Radiation detector - cylindrical ionising chamber

In summary, the conversation discusses finding the voltage at which the electron energy will reach 23eV in a wire with a given position and mean free path. The potential difference between the cathode and anode is found to be V = [Q/(2πϵL)]*log(b/a), and this can be substituted into the expression for potential difference to solve for the desired energy level.
  • #1
i_hate_math
150
2
Homework Statement
A cylindrical detector has a central anode and a cathode with a radius of 36.8 μm and 30 mm respectively. At what applied voltage will an electron which is at 6 mm from the centre get enough energy to ionise helium gas (Ie » 23 eV) when traveling a mean free path length of 1 mm.
Relevant Equations
E(r) = Q/(2πϵLr) for a line of charge where Q, L are the total charge and length enclosed by the chosen gaussian surface
C = Q/V
Energy = q*V
Let r = position of the electron = 6mm - 36.8μm; λ = mean free path traversed.

Integrate E(r) = Q/(2πϵLr) between the two shells gives:
V = [Q/(2πϵL)]*log(r/(r-λ))

I know that the question is asking for the voltage at which the electron energy will get to 23eV, but i am unsure how to get rid of L or Q in the expression for V ?

Thanks
 
Physics news on Phys.org
  • #2
You haven't made use of the wire radius yet. Where is the charge and what does it mean for V on the outside of the wire ?

Edit: nor of the 30 mm... where V = ... :wink:
 
  • Like
Likes i_hate_math
  • #3
BvU said:
You haven't made use of the wire radius yet. Where is the charge and what does it mean for V on the outside of the wire ?

Edit: nor of the 30 mm... where V = ... :wink:

The potential at the surface should be zero outside the surface since the total enclosed charge would be zero. Between the cathode and anode (outside the wire, inside the shell), the potential difference is:
V = [Q/(2πϵL)]*log(b/a)
where b=30mm and a=36.8μm

=> V/log(b/a) = [Q/(2πϵL)]

So perhaps i could substitute this into
ΔΦ = [Q/(2πϵL)]*log(r/(r-λ))
to get ΔΦ = V* [log(r/(r-λ)) / log(b/a)]
and solve for e*ΔΦ = 23 eV ?
 
  • #4
Good plan ... !
 
  • #5
BvU said:
Good plan ... !
Thanks heaps!
 

FAQ: Radiation detector - cylindrical ionising chamber

What is a radiation detector - cylindrical ionising chamber?

A radiation detector - cylindrical ionising chamber is a device used to measure the amount and type of radiation in a given area. It consists of a cylindrical chamber filled with gas and electrodes that detect radiation particles passing through the chamber.

How does a radiation detector - cylindrical ionising chamber work?

The gas inside the chamber is ionized when radiation particles pass through it, creating an electrical current that is measured by the electrodes. The strength of the current is proportional to the amount of radiation present.

What types of radiation can a cylindrical ionising chamber detect?

A cylindrical ionising chamber can detect both alpha and beta particles, as well as gamma rays. It can also detect X-rays and other forms of ionizing radiation.

What are the applications of a radiation detector - cylindrical ionising chamber?

Cylindrical ionising chambers are commonly used in medical imaging, radiation therapy, and environmental monitoring to measure and monitor radiation levels. They are also used in nuclear power plants and other industries to ensure safe levels of radiation exposure for workers.

How accurate are radiation detectors - cylindrical ionising chambers?

The accuracy of a cylindrical ionising chamber depends on various factors such as the type and strength of radiation being measured, the design of the chamber, and calibration. However, they are generally considered to be highly accurate and reliable in detecting and measuring radiation levels.

Similar threads

Replies
7
Views
7K
Replies
10
Views
3K
Back
Top