28.02.2013 Views

Building Design and Construction Handbook - Merritt - Ventech!

Building Design and Construction Handbook - Merritt - Ventech!

Building Design and Construction Handbook - Merritt - Ventech!

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

13.10 SECTION THIRTEEN<br />

Hence, this first law of thermodynamics can be expressed mathematically by the<br />

following equation:<br />

W � JQ (13.4)<br />

where W � work, ft-lb<br />

J � Joule’s constant � mechanical equivalent of heat<br />

Q � heat, Btu, generated by the work<br />

Experiments have shown that the mechanical equivalent of heat, known as Joule’s<br />

constant, is equivalent to 778 ft-lb/Btu. The first law is also known as the law of<br />

conservation of energy.<br />

The second law of thermodynamics states that it is impossible for any machine<br />

to transfer heat from a substance to another substance at a higher temperature (if<br />

the machine is unaided by an external agency). This law can be interpreted to imply<br />

that the available supply of energy for doing work in our universe is constantly<br />

decreasing. It also implies that any effort to devise a machine to convert a specific<br />

quantity of heat into an equivalent amount of work is futile.<br />

Entropy is the ratio of the heat added to a substance to the absolute temperature<br />

at which the heat is added.<br />

where S � entropy<br />

dQ � differential of heat (very small change)<br />

T a � absolute temperature<br />

dQ<br />

S � (13.5)<br />

T a<br />

The second law of thermodynamics can be expressed mathematically with the<br />

use of the entropy concept.<br />

Suppose an engine, which will convert heat into useful mechanical work, receives<br />

heat Q 1 from a heat source at temperature T 1 <strong>and</strong> delivers heat Q 2 at a<br />

temperature T 2 to a heat sink after performing work. By the first law of thermodynamics,<br />

the law of conservation of energy, Q 2 is less than Q 1 by the amount of<br />

work performed. And by the second law of thermodynamics, T 2 is less than T 1.<br />

The universe at the start of the process loses entropy �S 1 � Q 1/T 1 <strong>and</strong> at the end<br />

of the process gains entropy �S 2 � Q 2/T 2. Hence, the net change in the entropy of<br />

the universe because of this process will be �S 2 � �S 1.<br />

Furthermore, this law requires that this net change must always be greater than<br />

zero <strong>and</strong> that the entropy increase is <strong>and</strong> must always be an irreversible thermodynamic<br />

process.<br />

�S � �S � 0 (13.6)<br />

2 1<br />

Because of the irreversibility of the process, the energy that has become available<br />

for performing work is<br />

13.2.5 Absolute Temperature<br />

Q � T (�S � �S ) (13.7)<br />

u 2 2 1<br />

The definition of entropy given above involves the concept of absolute temperature<br />

measured on a ratio scale. The unit of absolute temperature is measured in degrees

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!