lamps electronic ballast

Upload: gamal-yones

Post on 03-Apr-2018

213 views

Category:

Documents


0 download

TRANSCRIPT

  • 7/29/2019 Lamps Electronic Ballast

    1/6

    High Efficiency Single-Stage Multi-Fluorescent

    Lamps Electronic Ballast

    Hung-Ching Lu and Te-Lung Shih

    Department of Electrical Engineering, Tatung University, Taiwan, R.O.C.

    Abstract- A single-stage electronic ballast topology with the

    properties of high efficiency and low stress is proposed in this

    paper. The ballast consists of a voltage fed half-bridge

    series-resonant series-parallel-load (SRSPL) inverter, playing the

    role of lamp driver, and a voltage boost converter, which shares

    low side switch device with half-bridge inverter and acts as

    power-factor-correction (PFC). The inverter of the ballast is

    loaded with resonant tanks which are designed and operated to be

    capacitive and inductive to theoretically achieve both of

    zero-voltage switching (ZVS) and zero-current switching (ZCS)

    that eliminate the reactive current circulating through the switches

    to prevent low switching and conduction losses. The boost

    converter of the ballast provides sufficient high voltage to ignite the

    lamp. In addition, prior to shaping the input current and reducing

    harmonic currents to ignite the lamp, a power factor correction

    stage is performed by the converter. The merit of a successive

    ignition of the lamps can be attained with proposed operation

    scheme so that current stress imposed on the switches can be

    reduced. The simulation results and experimental measurements

    are used to verify the theoretical prediction and analysis.

    Index Terms:Single-Stage electronic ballast topology, Half-bridge

    Series-resonant series-parallel-load (SRSPL) Inverter, Power Factor

    Correction, Multi-Fluorescent Lamps Electronic Ballast

    I. INTRODUCTIONIn recent years, electronic ballast has played a very important

    role in lighting gears. In fluorescent lamp applications, the

    electronic ballast is used widely because of its several

    advantages. At high frequency operation, luminous efficacy of

    fluorescent lamps is operated higher than 60Hz [1] and long

    lamp life can be sustained. Most of the electronic ballast is

    realized by resonant inverter operating at high frequency to

    provide a sufficient high voltage to ignite the lamp and limit the

    current. In conventional multiple fluorescent lamp lightingsystem, each lamp is equipped with its own LC network to

    constitute a resonant tank. When all of the resonant tanks are

    designed to operate at the same frequencies as the LC network,

    the switching losses can be reduced; nevertheless, where

    relatively large current will generated and flow through the

    switches. This would also result in considerable conduction

    losses and undesired current stress. In addition, a

    power-factor-correction (PFC) circuit is attached to the ballast,

    for the purpose of reducing the input line current harmonics.

    The cost has increased when PFC stage cascade in front of

    DC-AC inverter. In order to reduce the cost of the electronic

    ballast, one single stage converter is used to perform both

    function of the PFC and the DC-AC conversion simultaneously.

    In this paper, a circuit operation scheme for multiple

    fluorescent lamp lighting system is proposed. The scheme is to

    operate all of the resonances for each resonant tank. By properly

    selecting the component values of the overall tanks, an

    equivalent resistive impedance of the overall tank can be derivedso as the switches can theoretically operate with both of

    zero-voltage switching (ZVS) and zero-current-switching

    (ZCS). Furthermore, conduction losses and current stress on the

    switches can be reduced significantly since no reactive current

    flows through switches. During startup transition, the lamps are

    subsequently ignited because of switching frequency is

    controlled to decrease monotonically. Hence, a small transition

    peak current, as compared to that in the conventional ballast

    system, will follow through switches during the glow-to-arc

    transition.

