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European Journal of Scientific Research - EuroJournals

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A Predictive Current Control Technique on Fuel Cell Based Distributed<br />

Generation in a Standalone AC Power Supply 892<br />

1. Introduction<br />

Previous empirical research provides contradictory and inconclusive evidence on the value relevance<br />

<strong>of</strong> comprehensive income disclosures promulgated in different countries. Thus, present study using<br />

comprehensive income <strong>of</strong> Iranian firm's data shed more lights on the issue.<br />

Fuel cells are devices capable <strong>of</strong> converting chemical energy into heat and dc electrical energy<br />

by means <strong>of</strong> the oxidation <strong>of</strong> a fuel, usually hydrogen (Padulles et al, 2000). Distributed generation<br />

(DG) technologies can provide energy solutions to some customers that are more cost-effective, more<br />

environmentally friendly, or provide higher power quality or reliability than conventional solutions.<br />

The voltage <strong>of</strong> fuel cell stack decreases largely as the load current increase, and the voltage increases<br />

as the temperature increase at the same current. Thus DGS should be interfaced with Power Electronic<br />

systems such as DC to DC or/and DC to AC power converters to obtain a sinusoidal AC output voltage<br />

with fixed frequency from variable or high-frequency AC voltage sources or DC voltage sources<br />

(Haiping et al, 2005). So the DC-DC converter plays a key role in making the fuel cell DC power<br />

available for stand-alone applications.<br />

To boost low output DC voltage <strong>of</strong> the fuel cell to high DC voltage, a forward DC to DC boost<br />

converter, a push-pull DC to DC boost converter or an isolated full-bridge DC to DC power converter<br />

can be selected. In addition, various topologies such as the H-bridge series resonant buck and boost<br />

converters have been presented in (Blaabjerg et al, 2004). Anderson et al, (2002) present a current fed<br />

push-pull converter. This topology decreases the conduction losses in the switches due to the low fuel<br />

cell voltage. Nergaard et al, (2002) suggest an interleaved front-end boost converter. This topology<br />

considerably reduces the current ripple flowing into the fuel cell. A dual loop control strategy (current<br />

and voltage loop) has been used for the interleaved converter. Jung et al, (2005;2005) introduce a Zsource<br />

converter. This is a new concept in which a shoot-through vector directly steps up the DC<br />

source voltage without using a boost DC-DC converter. The boost voltage rate depends on the total<br />

duration <strong>of</strong> the shoot-through zero vectors over one switching period Jung et al, (2005). Also, In<br />

reference (Wang and Nehrir, 2006) a non-isolated boost converter with a conventional PI controller has<br />

been used for the converter control. Akkinapragada (2007) had been employed a non-isolated buckboost<br />

DC-DC converter with a closed loop PWM (pulse width modulation) control strategy as<br />

described in Reference (Mohan et al, ). The reference (Duran-Gomez et al, 2006) had been presented<br />

an approach to convert the generated dc output voltage <strong>of</strong> a PV cell array into a higher regulated dc<br />

voltage. The approach employs a series-combined connected boost and buck boost dc-dc converter for<br />

power conditioning <strong>of</strong> the dc voltage provided by a photo-voltaic array. Chandrasekaran and Gokdere<br />

(2004) introduce a novel composite integrated magnetic (IM) core structure, which minimizes inductor<br />

current ripple. Their subject is a compact, IM core structure for a three-phase interleaved, DC-DC<br />

boost converter that feeds <strong>of</strong>f the fuel cell output and can provide a programmable, regulated, high<br />

voltage DC bus for the distributed power system.<br />

In recent years, the higher efficiency and the more advanced power conversion, energy<br />

utilization equipment, a variety <strong>of</strong> circuit topologies <strong>of</strong> the s<strong>of</strong>t-switching DC-DC power converter are<br />

urgently required. The reference (Ogura et al, 2003) has introduced a boost type ZVS-PWM chopperfed<br />

DC-DC power converter with a single active auxiliary resonant snubber in the load side for the<br />

power interface <strong>of</strong> solar photovoltaic and fuel cell power conditioners. The character <strong>of</strong> this boost type<br />

ZVS-PWM chopper-fed DC-DC power converter is feasible. Also, a unidirectional isolated full-bridge<br />

DC to DC power converter can be used to boost low fuel cell voltage (Bendre et al, 2003; Aydemir,<br />

2002; Kim et al, 1997; Jain et al, 2002; Brunoro and Vieira, 1999; Jeon and Cho, 2001). In addition, a<br />

bidirectional full-bridge DC to DC power converter can be used for stepping up low battery voltage or<br />

stepping down high-voltage-side DC link according to battery discharge or recharge mode (Peng et al,<br />

2004; Jiang and Dougal, 2003). Among the presented power converters, two phase-shifted full-bridge<br />

DC to DC converters, which are one <strong>of</strong> the most attractive topologies for high power generation are<br />

adopted as described in (Jung, 2005; Keyhani and Jung, 2004) with a unidirectional full-bridge DC to<br />

DC boost converter for the fuel cell and a bidirectional full-bridge DC to DC boost/buck converter for

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