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Specialized - Radiation Counter ·GeigerMullerCounter

18500

Philips self-quenching Geiger-Müller radiation counter intended for ionizing-radiation measurement. Manufacturer data specify counting plateau, background, timing, life, and construction characteristics for laboratory instrumentation.

Directly heatedCold cathodeCommon cathodeDissimilarSpecialized
Sections
1
Base
-
Socket code
-
Base pins
-
Nominal heater
-

Description

18500 — Non-Self-Quenching Geiger-Müller Radiation Counter Tube

The 18500 is a non-self-quenching, argon-hydrogen filled Geiger-Müller radiation counter tube. It is designed for the detection and measurement of ionizing radiation, including X-rays, gamma rays, and neutrons. Because it is a non-self-quenching design, it requires external circuitry to terminate the ionization discharge after each event.

Construction and Mechanical Specifications

The 18500 features a robust coaxial construction optimized for stable radiation detection. The cathode is fabricated from a specialized alloy consisting of 28% chromium and 72% iron.

Cathode and Physical Dimensions

  • Cathode Wall Thickness: 250 mg/cm²
  • Cathode Inside Diameter: 14.4 mm
  • Cathode Effective Length: 40 mm
  • Main Body Length: 47 mm
  • Overall Length: Maximum 135 mm
  • Body Diameter: 16 mm to 19 mm

Terminals and Mounting

Electrical connections to the tube are made via dedicated anode and cathode terminals:

  • Anode Connection: An M4 threaded stud (screw) with a length of 15 ± 0.5 mm.
  • Cathode Connection: A clip terminal with a width of 15 ± 0.5 mm, located 40 ± 0.5 mm from the non-anode end (with a cathode terminal length of 40 ± 0.5 mm).

To ensure proper operation and minimize parasitic effects, the tube requires a low-capacity mounting configuration utilizing short electrical connections. Additionally, the tube must be kept dry and thoroughly cleaned to prevent the formation of leakage currents across its surface.

Electrical and Operating Characteristics

The electrical behavior of the 18500 is characterized by a high operating voltage and a well-defined plateau region. The tube exhibits an internal electrical capacitance of 2 pF.

Voltage Parameters and Plateau

The tube begins to register counts at a starting voltage of 900 V. The plateau region, where the count rate remains relatively independent of the applied voltage, begins at 950 V and extends for a length of 150 V. Within this plateau, the slope is extremely flat, with a maximum change of 0.02% per Volt.

The recommended operating conditions are structured as follows:

  • Minimum Operating Voltage: 1000 V
  • Recommended (Typical) Operating Voltage: 1050 V
  • Maximum Operating Voltage: 1100 V

Performance and Lifetime

When operated under specified quenching conditions, the tube has a dead time of 75 µs. It exhibits high sensitivity and efficiency, with a documented cosmic ray efficiency of 98.5%. The expected operational lifetime of the tube is 10¹⁰ counts.

When shielded with 2 inches of lead (Pb) and 1/8 inch of aluminum (Al), the background count rate is kept to a maximum of 20 counts per minute.

Circuit-Specific Operating Requirements

Because the 18500 is a non-self-quenching tube, it cannot terminate the gas discharge on its own. It must be operated in conjunction with an external quenching circuit. Specifically, a Neher-Harper quenching circuit must be utilized to quench the discharge and reset the tube for subsequent events.

The output of the tube and its quenching circuit must be connected to an external amplifier and scaler system. This processing system must meet the following minimum specifications:

  • Sensitivity: Approximately 0.1 V
  • Resolving Time: Less than 5 µs (< 5 µs)

Applications and Detection Methods

The 18500 is designed for the measurement of X-ray, gamma, and neutron radiation.

For the specific application of thermal neutron detection, the tube must be wrapped in a cadmium foil with a thickness of approximately 0.5 mm. The cadmium foil acts as a converter, interacting with thermal neutrons to produce secondary radiation that can be readily detected by the argon-hydrogen filled active volume of the tube.

Technical Summary

ParameterSpecification
Tube TypeGeiger-Müller counter tube (non-self-quenching)
Gas FillingArgon-hydrogen
Cathode Composition28% Cr, 72% Fe
Capacitance2 pF
Starting Voltage900 V
Operating Voltage Range1000 V to 1100 V (1050 V typical)
Plateau Length150 V (starting at 950 V)
Plateau SlopeMax. 0.02% per V
Dead Time75 µs
Cosmic Ray Efficiency98.5%
Expected Life10¹⁰ counts
Required Quenching CircuitNeher-Harper

General specifications

Tube and section characteristics

Properties common to every published source and operating point.

Heater and base

Base
-
Socket code
-
Base pins
-
Nominal heater voltage
-
Nominal heater current
-
Parallel heater voltage
-
Parallel heater current
-
Series capable
No

Terminal pinout

Electrical assignments shared by every tube using this base designation.

No verified pinout is recorded for this base designation.

Section ratings

1 physical section, each with unique specifications.

Section 1

GeigerMullerCounter

X-ray radiationInterelectrode capacitances

No fixed ratings are recorded for this section.

Radiation-counter discharge tube.

Source-dependent data

Operating conditions by source

Each block preserves the test conditions and published values from one reference. Values from different sources are intentionally kept separate.

Data set 01

1957 Philips Receiving and Amplifying Tubes

Published operating points and test conditions from this source.

SECTION 1

GeigerMullerCounter

Characteristics

  • Starting Voltage

    900 V

  • Operating Voltage

    1050 V

  • Capacitance

    2 pF

Data set 02

1999 Philips 0-D

Published operating points and test conditions from this source.

SECTION 1

GeigerMullerCounter

Characteristics

  • Capacitance

    2 pF

    Counter tube

  • Cosmic ray efficiency

    98.5 %

    Published counter efficiency

Other

  • Operating voltage minimum

    1000 V

    Geiger-Muller operation

  • Operating voltage maximum

    1100 V

    Geiger-Muller operation