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 Lecture 1 1. Combi nations of Resist ors, Ki rch hoff ’s Rules Outline: Resistor Circuits. Voltage and Current Sources. Voltmeters and Ammeters. Kirchhoff’s Rules. Lecture 10: Batteries: the potential energy of charge carriers is increased by non- electrost atic (non-conservativ e) forces. Non-ideal batteries: internal resistance. Potential distribution around a complete circuit. Energy and power in electric circuits. 1 = ℰ  

L11 Connection of Resistors Kirchhoff Rules

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  • Lecture 11. Combinations of Resistors, Kirchhoffs Rules

    Outline:

    Resistor Circuits. Voltage and Current Sources. Voltmeters and Ammeters. Kirchhoffs Rules.

    Lecture 10: Batteries: the potential energy of charge carriers is increased by non-electrostatic (non-conservative) forces. Non-ideal batteries: internal resistance. Potential distribution around a complete circuit. Energy and power in electric circuits.

    1

    =

  • More Complex Circuits

    8

    1 = 13 + 13 + 13 1 = 1 2 = 1 21 + 2 + 13 = 1 2 5 = 1 + 1 = 2 4 2 5 = 1 21 + 2 = 23 3 4 2 5 = 23 + 13 = 1

    = 1 3 4 2 5 = 1 11 + 1 = 0.5

    3 3 3 1 1

    1 2 1/3

    1/3 3 3 3

    1 1

    1 2 1/3

    1/3

    R1

    R2

    R3

    R4

    R5

    = 100.5 = 20 = = 200

  • Voltage Source

    10

    The goal: to provide output voltage that is independent of the load resistance.

    An ideal voltage source:

    A. has zero internal resistance (zero means that > all possible values of load ).

    = +

  • Current Source

    12

    The goal: to provide output current that is independent of the load resistance.

    An ideal current source:

    A. has zero internal resistance (zero means that > all possible values of load ).

    = +

  • Voltmeters and Ammeters

    13

  • Voltmeters

    15

    The goal: to measure the voltage difference across an element (ideally, without affecting the circuit due

    to the voltmeter connection).

    An ideal voltmeter:

    Voltmeter: high internal resistance

    V

    V

    A. has = and should be connected in parallel with the circuit element being measured.

    B. has = and should be connected in series with the circuit element being measured.

    C. has = and should be connected in parallel with the circuit element being measured.

    D. has = and should be connected in series with the circuit element being measured.

  • Battery Tester

    16

    typical Rload

    Can we use a voltmeter (very

    high r) to test the freshness of a

    battery?

    The voltmeter will measure provided . But can be as high as 106 107 , and even if ~103 104 , we wont notice the battery

    aging.

  • Ammeters

    18

    The goal: to measure the current in a circuit element (ideally, without affecting the current due to the

    ammeter connection).

    An ideal ammeter:

    Ammeter: low internal resistance

    I

    I

    A. has = and should be connected in parallel with the circuit element being measured.

    B. has = and should be connected in series with the circuit element being measured.

    C. has = and should be connected in parallel with the circuit element being measured.

    D. has = and should be connected in series with the circuit element being measured.

  • Kirchhoffs Junction Rule

    19

    Junction Rule (for currents): charge conservation

    = 0 Currents flowing in + Currents flowing out -

  • Kirchhoffs Loop Rule

    20

    Loop Rule (energy conservation):

    = 0

    +

    = 0 for any closed loop

    if we neglect the difference between s and s, and accept the sign conventions.

    :

  • Example

    21

    We dont need to know the actual direction of the current: if we get the negative value of I, that would mean that the current flows in the direction opposite to the direction of travel.

    +

    = 0 4 + 12 7 + 2 + 3 + 4 = 0

    = 816 = 0.5

  • Example (contd)

    22

    a reference voltage =0

    V

    4 7

    2 3

    4V 12V

  • More Examples

    25

    Problem 26.77: (a) what is the potential difference Vab when the switch is open? (b) What is the current through the switch when the switch is closed? (c) What is the equivalent resistance when the switch is closed?

    6

    3 6

    3 3

    = 36 6 4 = 12 (a) = 369 = 4 = 36 3 4 = 24

    = 12 24 = 12

  • More Examples (contd)

    26

    Problem 26.77: (b) What is the current through the switch when the switch is closed?

    loop 1: 36 6 1 3 1 3 = 0 loop 2: 6 1 3 3 + 3 2 = 0 loop 3: 3 1 3 + 6 2 + 3 + 3 3 = 0 1 2

    3 + 3 = 2 21

    3 1 + 12 3 + 6 2 = 0 (from Eq.2) (from Eq.3) 3 1 + 12 2 24 1 + 6 2 = 0 2 = 32 1 36 6 1 3 1 + 3 2 21 = 36 10.5 1 = 0

    1 = 3610.5 3 = 32 1 21 = 0.51 3 = 1810.5 = 1.71 - means that our initial direction of I3 has to be reversed.

    6

    3 6

    3 3

    (b) Choose (arbitrary) directions of currents and travel along the loops.

  • More Examples (contd)

    27

    Problem 26.77: (a) what is the potential difference Vab when the switch is open? (b) What is the current through the switch when the switch is closed? (c) What is the equivalent resistance when the switch is closed?

    1 2

    3 + 2 = 32 1 = 1 + 2

    1 = 3610.5

    6

    3 6

    3 3

    (c) =

    8.6 = 368.6 = 4.2

  • Conclusion

    28

    Next time: Lecture 12: RC circuits 26.4

    Resistors in Series and Parallel Voltmeters and Ammeters Kirchhoffs Rules

    Lecture 11. Combinations of Resistors, Kirchhoffs RulesIclicker QuestionIclicker QuestionIclicker QuestionIclicker QuestionIclicker QuestionIclicker QuestionMore Complex CircuitsVoltage SourceVoltage SourceCurrent SourceCurrent SourceVoltmeters and AmmetersVoltmetersVoltmetersBattery TesterAmmetersAmmetersKirchhoffs Junction RuleKirchhoffs Loop RuleExampleExample (contd)Iclicker QuestionIclicker QuestionMore ExamplesMore Examples (contd)More Examples (contd)ConclusionExample: Built-in Battery TesterMore Complicated Resistor CircuitsSlide Number 31