    The electronic ballast can be categorized systemically as dual

    stage and single stage. The dual stage electronic ballastcompresses three switches and two controllers to consist of

    AC-DC boost converter as PFC stage in front and DC-AC

    half-bridge Inverter. However, dual stage electronic ballast has

    better performance of power factor and current factor, where

    cost increased by result of more complex circuitry. Therefore,

    single stage electronic ballast was introduced to prevent the cost

    drawback of dual stage electronic ballast, which has one switch

    and one PFC controller of the boost converter can be omitted

    [2-5]. Where the integrated boost converter and half-bridge

    resonant inverter as shown in Fig. 1, in which boost converter is

    operating in both of discontinue/continue modes with fixed

    frequency and fixed duty cycle. The operating behavior is boostinductance current follow phase of input voltage to archive high

    power factor [6, 7].

    II. CIRCUIT OPERATIONIn this paper, work has been selected with four lamps in the

    ballast; however, it could be three, five, six, etc. Next, the basic

    multi-lamp requirements can be simply stated as follows:

    (1) While a lamp is added; it should be ignited and kept in

    1175

  • 7/29/2019 Lamps Electronic Ballast

    2/6

    operation independently and should not disturb the operation of

    other working lamps.

    (2) While a lamp is removed from the light system; other

    lamps should be kept in operation without interruption.

    Fig 1. The proposed topology of Single-Stage Multi-Fluorescent Lamps

    Electronic Ballast

    With the above assumptions, that simplified electronic ballast,

    explained as a half-bridge inverter, is used to supply the four

    lamps, the connections between the lamps and the converter

    have to be determined. But, before this discussion, it is

    necessary to review the characteristics of the fluorescent lamp

    firstly.

    These lamps have a negative dynamic resistance behavior

    which makes it necessary as the use of a ballast to limit the

    current. A lamp modeling development which can predict the

    fluorescent lamp electrical characteristics is necessary to do the

    simulation of electronic ballasts due to the fluorescent lamp

    nonlinear behavior. The lamp equivalent resistance of a

    fluorescent can be expressed as

    O SH

    lamp S

    O O H

    V RVR R

    I V V

    = + =

    (1)

    where VOas well asIO are the rms lamp voltage and current,RS

    and VHare defined as the parameters in the plasma model of

    lamp.

    The resonant tank design basin in [8] the method consists of

    choosing the correct phase angle of the LCC resonant circuit that

    will concern the lamp starting and the correct lamp power in

    steady state. This analysis has just done for one of the lamps, and

    the found values are repeated for all other ballast lamps.

    Then, the phase angle is determined by

    ( ) ( )1 1 1 2 2 2 2 2tan 1lamp S P lamp lamp P R L C C R R C = +

    (2)

    where 2S

    f = is the angular switching frequency, is

    resonant tank impedance phase angle.

    The half-bridge series-resonant series-parallel load resonant

    circuits take account of resonant frequency operating characters

    have both of capacitance and inductance, where parallel load

    being capacitance are provided voltage gain and generated high

    voltage with high equivalent lamp resistance to ignite the lamp.

    However, the series load has well current regulation with

    inductance characteristic, in which the voltage gain is reduced to

    decrease the output voltage. When the lamp has beensuccessively ignited; the resonant frequency will be decreased

    monotonically. Thus, the current stress imposed on the switches

    can be reduced.

    The voltage transfer function of the resonant circuit is given

    as

    2

    ( ) 1

    ( ) 1

    1

    11

    1

    lamp

    lamp P lamp

    lampin

    S P lamp

    PP

    S lamp S lamp

    R

    V j j C R

    RV jj L

    j C j C R

    C LLC j

    C R C R

    +

    =

    + +

    +

    =

    + +

    (3)

    The series resonant frequency and CPmore then CSderived as

    1S

    SLC = (4)

    The quality factor with (1) is

    lamp

    LCQR

    = (5)

    Take absolute value of (3) can be obtained as

    22 2

    2

    ( ) 1

    ( )

    1

    lamp

    in

    SP P

    S S S S

    V j

    V jC C

    QC C

    =

    + +

    (6)

