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2 EE462L Triac Light Dimmer PPT

Date post: 14-Apr-2018
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    EE462L, Fall 2012

    Triac Light Dimmer

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    Triac Light Dimmer

    Triac(front view)

    MT1 MT2 G

    +Van

    (from Variac)

    Lightbulb

    G

    MT2

    MT1

    0.1F

    3.3k

    250klinear pot

    Triac

    Bilateraltrigger diode

    (diac)

    a

    c

    n

    b

    Lightbulba

    n

    b

    Before firing , the triac is an openswitch, so that practically no voltageis applied across the light bulb. Thesmall current through the 3.3kresistor is ignored in this diagram.

    + 0V +Van

    +Van

    Ingenious

    Simple

    Efficient

    Inexpensive

    After firing , the triac is a closedswitch, so that practically all of V an is applied across the light bulb.

    Lightbulba

    n

    b

    + Van +Van

    +0V

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    Triac Open

    Light bulb resistance is a few ohms when cold, and about 100- 200when bright (use to get light bulb resistance R)R V P rm s /

    2

    The light bulb resistance is small compared to the 3.3k andpotentiometer combination and can be ignored when analyzing theRC electronic circuit

    When the voltage across thediac reaches about 35V, itself-fires and its voltagecollapses to about 5V

    The circuit resets and the process repeats every half-cycle of 60Hz

    Capacitor dischargesinto triac gate

    +Van

    (from Variac)

    Lightbulb

    0.1F

    3.3k

    250klinear

    pot Bilateraltrigger diode

    (diac)

    Triac Closed

    +Van

    (from Variac)

    Lightbulb

    0.1F

    3.3k

    250klinear

    pot Bilateraltrigger diode

    (diac)

    !

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    Flat rubber washers between#8 x 1 screws and porcelain

    Removethis

    center screw

    #6-32, machine screw,flat washer, split washer, andhex nut

    #8 x 3/4screws for terminal blocks

    #8 x screwsfor corner

    brackets

    The potentiometer is connected so that turning it clockwise lowers the resistanceof the firing circuit, fires the triac sooner, and makes the light brighter

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    5

    The back of the triac fitsfirmly against the heat sink,

    with maximum surfacecontact. The flat washer,

    then split washer, then hexnut fit on the other side of the

    corner bracket.

    Removethis

    center screw

    9.6C rise above ambientair per Watt

    To make it easy to connect an oscilloscope

    probe, it helps to put an extra spadeconnector, bent upwards at a 90 angle,under the back terminal block screws

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    Hookup

    Isolation transformer

    Variac (plugged intoisolation transformer)

    Light dimmer

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    Connection to Variac

    Light dimmer connected to black

    and white terminal posts

    Variac knob set to zero

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    No-Firing Condition Actual

    When potentiometer resistance is large, there is no firing because thecapacitor voltage never exceeds (positive or negative) the diacbreakover voltage

    Variac voltage

    Capacitor voltage

    Capacitor voltage lags variac voltage almost 90 for large

    potentiometer resistance

    !

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    No-Firing Condition Simulated(EE362L_Triac_Light_Dimmer.xls)

    Fixed Potentiometer Diac DiacSource Freq R kohm C breakover on voltsVrms Hz kohm uF V V

    70 60 3.3 96 0.1 35 5

    Denom-mag3.874785

    Denom-ang75.0439

    VCrms18.06552

    VCang-75.0439

    Tau0.00993

    -150

    -100

    -50

    0

    50

    100

    150

    0 30 60 90 120 1 50 180 2 10 240 270 3 00 330 3 60

    Angle

    V o

    l t a g e

    Source voltage Capacitor voltage Diac breakover

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    Firing Condition Actual

    Capacitor voltage Vcn does not go into steady state AC right away asVan crosses the zero axis. There is a time delay due to the RC timeconstant.

    The RC time constant delay plus phase shift of the AC solution for

    Vcn determines the point at which the diac breakover is achieved

    Van Vcn

    = 90 16.67ms 4

    Diac conducts when V cn reaches 32-35V (diac

    breakover voltage). Thecapacitor then dischargesthrough the triac gate.

    !

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    Firing Condition Simulated(EE362L_Triac_Light_Dimmer.xls)

    Fixed Potentiometer Diac DiacSource Freq R kohm C breakover on voltsVrms Hz kohm uF V V

    70 60 3.3 49 0.1 35 5

    Denom-mag2.210759

    Denom-ang63.10652

    VCrms31.66333

    VCang-63.1065

    Tau0.00523

    -150

    -100

    -50

    0

    50

    100

    150

    0 30 60 90 120 1 50 1 80 2 10 2 40 270 3 00 3 30 3 60

    Angle

    V o

    l t a g e

    Source voltage Capacitor voltage Diac breakover

    EE362L_Triac_Light_Dimmer.xlsVan and V cn waveforms with

    potentiometer adjusted for = 90

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    0 30 60 90 120 150 180 210 240 270 300 330 360

    Angle

    C u r r e n t

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    0 30 60 90 120 150 180

    Alpha

    P

    22sin

    12 ,2

    , rmsanrmsabV V

    0 30 60 90 120 150 180 210 240 270 300 330 360

    Angle

    C u r r e n

    t

    0 30 60 90 120 150 180 210 240 270 300 330 360

    Angle

    C u r r e n t

    Power to Light (per unit of sinewave,i.e., = 0)

    !

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    Remember to Calibrate Your Scope Probe

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    Measuring the dB difference between 60Hz and 180Hzcomponents of V ab

    60Hz component

    180Hz component

    100Hz

    Save screensnapshot #3

    Vrms

    V

    dbHz

    1log2081.3260

    10

    2081.32

    60 101VrmsV Hz

    Vrms

    V db Hz

    1log2087.26 18010

    2087.26

    180 101VrmsV Hz

    = 43.7Vrms

    = 22.1Vrms

    Magnitude of Voltage Harmonics Depends on Alpha !


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