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Exergy saving and exergy production in municipal wastewater ...

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<strong>Exergy</strong> <strong>sav<strong>in</strong>g</strong> <strong>and</strong> <strong>exergy</strong> <strong>production</strong> <strong>in</strong> <strong>municipal</strong> <strong>wastewater</strong> treatment<br />

human or the system will disappear. This heat dra<strong>in</strong> has been called as<br />

the energy tax which if it gets elim<strong>in</strong>ated the system will collapse<br />

(Bendoricchio, 1997).<br />

The system tends to <strong>in</strong>crease the negative entropy or negentropy<br />

(produce more ordered or higher quality material) <strong>in</strong>side itself <strong>in</strong> order to<br />

survive. This k<strong>in</strong>d of system is called dissipative system as Prigog<strong>in</strong>e<br />

def<strong>in</strong>es <strong>and</strong> it dissipates energy <strong>and</strong> entropy. The methods that are used<br />

<strong>in</strong> the food science for analyz<strong>in</strong>g the calorie-contents can also be used<br />

for the <strong>wastewater</strong> treatment plant <strong>in</strong> order to evaluate the processes,<br />

flows <strong>and</strong> storages (Bendoricchio, 1997). The rate of flow of useful<br />

energy is power <strong>and</strong> <strong>in</strong> SI system it can be measured by joules per unit of<br />

time or watt<br />

1.6. Thermodynamic view of the treatment plant<br />

In biological treatment units <strong>in</strong> a treatment plant, the bacteria digest the<br />

biodegradable material flow<strong>in</strong>g <strong>in</strong> the treatment plant <strong>and</strong> use them to<br />

run the catabolic <strong>and</strong> anabolic reactions of their cells.<br />

If the microorganism is imag<strong>in</strong>ed as a human body its metabolism can be<br />

described with the above described view us<strong>in</strong>g classical thermodynamic<br />

concepts like entropy, Gibb’s free energy <strong>and</strong> enthalpy. This way<br />

thermodynamic science can tell if a specific biological reaction is possible<br />

to happen (Von Stockar et al, 2006). The biological life <strong>in</strong> the treatment<br />

plant can also be a basis for description of treatment plant as a human<br />

body which metabolizes <strong>wastewater</strong>.<br />

Another view to the treatment plant can be achieved from the<br />

description of the ecosystem by Odum where <strong>in</strong> his book he says “an<br />

entity can be considered an ecosystem as long as the major components<br />

are present <strong>and</strong> operate together to achieve some sort of functional<br />

stability, even if for only a short period of time.” He mentions that the<br />

ma<strong>in</strong> feature of all the ecosystems is that <strong>in</strong> all of the ecosystems<br />

autotrophic <strong>and</strong> heterotrophic components have <strong>in</strong>teraction with each<br />

other (Odum et al, 2004). This is similar to what is happen<strong>in</strong>g <strong>in</strong> the<br />

treatment plant. The pollution enter<strong>in</strong>g the treatment plant <strong>in</strong>troduces<br />

entropy <strong>in</strong>to the facility which turns <strong>in</strong>to <strong>in</strong>formation <strong>and</strong> ATP (<strong>exergy</strong>)<br />

<strong>in</strong> the microorganisms through their respiration process.<br />

The Second law of thermodynamic which describes the entropy change<br />

of an open system is as follows:<br />

d S(t) = d e S(t) + d i S(t) (2)<br />

d e S(t) = Entropy provided by the surround<strong>in</strong>g to the system (Entropy<br />

flow) associated with the flow of energy <strong>and</strong> matter<br />

d i S(t) = The entropy produced <strong>in</strong>side the system by<br />

irreversible processes<br />

d i S(t) = dQ(t)/T(t) (3)<br />

dQ (t)= heat <strong>production</strong> caused by irreversible processes <strong>in</strong>side<br />

the system<br />

T (t) = current temperature (◦K) at a given po<strong>in</strong>t <strong>in</strong> the system<br />

Β = dS/dt = (d e S)/dt+ (d i S)/dt (4)<br />

β = rate of entropy <strong>production</strong> or energy dissipation<br />

(dissipative function)<br />

This law says d iS must be zero for reversible transformations <strong>and</strong> should<br />

be positive for irreversible transformation of the system. However,<br />

can be zero, positive or negative for an open system. For adiabatic<br />

7

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