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    1

    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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    2

    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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    3

    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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    4

    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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    5

    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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    6

    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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    14

    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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    15

    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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    16

    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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    17

    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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    23

    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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    24

    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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    28

    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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    29

    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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    30

    Introduction to Current Divider

    Is R2R1

    I1 I2

    R3

    I3

    How do we findI1,I2, andI3?

    VS

    +

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    31

    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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    32

    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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    33

    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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    34

    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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    35

    (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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    37

    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

    39

    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