Proceedings World Bioenergy 2010
Proceedings World Bioenergy 2010
Proceedings World Bioenergy 2010
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in the adsorber is separated, carbon dioxide is adsorbed<br />
entirely and pure methane is obtained. Adsorption lasts<br />
for about 950 sec and is ended when breakthrough of<br />
carbon dioxide occurs.<br />
Figure 3: TSA process with desorption by indirect<br />
heating with hot water<br />
Desorption is achieved by heating the adsorbent<br />
indirectly with hot water. Thereby, water is heated and is<br />
let through tube bundles placed inside the adsorber. As a<br />
consequence, heat exchange between the hot water and<br />
the cold adsorbent takes place and heats the adsorbent.<br />
During the desorption step methane is desorbed at<br />
first. Methane comes to the most part from the space<br />
between the adsorbent grains (porosity approx. 45%) as<br />
well as from the space under the adsorber, since<br />
adsorption capacity of the adsorbent with regard to<br />
methane is quite low. The peak of carbon dioxide<br />
desorption occurs after methane desorption, but after this<br />
peak the flow rate of carbon dioxide decreases steadily<br />
and in the end remains at a very low level. Desorption<br />
lasts about 2000 s what is twice as long as adsorption<br />
time.<br />
Referring to temperature, the temperature increase<br />
during the adsorption step indicates the arrival of the<br />
adsorption layer. Adsorption is an exothermic process, so<br />
heat is released and it heats the adsorbent. This<br />
phenomenon can be clearly seen with the steep rise of the<br />
temperature of 30°C. Although cold water is applied<br />
during the entire adsorption step, its coolness is not<br />
sufficient in order to carry off the released heat.<br />
Nevertheless, cold water application has an effect<br />
because after the peak the temperature decreases very fast<br />
and this allows adsorption to take place for a prolonged<br />
time period. Temperature during desorption increases<br />
steadily but it takes about 2000 s in order to get to a<br />
temperature of 70°C.<br />
Regarding the following cycles of this experiment,<br />
adsorption capacity in each of them decreased to one<br />
third of the capacity in the first cycle. The reason for this<br />
lies in the only partial desorption of carbon dioxide.<br />
Desorption by heating with hot water does not allow<br />
complete desorption of the entire adsorbed gas<br />
components; only partial desorption, correlated to the<br />
equilibrium and adsorption capacities at certain<br />
temperatures, is possible.<br />
Desorption by indirect heating with water is<br />
considered as a very inefficient way of desorption due to<br />
long desorption time as well as low desorption efficiency.<br />
7.2 Desorption by indirect heating with hot water and<br />
afterwards purging<br />
Figure 4 depicts the TSA process with desorption<br />
82 world bioenergy <strong>2010</strong><br />
carried out by indirect heating with hot water and<br />
afterwards purging with nitrogen.<br />
This process is very similar to that described above<br />
with one difference occurring not until the end of the<br />
desorption step.<br />
During the adsorption step separation performance is<br />
excellent as well and also here adsorption lasts for about<br />
950 s. Within the first 2000 s of desorption, desorption is<br />
also carried out indirectly by application of hot water<br />
functioning as heat exchange medium. The characteristics<br />
of desorbed gases are similar too, with methane<br />
desorbing at first followed by carbon dioxide.<br />
Figure 4: TSA process with desorption by indirect<br />
heating with hot water and afterwards purging<br />
After 2000 s of indirect heating, no more desorption<br />
of methane or carbon dioxide takes place. As already<br />
explained above, complete desorption is not achievable<br />
by indirect heating and therefore purge gas (N 2) was<br />
applied, for about 200 s. Desorption with purge gas<br />
allows complete desorption due to changes in partial<br />
pressure and the correlated adsorption capacity at<br />
equilibrium. As a consequence, still adsorbed gas<br />
components should theoretically be desorbed. Figure 4<br />
shows clearly that application of purge gas leads to<br />
further desorption of gas components. Obviously, the<br />
desorbed gas consists for the most part of carbon dioxide<br />
but also contains small amounts of methane.<br />
Regarding temperature, during the desorption step of<br />
indirect heating with hot water, temperature increases<br />
steadily but during purging temperature decreases again,<br />
although the purge gas is preheated to 75°C. The reason<br />
for temperature decrease is the desorption process itself<br />
which is of endothermic nature. Desorption of this<br />
remarkable amount carbon dioxide and methane needs<br />
energy and this causes temperature decrease.<br />
Referring to the following cycles of this experiment,<br />
adsorption capacity in each of them decreased only by<br />
approximately 1 w% compared to the capacity in the first<br />
cycle.<br />
Desorption by indirect heating with water is<br />
considered as a rather inefficient. However, application<br />
of purge gas led to further desorption of methane and<br />
carbon dioxide, what causes extended adsorption<br />
capacities (compared to desorption only with hot water)<br />
in the following cycles and therefore improves the entire<br />
process efficiency.<br />
7.3 Desorption by indirect heating with hot water and<br />
simultaneous direct heating with purge gas<br />
Figure 5 illustrates the TSA process with desorption<br />
carried out by indirect heating with hot water and<br />
simultaneous direct heating with purge gas.