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Isolated dc-dc converters with high-output voltage for TWTA - Ivo Barbi

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<strong>Isolated</strong> <strong>dc</strong>-<strong>dc</strong> Converters <strong>with</strong> High-Output Voltage<br />

For <strong>TWTA</strong> Telecommunication Satellite Applications<br />

Roger Gules and <strong>Ivo</strong> <strong>Barbi</strong><br />

Federal University of Santa Catarina -UFSC<br />

Power Electronic Institute - INEP<br />

P.O. Box 5 119 - 88010-970 - Florian6polis-SC-Brail<br />

Phone: +55-48-33 1-9204 - Fax: +55-48-234-5422<br />

E-mail: roger@,ineD.ufsc.br Intemet: http://www.ineD.ufsc.br<br />

Abstract-Two alternatives <strong>for</strong> the implementation of an<br />

isolated <strong>dc</strong>-<strong>dc</strong> converter <strong>with</strong> <strong>high</strong> <strong>output</strong> <strong>voltage</strong> are presented.<br />

The proposed topologies are especially well adapted <strong>for</strong> the<br />

implementation of Travelling Wave Tube Amplifiers (<strong>TWTA</strong>)<br />

utilized in telecommunication satellite applications. The<br />

<strong>converters</strong> studied follow different principles and the main<br />

operation aspect of each topology is analyzed. The experimental<br />

results obtained from two prototypes <strong>with</strong> 150W of <strong>output</strong><br />

power, total <strong>output</strong> <strong>voltage</strong> of 3.2kV and an input <strong>voltage</strong><br />

variable from 26V until 44V are presented. The efficiency<br />

obtained operating <strong>with</strong> the nominal <strong>output</strong> power is <strong>high</strong>er<br />

than 93.4 YO <strong>for</strong> both structures.<br />

I. INTRODUCTION<br />

There are different applications where is necessary the<br />

use of <strong>high</strong> level DC <strong>voltage</strong>s (thousands volt). Typical<br />

examples are COz laser-based systems, X-ray equipment <strong>for</strong><br />

medical and industrial applications, cathode-ray-tubes and<br />

telecommunication equipment <strong>with</strong> vacuum tubes, like<br />

Travelling Wave Tube (TWT) utilized in communication<br />

satellite.<br />

The choice of most adequate solution depends of the<br />

design requirements of each specific application as cost,<br />

mass, volume, efficiency, reliability, etc.<br />

Other point in the choice of the converter is the <strong>high</strong><strong>voltage</strong><br />

circuit non-idealities that present an important<br />

influence in the converter operation and the topology adopted<br />

must integrate these intrinsic parameters into the operation<br />

principle. Besides the leakage inductance, the <strong>high</strong>-<strong>voltage</strong><br />

trans<strong>for</strong>mer also presents a winding capacitance referred to<br />

the primary side that due to the <strong>high</strong> number of tums in the<br />

secondary winding and the <strong>high</strong> trans<strong>for</strong>mer tums ratio,<br />

becomes important in-the converter operation. Fig. 1 presents<br />

the <strong>high</strong>-<strong>voltage</strong> trans<strong>for</strong>mer simplified model constituted by<br />

the primary leakage inductance (L d), magnetizing inductance<br />

(L,,,)and the equivalent capacitance referred to the primary<br />

side (C,) [ 1,2].<br />

-HK<br />

nl: n2<br />

Fig. 1. Simplified equivalent circuit of the <strong>high</strong> <strong>voltage</strong><br />

and <strong>high</strong> frequency trans<strong>for</strong>mer.<br />

In the particular case of communication satellite<br />

applications studied in this paper, severe requirements must<br />

be attended due to the environmental conditions, reliability,<br />

mechanical and electrical specifications.<br />

The launch cost .is very <strong>high</strong> and there is a permanent<br />

interest in the efficiency improvement and reduction of the<br />

mass and volume in satellite equipment. High efficiency is<br />

important to achieve since the primary power source of a<br />

satellite is in general a solar array and batteries, presenting an<br />

important impact on total mass, volume and cost.<br />

The final stage amplifier in the transponder of the<br />

communication satellite is the Travelling Wave Tube<br />

Amplifier (<strong>TWTA</strong>). In this kind of satellite, the payload mass<br />

