10.4 Nuclear radioactivity  (Page 4/12)

Different types of radiation have different ranges when compared at the same energy and in the same material. Alphas have the shortest range, betas penetrate farther, and gammas have the greatest range. This is directly related to charge and speed of the particle or type of radiation. At a given energy, each $\alpha$ , $\beta$ , or $\gamma$ will produce the same number of ionizations in a material (each ionization requires a certain amount of energy on average). The more readily the particle produces ionization, the more quickly it will lose its energy. The effect of charge is as follows: The $\alpha$ has a charge of $+{2q}_e$ , the $\beta$ has a charge of $-q_e$ , and the $\gamma$ is uncharged. The electromagnetic force exerted by the $\alpha$ is thus twice as strong as that exerted by the $\beta$ and it is more likely to produce ionization. Although chargeless, the $\gamma$ does interact weakly because it is an electromagnetic wave, but it is less likely to produce ionization in any encounter.

The speed at which they travel is the other major factor affecting the range of $\alpha$ s, $\beta$ s, and $\gamma$ s. The faster they move, the less time they spend in the vicinity of an atom or a molecule, and the less likely they are to interact. Since $\alpha$ s and $\beta$ s are particles with mass (helium nuclei and electrons, respectively), their energy is kinetic. The mass of the $\beta$ particle is thousands of times less than that of the $\alpha$ s, so that $\beta$ s must travel much faster than $\alpha$ s to have the same energy. Since $\beta$ s move faster, they have less time to interact than $\alpha$ s. Gamma rays are photons, which must travel at the speed of light. They are even less likely to interact than a $\beta$ , since they spend even less time near a given atom (and they have no charge). The range of $\gamma$ s is thus greater than the range of $\beta$ s.

Alpha radiation from radioactive sources has a range much less than a millimeter of biological tissues, usually not enough to even penetrate the dead layers of our skin. On the other hand, the same $\alpha$ radiation can penetrate a few centimeters of air, so mere distance from a source prevents $\alpha$ radiation from reaching us. This makes $\alpha$ radiation relatively safe for our body compared to $\beta$ and $\gamma$ radiation. Typical $\beta$ radiation can penetrate a few millimeters of tissue or about a meter of air. Beta radiation is thus hazardous even when not ingested. The range of $\beta$ s in lead is about a millimeter, and so it is easy to store $\beta$ sources in lead radiation-proof containers. Gamma rays have a much greater range than either $\alpha$ s or $\beta$ s. In fact, if a given thickness of material, like a lead brick, absorbs 90% of the $\gamma$ s, then a second lead brick will only absorb 90% of what got through the first. Thus, $\gamma$ s do not have a well-defined range; we can only cut down the amount that gets through. Typically, $\gamma$ s can penetrate many meters of air, go right through our bodies, and are effectively shielded (that is, reduced in intensity to acceptable levels) by many centimeters of lead. One benefit of $\gamma$ s is that they can be used as radioactive tracers (see [link] ).

Section summary

• Some nuclei are radioactive—they spontaneously decay destroying some part of their mass and emitting energetic rays, a process called nuclear radioactivity.
• Nuclear radiation, like x rays, is ionizing radiation, because energy sufficient to ionize matter is emitted in each decay.
• The range (or distance traveled in a material) of ionizing radiation is directly related to the charge of the emitted particle and its energy, with greater-charge and lower-energy particles having the shortest ranges.
• Radiation detectors are based directly or indirectly upon the ionization created by radiation, as are the effects of radiation on living and inert materials.

Conceptual questions