    During lamp igniting with character of series parallel resonant,

    the lamp equivalent resistor can be considered as open circuit, (3)is used and the quality factor is close to zero, where ignite

    voltage can be determined as

    2

    2 1

    1

    dc

    strike

    PP

    S

    VV

    CLC

    C

    =

    +

    (7)

    And the lamp stable voltage has been ignited can be derived

    1176

  • 7/29/2019 Lamps Electronic Ballast

    3/6

    as

    ,22

    2

    2 1

    11

    in

    lamp rms

    PP

    S lamp S lamp

    VV

    C LLC

    C R C R

    =

    + +

    (8)

    Since operating frequency is 4 times of resonant frequency [5],

    the resonant tank series inductorL and isolation capacitor CS

    with operating frequency is expressed as

    2S

    S

    fLC

    = (9)

    The capacitorCPon the resonant circuit is sustained the lamp

    voltage during the lamp ignition,

    1P

    lamp

    CR

    = (10)

    Therefore, with given stable lamp voltage Vlapm,rms, input DC

    voltage Vdc and lamp equivalent resisterRlamp; the equations as

    mention above can be solved to obtain resonator inductorL,

    capacitorCSand ignition capacitorCP.

    The ballast is obtained from the integration of the boost

    converter design which considers output voltage is higher than

    input voltage, which provides minimum ignition voltage and

    operating voltage after lamp has ignited. The boost inductance

    current into switch device on each switching cycle can be

    obtained as of the boost converter and the half-bridge series

    resonant parallel-loaded inverter. The operation of the boost

    converter is in discontinued-current mode (DCM) providesunity power factor with constant frequency. In case of operating

    partial lamps, a high power factor at the line input terminal will

    be always retained. Thus, once the boost PFC stage is designed

    to operate at DCM with fixed switching frequency, the input

    current naturally follows the sinusoidal waveform of the ac line

    source, that switching current of each cycle on the switch device

    can be derived as

    2

    ( ) sin(2 )2

    m S

    in

    V D TI t ft

    L= (11)

    Furthermore, the input current and input voltage are operating

    in same phase, which not only accomplish high input power

    factor but also constraint total harmonic distortion of input

    current, where the input power can be determined as

    2

    0

    2 2

    1sin(2 ) ( ) (2 )

    2

    4

    in m in

    m

    P V ft I t d ft

    V D

    fL

    =

    =

    (12)

    With (11) the inductance of boost inductor can be derived as

    2 2

    4

    m

    in

    V DL

    fP L= (13)

    III. SIMULATIONSome simulations have been done in order to verify the

    multi-lamp arrangement behavior. To simulate, the fluorescent

    lamp have been assumed same as the equivalent resistance

    obtained from (1), the lamp as a resistor considered.

    Additionally, the AC line voltage, rectifier bridge, and filter

    capacitor have been used as a DC source, once that our aim is to

    verify the multi-lamp arrangement behavior.

    Simulation results are shown in Fig. 2, voltage in the lamps 1,

    2, 3, and 4, in relation to Fig. 1. We can see that the lamp voltage

    and switch voltage operation.

    Fig 2. Thelamp voltage and one of switch voltage operation.

    IV. EXPERIMENTAL RESULTSTo verify the predicted operation principles and theoretical

    analysis of the proposed high efficiency single-stage ballast for

    multiple fluorescent lamps, a laboratory electronic ballast of Fig.

    1 is designed and built. The input voltage is 110Vat 60Hz, and

    this circuit uses a dedicated integrated circuit TL494 to do the

    high-frequency command, which switching frequency is fixed at

    63kHz, and fixed duty 49.9%. Thus, the ballast can supply any

    number of lamps and its frequency will not suffer variation. The

    design parameters of circuit are shown in Table I.

