IEEE TRANSACTIONS ON POWER ELECTRONICS, VOL. 23, NO. 2, MARCH 2008 635 A Unity Power Factor Correction Preregulator With Fast Dynamic Response Based on a Low-Cost Microcontroller Diego G. Lamar, Student Member, IEEE, Arturo Fernández, Member, IEEE, Manuel Arias, Student Member, IEEE, Miguel Rodríguez, Student Member, IEEE, Javier Sebastián, Member, IEEE, and Marta Maria Hernando, Member, IEEE Abstract—Low cost passive power factor correction (PFC) and single-stage PFC converters cannot draw a sinusoidal input current and are only suitable solutions to supply low power levels. PFC preregulators based on the use of a multiplier solve such drawbacks, but a second stage dc–dc converter is needed to obtain fast output voltage dynamics. The output voltage response of PFC preregulators can be improved by increasing the corner frequency of the output voltage feedback loop. The main drawback to obtaining a faster converter output response is the distortion of the input current. This paper describes a simple control strategy to obtain a sinusoidal input current. Based on the static analysis of output voltage ripple, a modified sinusoidal reference is created using a low cost microcontroller in order to obtain an input sinusoidal current. This reference replaces the traditional rectified sinusoidal input voltage reference in PFC preregulators with multiplier control. Using this circuitry, PFC preregulator topologies with galvanic isolation are suitable solutions to design a power supply with fast output voltage response (10 or 8.33 ms) and low line current distortion. Finally, theoretical and simulated results are validated using a 500 W prototype. Index Terms—EN 61000-3-2 regulations, fast output voltage dynamics, modified sinusoidal reference, power factor correction (PFC). I. INTRODUCTION P OWER factor correction (PFC) used to be synonymous with sinusoidal input current and extremely low total harmonic distortion (THD). When IEC 61000-3-2 regulations came into force in 2001, the PFC solutions with low power converters became even more evident. A sinusoidal waveform is not needed to comply with this regulation. The only requirement is for the harmonic content of the input power to be measured at nominal input voltage and for the input current to be below a limit set by the regulation. In short, the philosophy of the PFC has changed. Simple passive PFC solutions based on reactive devices are robust and economical solutions. Some simple passive circuits have already been presented in other papers: single-phase rectiManuscript received April 1, 2007; revised July 10, 2007. This paper was presented at the IEEE Applied Power Electronics Conference (APEC), Anaheim, CA, February 27, 2007. This work was supported by the Spanish government, under Project MEC04-TEC2004-02468. Recommended for publication by Associate Editor S. Pekarek. The authors are with Grupo de Sistemas Electrónicos de Alimentación, Universidad de Oviedo, Gijón 33204, Spain (e-mail: gonzalezdiego@uniovi.es). Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TPEL.2007.915657 fiers with an filter [1]–[3], inductance or resistance between the input rectifiers and the bulk capacitor [4], etc., all of which are good solutions for low power levels. However, the input current harmonic content is very close to the limit and some solutions have many drawbacks with the universal input line voltage range. PFC preregulator circuits are widely considered the best solution for high power levels and the universal input line voltage range [5]. The injection of current harmonics to the line is very low due to the quasi-sinusoidal input current waveform. Moreover, an input current with a very low distortion guarantees compliance with international regulations even if regulatory limits change in the future. The main disadvantage of these circuits is their poor output voltage dynamics. This is due to the fact that the output voltage regulator has a low pass-filter (10–20 Hz bandwidth) needed to reduce the THD of the input line current. If the specification requires fast output voltage regulation, a second stage is needed to improve output converter dynamics. In fact, the dc–dc converter placed in cascade defines the twostage converter output voltage response. However, for low and medium power levels, unity PFC topology dc–dc converter can be an expensive and complex solution. When a unity power factor is not needed, single-stage PFC converters are a possible solution [6]–[11]. These topologies exhibit fast output voltage dynamics (more or less of the same order as two-stage