review psc kcl and kvl
TRANSCRIPT
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Electric circuitan interconnection of circuit elements.There must be a closed loop for the current to flow.
+
+
There is a closed loop, enabling
current to flow into resistorNo closed loop
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Circuit elementeach component of a circuit.
* A two terminal electrical device, it can be completely
characterized by its voltage and current relationship
-active elements generate energy (voltage and current sources)
-passive elements cannot generate energy (resistors, capacitors,inductors)
This course deals with:1. Power for an element
2. Voltage across an element
3. Current through an element
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Voltage is the energy needed to move a unit charge between 2 points in space orin a circuit. It is expressed in volts (V).
Voltage must be an oriented variable. The (+) and (-) signs indicate voltage polarity:
+ vab -
a b- vba +
* Above, point a is vab potential higherthan point b.
* voltage rise from b to a is vab* Since voltage vba is defined with the opposite orientation, it has theopposite value of voltage vab.
vba = - vab
dq
dwvab
dw is energy in joules required to move
a negative charge dq from a to b
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Voltage
Lowercase letter represents general case
v may or may not be time varying
Uppercase letter if quantity is not time varying
V is not time varying (DC Voltage)
Lowercase letter followed by a (t) is time varying
v(t) is time varying (AC Voltage)
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Electric current is the flow of electric charges through space per unit time.It is measured in ampheres (A).
current, positive charges
electrons
Current is oriented with a directed arrow
Current through an object is the same going in, as it is coming out of the objectChanging the orientation of current changes its sign (see below)
dt
dqi
i i
-i-i
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Current
Lowercase letter represents general case
i may or may not be time varying
Uppercase letter if quantity is not time varying
I is not time varying (DC Current)
Lowercase letter followed by a (t) is time varying
i(t) is time varying (AC Current)
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Passive Sign Convention
Passive Sign Convention is satisfied when current enters through the + terminal
of an element and leaves through theterminal.
Circuit Element
E1
+ i1v1
PSC NOTPSC
E2
+ v2 i2
E3+
i3
v3
PSC
i1
Pabs = i vWhen PSC is satisfied
When PSC is NOT satisfied Pabs = - (i v)
Power absorbed by an element
Power absorbed by device = - Power delivered by
device / supplied by device
i2
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PSC Examples
Given v1 = - 3 volts, i1 = 3 amps
What is PABS_E1?
Notice: v1 and i1 are not PSC
But ix and v1 are PSC
ix = - i1 = - (3 amps)
Therefore, PABS_E1= ix v1= (-3 amps)(-3 volts)= 9 watts
Similarly, PABS_E1= -(i1 v1 )= -(3 amps)(-3 volts)= 9 watts
E2
+
vx
ix Given vx = 10 Volts, ix = - 4 ampsWhat is PABS_E2?
vx and ixfollow PSC
PABS_E2= ix vx= (- 4 amps)(10 volts)= - 40 watts
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But what is a circuit element?
A Circuit Element is mathematical model of a 2 terminal electrical device, it can
be completely characterized by its voltage and current relationshipResistors:
R
i
+
-
01
vR
i
y = mx + b
R>0
i
v
1/R
Current voltage
characteristic
equation
Ohms law variationsv = i R
R= , i 0
i
v
Unit of resistance is ohm ()
Note: The above relations assume PSC as we
have drawn, if i and v do not follow PSC for aresistor then v = - i R
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Ohms Law and PSC
PSC is satisfied:given i = 2mA, R = 5 K
R1
i+
-
v = i R = (2mA)(5K) = 10 V
PABS_R1 = i v = (2mA)(10V) = 20 mW
Note: if i and v do not follow PSC for a resistor then v = - i R
+
-
iPSC is not satisfied:given i = 4A, R = 2v = -(i R) = - (4A)(2) = - 8 V
PABS_R2 = -( i v) = -(4A)(-8V) = 32W
R2
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Open Circuit
i
v
As R increases the line flattens out
As R the function approaches any voltage, but
i=0
Open Circuitno path for current to flow
i=0
+
-
vR =
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Short Circuit
i
v
As R0 the line gets vertical
At R=0 we have a Short Circuit
v = iR = 0
i can be anything, but v=0
i+
-
R = 0 v = 0
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Examples Short Circuit/Open Circuit
13
Short circuit between terminals a and b
Open circuit between terminals c and d
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Independent Voltage SourcesOrientation indicated by polarity inside bubble
Current assigned follows PSC
i
v+
i
v(t)+
i
VB
+
-
V indicates a constantsource like a battery
v(t) indicates a time varying source(typically sinusoidal)
i
v
Current-voltage
characteristics
3
i
v=V=3 volts+
Current is unknown until you
find out what is connected to
the source!
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Independent Current Sources
Orientation indicated by arrow inside.
Guarantees a motion of charge but musthave path to flow and must be connected to
an object.v+
-
i, I, i(t)
i
v
3
v
+
-
I=3A
Example: constant current source
Current is fixed at 3 A.
Voltage can be anything!
Note: Ohms law does not apply to current or voltage sources.
Also, current and voltage sources can apply OR absorb power to a circuit.
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Circuit Terminology
A node is the point of connection of one or more circuit
elements If a short circuit (a wire) connects 2 nodes, they constitute a single
node
A loop is any closed path (starting & ending at the same
location)How many nodes and loops in the circuits below?
+
+
+
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Circuit Terminology
+
+
+
2 nodes
1 loop2 nodes
3 loops
3 nodes
1 loop
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Series/Parallel Resistors ?
19
36 V
10
20
30
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Series/Parallel Resistors ?
