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nuclear stability
stability of the nucleus depends on both N and Z
Z < 20 N=Z N/Z=1
20 < Z < 92 N > Z N/Z = 1-1.6
Z > 92 spontaneous fission
if N/Z <or> stable ratio, nucleus is radioactive
beta - decay (negatron emission)
its easier to convert a neutron to a proton then expel a neutron from the nucleus
Y decay
B decay always results in a daughter in an excited state - if this state is long live its called a meta-stable state
XS energy is lost by expelling a y-ray
B + - decay (positron emission)
easier to convert a proton to neutron than expel a proton from the nucleus
alpha decay
nuclei that are simply too big need to lose both n and p as quickly as possible
a = helium nucleus ^4 2He
2 protons + 2 neutrons
half life
time taken for activity of a radioisotope to each half its value
radioactive - decay equation
At = Are ^-ht
At - activity at time t
Ao - activity at time 0 (initial activity)
h - decay constant (rate constant) and h= 1n2/t1/2
t - time
Ln (At) = Ln(A0) - ht straight line graph intercept gradient
biological effects of radiation
radiation passing through cells of living tissue —> ions and free radicals
react with compounds in the cell, distributing or altering normal metabolic process
changes can result in death, cell ability to divide or abnormal cell division, changes in genetic material, increases in rate of ageing
penetrating power of radiation
different types of radiation have different abilities to penetrate matter
penetration affects how radiation interacts with tissues and materials
absorbed dose
measures the amount of energy absorbed by tissue
unit - grey (Gy)
1 Gy = 1Jkg-1
an absorbed energies can severely disrupt biological processes
dose equivalent
different radiation types cause different levels of biological damage
doe equivalent accounts for biological effect not just energy absorbed
represents damage done to humans
unit: sievert (sv)