PFC converters) at relatively low cost and small size. Their efficiency with narrow voltage ranges is very high because most of the power is only processed once, or at least only a small part is processed twice. However, these advantages are only valid for low power levels. Nevertheless, there are many applications in which the load remains more or less constant and no extremely fast output voltage response is needed. In some of these applications, PFC preregulator converters can be used without the cascade connected dc–dc converters. The poor dynamic response of standard PFC preregulators can be improved by increasing the traditional output voltage regulator bandwidth from 10 Hz to 1 kHz thereby allowing a moderate distortion of the input current [12]. In this case, the design philosophy of the PFC preregulator changes: the main objective is to improve the output response instead of drawing a sinusoidal input current. So PFC preregulators with fast dynamic response can be used to design an ac–dc complete power supply in the hundred watts range. In this case, PFC preregulators must have galvanic isolation (that is, is based on a dc–dc converter with a transformer, 0885-8993/$25.00 © 2008 IEEE 636 IEEE TRANSACTIONS ON POWER ELECTRONICS, VOL. 23, NO. 2, MARCH 2008 Fig. 1. PFC preregulator. i.e., Flyback PFC). Moreover, the output voltage must be sufficiently high and the output voltage ripple specification must be not very restrictive. This is because the size of the bulk capacitor of the PFC preregulator increases when the output voltage decreases or when the output voltage ripple decreases, for a given power. Also the dynamic requirements of the power supply can be achieved by a PFC preregulator. Finally, these kinds of converters are not available solutions when the converter must satisfy hold-up time specifications. The conclusion is that a complete power supply can be designed using the PFC preregulator solution for both high power ( 600 W) and medium power levels ( 600 W). It is also a cheaper circuit than the traditional two-stage solution. However, this solution has the above mentioned limitations. The use of only a PFC preregulator as a complete power supply is an interesting option for some specific applications (i.e.,: analog loads, battery chargers, audio switching amplifiers, etc ). This paper presents a simple control strategy to achieve fast dynamic response and sinusoidal input current. This control is based on the use of a low-cost microcontroller ( C) as voltage waveform reference. First the paper presents an analysis of the PFC preregulator with fast dynamic response describing the trade-off between input current distortion and dynamic response of the output voltage. It then describes a simple control strategy based on a modified sinusoidal reference. Finally a simple strategy with a low-cost microcontroller is proposed using this modified sinusoidal reference to obtain a sinusoidal input current compatible with a ‘relatively’ fast response (10 ms if the line frequency is 50 Hz or 8.33 ms if the line frequency is 60 Hz). II. STATIC ANALYSIS OF POWER FACTOR CORRECTOR PREREGULATORS WITH FAST DYNAMICS PFC preregulators have an inner feedback loop, the current loop, and an outer one, the voltage loop (Fig. 1). The current loop makes the line current follow a reference signal. In general, the input current in PFC preregulators follows a sinusoidal reference. The voltage loop regulates output voltage. This paper will next review typical static analysis of the PFC preregulators [13], [14]. Fig. 2. PFC preregulator waveforms: (a) traditional, with a 10 Hz corner frequency of the low-pass filter of the output voltage feedback loop and (b) with fast dynamics, with a 1 kHz corner frequency of the low-pass filter of the output voltage feedback loop. Traditionally, a low-pass filter is included in the output voltage feedback loop to eliminate 100–120 Hz output voltage ripple. The output voltage of the voltage feedback loop is . The input line current reference is therefore a dc value therefore a sinusoidal waveform and the input line current (t) (assuming the current loop to be ideal) has no distortion (1) is the voltage peak of the input voltage ( ), where is the line angular frequency and K is a constant value. PFC preregulators have a high efficiency (around 95%). So output power before the output bulk capacitor (t) is equal to () input power (2) Moreover, the output bulk capacitor C is big enough to keep the constant, so the output current expression is output voltage (3) As can be seen in Fig. 