and power consumption is mainly given by the presence of<br />

the <strong>TWTA</strong> which can represent about 35% of the total mss<br />

and from 70% to 90% of the overall DC power consumption<br />

[3]. There<strong>for</strong>e, the design of <strong>TWTA</strong> has been continuously<br />

improved in order to realize more light and efficient<br />

equipment.<br />

The <strong>TWTA</strong> consist of a microwave amplifier tube TWT<br />

mainly determining the radio frequency (RF) per<strong>for</strong>mance<br />

and by an Electronic Power Conditioner (EPC) <strong>for</strong> power<br />

matching of the DC interface. The <strong>high</strong> <strong>voltage</strong> <strong>dc</strong>-<strong>dc</strong><br />

converter is the most important part of the EPC because it is<br />

the critical point in the design of a <strong>high</strong> efficiency and<br />

competitive <strong>TWTA</strong>. The input <strong>voltage</strong> of the <strong>dc</strong>-<strong>dc</strong> converter<br />

is an unregulated low <strong>voltage</strong> bus (from 26V until 44V) and<br />

in order to produce the TWT supply <strong>voltage</strong>s there are<br />

multiple <strong>output</strong>s in the <strong>dc</strong>-<strong>dc</strong> converter, resulting in a total<br />

cathode-anode <strong>voltage</strong> of thousands volts.<br />

11. HIGH VOLTAGE DC-DC CONVERTERS<br />

There are different altematives <strong>for</strong> the implementation of<br />

an isolated <strong>dc</strong>-<strong>dc</strong> converter <strong>with</strong> <strong>high</strong> <strong>output</strong> <strong>voltage</strong>,<br />

however there are some operations characteristics that the<br />

converter must present in order to obtain <strong>high</strong> efficiency and<br />

reduced volume and mass. The main operation characteristics<br />

are:<br />

High switching frequency in order to reduce the reactive<br />

elements likes inductors, filter capacitors and the power<br />

trans<strong>for</strong>mer.<br />

Soft-commutation in the power switches, avoiding the<br />

reduction of the efficiency <strong>with</strong> the increment of the<br />

switching frequency.<br />

0-7803-6618-2/011$10.000 2001 IEEE 296


Integration in the converter operation of the intinsic<br />

elements of the <strong>high</strong>-<strong>voltage</strong> power trans<strong>for</strong>mer like<br />

leakage inductance and distributed capacitance, avoiding<br />

the dissipation of the energy stored in these elements.<br />

Constant switching frequency, allowing the choice of an<br />

optimum switching frequency <strong>with</strong> respect to the mass,<br />

volume and efficiency.<br />

0 Voltage source <strong>output</strong> characteristic, because the multiple<br />

<strong>high</strong>-<strong>voltage</strong> <strong>output</strong>s necessaries <strong>for</strong> to supply the TWT<br />

become unfeasible the utilization of <strong>high</strong>-<strong>voltage</strong> <strong>output</strong><br />

filter inductors <strong>for</strong> a current source <strong>output</strong> characteristic.<br />

Others operation characteristics are also desirable in <strong>TWTA</strong><br />

application:<br />

Input current source behavior that minimizes the volume<br />

of the input filter.<br />

A step-up <strong>output</strong> characteristic, allowing the reduction of<br />

the trans<strong>for</strong>mer turns ratio and minimizing the effects of<br />

the trans<strong>for</strong>mer equivalent capacitance in the converter<br />

operation.<br />

Good load regulation and support a large variation of the<br />

input <strong>voltage</strong>.<br />

Considering as choice criterion of the <strong>converters</strong> all<br />

operation characteristics presented above, two topologies<br />

were selected and studied. Two <strong>dc</strong>-<strong>dc</strong> <strong>converters</strong> connected<br />

in series (two-stage topology) compose most part of the<br />

structures developed <strong>for</strong> this application and the first<br />

topology adopted follows this principle. The second topology<br />

studied is based on a new single-stage structure <strong>for</strong> <strong>TWTA</strong><br />

applications.<br />

111. TWO-STAGE TOPOLOGY<br />

A. Proposed Circuit<br />

The first converter that composes the two-stage topology<br />

is a regulator (normally a classical buck or boost <strong>dc</strong>-<strong>dc</strong><br />

converter). The second structure is an isolated <strong>dc</strong>-<strong>dc</strong><br />

converter operating in resonant way, generating the different<br />

<strong>high</strong> <strong>voltage</strong> <strong>output</strong>s <strong>for</strong> supply the TWT. In this case, the<br />

isolated <strong>dc</strong>-<strong>dc</strong> converter operates in an optimized operation<br />

point, <strong>with</strong> constant switching frequency and fix duty-ratio.<br />

