Neutrinos do not interact with material in any significant way. They pass through the atmosphere, the earth crust, and the planet as if they do not exist. Because of the low probability of interaction, their detection is very difficult. The escape detection for more than 50 years after they were know to be emitted simultaneously with beta particles.
The major interaction of neutron with matter is nuclear reaction. Neutron absorption usually induces beta-emitting nuclides in a material. Thus neutrons are also hazardous to living organisms.
An electroscope consists of two gold leaves suspended from a metallic
conductor in a glass jar. Touching the conductor with electric charges
causes the leaves stay apart - a charged state due to repulsion of
like charges. When electricity is conducted away from the leaves,
or neutralizied, the leaves collapse into a discharged state.
A charged and a discharged electroscope are shown here.
When radioactive and X-ray sources are brought near a charged electroscope, it became discharged, observed Curie, Rutherford and others soon after their discoveries.
Due to ionization by radioactivity or X-rays, the air contains ions and electrons and becomes conducting. The electroscope discharges as a result.
| Ionization Potential (IP in eV) of Some Substances | |
|---|---|
| Material | IP eV |
| Air | 35 |
| Xenon | 22 |
| Helium | 43 |
| Ammonia | 39 |
| Ge crystal | 2.9 |
High-energy charged particles and photons able to ionize molecules are called ionizing radiation. Some examples are:
A liter of water contains 3.3x1025 molecules, 1,200 times denser
than that of a gas. So are atomic densities of other solids and liquid.
Thus, ionizing radiation interacts with many atoms per unit length on its path.
The production of ion pairs by a high-energy particle on its path is depicted in a diagram here. Electrons directly removed from atoms and molecules by radiation are called primary electrons. Some of these electrons carry a very high kinetic energy, and they, cause further ionization. Electrons knocked out by primary electrons are secondary electrons.
Example
Solution
| 1 mol -------- 22.4 L | 6.022e23 molecule ----------- 1 mol | = 2.69x1022 molecules/L |
|---|
Example 2
Solution
| 1000 g / L | 1 mol ----- 18 g | 6.022e23 molecule ----------- 1 mol | = 3.3x1025 molecules/L |
|---|
Example 3
Solution
| 2.330e6 g --------- 1 m3 | 1 mol ----- 28.1 g | 6.022e23 molecule ----------- 1 mol | = 4.99x1028 molecules m-3 | = 4.99x1025 molecules cm-3 or molecules/L |
|---|
Example 1
Solution
| 1.0e6 eV --------- 35 eV | = 28600 pairs. | |
|---|---|---|
| 2.86e4 pairs | 2 x 1.6022e-19 C --------- pair | = 9.16e-15 C (positive and negative) |