2(a) and in (3), the output current has a dc value and a second harmonic. This second harmonic is processed through the bulk capacitor. A voltage ripple thus appears at the output voltage and is transmitted into the output voltage feedback loop. For this reason, a low-pass filter is needed in order to attenuate and quasi-eliminate this distortion and keep the input line current sinusoidal, as can be seen in (1). However, the low pass-filter decreases the feedback bandwidth of the output voltage, causing a poor dynamic response of the output voltage in PFC preregulators. This paper will next consider the situation in which the corner placed in the output voltage frequency of the low-pass filter feedback loop is increased in order to improve the response of output voltage in PFC preregulators. The PFC preregulators priorities change: the main objective is to improve the output response instead of drawing a sinusoidal input current to obtain PFC preregulators with fast dynamics. The output voltage ripple LAMAR et al.: UNITY POWER FACTOR CORRECTION PREREGULATOR 637 Fig. 3. Static analysis of the second harmonic of the output current to obtain the ripple characteristics of v (t): V of double line frequency value 2 2 2 is transferred into the output voltage feedback loop. Thus, the voltage is not a constant of the output voltage feedback loop value (4) where is the second harmonic amplitude of ( ) and is the phase lag with respect to of the second harmonic ( ) [see Fig. 2(b)]. of The input line current can be easily calculated by substituting for ( ) in (1) he value of and . In this study, the influence of the fourth harmonic of the output ( ), is not included in the calculations to simplify the current, static study because is strongly attenuated by the output filter. In consequence, only the second harmonic of ( ) is processed through the PFC preregulator power stage and the output voltage feedback loop in order to calculate the ripple characteristics of ( ). Its value can be obtained from (6b) (5) (8) The input line current, therefore, is not sinusoidal. The second ( ) is transformed into the third harmonic of the harmonic of input line current. Furthermore, input line current distortion is defined by the ripple characteristics of the output voltage of the and ). The ripple of ( ) can voltage feedback loop ( be calculated from (t), from the power stage characteristics of the PFC preregulator and from the transfer function of the output voltage feedback loop. Substituting (5) in (2) and supposing an output bulk capacitor constant, the input big enough to keep the output voltage current is The second harmonic of the output current passes through the output filter (composed of the bulk capacitor and the load ), the output voltage divider and the output voltage regulator in order to obtain the voltage ripple of the voltage feedback loop (6) (6a) (9) It should be noted that the output voltage remains constant due to the large value of the bulk capacitor and influence of in the output filter disappears, as it shown in Fig. 3. The value of the output capacitor needed for a specific output voltage ripple of the PFC preregulator is (10) (6b) (6c) Moreover, can be easily calculated as a function of averaged power processed by the PFC preregulator ( ) from (6a) (7) is the amplitude ripple of the output voltage exwhere pressed as a percentage of the output voltage. The output voltage divider scales the output voltage ripple . Finally, the output voltage regulator processes the of 2 ( ). As a result, output voltage ripple in order to obtain and its the voltage regulator characteristics, (i.e., dc gain 2 ) also define the ( ) ripple corner frequency characteristic. Therefore, if the transfer function between ( ) 638 IEEE TRANSACTIONS ON POWER ELECTRONICS, VOL. 23, NO. 2, MARCH 2008 and ( ) is studied, then the expressions of and can be easily calculated following the above mentioned process: (11) Fig. 4. Averaged model described in [12] with its output voltage feedback loop. (12) where is the voltage regulator gain at 2 corner angular. and is its III. NEW CONTROL STRATEGY BASED ON A MODIFIED SINUSOIDAL FIXED REFERENCE IN THE MULTIPLIER CONTROL OF PFC PREREGULATORS WITH FAST DYNAMICS This section will study the expressions calculated above to obtain quantitative and qualitative conclusions about ( ) dis( ) dependence analysis will be described tortion. First, a which will lead to further conclusions. As can be seen in the input current expression (5), ( ) dis, the tortion is defined by the amplitude of the ripple and