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 "T_{tp}" 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 "h_{tp}" the pressure, "p_{tp}" 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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