Capacitors - PowerPoint PPT Presentation

About This Presentation
Title:

Capacitors

Description:

Chapter 10 Capacitors & Capacitance – PowerPoint PPT presentation

Number of Views:279
Avg rating:3.0/5.0
Slides: 31
Provided by: emate
Category:

less

Transcript and Presenter's Notes

Title: Capacitors


1
  • Chapter 10
  • Capacitors Capacitance


2
  • 10.1 Capacitance (p. 386)
  • Capacitor
  • Consists of 2 conductors separated by an
    insulator.
  • Basic form parallel-plate capacitor Fig. 10-1,
    page 386 which consists of two metal plates
    separated by dielectric (e.g. air).
  • Charging capcitor
  • When DC source is connected to two metal plates
    Fig. 10-2, page 386, electrons are removed from
    ve plate and an equal number of electrons will
    be deposited on -ve plate.
  • This leaves top plate positively charges and
    bottom plate negatively charged.
  • Capacitor can store charge, i.e. remains charged
    after DC source is removed.


3
  • Discharging Capacitor
  • By shorting a wire/resistor across the two leads.
  • Definition of Capacitance
  • Charge stored depends on applied voltage
  • Q CV or C Q/V unit Farads, F
  • C is defined as the capacitance of the capacitor
  • Example 10-1, page 387
  • a. How much charge is stored on a 10-?F
    capacitor when it is connected to
  • a 24-volt source?
  • b. The charge on a 20-nF capacitor is 1.7 ?C.
    What is its voltage?
  • Solution
  • a. From Equation 10-1, Q CV. Thus, Q (10 x
    10-6 F)(24 V) 240 ?C.
  • b. Rearranging Equation 10-1, V Q/C (1.7 x
    10-6 C)/(20 x 10-9 F) 85 V.


4
  • 10.2 Factors Affecting Capacitance (p. 387)
  • Effect of area
  • The more charge put on a capacitors plate for a
    given voltage, the greater will be its
    capacitance.
  • Capacitance is directly proportional to plate
    area. Fig. 10-4, page 387
  • Effect of Spacing
  • As space between plated decreases, the force of
    attraction increases and pulls more electrons
    from one plate to other.
  • Capacitance is inversely proportional to plate
    spacing.
  • Effect of Dielectric
  • Capacitance varies for different materials Table
    10-1, page 388.
  • This factor is called relative dielectric onstant
    or relative perrmittivity of a material Fig.
    10-6, page 388


5
  • Capacitance of a Parallel Capacitor (p. 389)
  • C ? A / d (F)
  • A plate area
  • d spacing
  • ? absolute dielectric constant (F/m)
  • For air or vacuum, ? ? o 8.85 x 10-12 F/m
  • Other materials, ? expressed as the product of
    the relative dielectric constant,
  • ? r times ? o , i.e. ? ? o ? r


6
  • Example 10-3, page 389
  • A parallel-plate capacitor with air dielectric
    has a value of C 12 pF. What is the
    capacitance of a capacitor that has the
    following
  • a. The same separation and dielectrric but
    five times the plate area?
  • b. The same dielectric but four times the
    area and one fifth the plate spacing?
  • c. A dry paper dielectric, six times the
    plate area, and twice the plate spacing?
  • Solution
  • a. Since the plate area has increased by a
    factor of five and everything else remains
  • the same, C increases by a factor of five.
    Thus, C 5(12 pF) 60 pF.
  • b. With four times the plate area, C increases
    by a factor of four. With one fifth the
  • plate spacing, C increases by a factor
    of five. Thus, C (4)(5)(12pF) 240 pF.
  • c. Dry paper increases C by a factor of 2.2.
    The increases in plate area increases
  • C by a factor of six. Doubling the plate
    spacing reduces C by one half. Thus,
  • C (2.2)(6)(½)(12 pF) 79.2 pF.