the dc value of the output voltage ripple phase lag and terms are merged of the voltage feedback loop. to simplify into a single term called relative ripple distortion analysis. This relative ripple of the output voltage of ( ) amplitude ripple the voltage feedback loop is defined as divided by its dc value. Furthermore, if the expression of (7) is substituted in the input current expression (5), the result highlights the proportionality between the averaged input power P and the input current ( ) and also the inverse proportionality and ( ), as (13) shows between the input voltage peak (13) This equation shows that the shape of the input current only and the ripple phase depends on the relative ripple and ) are lag . The values of these quantities ( shown in (11) and (12). As these expressions show, the output power does not determine the values of above mentioned quanand tities. The non-dependence of relative ripple on the averaged input power is of greater significance, because and determines the shape of the input current, as has been previously explained. Therefore, the shape of the input current does not depend on the power processed by the PFC preregulator with fast dynamics. In other words, the relationship between the amplitude of the first and third harmonic and the relative position of these harmonics are independent of the power processed for a PFC preregulator design. The previous conclusions can be applied when a load step occurs. The shape of the input current will be the same at the beginning and at the end of the load step, because the only difference between them will be the different power processed by the PFC preregulator. The large-signal averaged model described in [12] (Fig. 4) is proposed to simulate a load step and to check what the shape of the input current is like. It is a simple averaged model which can be easily implemented with simulation software (e.g., Pspice) to obtain the real distortion of the input line current. Fig. 5 illustrates the results of the simulation of two load steps of the PFC preregulator with different designs of the output voltage feedback loop. As can be seen, the shape of (t) remains constant at the initial and the final stage of the load step level changes, as has already been shown, and the harbut monic content of both stages are proportional. One simplification was made in the PFC preregulator static study: the second harmonic is the only output voltage ripple component which introduces distortion in ( ). In fact, higher order harmonics cause distortion in the input line current in a real PFC preregulator with fast dynamics. However, theoretical and simulation results are very close, demonstrating that the paper’s earlier hypothesis that was used to simplify the static study was correct. As has already been pointed out, if the shape of ( ) does not change in the initial and final stages of a load step, then a new control strategy can be implemented in the PFC preregulator with multiplier control. This new solution draws a sinusoidal input current and it keeps the dynamic response of the output voltage fast. A new properly modified sinusoidal reference as a fixed pattern is introduced in the multiplier in spite of the traditional sinusoidal reference sensed from the rectifier input voltage. This modified sinusoidal reference must first be calculated in order to obtain a sinusoidal input current (Fig. 6). The static ( ) waveform is like, so study has already shown what the it is easy to calculate this properly modified reference as a si( ) divided by ( ). A simple and low cost cirnusoidal cuitry must thus be implemented and inserted into the multiplier control to generate the fixed pattern at 2 frequency. In LAMAR et al.: UNITY POWER FACTOR CORRECTION PREREGULATOR 639 Fig. 7. Waveforms of the load step from 1/3P ulator with fast dynamics for proposed solution. to P of the PFC prereg- Fig. 5. Waveforms and harmonic content of i (t) of the load step from 1/3 P to P and the harmonic content of the PFC preregulator with two different output voltage feedback loop designs: (a) A 40 y f 10 Hz; (b) A 40 y f 1 kHz. = = = = Fig. 8. PFC preregulator with fast dynamics with the non sinusoidal reference strategy generated by a low cost C. IV. LOW COST MICROCONTROLLER GENERATING THE MODIFIED SINUSOIDAL REFERENCE Fig. 6. New control strategy based on a non sinusoidal reference in PFC preregulators with fast dynamics in order to obtain a sinusoidal input current. this case, a sinusoidal input current is drawn without a low-pass filter using this control strategy. Finally, if