20
36 V
10
20
30
No resistors in series
20 and 30 ohm resistances are in parallel
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More on Power
As in our example, power absorbed by a resistor must be positive!
VR = I RTherefore PABS_R = IV = I I R = I
2R 0
Conservation of Energy or Power Rule
The sum of all the power absorbed by all N elements tied together in a circuit must equal
zero!
From previous example, PABS_IS + PABS- R = -5/2W + 5/2W = 0 Watts
Power Delivered
Power delivered by an element is equal to the opposite of the power absorbed by that same
element
PDEL_VS = - PABS_VS
0_1
iABS
N
i
P
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Example 2
R=15 Find the voltage, current and power absorbed for
each element. Note: it is often easier to work with
resistors first!
Is = 3A
R=15Is = 3A
Make the arbitrary assignments shown in red font
IR = - 3 Amps
To apply Ohms law, use current following PSC (IS)
VR = ISR = (3A)(15) = 45 V
Note: PABS_R = ISVR = (IS)2R = (VR)
2/R
Because I = (1/R)V and IV= (1/R)VV= V2/R
PABS_R = ISVR =(3 A)(45 V) = 135 W
VS = - VR = - (45 V) = - 45 V
PABS_IS = ISVS = ( 3 A)(-45 V) = - 135 Watts
+
-
VS
+
-
VR
IR
0_1
iABS
N
i
P PABS_IS + PABS_R = -135 W + 135 W = 0 Watts
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Example 3: Using Conservation of Energy to find unknown current
(assume you dont know KCL)
0__ VSABSISABSABS PPP
10 VoltsIs = 5A
+
-
IVS=?
PABS_IS = -(5A10V) = - 50 Watts
PABS_VS = - PABS_IS = -( - 50 Watts) = 50 Watts
PABS_VS = IVSVS
IVS = = 50W/10V = 5 Amps
Find IVS
S
VSABS
V
P _
+
-
10V
-
10V
+
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Resistors in Series
In the circuit to the right, we wish to replace
resistors R1, R2, and R3 with one
Equivalent resistance!
For resistors in series:
RTOTAL=R1+R2+R3
N
N
i
iTOTAL RRRRR ...21
1
+
R1 R2
VS R3
Node A
Node B
+
VS RTOTAL
A
B
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Resistors in Parallel
In the circuit to the right, we wish to replace
resistors R1, R2, and R3 with one
Equivalent resistance!
For resistors in parallel:
Notation: R1//R2//R3
Note: if we had just two resistors R1 and R2 in parallel,
we could then apply the product-sum rule, that is:
NN
i i
TOTAL
RRR
R
R
/1.../1/1
1
1
1
21
1
+
R1 R3
VS R2
321 /1/1/1
1
RRRRTOTAL
Node A
Node B
+
RTOTAL
A
B
VS
21
2*1
RR
RRRTOTAL
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Introduction to Current Divider
Is R2R1
I1 I2
R3
I3
How do we findI1,I2, andI3?
VS
+
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KCL: IS= I1 +I2 +I3 ,1
1
R
VI
S ,
2
2R
VI
S
3
3
R
VI
S
IsR2 VS
+
R1
I1 I2
R3
I3
321321
111
RRRV
R
V
R
V
R
VI S
SSSS
321
111
1
RRR
IV SS
Solve for Vs
But we know:
+
VS
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IsR2 VS
+
R1
I1 I2
R3
I3+
VS
321
111
1
RRR
IV SS
Current Division
Equation for the above
circuit topology
321
1
11
1
111
1
1
RRR
RIVRR
VI SSS
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Current Divider
This leads to a general current divider equation for N parallel
resistors
The above equation assumes that source current and
current through the circuit element flow in oppositedirections (one into the node, one out of the node)
N
i i
j
Sj
R
RII
1
1
1
C Di id Diff O i i f
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Current DividerDifferent Orientations of
element currents
BA
ASB
RR
RII
Is RBRA
IA IB
VS
+
BA
BS
BA
ASA
RR
RI
RR
RII
11
1
IC
ID
BA
BSC
RR
RII
BA
ASD
RR
RII
But, if we define the currents in the opposite direction we get:
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(KVL) Kirchhoffs Voltage Law
*Sum of voltages around a closed path (loop) in a circuit
is zero.A closed pathmove from point to point, only the first
and last points repeat.
Voltage Polarity Conventionwhen using KVL
A voltage encountered from + to - is positive
A voltage encountered from - to + is negative
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KVL
+
-
+
+
+
+
+
-
-
--
-
+
-
V1V2V3
V5V4
V6V7
A
F
C
B
D
E
Closed Path:
A B C D E A+V1 +V6 +V5 V4 V3 = 0
Another Closed Path:
E A F C D E-V3 -V2 +V7 +V5 V4 = 0
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KVL
+
-
+
+
-
-
-V1
V3 V2
A
C
BD
Closed Path:
B C D A B+(V2 )(V3)(-V4)+(V1) = 0
Use parenthesis, especially for
negative voltage variablesV4
andV1.
-V4+
-
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KVL Example 1
38
Clockwise Starting at A:
+ V1V2 + (- V3) = 0+(2V) -(V2) +(-(8V)) = 0
V2 = - 6V
V3 = 8 Volts
V1 = 2 Volts
find V2
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KVL Example 2
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36 V
20
10
+
+ -
-
12 V
V2
Clockwise Starting at the bottom node:
- 36V +12V - V2 = 0
V2 = - 24 V
find V2
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KVL Example 3
find VZ
Clockwise Starting at positive terminal of 10 V:
+10V -5V -12V + VZ = 0
VZ = 12V + 5V -10V = 7V