This configuration is normally utilized due to the difficulty in<br />

to obtain <strong>high</strong> efficiency in the isolated <strong>dc</strong>-<strong>dc</strong> converter.<br />

The two-stage topology studied in this work is presented<br />

in Fig.2. The first converter is a classical boost <strong>dc</strong>-<strong>dc</strong><br />

converter composed by the input inductor L power switch<br />

SI, diode D1 and a filter capacitor C The boost regulator<br />

operates <strong>with</strong> hard switching but <strong>with</strong> the utilization of a<br />

Schottky diode in its <strong>output</strong>, <strong>high</strong>-efficiency operating <strong>with</strong><br />

<strong>high</strong> switching frequency is reached.<br />

The second converter is a resonant push-pull current fed<br />

<strong>dc</strong>-<strong>dc</strong> converter composed by two power switches S and<br />

$2, an input inductor L z, a resonant capacitor C and the<br />

push-pull trans<strong>for</strong>mer. The <strong>output</strong>s are composed by fullbridge<br />

rectifier and filter capacitors. The intrinsic parameters<br />

of the trans<strong>for</strong>mer are also presented in Fig.2.<br />

The push-pull converter operates <strong>with</strong> zero current and<br />

zero <strong>voltage</strong> switching techniques (ZCWZVS). The softcommutation<br />

is not dependent of the load current because the<br />

energy stored in the magnetizing inductance per<strong>for</strong>ms the<br />

<strong>voltage</strong> transitions in the circuit capacitance.<br />

The main theoretical wave<strong>for</strong>ms of the isolated converter<br />

are presented in Fig.3.<br />

There are two resonant circuits in the operation of this<br />

converter. During the conduction of one power switch S or<br />

Sp2 (to-tl), the resonance between center tap capacitor (C T)<br />

and the trans<strong>for</strong>mer leakage inductance (L d) occurs. When<br />

both power switches are turned-off (tl-t2) there is the<br />

resonance between the magnetizing inductance and the<br />

intrinsic circuit capacitance (power switches and trans<strong>for</strong>mer<br />

equivalent capacitance). The current (i) presented in Fig.3 is<br />

the current in the center tap of the push-pull trans<strong>for</strong>mer.<br />

Input <strong>voltage</strong>: Vin=26/44V<br />

Total <strong>output</strong> <strong>voltage</strong>: Vo=32o0V<br />

Nominal <strong>output</strong> power: Po=ISOW :<br />

PI=SP2=APTZOM22LZVR<br />

SI= IRFp2Y<br />

D,= 8TQlOo<br />

Reclifis diodes = MUR 1 lo0<br />

.----_.<br />

Ferrite colc ETD39-IPITIhomton<br />

Fig.2. Power circuit implemented of the two-stage topology.<br />

297


Reference [4] presents more details about the operation<br />

of this converter.<br />

VCI<br />

I<br />

The switch conduction period is represented by the<br />

relative parameter (tr). The current and <strong>voltage</strong> ef<strong>for</strong>t<br />

increase <strong>with</strong> the reduction of the switch conduction time (tr).<br />

The relative frequency F is the relationship between the<br />

resonance frequency of the leakage inductance and the center<br />

tap capacitance, <strong>with</strong> the switching frequency. This<br />

resonance occurs during the conduction of the power switch.<br />

Fr2 is the relationship between the resonant frequency of<br />

the magnetizing inductance and equivalent circuit<br />

capacitance, <strong>with</strong> the switching frequency. This resonance<br />

occurs when both switches are tumed off.<br />

Substituting the specification and parameters in (1) yields:<br />

VCI<br />

VCI<br />

11 U 0 %<br />

Fig.3. Main theoretical wave<strong>for</strong>ms.<br />

B. Simplified Design Procedure<br />

1) Specifications andparameters<br />

The following specifications are considered in the design:<br />

Input <strong>voltage</strong>:<br />

Vi,,=26/44V<br />

Total <strong>output</strong> <strong>voltage</strong><br />

V0=3200V<br />

Output power:<br />

P0=150W<br />

Push-pull switching frequency:<br />

Fs=801


,=atan.( z.Fr .(I - t ) )=0.549<br />

<strong>voltage</strong> is presented in Fig.7. The lowest efficiency obtained<br />