a load step occurs, ( ) remains sinusoidal because the shape of the input then current does not change so the fixed pattern previously calculated should be the same. In Fig. 7, a load step has been simulated using this new control strategy. As can be seen, the input line current is sinusoidal after and before the load step. Furthermore, dynamic response, at around 10 ms, is fast. As previously stated, simple circuitry is needed to generate the properly modified sinusoidal reference, which can easily be calculated using the earlier static analysis. Mathematical software (e.g., Mathcad) can be used for waveform calculation, enabling the reference waveform to be easily normalized to its peak value. Finally, a fixed and normalized reference pattern can be used as a properly modified sinusoidal reference. This pattern can be generated by a pulse width modulation (PWM) module of a low-cost microcontroller ( C), as can be seen in Fig. 8. The microcontroller reference voltage is smaller than the traditional reference sensed from the rectifier input voltage. However, traditional multiplier control chips (e.g., reference as a current reference. UC3854B) sense the Therefore, if the value of the current limit resistance [15] used in the traditional control is substituted by the adequate value then the chip levels are maintained. A low-cost microcontroller (PIC 16F627) working at 20 MHz was used to implement the new control strategy. This is a simple circuit, costing around 1 . repetitive pattern of the modified sinuThe fixed and 2 soidal reference also has to be synchronized. This reference and 640 IEEE TRANSACTIONS ON POWER ELECTRONICS, VOL. 23, NO. 2, MARCH 2008 Fig. 9. Experimental harmonic content of the PFC preregulator with fast dynamics with traditional sinusoidal reference and with a C modified sinusoidal reference. Fig. 11. Prototype dynamic response: (a) with traditional sinusoidal reference and traditional voltage loop bandwidth design; (b) with traditional sinusoidal reference and increased voltage loop bandwidth design; and (c) with a C modified sinusoidal reference and increased voltage loop bandwidth design. = p Fig. 10. Prototype input current at V 230 2 and P = 500 W: (a) with traditional sinusoidal reference and (b) with a C modified sinusoidal reference. the rectifier input voltage have to be “in phase” so a synchronization circuit has to be implemented (Fig. 8). This kind of circuits usually detects significant points of the input voltage. ( ) were chosen. When these points Zero voltage points of are detected, the microcontroller launches the fixed waveform of the modified sinusoidal reference. As a result, the reference signal is synchronized every 10 ms (or 8.33 ms if the line frequency is 60 Hz). The microcontroller algorithm is based on a look-up table with normalized values of the duty cycle. The program goes through the table from top to bottom when the synchronized point is detected. Apart from generating the reference, the microcontroller can also perform other functions: protection system, supervision system, soft start of the converter, etc. V. EXPERIMENTAL RESULTS A 500 W PFC preregulator prototype, based on a boost topology, was developed in order to test the averaged and theoretical models. The main specifications of the PFC boost converter are the following: input voltage: 85–265 V, output voltage: 400 V; output voltage ripple: less than 1% and 100 kHz switching frequency. Fig. 9 shows the experimental harmonic content when the 40 and output voltage feedback loop is designed as 1 kHz, with traditional sinusoidal reference and with a C modified sinusoidal reference. A sinusoidal input current can be obtained by using this new control strategy. In contrast, with the traditional control strategy the input current distortion is defined by the third harmonic, so the higher harmonic content can be ignored as it was said previously. Fig. 10 shows the input current when the design of the feed40 and 1 kHz with traditional sinuback loop is: soidal reference [Fig. 10(a)] and with a C modified sinusoidal Fig. 12. Prototype waveforms of the load step with a C modified sinusoidal reference. reference [Fig. 10(b)]. The input current is sinusoidal with the C modified sinusoidal reference. However, the distortion of ( ) is appreciable with the traditional sinusoidal reference. Standard regulations such as IEC 61000-3-2 cannot be complied at high power levels. Fig. 11 shows a prototype load step from 1/3 of full load to full load. This test was run with the previous output voltage feedback 40 