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The relevance of energy storages for an autarky of electricity supply ...

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generation, but novel materials are needed to reduce the temperature <strong>of</strong> operation.<br />

Stationary fuel cells are suitable <strong>for</strong> distributed power generation sited close to the<br />

customer load. Furthermore, costly investments in tr<strong>an</strong>smission <strong>an</strong>d distribution<br />

system upgrades c<strong>an</strong> be eliminated. (Barbir, 2007; Ellison, 2011)<br />

Storage<br />

Hydrogen has <strong>an</strong> enormous volume <strong>of</strong> 11 m 3 per kg at ambient temperature. To<br />

increase density, it has to be either compressed or the temperature has to be<br />

decreased below the critical temperature or repulsion is reduced by interaction with<br />

<strong>an</strong>other material. Hydrogen has a good <strong>energy</strong> density by weight (33.3 – 38 Wh/kg)<br />

but poor <strong>energy</strong> density by volume (2.5 Wh/l). <strong>The</strong>re<strong>for</strong>e, under normal conditions it<br />

requires about 3000 times more space th<strong>an</strong> gasoline <strong>for</strong> <strong>an</strong> equivalent amount <strong>of</strong><br />

<strong>energy</strong>. Hydrogen c<strong>an</strong> be stored in several different ways: as gaseous hydrogen in<br />

high-pressure t<strong>an</strong>ks, as liquid hydrogen in insulated t<strong>an</strong>ks or as protons in solids.<br />

Traditionally high pressure storage t<strong>an</strong>ks have been made out <strong>of</strong> steel but recently<br />

new fibre rein<strong>for</strong>ced composite materials have been developed that c<strong>an</strong> withst<strong>an</strong>d<br />

internal pressures up to 5,000 – 10,000 PSI. Even at such high pressures hydrogen<br />

has a relatively large volume, about twice that <strong>of</strong> liquid hydrogen. Hydrogen c<strong>an</strong> be<br />

stored liquid in thermally insulated containers at a temperature below 20.3 K. Liquid<br />

hydrogen has the huge disadv<strong>an</strong>tage that the process <strong>of</strong> liquefaction requires about<br />

30 – 40 % <strong>of</strong> the final <strong>energy</strong> content <strong>of</strong> the hydrogen. Furthermore, liquid hydrogen<br />

has to be consumed in rather a short time, as it continuously boils-<strong>of</strong>f. Hydrogen c<strong>an</strong>,<br />

furthermore, be stored in solids, which are called metal hydrids. <strong>The</strong> hydrogen is<br />

stored as protons (H + ) ions in this case. As the electrical charge in solids must always<br />

be bal<strong>an</strong>ced, <strong>an</strong> equal number <strong>of</strong> extra electrons exist. <strong>The</strong> capacity depends upon the<br />

amount <strong>of</strong> hydrogen the material c<strong>an</strong> absorb in their crystal structures. Normally heat<br />

arises during loading, which has to be removed to avoid a reduction <strong>of</strong> the storage<br />

capacity. Adding heat or lowering the pressure c<strong>an</strong> afterwards extract hydrogen from<br />

the solid. Table 4.4 summarizes the main figures <strong>of</strong> different storage media.<br />

(Huggins, 2010; Rummich, 2009; Ellison, 2011; Züttel, 2008)<br />

29

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