2010-01-18

Radioisotopes

            Radioisotopes

Radioisotopes are isotopes with radioactive properties.

Isotopes are elements whose atoms have the same number of proton but different number of neutrons.

Isotopes have different nucleon numbers but the same proton number.

Radioisotopes is isotopes with unstable nuclei.

Synthetic isotopes are produced by unstable nuclei that decay.

There are many uses of radioisotopes in the field of medicine, agriculture, industry and research.

Radioisotopes as used as tracers in scientific research, medical diagnosis and industry.

Half Life

Half-life

Concept of Half-life

The reactivity or activity of a radioactive material is the rate of decay of the material.

The rate of decay is the same as the number of atoms which decay or are emmited every second.

The rate of decay of a radioactive materials depends on the number of atoms that have not yet undergone decay. Thus, the reactivity of a radioactive material will decrease with time.

The half-life (t½) of a radioactive element is the time taken for half the number of atoms in a sample of radioactive atoms to decay.

After one half-life, the activity and the number of atoms remaining of any radioactive substance are halved.


Decay curve.

The half-life of the same radioactive element is the same but the half-lives of different radioactive elements are different.

The value of half-life is not influenced by factors such as temperatures, pressure and etc.

(Source: bbc.co.uk)

Examples of half lives of some common isotopes

Radioisotope
Half-life
Uranium-238
5000 million years
Uranium-235
700 million years
Plutonium-239
24 000 years
Carbon-14
5700 years
Calcium-137
30 years
Cobalt-60
5 years

Determining the Half-life

Nuclei in a radioactive sample disintegrate at random.

Each nucleus has the equal chance of being decayed. Which means that at any time, any nuclei can decay / disintegrate.

Activity = the average number of decay or disintegrations per unit time in a radioactive sample.

During the decay of a radioactive sample, the number of atoms which have disintegrated increases, while the number of atoms which have not disintegrated decreases. It has to be remembered that the total number of atoms remain constant during this process.

The rate of decay lessens as the number of intact atoms that remain decreases and  thus activity decreases with time as the number of undecayed atoms decreases.

It has to be noted that different radioactive elements decay at different rates.

Point:  Half-life, t½ , of a radioactive isotope is the time taken for the activity of atoms of that isotope to fall to half of its original value.

also

Half-life (t½) can also be stated as the time taken for the number of radioactive atoms to decrease to half of its original number.

Consider this:

i. If N is the number of original atoms in a radioactive sample.
ii. After one half-life has lapsed, half (1/2)N atoms remain and half (1/2)N atoms have disintegrated.
iii. After two half-lives, (1/2)X(1/2)N = (1/2)^2 N  = (1/4) N atoms remain and (3/4)N atoms have disintegrated.
*Remember: N - (1/4) N = (3/4) N
iv. This decay process continues until a stable atom is produced.
v. Say x = number of half lives
N = original number of atoms
Nx = number of atoms remaining after x half-lives, then we can say that

Nx = (1/2)^x N

(Remember the symbol ^ means to the power of)

Also, it is worth to consider these formulas:


An exponential decay process can be described by any of the following three equivalent formulas:
N(t) = N_0 \left(\frac {1}{2}\right)^{t/t_{1/2}}
N(t) = N_0 e^{-t/\tau} \,
N(t) = N_0 e^{-\lambda t} \,
where
  • N0 is the initial quantity of the substance that will decay (this quantity may be measured in grams, moles, number of atoms, etc.),
  • N(t) is the quantity that still remains and has not yet decayed after a time t,
  • t1/2 is the half-life of the decaying quantity,
  • τ is a positive number called the mean lifetime of the decaying quantity,
  • λ is a positive number called the decay constant of the decaying quantity.

The three parameters t_{1/2}\tau, and λ are all directly related in the following way:
t_{1/2} = \frac{\ln (2)}{\lambda} = \tau \ln(2)


Source: wikipedia.com


Usage of Half-life


Half-life in Archeology

Carbon-14 has a half-life of 5600 years.

Humus, animals and plants absorb carbon-14 through carbon dioxide gas in the atmosphere. A small amount in CO2 exists as carbon-14.

Living animals and vegetable have a constant amount of Carbon-14 because the c-14 decayed will always replaced.

However or dead beings the amount of C-14 in it will decrease because new C-14 will not be absorbed causing its reactivity to decrease.

When an antique or human skill are found, their age can be determined by

Measuring the reactivity of C-14 in it.