7
  • Quiz
  • For a given capacitor, it stores Q1 charges
    when voltage V1 applied across its two ends. It
    will store Q2 charges when voltage V2 applied
    across its two ends.
  • If V1 10V and V2 5V, Q1 is greater than
    Q2 by 2?C. Find the a capacitance of the
    capacitor.


8
  • 10.3 Electric Fields (p. 390)
  • Electric flux
  • Electric fields are force fields that exist in
    the region surrounding charged bodies. Fig.
    10-8, page 391
  • The direction of the field is defined as the
    direction of force on a positive charge. It is
    directed outward from the ve charge and inward
    toward the -ve charge.
  • Field lines never cross and density of lines
    indicates the strength of the field.
  • Fig. 10-8 (a) Field about a pair of
    positive and negative charges
  • (b) Field of parallel plate capacitor


9
  • Electric field of parallel-plate capacitor is
    uniform across the gap with some fringing near
    edges.
  • Electric flux lines are represented by
  • Electric Field Intensity, ?
  • Strength of an electric field, i.e. force that
    the field exerts on a small, ve test charge, Qt
  • ? F / Qt unit newtons / coulomb (N/C)
  • F Q Qt / (4 ? ? r2) for a point charge, Q
  • Hence ? Q / (4 ? ? r2)


10
  • Electric Flux Density, D (p. 391)
  • represent the density fo flux lnes in space
  • independent of the medium
  • D ? ?
  • or D Total flux / area
  • ? / A
  • The number of flux lines emanating from a charge
    is equal to the charge itself, i.e. ? Q
  • Figure 10-9 - In the SI system, total flux ?
    equals charge Q. page 392


11
  • Figure 10-10 - Work moving test charge Qt is
    force times distance. page 392
  • Work required to move the charge against the
    force (F) through distance (d)
  • W F d
  • Define voltage, V W / Qt for a test charge Qt
  • F d / Qt
  • ? V / d as ? F / Qt
  • i.e. electric field strength between capacitor
    plates
  • voltage across the plates divided by the
    distance between them.


12
  • Capacitance, C Q / V
  • ? / V
  • A D / ?d
  • (D / ?) (A / d)
  • ? A / d
  • EXAMPLE 10-4, page 392 Suppose that the
    electric field intensity between the plates of a
    capacitor is 50 000 V/m when 80 V is applied
  • a. What is the plate spacing if the dielectric
    is air? If the dielectric is
  • ceramic?
  • b. What is ? if the plate spacing is halved?
  • Solution
  • a. ? V/ d, independent of dielectric. Thus, d
    V/? 80V/50x103V/m
  • 1.6x10-3 m
  • b. Since ? V/d, will double to 100 000 V/m.


13
  • 10.4 Dielectrics (p. 393)
  • Voltage breakdown
  • If voltage applied across capacitor is increased
    beyond a critical value, force on electronics is
    so great that they are torn from orbit.
  • This is called dielectric breakdown.
  • Electric field intensity at breakdown is called
    dielectric strength of a material. E.g. air
    3kV / mm
  • Table 10-2, page 393
  • MATERIAL kV/mm
  • Air 3
  • Ceramic (high ?r) 3
  • Mica 40
  • Mylar 16
  • Oil 15
  • Polystyrene 24
  • Rubber 18
  • Teflon 60


14
  • Voltage rating
  • because of dielectric breakdown, capacitors are
    rated for max operating voltage (called working
    voltage).
  • EXAMPLE 10-5, page 394 A capacitor with plate
    dimensions of 2.5 cm by 2.5cm and a ceramic
    dielectric with ? r 7500 experiences breakdown
    at 2400 V. What is C?
  • Solution From Table 10-2 dielectric strength
    3 kV/mm. Thus, d 2400 V/3000 V/mm 0.8 mm 8
    x 10-4 m. So
  • C ?r ?o A/d
  • (7500) (8.85 x 10-12) (0.025m)2/(8x10-4m)
  • 51.9 nF


