13 Jul 2026

Characteristics of a Geiger-Muller Counter and Determination of Its Operating Voltage

practical pg-iii nuclear-physics gm-counter operating-voltage

Aim

To plot the counting characteristic of a Geiger-Muller counter and determine its starting voltage, plateau region, plateau slope, and operating voltage.

Apparatus

Geiger-Muller tube, GM scaler, high-voltage supply, radioactive check source, source holder, stopwatch or preset timer, and connecting leads.

Experimental arrangement

Labelled Geiger-Muller counter experimental arrangement
The radioactive source produces ionisation in the GM tube; the high-voltage supply collects the avalanche pulse and the scaler records the count.

Theory

An entering alpha, beta, or gamma ray produces ion pairs in the gas filling of the GM tube. The applied electric field drives the electrons towards the central anode. Above the starting voltage, the electrons gain enough energy between collisions to produce further ionisation, so one original event gives a large Townsend avalanche and a detectable pulse.

As the voltage is increased, the count rate first rises rapidly. It then becomes nearly independent of voltage over a range called the plateau. The midpoint of this stable region is selected as the operating voltage. Beyond the plateau, continuous discharge may occur and the tube can be damaged.

The plateau slope is expressed as the percentage increase in count rate per $100$ V:

\[\text{plateau slope}=\frac{N_2-N_1}{N_1}\frac{100}{V_2-V_1}\times100\ \%\text{ per }100\text{ V}.\]

The operating voltage is taken near the centre of the plateau,

\[V_0=\frac{V_1+V_2}{2},\]

where $V_1$ and $V_2$ are the lower and upper plateau limits.

Observations

Background count in $60$ s: $N_B=18$.

Applied voltage (V) Source count in 60 s Corrected count rate (counts s$^{-1}$)
400 42 0.40
450 310 4.87
500 443 7.08
550 456 7.30
600 462 7.40
650 468 7.50
700 474 7.60
750 520 8.37

Graph

GM counter plateau curve of count rate versus applied voltage
Count rate against applied voltage. The nearly horizontal section is the plateau region.

Calculation

The plateau extends approximately from $V_1=550$ V to $V_2=700$ V. Hence

\[V_0=\frac{550+700}{2}=625\text{ V}.\]

Using $N_1=7.30\ \text{s}^{-1}$ and $N_2=7.60\ \text{s}^{-1}$,

\[\text{plateau slope}=\frac{7.60-7.30}{7.30}\frac{100}{150}\times100=2.74\%\text{ per }100\text{ V}.\]

Result

The operating voltage of the GM counter is

\[\boxed{V_0=625\text{ V}}.\]

The plateau slope is approximately $2.74\%$ per $100$ V.

Precautions

  1. Increase the high voltage slowly and never operate in the continuous-discharge region.
  2. Keep the source position and counting time fixed for all readings.
  3. Follow the laboratory rules for handling radioactive sources.

Viva Questions

  1. What is the GM plateau? It is the voltage range over which the count rate changes only slightly with applied voltage.
  2. Why is the operating voltage chosen near the plateau centre? Small voltage fluctuations then produce only a small change in count rate.
  3. Why is a quenching gas used? It stops the discharge after one radiation event and prevents continuous discharge.

Maxima Code

Download the PG-III calculation file.

© Rajesh Kumar, SKMU · Physics Lecture Notes · rajeshphy.github.io

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