<strong>with</strong> nominal <strong>output</strong> power was 93.4% <strong>for</strong> the minimum<br />

input <strong>voltage</strong>.<br />

TO* *coo 25 OMS,*<br />

715 ACqc.<br />

is:<br />

The switch RMS current is:<br />

is, = ./%- = 3.09A (13)<br />

The maximum blocking <strong>voltage</strong> across the switch (VS pk)<br />

7<br />

Zn = .,/$<br />

= 1.34<br />

a<br />

Fig.5.Power switch <strong>voltage</strong> and current (25V/2A/2p/div).<br />

vs, =-<br />

cos(,)<br />

+2.V2 =IOW<br />

With the increment of the leakage inductance L d due to<br />

the constructive characteristic of the trans<strong>for</strong>mer, the<br />

capacitor CT must be lower <strong>for</strong> the same resonant frequency<br />

F, as shown in (9). Thus the parameter Zn calculated by (14)<br />

and the <strong>voltage</strong> ef<strong>for</strong>ts increase <strong>with</strong> the increment of L d.<br />

5) Output Filter Voltage Ripple<br />

The parameterized <strong>output</strong> <strong>voltage</strong> ripple is calculated by<br />

(16) and (17).<br />

-<br />

AV=<br />

AVc,,*C;F, -<br />

_-.<br />

1 2<br />

I O z F;cos(~)<br />

a=otang( w.F,.(l- t,) )<br />

Where:<br />

I, - Average <strong>output</strong> current.<br />

CO - Filter capacitor<br />

AV,, - Output <strong>voltage</strong> ripple<br />

C. Experimental Results<br />

A laboratory prototype was implemented following the<br />

optimized design procedure developed and some wave<strong>for</strong>ms<br />

obtained from this prototype operating <strong>with</strong> the minimal<br />

input <strong>voltage</strong> and the nominal <strong>output</strong> power are presented.<br />

The details about the power circuit implemented are shown in<br />

Fig.2. A typical configuration of load resistance representing<br />

the TWT <strong>for</strong> the test of the power supply is used. The<br />

different current i d <strong>voltage</strong> level in each <strong>output</strong> and the<br />

nominal <strong>output</strong> power are defined by the kind of TWT<br />

considered in the design.<br />

Fig.5 presents the soft-commutation obtained in the<br />

power switch of the push-pull converter. Fig.6 shows the<br />

<strong>voltage</strong> and current in a rectifier diode of the push-pull. The<br />

efficiency curve of the two-stage topology (boost and Pushpull)<br />

operating <strong>with</strong> nominal <strong>output</strong> power and variable input<br />

S.<br />

Fig.6. Rectifier diode <strong>voltage</strong> and current (lOOV/50mA/2p Jdiv).<br />

9s<br />

94.5<br />

t1W) 94<br />

93.5<br />

94-s-<br />

93<br />

25 30 3s<br />

Vin (V)<br />

40 45<br />

Fig.7. Efficiency operating <strong>with</strong> nominal <strong>output</strong> power<br />

and variable input <strong>voltage</strong>.<br />

IV-SINGLE STAGE TOPOLOGY<br />

The main drawback of the two-stage topologies is the<br />

converter series connection that causes a reduction of the<br />

overall efficiency. Both <strong>converters</strong> must present a very <strong>high</strong><br />

efficiency (close to 96%) in order to maintain an adequate<br />

efficiency <strong>for</strong> a satellite communication application (<strong>high</strong>er<br />

than 92%).<br />

There<strong>for</strong>e, a single stage topology can result in a <strong>high</strong>er<br />

efficiency and a lower mass and volume than the two-stage<br />

topology. However, the isolated <strong>dc</strong>-<strong>dc</strong> converter operates<br />

<strong>with</strong> a variable operation point (non-optimum) due to the<br />

converter's regulation action. Thus, the single stage topology<br />

candidate must present all suitable operation characteristics<br />

<strong>for</strong> <strong>high</strong>-<strong>voltage</strong> applications described be<strong>for</strong>e and maintain a<br />

<strong>high</strong> efficiency in all range of the input <strong>voltage</strong>.<br />

