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Title: Lesson 14


1
Lesson 14 Capacitors Inductors
2
Learning Objectives
  • Define capacitance and state its symbol and unit
    of measurement.
  • Predict the capacitance of a parallel plate
    capacitor.
  • Analyze how a capacitor stores energy.
  • Define inductance and state its symbol and unit
    of measurement.
  • Predict the inductance of a coil of wire.
  • Analyze how an inductor stores energy.

3
CAPACITORS AND INDUCTORS
  • For resistive circuits, the voltage-current
    relationships are linear and algebraic. Resistors
    can only dissipate energy they cannot store
    energy and return it to a circuit at a later
    time.
  • This is not the case for capacitors and
    inductors. Capacitors and inductors are dynamic
    elements.
  • The voltage-current relationships are non-linear
    and differential.
  • They are dynamic because they store energy.

4
Capacitor
  • A capacitor is passive element designed to store
    energy in its electric field. This energy can
    then be provided to a circuit at a later time.
  • Capacitors consist of two conductors (parallel
    plates) separated by an insulator (or
    dielectric).
  • Capacitors accumulate electric charge.
  • Conductive plates can become charged with
    opposite charges

5
Capacitor
  • Electrons are pulled from top plate (creating
    positive charge)
  • Electrons are deposited on bottom plate (creating
    negative charge)

6
Capacitor
  • While charging a capacitor
  • The voltage developed across the capacitor will
    increase as charge is deposited
  • Current goes to zero once the voltage developed
    across the capacitor is equal to the source
    voltage

7
Definition of Capacitance
  • Capacitance of the capacitor is a measure of the
    capacitors ability to store charge.
  • Unit is the farad (F).
  • Capacitance of a capacitor (C)
  • Is one farad if it stores one coulomb of charge
    when the voltage across its terminals is one volt

8
Effect of Geometry
  • Increased surface area means increased
    Capacitance
  • Larger plate will be able to hold more charge

9
Effect of Geometry
  • Reduced separation distance means increased
    Capacitance
  • As plates are moved closer together
  • Force of attraction between opposite charges is
    greater
  • Capacitance
  • Inversely proportional to distance between plates

10
Effect of Dielectric
  • Substituting a dielectric material for the air
    gap will increase the Capacitance
  • Dielectric Constant ? epsillon is calculated by
    using the relative dielectric constant and the
    absolute dielectric constant for air
  • ? ?r ?0 (F/m)
  • where ?0 8.854 x 10-12 F/m

11
Capacitance of Parallel-Plates
  • Putting the factors together, capacitance of
    parallel-plate capacitor is given bywhere ?r
    is the relative dielectric constant ?0 8.854
    x 10-12 F/m
  • A is area d is the distance between plates

12
Example Problem 1
  • A parallel-plate capacitor with a vacuum
    dielectric has dimensions of 1 cm x 1.5 cm and
    separation of 0.1 mm. What is its capacitance?
  • What would its capacitance be if the dielectric
    were mica?

13
Dielectric Voltage Breakdown
  • High voltage will cause an electrical discharge
    between the parallel plates
  • Above a critical voltage, the force on the
    electrons is so great that they become torn from
    their orbit within the dielectric
  • This damages the dielectric material, leaving
    carbonized pinholes which short the plates
    together

14
Dielectric Voltage Breakdown
  • The working voltage is the maximum operating
    voltage of a capacitor beyond which damage may
    occur
  • This voltage can be calculated using the
    materials dielectric strength K (kV/mm)

Dielectric Strength (K) Dielectric Strength (K)
Material kV/mm
Air 3
Ceramic (high ?r) 3
Mica 40
Myler 16
Oil 15
Polystyrene 24
Rubber 18
Teflon 60
15
Capacitance and Steady State DC
  • In steady state DC, the rate of change of voltage
    is zero, therefore the current through a
    capacitor is zero.
  • A capacitor looks like an open circuit with
    voltage vC in steady state DC.

16
CAPACITORS IN SERIES AND IN PARALLEL
  • Capacitors, like resistors, can be placed in
    series and in parallel.
  • Increasing levels of capacitance can be obtained
    by placing capacitors in parallel, while
    decreasing levels can be obtained by placing
    capacitors in series.

17
CAPACITORS IN SERIES AND IN PARALLEL
Capacitors in series are combined in the same
manner as resistor sin parallel.
Capacitors in parallel are combined in the same
manner as resistors in series.
18
Power and work
  • The energy (or work) stored in a capacitor under
    steady-state conditions is given by

19
Inductor
  • An inductor is a passive element designed to
    store energy in its magnetic field.
  • Inductors consist of a coil of wire, often wound
    around a core of high magnetic permeability.

20
Faradays Experiment 4 Self-induced voltage
?
  • Voltage is induced across coil when i is
    changing.
  • When i is steady state, the voltage across coil
    returns to zero.

21
Faradays Law
  • From these observations, he concludedA voltage
    is induced in a circuit whenever the flux linking
    the circuit is changing and the magnitude of the
    voltage is proportional to the rate of change of
    the flux linkages.

22
EMF in an Inductor
23
Counter EMF
  • Induced voltage tries to counter changes in
    current so it is called counter emf or back
    voltage.
  • BEMF ensures that any current changes in an
    inductor are gradual.
  • An inductor RESISTS the change of current in a
    circuit
  • Acts like a short circuit when current is constant

24
INDUCTANCEInductor Construction
  • The level of inductance is dependent on the area
    within the coil, the length of the unit, to the
    number of turns of wire in the coil and the
    permeability of the core material.

25
Inductor calculations
  • Induced emf in an inductor can be calculated
  • L is the self-inductance of the coil. Units are
    Henry (H).
  • The inductance of a coil is one henry if changing
    its current at one ampere per second inducesa
    potential difference of one volt across the coil.

26
Example Problem 2
  • The current in a 0.4 H inductor is changing at
    the rate of 200 A/sec. What is the voltage across
    it?

27
Inductance and Steady State DC
  • In steady state DC, the rate of change of current
    is zero, therefore the induced voltage across an
    inductor is also zero.
  • An inductor looks like a short circuit in steady
    state dc.

28
INDUCTORS IN SERIES AND IN PARALLEL
  • Inductors, like resistors and capacitors, can be
    placed in series or in parallel.
  • Increasing levels of inductance can be obtained
    by placing inductors in series, while decreasing
    levels can be obtained by placing inductors in
    parallel.

29
INDUCTORS IN SERIES AND IN PARALLEL
  • Inductors in series are combined in the same way
    as resistors in series.
  • Inductors in parallel are combined in the same
    way as resistors in parallel.

30
Inductor Energy Storage
 
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