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96 3 Physical Principles <strong>of</strong> Sensing<br />

the other point at 96 degrees which is “…found in the blood <strong>of</strong> a healthy man…”. 14<br />

On his scale, the melting point <strong>of</strong> water was at 32 ◦ and boiling at 212 ◦ . In 1742,<br />

Andreas Celsius, pr<strong>of</strong>essor <strong>of</strong> astronomy at the University <strong>of</strong> Uppsala, proposed a<br />

scale with zero as the melting point <strong>of</strong> ice and 100 at the boiling point <strong>of</strong> water.<br />

Currently, in science and engineering, Celsius and Kelvin scales are generally<br />

employed. The Kelvin scale is arbitrarily based on the so-called triple point <strong>of</strong> water.<br />

There is a fixed temperature at a unique pressure <strong>of</strong> 4.58 mm Hg, where water vapor,<br />

liquid, and ice can coexist. This unique temperature is 273.16 K (kelvin) which<br />

approximately coincides with 0 ◦ C. The Kelvin scale is linear with zero intercept (0<br />

K) at a lowest temperature where the kinetic energy <strong>of</strong> all moving particles is equal<br />

to zero. This point cannot be achieved in practice and is a strictly theoretical value.<br />

It is called the absolute zero. Kelvin and Celsius scales have the same slopes 15 (i.e.,<br />

1 ◦ C=1 Kand0K=−273.15 ◦ C):<br />

◦ C = ◦ K − 273.15 ◦ (3.107)<br />

The boiling point <strong>of</strong> water is at 100 ◦ C=373.15 K. A slope <strong>of</strong> the Fahrenheit scale is<br />

steeper, because 1 ◦ C=1.8 ◦ F. The Celsius and Fahrenheit scales cross at temperature<br />

<strong>of</strong> −40 ◦ C and ◦ F. The conversion between the two scales is<br />

◦ F = 32 + 1.8 ◦ C, (3.108)<br />

which means that at 0 ◦ C, temperature in the Fahrenheit scale is +32 ◦ F.<br />

3.11.2 Thermal Expansion<br />

Essentially, all solids expand in volume with an increase in temperature. This is a result<br />

<strong>of</strong> vibrating atoms and molecules. When the temperature goes up, an average distance<br />

between the atoms increases, which leads to an expansion <strong>of</strong> a whole solid body. The<br />

change in any linear dimension (length, width, or height) is called a linear expansion.<br />

A length, l 2 , at temperature, T 2 , depends on length, l 1 , at initial temperature T 1 :<br />

l 2 = l 1 [1 + α(T 2 − T 1 )], (3.109)<br />

where α, called the coefficient <strong>of</strong> linear expansion, has different values for different<br />

materials. It is defined as<br />

α = l 1<br />

l T , (3.110)<br />

14 After all, Fahrenheit was a toolmaker and for him 96 was a convenient number because to<br />

engrave the graduation marks he could easily do so by dividing by 2: 96, 48, 24, 12, and<br />

so forth. With respect to nationality <strong>of</strong> the blood, he did not care if it was <strong>of</strong> Englishman or<br />

not. Now, it is known that the blood temperature <strong>of</strong> a healthy person is not really constant<br />

and varies between approximately 97 ◦ F and 100 ◦ F (36 ◦ C and 37.7 ◦ C), but during his time<br />

he did not have a better thermostat than the human body.<br />

15 There is a difference <strong>of</strong> 0.01 ◦ between Kelvin and Celsius scales, as Celsius’ zero point is<br />

defined not at a triple point <strong>of</strong> water as for the Kelvin, but at temperature where ice and<br />

air-saturated water are at equilibrium at atmospheric pressure.

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