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Chapter 20: Circuits

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Title: Chapter 20: Circuits


1
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

2
Current and EMF
  • A few definitions
  • Circuit A continuous path made of conducting
    materials
  • EMF an alternative term for potential
    difference or voltage, especially when applied
    to something that acts as a source of electrical
    power in a circuit (such as a battery)
  • Current the rate of motion of charge in a
    circuit
  • Symbol I (or sometimes i).
  • SI units C/s ampere (A)

3
Current and EMF
  • Conventional current assumed to consist of the
    motion of positive charges.
  • Conventional current flows from higher to lower
    potential.

4
Current and EMF
  • Direct current (DC) flows in one direction around
    the circuit
  • Alternating current (AC) sloshes back and
    forth, due to a time-varying EMF that changes its
    sign periodically

5
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

6
Ohms Law and Resistance
  • The current that flows through an object is
    directly proportional to the voltage applied
    across the object
  • A constant of proportionality makes this an
    equation

7
Ohms Law and Resistance
  • The constant of proportionality, R, is called the
    resistance of the object.
  • SI unit of resistance ohm (W)

8
Ohms Law and Resistance
  • Resistance depends on the geometry of the object,
    and a property, resistivity, of the material from
    which it is made
  • Resistivity symbol r
  • SI units of resistivity ohm m (W m)

9
Ohms Law and Resistance
  • In most materials, resistivity increases with
    temperature, according to the materials
    temperature coefficient of resistivity, a
  • (resistivity is r0, and R R0, at temperature
    T0)
  • SI units of a (C)-1

10
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

11
Electrical Power
  • Power is the time rate of doing work
  • Voltage is the work done per unit charge
  • Current is the time rate at which charge goes by
  • Combining

12
Electrical Power
  • Ohms Law substitutions allow us to write several
    equivalent expressions for power
  • Regardless of how specified, power always has SI
    units of watts (W)

13
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

14
Alternating Current
  • EMF can be produced by rotating a coil of wire in
    a magnetic field.
  • This results in a time-varying EMF

time, s
peak voltage
frequency (Hz)
15
Alternating Current
16
Alternating Current
  • The time-varying voltage produces a time-varying
    current, according to Ohms Law

peak current
time, s
frequency (Hz)
17
Alternating Current
18
Alternating Current
  • Calculate the power

19
Alternating Current
20
Alternating Current
  • Calculate the power
  • Average power

21
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

22
Series Connection
  • A circuit, or a set of circuit elements, are said
    to be connected in series if there is only one
    electrical path through them.

23
Series Connection
  • A circuit, or a set of circuit elements, are said
    to be connected in series if there is only one
    electrical path through them.
  • The same current flows through all
    series-connected elements. (Equation of
    continuity)

24
Series Connection
  • A circuit, or a set of circuit elements, are said
    to be connected in series if there is only one
    electrical path through them.
  • The same current flows through all
    series-connected elements. (Equation of
    continuity)
  • A set of series-connected resistors is equivalent
    to a single resistor having the sum of the
    resistance values in the set.

25
Series Connection
26
Series Connection
  • Potential drops add in series.

27
Parallel Connection
  • A circuit, or a set of circuit elements, are said
    to be connected in parallel if the circuit
    current is divided among them.
  • The same potential difference exists across all
    parallel-connected elements.

28
Parallel Connection
29
Parallel Connection
  • What is the equivalent resistance?
  • The equation of continuity requires that I I1
    I2 I3

30
Parallel Connection
  • Applying Ohms Law

31
Series - Parallel Networks
  • Resistive loads may be so connected that both
    series and parallel connections are present.

32
Series - Parallel Networks
  • Simplify this network by small steps

33
Series - Parallel Networks
  • Continue the simplification

34
Series - Parallel Networks
  • Finally

35
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

36
Kirchoffs Rules and Circuit Analysis
  • The Loop Rule
  • Around any closed loop in a circuit, the sum of
    the potential drops and the potential rises are
    equal and opposite or
  • Around any closed loop in a circuit, the sum of
    the potential changes must equal zero.
  • (Energy conservation)

37
Kirchoffs Rules and Circuit Analysis
  • The Junction Rule
  • At any point in a circuit, the total of the
    currents flowing into that point must be equal to
    the total of the currents flowing out of that
    point.
  • (Charge conservation equation of continuity)

38
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

39
Internal Resistance
  • An ideal battery has a constant potential
    difference between its terminals, no matter what
    current flows through it.
  • This is not true of a real battery. The voltage
    of a real battery decreases as more current is
    drawn from it.

40
Internal Resistance
  • A real battery can be modeled as ideal one,
    connected in series with a small resistor
    (representing the internal resistance of the
    battery). The voltage drop with increased
    current is due to Ohms Law in the internal
    resistance.

41
Chapter 20 Circuits
  • Current and EMF
  • Ohms Law and Resistance
  • Electrical Power
  • Alternating Current
  • Series and Parallel Connection
  • Kirchoffs Rules and Circuit Analysis
  • Internal Resistance
  • Capacitors in Circuits

42
Capacitors in Circuits
  • Like resistors, capacitors in circuits can be
    connected in series, in parallel, or in
    more-complex networks containing both series and
    parallel connections.

43
Capacitors in Parallel
  • Parallel-connected capacitors all have the same
    potential difference across their terminals.

44
Capacitors in Series
  • Capacitors in series all have the same charge,
    but different potential differences.

V1
V2
V3
45
RC Circuits
  • A capacitor connected in series with a resistor
    is part of an RC circuit.
  • Resistance limits charging current
  • Capacitance determines ultimate charge

46
RC Circuits
  • At the instant when the circuit is first
    completed, there is no potential difference
    across the capacitor.
  • At that time, the current charging the capacitor
    is determined by Ohms Law at the resistor.

47
RC Circuits
  • In the final steady state, the capacitor is fully
    charged.
  • The full potential difference appears across the
    capacitor.
  • There is no charging current.
  • There is no potential difference across the
    resistor.

48
RC Circuits
  • Between the initial state and the final state,
    the charge approaches its final value according
    to
  • The product RC is the time constant of the
    circuit.

49
RC Circuits
R 100 KW C 10 mF (RC 1 s) V 12 V
50
RC Circuits
  • During discharge, the time dependence of the
    capacitor charge is

51
RC Circuits
R 100 KW C 10 mF (RC 1 s) V 12 V
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