A. Proposed Circuit<br />

For the implementation of a competitive <strong>high</strong>-<strong>voltage</strong><br />

isolated <strong>dc</strong>-<strong>dc</strong> converter, a single-stage <strong>high</strong>-efficiency<br />

topology is proposed. The power circuit adopted, presented in<br />

299


-____.<br />

Fig.8, is. based -on the current-fed push-pull <strong>dc</strong>-<strong>dc</strong><br />

converter operating <strong>with</strong> PWM modulation, active clamping<br />

and ZVS commutation [SI.<br />

Two main switches (S p1 and SP2), two auxiliary clamping<br />

switches (Sal and Sa), a clamping capacitor C G and a pushpull<br />

trans<strong>for</strong>mer compose the converter. The current feeding<br />

is provided by the <strong>voltage</strong> source V in in series <strong>with</strong> the input<br />

inductor Li,. The <strong>output</strong>s are <strong>for</strong>med by full-bridge rectifiers<br />

and by filter capacitors. The anti-parallel diode and intrinsic<br />

capacitance of the MOSFET are used in the circuit operation.<br />

The intrinsic parameters of the trans<strong>for</strong>mer are also presented<br />

in Fig.8.<br />

The main operation wave<strong>for</strong>ms are shown in Fig.9.<br />

Fig.8. Power circuit implemented of the single-stage topology.<br />

- - - __<br />

The- active clamping allows the operation <strong>with</strong> softcommutation<br />

in all switches until a minimum load and the<br />

<strong>voltage</strong> across the blocking switch is equal the clamping<br />

<strong>voltage</strong>.<br />

An important characteristic of this structure is to operate<br />

<strong>with</strong> a main switch duty-ratio (D) <strong>high</strong>er than and lower than<br />

0.5 (<strong>with</strong> overlapping and <strong>with</strong>out overlapping). The<br />

auxiliary switches operate in a complementary way in<br />

relation the respective main switch.<br />

For a main switch duty-ratio lower than 0.5, the converter<br />

operates like a sepic <strong>dc</strong>-<strong>dc</strong> converter and <strong>with</strong> a step-down<br />

<strong>output</strong> characteristic. For the operation <strong>with</strong> a main switch<br />

duty-cycle <strong>high</strong>er than 0.5, the converter operates like an<br />

isolated boost converter <strong>with</strong> a step-up <strong>output</strong> characteristic.<br />

There<strong>for</strong>e, this converter does not present inrush current <strong>for</strong> a<br />

progressive variation of the duty-cycle and support a large<br />

variation of the input <strong>voltage</strong>.<br />

There is the resonance between the leakage inductance<br />

and the parasitic trans<strong>for</strong>mer capacitance when both main<br />

switches are conducting. During this period the input<br />

inductance (Lin) stores energy and the oscillations does not<br />

present influence in the converter's operation.<br />

I .<br />

"spl " Sal ' Spl<br />

Gat ,<br />

, ' Sp2 Sa2 I'SP2 '* I<br />

' -4.T " M.T,, 4.T , , .PI 4" '<br />

T ><br />

D.T<br />

>'<br />

Fig.9. Main theoretidl wave<strong>for</strong>ms.<br />

t<br />

B. Simplified Design Procedure<br />

1) Specifications and parameters<br />

The following specifications are considered in the design:<br />

Input <strong>voltage</strong>:<br />

Vin=26144V<br />

Total <strong>output</strong> <strong>voltage</strong><br />

V,=3200V<br />

Output power:<br />

P,=150W<br />

Push-pull switching frequency: FS=80k&<br />

The parameters of the implemented circuit are:<br />

Magnetizing inductance:<br />

Lm=85W<br />

Leakage inductance:<br />

Ld26@<br />

Winding capacitance:<br />

Cp=8.75nF<br />

2) Operation point of the Push-pull converter<br />

The <strong>output</strong> <strong>voltage</strong> referred to the primary side (V op)<br />

adopted in the design is equal to SOV, considering the main<br />

300


switch duty-ratio <strong>high</strong>er than 0.5 and a step-up <strong>output</strong><br />