    Some experimental results have been done in order to verify

    the experimental prototype behavior. The measured results are

    presented the input voltage and current waveforms under

    different operating conditions from single lamp, dual lamps and

    triple lamps to quad lamps are shown in Fig. 3. Experimental

    results are presented in Table. II. It is a prototype comparative

    table to the different lamp numbers (4, 3, 2, and 1). where results

    are illustrated of the input current is approximately sinusoidal

    and operating same phase with input voltage, the power factor

    1177

  • 7/29/2019 Lamps Electronic Ballast

    4/6

    measured shown in Table II, and conclude it over 0.95 for all

    lamps of experimental.

    TABLE I. PARAMETER OF CIRCUIT

    Designed Parameters

    Design Reference Designed Value

    1. Boost Inductor 1.1mH

    2. Isolate CapacitorCS 60nF

    3. Resonant CapacitorCP 3.5nF

    4. Resonant Inductor 2.1mH

    5. DC-link Capacitor 120uF

    6 TL Lamp T5 28W

    (a)

    (b)

    (c)

    (d)

    Vin50 V/divIin1 A/div time5 ms/div

    Fig. 3. The waveform of Input voltage and current, Driving (a) single lamp,

    (b)dual lamps, (c)triple lamps, and (d)quad lamps

    TABLE II. EXPERMINTAL RESULTS

    Number

    of lamps

    Single

    lamp

    Dual

    lamps

    Triple

    lamps

    Quad

    lamps

    Power

    Factor0.953 0.961 0.968 0.973

    The total ignition current ia for all lamps is 2.7A which is

    shown in Fig. 4; with this current we can determine the

    minimum rating of semiconductor switch device is 2.7A. In

    order to prevent from destroying the device, the safe operation

    rating of the MOSFET should be 5A or above. Next, Fig. 5

    shows voltage over one lamp during its ignition process, which

    maximum voltage is 827V. From these figures, it is possible to

    verify the correct operation of the proposed electronic ballast,

    during ignition and dimming control of the fluorescent lamps.Finally, Fig. 6.illustrates single lamp maximum start up current

    is 390mA.

    Iin1A/div time1 s/div

    Fig. 4. Four Lamps ignited current waveform

    0

    0

    Iin

    Vin

    Iin

    0

    Vin

    Iin

    Vin

    0

    Vin

    Iin

    0

    1178

  • 7/29/2019 Lamps Electronic Ballast

    5/6

    Vin200 V/div time5 ms/div

    Fig 5. Lamp ignited voltage waveform

    Iin100 mA/div time1 s/div

    Fig 6. Single Lamp ignited current waveform

    Fig. 7 shows the voltage and current waveforms through one

    fluorescent lamp during operation at the maximum lighting

    output condition. And Fig. 8 is shown the lamp 1, 2 and 3, 4 are

    operating symmetrically and in 180o

    opposite phase.

    Fig. 9 is illustrates the voltage cross of the switches and

    current waveform of boost inductor and resonant tanks which is

    shown that the switching and conducting losses of the switches

    in the proposed system are less than those in the conventional

    system. In addition, the current stress imposed on the switches

    in the proposed system is reduced significantly as compared to

    that in the conventional one.

    Vin100 V/div Iin200 mA/div time5 us/div

    Fig 7. Lamp current and voltage are same phase driving

    Vin100 V/div time5 us/div

    Fig 8. Lamp current and voltage are same phase driving

    Vin50 V/divIin200mA/div time2 us/div

    Fig 9. Waveform driving signal and lamp current and boost inductor voltage

    zero current switching and zero voltage switching

    The solution to this problem is to determine an estimate of the

    overall efficiency, measuring the input active power and the

    active power of each lamp, one by one, using an oscilloscope. In

    the maximum lighting condition, the total active power

    processed through the lamps is approximately 112W, whereas

    input active power is about 122W. Thus, the overall efficiency

    of the proposed ballast is 91.8 0%, at the maximum lighting

    condition.

