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EE101Lect3- Circuit Laws
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Ohm’s Law
Alternatively
n Resistors (Rk) in series
n Conductors (Gk) in parallel
• m Resistors (Rk) in p
v=Ri (units: v[V], i[A], R[Ω]
i=Gv where G=1/R [ʊ]
Rtotal= n1 Rk
Gtotal= n1 Gk
Rtotal=1/
EE101 Fall 2012 Lect 2- Kang
𝑚 1
1 (𝑅𝑘)
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Serial and Parallel Connections
EE101 Fall 2012 Lect 2- Kang
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Series Connection of Resistances
V = V1 + V2 = R1 x i + R2 x i = (R1 + R2) i
Thus Req = R1 + R2
When n resistors are in series, Req
EE101 Fall 2012 Lect 2- Kang
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Parallel Connection of Resistances
i = i1 + i2 = v/R1 + v/R2 = v (1/R1 + 1/R2)
Thus 1/Req = 1/R1 + 1/R2, or Geq = G1 + G2
Alternatively, Req = 1/ (1/R1 + 1/R2) = R1x R2/(R1 + R2)
Generally stating, when m resistances are in parallel,
Req=1/
𝑚 1
1 (𝑅𝑘)
EE101 Fall 2012 Lect 2- Kang
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How to find an Req?
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What is the equivalent Resistance Req ?
Approach from the right end
1.Series resistance: 4 + 5 + 3 = 12
2.Parallel resistance: 4//12= 1/(1/4 + 1/12)= 4x12/(4+12)= 3
3.Series resistance: 3+3=6
4.Parallel resistance: 6//6= 1/(1/6+1/6)= 6x6/(6+6)=3
5.Series resistance: 4+3+3= 10 Ω (ans)
EE101 Fall 2012 Lect 2- Kang
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Another example of calculating Req
(2+2)//6= 4x6/(4+6)=2.4
Thus Req= 4 + 2.4 + 8= 14.4Ω
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What is the resistance between terminals
a and b (Rab)?
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What is Rab?
1P) 20//5= 20x5/(20+5)=4
2S) 4+1= 5
3P) 5//20= 5x20/(5+20)=4
4S) 4+2=6
5P) 9//6=9x6/(9+6)=54/15=5.6
6P) 18//5.6=18x5.6/(18+5.6)=4.27
7S) 16+4.27= 20.27Ω= Req
EE101 Fall 2012 Lect 2- Kang
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Kirchhoff’s Laws
The sum of voltages in a loop is zero.
(𝑣𝑜𝑙𝑡𝑎𝑔𝑒𝑠 𝑖𝑛 𝑎 𝑙𝑜𝑜𝑝) = 0
This is called Kirchhoff’s Voltage Law (KVL)
The Sum of the currents at a node is zero.
(what goes into a node comes out, that is
𝑐𝑢𝑟𝑟𝑒𝑛𝑡 𝑖𝑛𝑤𝑎𝑟𝑑 = ∑𝑐𝑢𝑟𝑟𝑒𝑛𝑡 out𝑤𝑎𝑟𝑑
Another way of saying this is
(𝑐𝑢𝑟𝑟𝑒𝑛𝑡𝑠 𝑖𝑛𝑡𝑜 𝑎 𝑛𝑜𝑑𝑒) = 0
This is called Kirchhoff’s Current Law (KCL)
EE101 Fall 2012 Lect 2- Kang
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What is the current through R1?
Find an equivalent resistance of R2 and R3
In parallel
R2//R3= 1/(1/R2 + 1/R3)= 1/(1/30 + 1/60)
= 20Ω
The total resistance across Vs = 10 + 20=30Ω
The current through R1 = 90V/30Ω= 3A
What about currents through R2 and R3?
3A is divided into two branchesThrough R2 is 2X of that R3, and thus 2A
through R2 and 1A through R3.
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Finding Currents using Nodal Analysis
SOLUTION:
Problem:
N1
Let us note the voltage at node N1 as V1,
Then we have the following nodal equationBy KCL (sum of entering current s=sum of leaving currents
At each node):
(90-V1)/10 = V1/30 + V1/60
Multiplying both sides by 60, we obtain
6(90-V1)=2 V1 + V1 = 3 V1
540= 9 V1
Thus V1= 60V
[Q] Find is the current through R3
[Q] Find the power dissipated in R3
iR3 = 60/60= 1A
iR2 = 60/30= 2A
iR1 = (90-60)/10= 3A
The power dissipation in R3 is
P3= V1xiR3 = 60V x 1A= 60W.
EE101 Fall 2012 Lect 2- Kang
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∆-Y Transformation
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∆-Y Transformation
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