characteristic.<br />

The static gain, operating <strong>with</strong> the minimum and<br />

maximum input <strong>voltage</strong> are determined respectively by:<br />

gm = -%- = -<br />

50<br />

= 1.9231<br />

Vin,, 26<br />

vop 50<br />

4, =-- - - = I. I364<br />

Vin,, 44<br />

(19)<br />

The nominal input current operating <strong>with</strong> the minimum<br />

and maximum input <strong>voltage</strong>, considering the operation<br />

<strong>with</strong>out losses is:<br />

Po<br />

Iin, =-=5.77A<br />

Vin (20)<br />

Po<br />

Iin, = - = 3.41A<br />

Vin m,<br />

The parameter y represents a reduction of the effective<br />

converter duty-ratio due to the presence of the active<br />

clamping circuit. This characteristic is common in the most<br />

part of the ZVS-PWM <strong>converters</strong>. This parametet is<br />

proportional to the leakage inductance and input current.<br />

For the minimum and maximum input <strong>voltage</strong> results:<br />

Iin, * L, . F,<br />

Yvm = = 0.08308<br />

VOP<br />

lin, . L, . F, =<br />

Y, =<br />

0.04909<br />

VOP<br />

The nominal converter duty-ratio <strong>for</strong> the minimum and<br />

maximum input <strong>voltage</strong> is:<br />

Auxiliary switch:<br />

iSa, = lin, .&e,/-12 = 0.945A (29)<br />

4) Current ef<strong>for</strong>ts operating <strong>with</strong> the maximum input<br />

<strong>voltage</strong><br />

Main switch:<br />

iSp, = lin, . -. ,/15.y,+13-7.d, ~2.4324 (30)<br />

12<br />

Auxiliary switch:<br />

5) Soff-commutation range<br />

The minimal input current that maintains the softcommutation<br />

is defined by:<br />

Where:<br />

Z, =E (33)<br />

The soft-commutation range increase <strong>with</strong> Z , and Ld. The<br />

soft-commutation was obtained in all input <strong>voltage</strong> variation<br />

range and in an adequate load variation range.<br />

6) Output Filter Voltage Ripple<br />

The parameterized <strong>output</strong> <strong>voltage</strong> ripple is variable <strong>with</strong><br />

the static gain (4) and calculated by (34).<br />

2) Voltage ef<strong>for</strong>ts<br />

The clamping <strong>voltage</strong> operating <strong>with</strong> nominal <strong>output</strong><br />

power and minimum and maximum input <strong>voltage</strong> is:<br />

2<br />

V,, = Vin,, - = 147V<br />

l-dvm<br />

(26)<br />

L<br />

V,, = fin,, = 112.5V<br />

1 - d”X<br />

Thus the maximum blocking <strong>voltage</strong> across the active<br />

switches is equal to 147V.<br />

3) Current ef<strong>for</strong>ts operating <strong>with</strong> the minimum input<br />

<strong>voltage</strong><br />

Main switch:<br />

Where:<br />

I, - Average <strong>output</strong> current.<br />

CO - Filter capacitor<br />

AVco - Output <strong>voltage</strong> ripple<br />

C. Experimental Results<br />

A laboratory prototype was implemented following an<br />

optimized design procedure developed and some wave<strong>for</strong>ms<br />

obtained operating <strong>with</strong> the minimal input <strong>voltage</strong> and the<br />

nominal <strong>output</strong> power are presented. The details about the<br />

power circuit implemented are presented in Fig.8.<br />

Fig.10 shows the main switch current and <strong>voltage</strong><br />

wave<strong>for</strong>ms. The soft-commutation is obtained and the<br />

maximum switch <strong>voltage</strong> is equal the clamping <strong>voltage</strong>.<br />

The auxiliary switch <strong>voltage</strong> and current wave<strong>for</strong>ms are<br />

presented in Fig. 1 1. The auxiliary switch also presents soft-<br />

301


commutation and the RMS current and the conduction losses<br />

are very low.<br />

The efficiency curve operating <strong>with</strong> nominal <strong>output</strong><br />

power and variable input <strong>voltage</strong> is present in Fig.12. The<br />

lowest efficiency obtained <strong>with</strong> nominal <strong>output</strong> power was<br />

94.1 Yo.<br />

TeK StOL 25 OMS/5<br />

2<br />

503 ncqs<br />

FiglO. Main switch <strong>voltage</strong> and current (5OV/2A/2pddiv).<br />

TeK 5tOP 25 OMW5<br />

114 ncqs<br />

I<br />

The proposed <strong>converters</strong> are suitable <strong>for</strong> low input <strong>voltage</strong><br />

applications, because the blocking <strong>voltage</strong> switch is <strong>high</strong>er<br />

than two times the input <strong>voltage</strong> <strong>for</strong> both structures.<br />