15
  • 10.5 Nonideal Effect (p. 394)
  • Leakage current
  • charged capacitor will discharge after
    disconnected from source
  • small leakage current will pass through
    dielectric when capacitor connected to a source.
  • Charge leaks through the dielectric Fig. 10-12,
    page 394
  • R hundreds of Mohm
  • Figure 10-12 - Leakage current. page 394


16
  • Equivalent series resistance
  • resistance (RS) may develop in capacitors leads
    as its internal connections begins to fail
  • cause problems in high-frequency circuits
  • dissipation factor
  • D RS / XC where XC 1/2?fC
  • Dielectric absorption
  • after shorting two leads of a capacitor, a
    residual voltage remains
  • Disadv. upset circuit voltage levels
  • Temperature coefficient
  • ve / zero / -ve temperature coefficient imply
    capacitance increases / no change / decreases
    with increasing temp.
  • in parts per million (ppm)

17
  • 10.6 Types of Capacitors (p. 395)
  • Fixed capacitor Fig. 10-13, 10-14, page 396
  • Variable capacitor Fig. 10-19, page 399
  • Figure 10-13 Stacked capacitor construction.
    The stack is compressed, leads attached, and
    the unit coated with epoxy resin or other
    insulting material.


18
  • Fixed capacitor
  • Ceramic
  • relative permittivity 30 to 7500
  • extremely high permittivity permit small
    packaging but characteristics vary wifely with
    temp. and operating voltage. Use in limited temp
    applications where small size and cost are
    important
  • many surface mount capacitors use ceramic
    dielectrics
  • Plastic film
  • film/foil Fig. 10-14, page 396 use metal foil
    use metal foil separated by plastic film
  • metallized-film have foil material vaccum
    deposited directly onto plastic film
  • Mica
  • low in cost with low leakage and good stability


19
  • Electrolytic
  • provide large apacitance up to hundred thousand
    microfarads
  • relatively low cost
  • leakage is relatively high and breakdown voltage
    is relatively low
  • Surface mount extremely small and provide high
    packaging density
  • Variable capacitor
  • used in radio tuning circuits
  • stationary plates and set of movable plates which
    are ganged together and mounted on a shaft
  • as shaft is rotated, the effective area change


20
  • 10.7 Capacitors in parallel and series
  • capacitors in parallel fig. 10-20, page 400
  • . Voltage is the same across each.


21
  • Example 10-6, page 401
  • Example 10-6 A 10-?F, a 15-?F, and a 100-?F
    capacitor are connected in parallel across a 50-V
    source. Determine the following
  • a. Total capacitance.
  • b. Total charge stored.
  • c. Charge on each capacitor.
  • Solution
  • a. Cr C1 C2 c3 10?F 15 ?F 100 ?F
    125 ?F
  • b. QT CTV (125 ?F)(50 V) 6.25 mC
  • c. Q1 C1V (10 . Q1 C1V (10 ?F)(50 V)
    0.5 mC)(50 V) 0.5 mC
  • Q2 C2V (15 ?F)(50 V) 0.75 mC
  • Q3 C3V (100 ?F)(50 V) 5.0 mC
  • Note Q1 Q2 Q3 (0.5 0.75 5.0) mC 6.25
    mC, which checks with (b).


22
  • Capacitors in series Fig. 10-21, page 401
  • Charge is the same on each.


23
  • EXAMPLE 10-7 (p. 402)
  • Refer to Figure 10-22(a)
  • a. Determine Cr .
  • b. If 50 V is applied across the capacitors,
    determine Q.
  • d. Determine the voltage on each capacitor.
  • Solution
  • a. 1/Cr 1/C1 1/C2 1/C3 1/30µF 1/60µF
    1/20µF
  • 0.0333 x 106 0.0167 x 106 106 0.1 x 106
  • Therefore,
  • Cr 1/(0.1 x 10-6) 10 ?F
  • b. Q CTV (10 x10-6F)(50 V) 0.5 mC
  • c. V1 Q/C1 (0.5 x 10-3 C) / (30 x 10-6F)
    16.7V
  • V2 Q/C2 (0.5x10-3C)/(60x10-6F) 8.3V
  • V3 Q/C3 (0.5x10-3C)/(20x10-6F) 25.0V


24
  • EXAMPLE 10-8 page 403
  • For the circuit of Figure 10-23(a), determine CT
  • Refer to Figure 10-23 Systematic reduction.


