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In vapor-compression refrigeration the work of compression is usually supplied by an electric motor But the source of the electric energy for the motor is probably a heat engine (central power plant) used to drive a generator Thus the work for refrigeration comes ultimately from heat at a high temperature level This suggests the direct use of heat as the energy source for refrigeration The absorption-refrigeration machine is based on this idea The work required by a Carnot refrigerator absorbing heat at temperature Tc and rejecting heat at the temperature of the surroundings, here designated Ts, follows from Eqs (92) and (93):

When it is told to enter a runlevel, init executes a script, as dictated by the /etc/inittab file The default runlevel that the system boots into is determined by the initdefault entry in the /etc/inittab file If, for example, the entry in the file is

where I Qc I is the heat absorbed If a source of heat is available at a temperature above that of the surroundings, say at T H ,then work can be obtained from a Carnot engine operating between this temperature and the surroundings temperature Ts The heat required I QHI for the production of work I W I is found from Eq (58):

id:3:initdefault:

= lwl-

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I created a new VARIABLE block called Pressed that holds a Logic value. I next drop a VARIABLE block after the NXT BUTTONS SENSOR block. I choose my new variable, Pressed, and in the Action section, I choose Write. I also drag a data wire out of the NXT BUTTONS SENSOR block s output data plug into the input data plug on the VARIABLE block (see Figure 18-13).

this means that the system will boot into runlevel 3 But if, on the other hand, the entry in the file is

Substitution for ( W ( gives:

id:5:initdefault:

The value of I QH1 Qc I given by this equation is of course a minimum, because Carnot cycles 1 1 cannot be achieved in practice A schematic diagram for a typical absorption refrigerator is shown in Fig 94 The essential difference between a vapor-compression and an absorption refrigerator is in the different means employed for compression The section of the absorption unit to the right of the dashed line in Fig 94 is the same as in a vapor-compression refrigerator, but the section to the left accomplishes compression by what amounts to a heat engine Refrigerant as vapor from the evaporator is absorbed in a relatively nonvolatile liquid solvent at the pressure of the evaporator and at relatively low temperature The heat given off in the process is discarded to the surroundings at Ts This is the lower temperature level of the heat engine The liquid solution from the absorber, which contains a relatively high concentration of refrigerant, passes to a pump, which raises the pressure of the liquid to that of the condenser Heat from the higher temperature source at THis transferred to the compressed liquid solution, raising its temperature

this means the system will boot into runlevel 5, with the X Window subsystem running with a graphical login screen

and evaporating the refrigerant from the solvent Vapor passes from the regenerator to the condenser, and solvent, which now contains a relatively low concentration of refrigerant, returns to the absorber The heat exchanger conserves energy and also adjusts stream temperatures toward proper values Low-pressure steam is the usual source of heat for the regenerator The most commonly used absorption-refrigeration system operates with water as the refrigerant and a lithium bromide solution as the absorbent This system is obviously limited to refrigeration temperatures above the freezing point of water It is treated in detail by Perry and re en^ For lower temperatures ammonia can serve as refrigerant with water as the solvent An alternative system uses methanol as refrigerant and polyglycolethers as absorbent Consider refrigeration at a temperature level of [Tc = 26315 K (-10 C)] with a heat source of condensing steam at atmospheric pressure [TH = 37315 K (lOO C)] For a surroundings temperature of [Ts = 30315 K (30 C)], the minimum possible value of 1 QH11Qc 1 is 1 found from Eq (96):

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