The operation characteristics were verified by the<br />

implementation of the laboratory prototypes operating <strong>with</strong> a<br />

variable input <strong>voltage</strong> (26V/ 44V) and <strong>with</strong> 3.2kV of total<br />

<strong>output</strong> <strong>voltage</strong>. The lowest efficiency obtained operating <strong>with</strong><br />

the nominal <strong>output</strong> power is equal to 94.1% <strong>for</strong> the singlestage<br />

topology and equal to 93.4% <strong>for</strong> the two-stage<br />

topology. The single-stage topology proposed presents a<br />

lower mass and volume and <strong>high</strong>er efficiency than the two<br />

stages-topology studied.<br />

The <strong>output</strong> <strong>voltage</strong> ripple of the single-stage topology<br />

operating in the worst operation condition (<strong>high</strong>er static gain)<br />

was 30% <strong>high</strong>er than the two-stage topology <strong>with</strong> the same<br />

<strong>output</strong> filter.<br />

REFERENCES<br />

a<br />

I I I II/F I I I I<br />

Fig.11. Auxiliary switch <strong>voltage</strong> and current (50V/2A/2pddiv).<br />

94.9<br />

94.7<br />

94.5<br />

943<br />

94.1<br />

*<br />

93.7 93*9<br />

25 30 35 40 45<br />

Vin (V)<br />

Fig. 12. Efficiency operating <strong>with</strong> nominal <strong>output</strong> power<br />

and variable input <strong>voltage</strong>.<br />

V. CONCLUSIONS<br />

[ ‘1 B. Tala-Ighil, J-M. Nyobe-Yome and C. Glaize, “High-Voltage Variable-<br />

Frequency Double-Resonant DC-DC Converters Utilizing the<br />

l<br />

Tmsfomer Parasitic Elements,” Proceedings of the European Space<br />

Power Conference, Austria, p. 245-250, Aug. 1993.<br />

[ 1 J. Uceda, C. Blanco, M. A. Ptrez and M. RICO, “Design of the Delay<br />

Line Power Supply of a TWT,” Proceedings of the European Space<br />

Power Conference, Spain, p. 2123-2128, Aug. 1995.<br />

[3] LCeruti, M. Gambarara and D.Vigano, ‘Yew Generation EPC <strong>for</strong><br />

Medium Power TWTs,” Proceedings of the European Space Power<br />

Conference, Spain, p. 299-316, Sep. 1998.<br />

[4] A. H Weinberg and L.Ghislanzoni, “A New Zero-Voltage Zero-Current<br />

Power Switching Technique,” IEEE Transactions on Power Electronics,<br />

vol. 7, no. 8, p. 655-665, Oct. 1992.<br />

[5] F. J. Nome and 1. <strong>Barbi</strong>, “A ZVS Clamping Mode Current-Fed Push Pull<br />

DC-DC Converter,” ISIE’98, Pretoria, South Afric, pp. 617-621, Ju1.1998,<br />

[6] I. Arens and F. Tonicello, “ Conductance Control <strong>with</strong> a Boost Regulator<br />

<strong>for</strong> a High-Voltage Power Conditioner <strong>for</strong> a <strong>TWTA</strong>,” Proceedings ofthe<br />

European Space Power Conference, Ita&. p. 343-350, Sep. 1991.<br />

r71 P. Delporte, P. Fa9 and E. Pequet, “EPC and <strong>TWTA</strong> <strong>for</strong><br />

Telecommunication Satellites,” Proceedings of the European Space<br />

Power Conference, Spain, p. 305-310, Sep. 1998.<br />

Two alternatives <strong>for</strong> the implementation of a <strong>high</strong>efficiency<br />

isolated <strong>dc</strong>-<strong>dc</strong> converter <strong>with</strong> <strong>high</strong>-<strong>output</strong> <strong>voltage</strong><br />

<strong>for</strong> <strong>TWTA</strong> application were proposed and studied. Both<br />

structures present several operation characteristics suitable<br />

<strong>for</strong> <strong>high</strong> <strong>output</strong> <strong>voltage</strong> applications supplied by an<br />

unregulated input <strong>voltage</strong>.<br />

302

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