25
  • Quiz Consider capacitors of 1?F, 1.5?F, and
    10?F. If equivalent capacitance is equal to
    10.6?F. How are the capacitors connected?
  • Solution
  • To yield 10.6 ?F, the 10 ?F capacitor must be
    connected in parallel with some combination of
    the 1 ?F and 1.5?F capacitors. Only the
    connection shown below works.
  • 10.8 Capacitor current and voltage page 404
  • (Refer to Fig. 10-25, page 405)
  • During charging
  • movement of electrons constitutes current
  • current lasts for capacitor to be charged
  • no current pass through dielectric
  • capacitor voltage builds as charge deposited on
    plates
  • as capacitor voltage increases, charging current
    decreases


26
  • Capacitor V-1 relationship, page 405
  • q C VC
  • ic dq / dt d (C VC) / dt
  • ic C d Vc / dt
  • Current through a capacitor is equal to C times
    the rate of change of voltage across it.
  • Example 10-9 page 406 A signal generator
    applies voltage to a 5-µF capacitor with a
    wavefrom as in Figure 10-27(a). The voltage
    rises linearly from 0 to 10V in 1ms, falls
    linearly to -10V at t3ms, remains constant until
    t4ms, rises to 10V at t5ms, and remains
    constant thereafter.
  • a. Determine the slope of vc.
  • b. Determine the current and sketch its graph.


27
  • Solution
  • a. We need the slope of vc during each time
    interval where slope rise/run ? v/?t.
  • 0 ms to 1 ms ?v 10 V ?t 1 ms Therefore,
    slope 10 V/1 ms 10 000 V/s.
  • 1 ms to 3 ms Slope -20 V/2 ms -10 000 V/s.
  • 3 ms to 4 ms Slope 0 V/s.
  • 4 ms to 5 ms Slope 20 V/1 ms 20 000 V/s.
  • b. ic Cdvc/dt C times slope. Thus,
  • 0 ms to 1 ms i (5 x 10-6F) (10 000 V/s) 50
    mA.
  • 1 ms to 3 ms i -(5 x 10-6F) (10 000 V/s)
    -50 mA.
  • 3 ms to 4 ms i (5 x 10-6F) (0 V/s) 0 mA.
  • 4 ms to 5 ms i (5 x 10-6F) (20 000 V/s) 100
    mA.
  • Refer to Figure 10-27, page 406


28
  • 10.9 Energy stored by a capacitor page 407
  • an ideal capacitor does not dissipate power
  • when power is transferred to a capacitor, all of
    it is stored as energy in the capacitors
    electric field
  • Stored energy, W 1/2 C V2
  • 10.10 Capacitor failures and troubleshooting
    page 408
  • Failures
  • short internally
  • leads open
  • dielectric leaky
  • (Noted if electrolytic capacitor is connected
    with its polarity reversed, it may explode.)


29
  • Capacitors fail because of
  • misapplication
  • excessive voltage, current, or temperature
  • aging
  • Basic testing with an ohmmeter
  • out-of-circuit tests with analog ohmmeter
  • - detect opens and shorts
  • - leaky dielectrics
  • (Noted discharge capacitor first before
    measurement)
  • for normal capacitor, the ohmmeter reading should
    be low initially and gradually increase to
    infinity.


30
  • Capacitor testers page 408
  • some digital multimeter can measure capacitance
  • LCR (inductance, capacitance, resistance)
    analyzer can determine capacitance as well as
    detect opens and short

Write a Comment
User Comments (0)
About PowerShow.com