3. Content:
Definition
Define Thermal conductivity
History
Principle
Description
Working
Application
Advantages
Limitations
Alternative
References
4. Definition:
• The Pirani gauge is a robust thermal
conductivity gauge used for the
measurement of the pressures in vacuum
systems or in very low pressure region.
5. What is Thermal Conductivity
Gauge?
Thermal conductivity gauges measure pressure by
measuring the change in ability of a gas to
conduct heat.
• The ability of a material to carry heat by
conduction is called Thermal Conductivity.
6. History:
• It was invented in 1906 by Marcello Pirani.
• In 1906 he described his “Directly Indicating Vacuum
Gauge" that used a heated wire to measure vacuum by
monitoring the heat transfer from the wire by the
vacuum environment.
7. Principle:
• A conducting wire gets heated when electric
current flows through it.
The rate at which heat is dissipated from this
wire depends on the conductivity of the
surrounding media.
The conductivity of the surrounding media in
turn depends on the density of the surrounding
media
If the density of the surrounding media is low,
its conductivity also will be low causing the
wire to become hotter for a given current flow,
and vice versa.
8. Description:
The main parts of the arrangement are:
• A pirani gauge chamber which encloses a platinum
filament.
• A compensating cell to minimize variation caused
due to ambient temperature changes.
• The pirani gauge chamber and the compensating cell
is housed on a wheat stone bridge circuit as shown in
diagram.
9.
10. Working:
• A constant current is passed through the filament in
the pirani gauge chamber. Due to this current, the
filament gets heated and assumes a resistance which
is measured using the bridge.
• Now the pressure to be measured (applied pressure)
is connected to the pirani gauge chamber. Due to the
applied pressure the density of the surrounding of the
pirani gauge filament changes.
11. • Due to this change in density of the surrounding
of the filament its conductivity changes causing
the temperature of the filament to change.
• When the temperature of the filament changes,
the resistance of the filament also changes.
12. • Now the change in resistance of the filament is
determined using the bridge.
• This change in resistance of the pirani gauge
filament becomes a measure of the applied pressure
when calibrated.
Note: higher pressure – higher density – higher
conductivity – reduced filament temperature –
less resistance of filament & vise versa
13.
14. • The gauge may be used for pressures between 0.5
Torr to 10−4 Torr.
• The thermal conductivity and heat capacity of the
gas may affect the readout from the meter, and
therefore the apparatus may need calibrating
before accurate readings are obtainable.
• For lower pressure measurement other
instruments such as a Penning gauge are used.
15. Applications:
Used to measure low vacuum and ultra high
vacuum pressures.
Used to Plot graph on basis of data obtained.
Curve to convert Air reading into other Gases.
16.
17. Advantages:
• They are rugged and inexpensive
• Give accurate results
• Good response to pressure changes.
• Relation between pressure and resistance is linear
for the range of use.
• Readings can be taken from a distance.
18. Limitations:
• Pirani gauge must be checked frequently.
• Pirani gauge must be calibrated from different
Gases
• Electric power is a must for its operation.
19. Alternative:
An alternative to the Pirani gauge is
the thermocouple gauge, which works on the
same principle of detecting thermal conductivity
of the gas by a change in temperature.
In the thermocouple gauge, the temperature is
sensed by a thermocouple rather than by the
change in resistance of the heated wire.