Determine the ratio of decay carbon-14 against intact carbon-14.

Industries:

Radioisotopes can be used as tracers, in order for it to be feasible, the radioisotopes used must have long enough half-lives. For example: the leaks in undergound pipes carrying oil can be detected by injecting radioactive tracer into the flow. Afterwards a GM tube can be utilised to sense the leakage from the surface above the pipe.

Medicine:

To be useful in the medical field, the radioisotope must have a short half-life. This is to prevent over exposure to radiation for an unnecessarily long period of time.

The isotope Iron, 59Fe with a half life of 45 days is used in testing for iron in blood plasma.
Iodine, 131 I with a half life of 8 days can be used in thyroid tests and treatments.




Radioactive Detectors

Radioactive Detectors



Geiger-Muller Tube



  1. The Geiger-Muller tube is an effective radioactive detector. It can trace alpha particles, beta particles and gamma rays.

  2. The outer part of the G-M tube is made of aluminium which acts as the cathode.

  3. The middle part of the G-M tube is a metal wire which acts as the anode.

  4. The G-M tube is filled with argon gas at low pressure.

  5. Initially, the G-M tube must be connected to a high voltage before being used.

  6. This high voltage causes some ionization of argon gas.


Cloud Chamber



  1. The cloud chamber is made by using a transparent plastic box. The space in it is divided into two parts by a metal.

  2. The lower part is filled with solid carbon dioxide. Sponge is used to push the solid carbon dioxide towards the metal plate.

  3. The upper part is filled with molecules of alcohol vapour released from the felt which is initially soaked in alcohol.

  4. When the alcohol vapour diffuses downwards, it will become colder. Thus, a supersaturated condition will be produced in the space in the lower part of the chamber.

  5. When the radioactive rays enter the upper part, the ionization of air will occur. Saturated alcohol vapour will move above the ions. Droplets of liquid alcohol on the ions will cause the formation of misty tracks.

  6. Steps to ensure clear tracks:


    • The transparent Perspex cover is rubbed with a soft cloth to produce charges which will remove all ions in the chamber before any radioactive rays enter.

    • The cloud chamber must be placed horizontally to ensure smooth flow of particles in it.

    • If light is used, it must shine on the area superated with vapour and not on the black base of the chamber in order to avoid heating it.

  7. Normally, the tracks produced are not uniform. This shows that the radioactive rays are produced randomly.

  8. There are three types of tracks as shown in Table below.
















Types of radioactive rays


Explanation



  1. Tracks of alpha particles

The alpha tracks are thick and straight. This shows that alpha particles have the strongest ionizing power and the biggest mass.



  1. Tracks of beta particles

The beta tracks are thin and curvy. This shows that beta particles have low ionizing power and small mass.



  1. Tracks of gamma ray

Their tracks are short, curvy and spiky from the middle. It shows that it has the lowest ionizing power.



  1. The number of radioactive tracks produced will decrease after a while. This is because after some time, the condensation of alcohol vapour on the radioactive source will block the emission of radioactive rays.


Spark counter


The wire gauze and thin wire are connected to a voltage of more than 2000 V.


The voltage is increased slowly until sparks are produced in between.


The sparks are formed due to ionisation of the air.


The voltage is then decreased until no sparks are formed.


The radioactive source is brought close to the wire gauze.


The radioactive rays will ionize the air molecules between the wire gauze and thin wire. Positively charged ions will be attracted to the negatively charged gauze and the negatively charged ions will be attracted to the positively charged thin ions.


Secondary ionization will occur due to the collision between the ions and the air molecules.


Therefore, sparks are formed.


The number of sparks measured the intensity of radioactive rays from its source randomly.


The spark counter can only trace alpha particles which have high ionizing power.



Electroscope


When charged plate of the electroscope is exposed to the source of alpha particles, the gold leaf will collapse slowly.


This is due to the ions and electron are produced by the alpha particles which will neutralize the charge in the electroscope.


The rate of collapse of the gold leaf indicates the strength of the radioactive source.



Photographic Plate


All types of radioactive rays will darken the photo film. The effect is like sunlight acting on it.


The ionization effect by the radioactive rays will decompose silver bromide crystals on the film.


Films which are exposed to sunlight will show white lines representing radioactive tracks.


Films are kept in the badges worn by workers as a tracer device of radioactive rays.


The main disadvantage of using a film as a radioactive tracer is that it needs to be processed in order to prove the presence of radioactive rays.