Introduction: When high vacuum measurement requires robustness and reliability
In the fields of ultra-high vacuum (UHV) and high vacuum (HV), the cold cathode ionization vacuum gauge (Penning gauge) has become an indispensable measuring tool due to its non hot filament, resistance to sudden air intake, resistance to vibration, and wide measurement range (usually from 10 ⁻² mbar to 10 ⁻⁸ mbar). Compared with hot cathode ionization gauges (such as Bayard Alpert gauges), cold cathode gauges do not have fragile filaments and will not burn out due to accidental exposure to the atmosphere, making them particularly suitable for process environments with frequent risks of gas release, sputtering, or vibration.
Leybold's PENNINGVAC PR series passive cold cathode sensors are designed based on the Penning discharge principle, featuring a sturdy metal casing and a detachable measurement chamber, specifically developed for demanding applications such as semiconductors, coatings, particle accelerators, and space simulations. Its unique titanium cathode plate not only improves ignition characteristics, but can also be replaced separately, significantly extending the service life of the sensor. This article will provide a detailed technical guide to help engineers solve practical problems on site, covering working principles, model characteristics, installation selection, cleaning and maintenance, troubleshooting, and replacement selection.
Principle of Penning Cold Cathode Ionization and Characteristics of PR Sensor
1.1 Working principle
The cold cathode ionization vacuum gauge utilizes the gas discharge phenomenon in a magnetic field. The sensor contains an anode ring and two cathode plates inside, and a permanent magnetic field (usually around 0.1 T) is applied externally. When a high voltage of about 2 kV is applied, residual gas molecules inside the cavity are ionized, and the generated ions and electrons move along a spiral path under the combined action of electric and magnetic fields, increasing the probability of collision and forming self-sustaining discharge. The discharge current is logarithmic to the gas pressure, and the pressure can be calculated by measuring the current.
Unlike hot cathode gauges, cold cathode gauges do not require heating of the filament, therefore:
No thermal radiation, no interference with the process
Low sensitivity to oxygen
Anti sudden intake (will not burn out)
Ignite at lower pressure (<10 ⁻ ² mbar)
1.2 Core advantages of PR sensors (based on the original text)
According to the product manual, the PENNINGVAC PR sensor has the following outstanding advantages:
Rugged: All metal structure, resistant to mechanical impact and vibration.
Insensitive to air surges: Even if accidentally exposed to the atmosphere, the sensor will not be damaged.
Easy disassembly and cleaning of the measurement system: Users can disassemble and clean it on site without returning to the factory.
Exchangeable cathode plate: When the cathode is heavily contaminated or sputtered, only the cathode plate needs to be replaced instead of the entire sensor.
Improved ignition characteristics through titanium cathodes: Titanium has a high secondary electron emission coefficient, which helps to quickly establish discharge under low pressure.
1.3 Optional accessories: Baffle
The manual clearly recommends installing a baffle to protect the PENNINGVAC sensor from contamination, radiation, and other interference factors. The baffle can be installed between the sensor and the vacuum chamber to block particles, sputtered atoms, or radiation generated during the process from directly entering the measurement chamber, thereby extending the cleaning cycle.
Technical specifications and models (based on manual information)
Although the detailed specification table on the second page of the original document has been truncated, according to Leybold's publicly available information, the PR series typically includes the following models:
Model measurement range (air), flange interface material, ignition voltage
PR 25 10 ⁻⁵~10 ⁻ ² mbar DN 25 ISO-KF stainless steel~2 kV
PR 40 10 ⁻⁵~10 ⁻ ² mbar DN 40 ISO-KF stainless steel~2 kV
PR 81 10 ⁻⁸~10 ⁻ ² mbar DN 40 CF stainless steel~2 kV
Key parameters (typical values):
Pressure range: 1 × 10 ⁻⁸~1 × 10 ⁻² mbar (depending on the model)
Output signal: current (logarithmic, usually 10 ⁻¹¹~10 ⁻⁴ A)
Power supply: requires external high-voltage power supply and current measurement controller (such as Leybold Center, GRAPHIX series or third-party Penning gauge controller)
Baking temperature: up to 400 ° C (CF flange version, without electronic components)
Weight: Approximately 0.3~1.5 kg
Note: PR sensors are "passive", meaning they do not include built-in electronic circuits or signal processing units and only provide discharge current output. The user needs to be equipped with a dedicated Penning gauge controller (providing high voltage and current measurement). This is different from integrated models such as the PENNINGVAC PTR series.