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

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Entropy and Information<br />

society - one has to switch currents off and on as fast as possible. In each half wave of an alternat<strong>in</strong>g<br />

current, one bit of <strong>in</strong>formation can be stored (whether or not the half wave is at full<br />

amplitude). <strong>The</strong>refore, the feasibility of communication networks was l<strong>in</strong>ked historically to the<br />

progress of high-frequency technology. <strong>The</strong> highest requirements are posed by television. Each<br />

television picture consists of, say, 500 l<strong>in</strong>es conta<strong>in</strong><strong>in</strong>g 600 po<strong>in</strong>ts each, i.e. a total of 3 X 10’<br />

po<strong>in</strong>ts. If we assume, for the sake of simplicity, that each po<strong>in</strong>t can be either black or white, the<br />

total <strong>in</strong>formation content of one picture becomes 3 X IO5 bit. S<strong>in</strong>ce 25 pictures have to be<br />

transmitted per second, the total <strong>in</strong>formation flow becomes 7.5 X lo6 bit/s. From this we can<br />

easily calculate the band width required for the transmission of television pictures. S<strong>in</strong>ce each<br />

bit corresponds to a half wave, the total band width becomes<br />

Af=?hX7.5X 106/s~4MHz.<br />

<strong>The</strong> frequency f of the carrier signal should be at least f x l0OAf~ 400 MHz. From the relation<br />

fX=c we can now calculate the wavelength used <strong>in</strong> television:<br />

X=c/f= 3 X i08ms-l/4 X lo8 s-l x 1 m.<br />

Return<strong>in</strong>g to our examples from biology we can calculate to how many seconds of television<br />

commercials the genetic <strong>in</strong>formation conta<strong>in</strong>ed <strong>in</strong> man corresponds. S<strong>in</strong>ce roughly 1 O7 bit can<br />

be transmitted per second we obta<strong>in</strong> for the time T needed:<br />

lo7 bit/s X T = lo9 bit or T= 100 s.<br />

<strong>The</strong>refore it would take about two m<strong>in</strong>utes to transmit the genetic make-up of man <strong>in</strong> the form<br />

of a television commercial.<br />

In another example us<strong>in</strong>g television we can check the proverb: ‘A picture says more than a<br />

thousand words.’ One word conta<strong>in</strong>s about 30 bit of <strong>in</strong>formation, if we assume that it consists<br />

of six letters. <strong>The</strong>refore the <strong>in</strong>formation conta<strong>in</strong>ed <strong>in</strong> 1000 words is 3 X lo4 bit. Bear<strong>in</strong>g <strong>in</strong> m<strong>in</strong>d<br />

that one television picture conta<strong>in</strong>s about 3 X lo5 bit, it follows that one picture corresponds<br />

to roughly 10 000 words (or about 30 pages).<br />

In conclusion, we refer to another problem which can also be solved with the help of <strong>in</strong>formation<br />

theory. Of twelve balls, one ball is either heavier or lighter than the other eleven balls. <strong>The</strong><br />

object is to f<strong>in</strong>d out, us<strong>in</strong>g a balance, which ball is the odd one out and whether it is heavier or<br />

lighter than the rest. This problem is clearly one of miss<strong>in</strong>g <strong>in</strong>formation, which is to be ga<strong>in</strong>ed by<br />

us<strong>in</strong>g the balance. How many times do the balls have to be weighed <strong>in</strong> order to supply the miss<strong>in</strong>g<br />

<strong>in</strong>formation? 171.<br />

ENTROPY AND INFORMATION<br />

With the help of the metric concept of <strong>in</strong>formation we can characterize the <strong>in</strong>formation miss<strong>in</strong>g<br />

about thermodynamic systems. While a detailed knowledge of the <strong>in</strong>itial positions and velocities<br />

of all mass po<strong>in</strong>ts conta<strong>in</strong>ed <strong>in</strong> an n-body problem is assumed <strong>in</strong> mechanics, the exact positions<br />

and velocities of the numerous molecules conta<strong>in</strong>ed <strong>in</strong> a gas or another thermodynamic system<br />

are never known exactly. This lack of <strong>in</strong>formation about thermodynamic systems is described<br />

by entropy.<br />

At first it might seem that the lack of knowledge about the <strong>in</strong>itial conditions of the molecules<br />

43

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