AITCOOL Model ADG-01 Pirani Digital Vacuum Gauge



  • Maximum Over pressure : 14PSI/96kPa
  • Resolution: 1 Micron < 30,000 microns)
  • Accuracy: +- 5% of reading (2-100pa) at 20 DegC
  • Operating Temperature: 0-50 Deg C
  • Units of Measurement; Pa, mbar, Torr, Microns
  • Refresh Rate: 0.5 seconds
  • Connection 1/4″ SAE Female , brass with depressor and Teflon Seals for long life
  • Sensor; Genuine Pirani Sensor
  • Power: Lithium Battery (rechargeable) 1800mah (standby time -approx 80 hours)
  • Charging parameters: 5V 1A, charging time approx 3-4 hours, Micro USB cable supplied
  • Auto Power off: 10 minutes
  • Other functions: Accoustic-opto alarm, leakage alarm and Timer


7 in stock

SKU: ADG-01 Category: Tag:


This Vacuum Gauge from AITCOOL Model ADG-01 is fitted with a genuine “Pirani Professional Vacuum Sensor” which features high accuracy across the full measurement range and low sensitivity to Oil and other contaminants. A carry bag is provided to protect the instrument from moisture and dust etc.

The gauge provides an audio signal when the target vacuum is reached and again when the lower Vacuum Limit is reached following shut-off.

This feature provides the user with an indication of system leakage rate.

The built in timer also keeps track of total time to reach target vacuum level.

Pirani gauge – A Thermal conductivity Gauge

Basic principle of Pirani gauge

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 (that is, lower pressure of the surrounding media, lower will be its density). 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.

Description of Pirani gauge

Pirani gauge

The main parts of the arrangement are:

  1. A Pirani gauge chamber which encloses a platinum filament.
  2. A compensating cell to minimize variation caused due to ambient temperature changes.
  3. The Pirani gauge chamber and the compensating cell is housed on a wheat stone bridge circuit as shown in diagram.

Operation of Pirani gauge

  1. 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.
  2. 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. Due to this change in density of the surrounding of the filament its conductivity changes causing the temperature of the filament to change.
  3. When the temperature of the filament changes, the resistance of the filament also changes.
  4. Now the change in resistance of the filament is determined using the bridge.
  5. 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] and vice versa.

Applications of Pirani gauge

Used to measure low vacuum and ultra high vacuum pressures.

Advantages of Pirani gauge

  1. They are rugged and inexpensive
  2. Give accurate results
  3. Good response to pressure changes.
  4. Relation between pressure and resistance is linear for the range of use.