and 1 kHz with loop design [Fig. 10(b) and (c)]: traditional sinusoidal reference and with a C modified sinusoidal reference. The dynamic responses of both control strategies are similar: around a 10 ms output voltage response. In this case, the C control strategy response is faster than the traditional response of the unity PFC of around 100 ms [Fig. 10(a)] keeping a sinusoidal input current. Finally, Fig. 12 shows a prototype load step from full load to 1/3 of full load for the proposed control strategy. The input current remains sinusoidal after and before the load step, as was deduced in the previous static analysis. Moreover, the dynamic response of the output voltage is fast (around 20 ms), so PFC LAMAR et al.: UNITY POWER FACTOR CORRECTION PREREGULATOR preregulators with galvanic isolation (e.g., Flyback PFC preregulator) can be implemented as sometimes as ac-dc power supplies without using a second stage dc–dc to obtain a sinusoidal input current. VI. CONCLUSION PFC preregulators are traditionally used as first stage in ac–dc power supply designs. A second stage is needed to improve output voltage dynamics, reduce output voltage and provide galvanic isolation. However, a relatively high output response can be achieved by increasing the corner frequency of the low-pass filter of the output voltage feedback loop (PFC preregulators with fast dynamics). In contrast, the output voltage ripple of the voltage regulator distorts input line current. This paper shows that the relative ripple at the output of the voltage feedback loop does not depend on the power. A new control strategy is presented: if a properly modified sinusoidal reference (based on the static analysis presented) is employed as a fixed pattern in spite of the traditional sinusoidal reference, then a sinusoidal current can be drawn in PFC preregulators with fast dynamics. The fixed pattern can be generated in a low cost microcontroller. Moreover, the microcontroller ( C) circuitry can be easily used with commercial chips of PFC preregulators with multiplier control. Therefore, sinusoidal input current ac-dc power supplies based on PFC preregulators with fast dynamic response and galvanic isolation (e.g., Flyback PFC preregulator) can be designed without using a second stage dc–dc. They provide unity power factor correction solutions with a 10 ms (8.33 ms) maximum dynamic response of the output voltage. So the use of only PFC preregulator is another option to design a complete power supply for some specific cases. However, some restrictions must be considered in this application: hold-up time must not be required, the output voltage must be sufficiently high due to the real bulk capacitor characteristics and the dynamic requirements can be achieved by the PFC preregulator. REFERENCES [1] M. M. Jovanovic and D. E. Crow, “Merits and limitations of full-bridge rectifier with LC filter in meeting IEC-1000-3-2 harmonic limit specifications,” IEEE Trans. Ind. Appl., vol. 33, no. 2, pp. 551–557, Mar./Apr. 1997. [2] V. Vorperian and R. B. Ridley, “A simple scheme for unity powerfactor rectification for high frequency AC buses,” IEEE Trans. Power Electron., vol. 1, no. 1, pp. 77–87, Jan. 1990. [3] W. H. Wolfle and W. G. Hurley, “Quasi-active power factor correction with a variable inductive filter: Theory, design and practice,” IEEE Trans. Power Electron., vol. 18, no. 1, pp. 248–255, Jan. 2003. [4] A. Fernandez, J. Sebastian, M. M. Hernando, P. Villegas, and J. García, “Helpful hints to select a power-factor-correction solution for low- and medium-power single-phase power supplies,” IEEE Trans. Ind. Electron., vol. 52, no. 1, pp. 46–55, Feb. 2005. [5] O. Garcia, J. A. Cobos, R. Prieto, P. Alou, and J. Uceda, “Power factor correction: A survey,” IEEE Trans. Power Electron., vol. 18, no. 3, pp. 749–755, May 2003. [6] J. Qian, Q. Zhao, and F. C. Lee, “Single-stage single-switch powerfactor-correction ac–dc converters with dc-bus voltage feedback for universal line applications,” IEEE Trans. Power Electron., vol. 13, no. 6, pp. 1079–1088, Nov. 1998. [7] J. Qian and F. C. Lee, “Voltage-source charge-pump power-factor-correction ac-dc converters,” IEEE Trans. Power Electron., vol. 14, no. 2, pp. 350–358, Mar. 1999. 