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New trends in physics teaching, v.4; The ... - unesdoc - Unesco

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<strong>New</strong> Trends <strong>in</strong> Physics Teach<strong>in</strong>g IV<br />

This statement conta<strong>in</strong>s the qualitative content of the second law of thermodynamics. Accord<strong>in</strong>g<br />

to Brillou<strong>in</strong> [3, p.3221, ‘the <strong>in</strong>animate world, governed by <strong>physics</strong> and chemistry, obeys a<br />

natural law of degradation, of loss of value. This law sums up the essentials of thermodynamics,<br />

but the notion of value rema<strong>in</strong>s l<strong>in</strong>ked to. . . energy. Physics has not been able to (and probably<br />

cannot) separate these two entities.’<br />

THE QUALITATIVE CONCEPT OF ENERGY DEGRADATION<br />

~<br />

In order to compare different processes with respect to their different degrees of degradation, the<br />

concept itself must be made more precise. This requires us to free the valuation of energetic<br />

processes from their subjective attributes. This cannot be done without <strong>in</strong>troduc<strong>in</strong>g a certa<strong>in</strong><br />

artificiality <strong>in</strong> explanation which must be accepted as the price we pay for a ga<strong>in</strong> <strong>in</strong> .precision.<br />

As may be concluded from the examples given above, degradation consists (objectively) of a<br />

k<strong>in</strong>d of irrevocable change; one which cannot be undone. <strong>The</strong> cool<strong>in</strong>g of the hot water <strong>in</strong> a cold<br />

room is no more reversible than is the transformation of the k<strong>in</strong>etic energy of a motor-car <strong>in</strong>to<br />

thermal energy of its surr0und<strong>in</strong>gs.l<br />

To object that the mechanical energy of the motor-car could be recovered by the consumption<br />

of additional chemical energy of petrol and that the cooled water can be re-heated is <strong>in</strong>valid. For,<br />

<strong>in</strong> addition to restor<strong>in</strong>g the orig<strong>in</strong>al states, there is an <strong>in</strong>crease <strong>in</strong> the thermal energy of the<br />

surround<strong>in</strong>gs and an equal decrease <strong>in</strong> the chemical energy of the petrol <strong>in</strong> the first case and a<br />

further <strong>in</strong>put of electrical energy <strong>in</strong> the second case.<br />

A process is accompanied by a degradation of energy if it cannot be reversed<br />

without caus<strong>in</strong>g an additional change <strong>in</strong> its surround<strong>in</strong>gs. (2)<br />

Such irreversible, energy-degrad<strong>in</strong>g processes which run spontaneously <strong>in</strong> a certa<strong>in</strong>, natural<br />

direction we shall call ‘spontaneous processes’.<br />

Extend<strong>in</strong>g this consideration to composite processes, proposition (2) even holds <strong>in</strong> situations<br />

where a part of a whole process consists of a process runn<strong>in</strong>g opposite to its natural direction<br />

(e.g. the objection already referred to).<br />

Revers<strong>in</strong>g the ‘cool<strong>in</strong>g of water’, i.e. the ‘heat<strong>in</strong>g of water’ comb<strong>in</strong>ed with the ‘consumption<br />

of electrical energy’ considered as a whole, is a process which runs down without caus<strong>in</strong>g any<br />

additional change <strong>in</strong> the surround<strong>in</strong>gs and, therefore, gives rise of an energy degradation.<br />

Thus although the spontaneous process ‘cool<strong>in</strong>g of water’ is reversed and therefore accompanied<br />

by an upgrad<strong>in</strong>g of energy, it may take place because simultaneously, another process, ‘the consumption<br />

of electrical energy’ is runn<strong>in</strong>g down provid<strong>in</strong>g for an even larger degradation. Overall,<br />

a small degradation results.<br />

Or, more generally:<br />

<strong>The</strong> energy degradation due to a spontaneous process a is greater than that due to a<br />

second spontaneous process /3 if a can drive /3 backwards (i.e. <strong>in</strong> the opposite direction<br />

to the natural one). This implies that the degradation of energy associated with a<br />

exceeds the upgrad<strong>in</strong>g of energy due to the reversed process 0, (3)<br />

1. In the follow<strong>in</strong>g pages, the processes which are fully described as ‘cool<strong>in</strong>g of a hot system by transferr<strong>in</strong>g energy to the<br />

sunound<strong>in</strong>gs’ and ‘brak<strong>in</strong>g a mov<strong>in</strong>g system by transferr<strong>in</strong>g energy to the surround<strong>in</strong>gs’ are sometimes abbreviated to ‘cool<strong>in</strong>g’<br />

and ‘brak<strong>in</strong>g’.<br />

60

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