The schematic diagram of a constant-volume gas thermometer is shown in Fig.1. The
volume of an ideal gas in the sensing bulb D is kept constant by adjusting the level of
mercury in the arm B of the manometer. The arm B and the arm A are connected by a
flexible tube to form a U-tube manometer. The arm B is also connected to the gas bulb
D via a capillary tube C, while the other arm A of the manometers is open to
atmosphere and can be moved vertically to adjust the mercury level, so the mercury
just touches the mark L of the capillary. The pressure in the bulb b is used as a
thermometric property and can be given by
The gas bulb D is first placed in constant-temperature bath at the triple point
temperature of water and the level of mercury is adjusted to touch the mark L by
moving the manometer arm A up and down.
As the volume of the bulb becomes constant and the height difference of the mercury
in the two arms is recorded as the pressure, corresponding to the mercury column
at the triple point.
Now the bulb is brought in contact with a system whose temperature T, is to be
measured. Again, in a similar manner, by keeping the volume of gas in the bulb
constant, the height difference of the mercury in the two arms is recorded and the
corresponding new pressure p is calculated by Eq. (2).
From the ideal gas equation, the new temperature is given by
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