641 [8] L. Huber and M. M. Jovanovic, “Design optimization of single-stage single-switch input-current shapers,” IEEE Trans. Power Electron., vol. 15, no. 1, pp. 174–184, Jan. 2000. [9] L. Huber and M. M. Jovanovic, “Single-stage single-switch input-current-shaping technique with reduced switching loss,” IEEE Trans. Power Electron., vol. 15, no. 4, pp. 681–687, Jul. 2000. [10] J. Sebastian, A. Fernandez, P. J. Villegas, M. M. Hernando, and J. M. Lopera, “Improved active input current shapers for converters with symmetrically driven transformer,” IEEE Trans. Ind. Appl., vol. 37, no. 2, pp. 592–600, Mar./Apr. 2001. [11] J. Sebastian, M. M. Hernando, A. Fernandez, P. J. Villegas, and J. Díaz, “Input current shaper based on the series connection of a voltage source and a loss-free resistor,” IEEE Trans. Ind. Appl., vol. 37, no. 2, pp. 583–591, Mar./Apr. 2001. [12] A. Fernandez, J. Sebastián, P. Villegas, M. M. Hernando, and D. G. Lamar, “Dynamic limits of a power factor preregulator,” IEEE Trans. Ind. Electron., vol. 52, no. 1, pp. 77–87, Feb. 2005. [13] H. Dixon, “Average current mode control of switching power supplies,” presented at the Unitrode Switching Regulator Power Supply Design Seminar (SEM 700), 1990. [14] L. H. Dixon, “High power factor pre-regulators for off-line power supplies,” presented at the Unitrode Switching Regulator Power Supply Design Seminar (SEM 700), 1990. [15] P. C. Todd, “UC3854 controlled power factor correction circuit design,” in Unitrode Product & Applications Handbook. Merrimack, NH: Unitrode Corp., 1996, pp. 10;303–10;322. Diego G. Lamar (S’05) was born in Zaragoza, Spain, in 1974. He received the M.Sc. degree in electrical engineering from the University of Oviedo, Gijón, Spain, in 2003. In 2003, he became a Research Engineer at the University of Oviedo and since September 2005, he has been an Assistant Professor. His research interests are switching-mode power supplies, converter modeling, and power-factor-correction converters. Arturo Fernández (M’98) received the M.Sc. and Ph.D. degrees in electrical engineering from the Universidad de Oviedo, Gijón, Spain, in 1997 and 2000, respectively. In 1998, he joined the Universidad de Oviedo as an Assistant Professor and became an Associate Professor in 2003. Since 2007, he has been a Contractor at the European Space Agency and is currently working at the Power and Energy Conversion Division. He has been involved in around 20 power electronics research and development projects since 1997 and he has published over 50 technical papers. Regarding Power Factor Correction issues, he has been involved in the development of high power factor rectifiers for Alcatel and Chloride Power Protection. His research interests are switching-mode power supplies, low output voltage, converter modeling, high power factor rectifiers, and power electronics for space applications. Dr. Fernández is a member of the IEEE-PELS Spanish Chapter. Manuel Arias (S’05) was born in Oviedo, Spain, in 1980. He received the M.Sc. degree in electrical engineering from the University of Oviedo, Gijón, Spain in 2005 where he is currently pursuing the Ph.D. degree. Since February 2005, he has been a Researcher in the Electrical and Electronic Engineering Department, University of Oviedo, developing electronic systems for UPSs and electronic switching power supplies. Since February 2007, he has also been an Assistant Professor of electronics in the same University. His research interests include dc–dc converters, HF inverters, UPSs, and motor control. 642 IEEE TRANSACTIONS ON POWER ELECTRONICS, VOL. 23, NO. 2, MARCH 2008 Miguel Rodríguez (S’06) was born in Gijón, Spain, in 1982. He received the M.S. degree in telecommunication engineering from the University of Oviedo, Gijón, in 2006 where he is currently pursuing the Ph.D. degree. His research interests include dc–dc conversion, high frequency power conversion and power supply systems for RF amplifiers. Javier Sebastián (M’95) was born in Madrid, Spain, in 1958. He received the M.Sc. degree from the Polytechnic University of Madrid, in 1981 and the Ph.D. degree from the University of Oviedo, Gijón, Spain, in 1985. He was an Assistant Professor and an Associate Professor at both the Polytechnic University of Madrid and at the University of Oviedo. Since 1992, he has been with the University of Oviedo, where he is currently a Professor. His research interests are switching-mode power supplies, modelling of dc-to-dc converters, low output voltage dc-to-dc converters, and high power factor rectifiers. Marta María Hernando (M’94) was born in Gijón, Spain, in 1964. She received the M.S. and Ph.D. degrees in electrical engineering from the University of Oviedo, Gijón, Spain, in 1988 and 1992, respectively. She is currently an Associate Professor at the University of Oviedo. Her main interests include switching-mode power supplies and high-power factor rectifiers.