    V. CONCLUSIONA circuit operation scheme for a multiple fluorescent lamp

    lighting system is proposed in this paper. The ballast is obtained

    from the integration of a boost dc-to-dc converter and single

    half-bridge series-resonant series-parallel loaded inverter. This

    inverter circuit operation scheme is implemented with the

    resonant tanks of the electronic ballast being capacitive andinductive, which can achieve lower switching losses, lower

    conduction losses and lower current stresses over conventional

    ballast with all inductive resonant tanks. The boost converter is

    operated in discontinuous conduction mode and at constant

    frequency providing an input power factor high enough to

    satisfy present standard requirements. The operation of the

    proposed ballast has also been investigated in detail in this paper.

    A prototype of the ballast with proposed circuit operation

    scheme for a four-lamp lighting system is implemented with

    0

    Vlamp1,2

    Vlamp3,4

    Vlamp

    Ilamp

    Low side switchHigh side switch

    Lamp current ia

    Boost inductor voltage

    0

    0

    0

    0

    1179

  • 7/29/2019 Lamps Electronic Ballast

    6/6

    practical considerations. In comparison with the conventional

    electronic ballast for multiple fluorescent lamps, the proposed

    electronic ballast for multiple fluorescent lamps presents a

    significant reduction of cost. This reduction becomes even more

    meaningful with larger number of lamps. The proposed

    topology works as a good solution to implement low-cost

    single-stage high efficiency electronic ballast for multiple

    fluorescent lamps.

    VI. ACKNOWLEDGMENTFinancial support of this research by the National Science

    Council, Republic of China, under Grant NSC

    97-2221-E-036-025 and Tatung University, Taipei, Taiwan,

    under the grant B97-E04-040 is gratefully acknowledged.

    VII. REFERENCES[1] E. E. Hammer and C. Ferreira, F40 fluorescent lamp considerations for

    operation at high frequency, J. Illum. Eng. Soc., vol. 15, no. 1, 1985, pp.

    63-74.

    [2] L. Huber and M. M. Jovanovic, Single-Stage Single-SwitchInput-Current-Shaping Technique with Fast-Output-Voltage Regulation,IEEE Transactions on Power Electronics, Vol. 13, No. 3, May 1998, pp.

    476-486.

    [3] E. Deng, and S. Cuk, Single Stage, High Power Factor, Lamp Ballast,Proc IEEE Applied Power Electronics Conference, 1994, pp. 441-449.

    [4] C. S. Moo, S. Y. Chan, and C. R. Lee, A Single-Stage High Power FactorElectronic Ballast with Duty-Ratio Controlled Series Resonant Inverter,

    IEEE Transactions on Industrial Electronics, Vol. 46, No. 4, Aug. 1999, pp.

    830-832.[5] J. A. Alves ,A. J. Perin, and I. Barbi,An electronic ballast with high power

    factor for compact fluorescent lamps, Proc in Conf. Rec. IEEE-IAS Annu.Meeting, 1996, pp.2129-2135.

    [6] M. A. Co, D. S. L. Simonetti and J. L. F. Vieira, High Power FactorElectronic Ballast Operating at Critical Conduction Mode, Proc PESC 96Record. Power Electronics Specialists Conference, 1996 27th Annual

    IEEE, Vol. 2, June 1996, pp.962-968,.[7] J. Spangler and A. K. Behera, Power Factor Correction Techniques Used

    For Fluorescent Lamp Ballast, Proc Conference Record of the 1991 IEEE

    at Industry Applications Society Annual Meeting, Vol.2, , Oct. 1991, pp.1836-1841.

    [8] R. N. Prado, A. R. Seidel, F. E. Bisogno, and R. K. Pavo, Self-OscillatingElectronic Ballast Design based on Point of View of Control System,

    Thirty-Sixth IAS Annual Meeting. Conference Record of the 2001.

    1180