivalent resistor of a passive network.
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A linear active circuit with output terminals A and B isequivalent to a generator of e.m.f. equal to thedifference of potential between A and B, and an
internal resistance equal to the equivalent resistanceof the passive network between A and B (withoutideal generators).
Linear
Active
circuit
A
B
A
B
eqT RR =
ABT V=
Thevenins theorem
Its useful to analyze circuits by splitting it in little pieces.