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Nuclear Chemistry Prof. Jadhav S.S. MSc.BEd.
Introduction:-
Nuclear Chemistry is sub discipline of chemistry. i.e. concerned with
changes in the nucleus of atom. Nuclear changes are source of radioactivity &
nuclear power. That’s why nuclear chemistry is very important branch of
chemistry.
Atom of the element consists of three fundamental particles proton,
electron and neutron which are called sub-atomic particles. These particles are
mainly responsible for physical, chemical and also nuclear behavior of atoms of
all the elements. Out of them protons and neutrons are jointly called nucleon.
Nuclear reaction can be brought about by the interaction of two
nuclei or under the impact of a subatomic particle on the nucleus. Nuclear
chemistry deals with the study of nuclear particles, nuclear forces and nuclear
reactions.
Comparison of Chemical and Nuclear Reactions
Chemical Reactions Nuclear Reactions
One substance is converted into
another, but atoms never change
identity.
Atoms of one element typically are
converted into atoms of another
element.
Only Electrons take part in chemical
reaction
Nucleus of element takes part in
nuclear reaction.
Small amount energy evolved
during chemical reaction
Large amount energy evolved during
nuclear reaction
Reaction rates are influenced by
temperature, concentration and
catalyst.
Reaction rates are depend on
concentration of element, but not
influenced by temperature, catalyst.
Types of Nuclear Radiation:-
Radioactivity:-
Radioactivity is a phenomenon of spontaneous and uncontrollable
disintegration occurs by emission of active radiations from an unstable atomic
nucleus.
On the basis of effect of electric and magnetic field the radiations
emitted by naturally occurring radioactive elements are classified into three
types viz., α,  and  –radiations.
When these radiations are given out by radioactive element, the process
is called α -decay,  –decay and  -decay respectively.
α –decay:-
"Whenever the element emits an α-particle, the mass number
decreases by 4 units and atomic number decreases by 2 units."
This is known as α -decay.
ℎ +
+
α –decay involve emission of Helium nucleus.
 –decay :-
"Whenever the element emits a -particle, the mass number remains
unchanged and atomic number increases by 1 units."
This is known as  -decay.
+ ( )
+
Actually, the emission of -particle results due to transformation of a
neutron into proton and electron.
(The electron is ejected from the nucleus while the proton is retained by it and
thus the atomic number of nucleus increases by one unit)
+
 -decay:-
"Whenever the element emits a -rays, there is no change either in
mass number or in atomic number."
This is known as  -decay.
 - decay involve radiation of high energy photon.
Metastable Krypton-81 decays by  emission. This process simply results in
lower energy form of the nucleus.
+ 
Properties of α ,  and  -rays:-
Properties of α -rays:-
1. These rays consist of +vely chargedparticlescalled α -particles.
2. α -particles have +2 charge and mass of 4 unitsi.e.they arehelium nucleus.
3. They have lower velocity about 1/10th
that of the light.
4. They have highest ionizing power due to their considerable kinetic energy.
5. They possess least penetrating power due to their larger size and lowervelocity.
6. They produce luminosity in ZnS due tohighest kinetic energy.
7.They are deflectedinelectric and magnetic field to the smaller extent.
8. They affectphotographicplate tolesser extent.
Properties of  -rays:-
1. These rays consist of -vely chargedparticlescalled  -particles.
2.  -particles have -1 charge and negligible mass i.e.they areelectrons.
3. They have higher velocity about 9/10th
that of the light.
4. They have lower ionizing power due to their lower kinetic energy.
5. They have higher penetrating power due to their small size and higher velocity.
6. They produce lower luminosity in ZnS due tolower kinetic energy.
7.They are highlydeflected inelectric and magnetic field.
8. They affectphotographic plate to larger extent.
Properties of  -rays:-
1. These rays consist of electromagnetic radiations like -rays.
2.  -rays do not carry any charge.
3. They have highest velocity equal to that of the light.
4. They have least ionizing power due to their least kinetic energy.
5. They have highest penetrating power due to their non-material nature and
higher velocity.
6. They produce least luminosity in ZnS due to negligible kinetic energy.
7. They remain undeflected in electric and magnetic field.
8. They affect photographic plate to greater extent.
Rate of Radioactive Decay and Decay Constant:-
The number of radioactive atoms disintegrating per unit time is
called rate of radioactive decay or rate of radioactive disintegration.
It is proportional to the number of radioactive atoms present at the given instant.
Rate Expression (Expression for decay constant):-
Rate of radioactive disintegration varies with the concentration of
radioactive element.
Let N0 be the number of radioactive atoms present initially (i.e. when t=0).
Nt be the number of radioactive atoms present after time t.
If ‘dNt’ number of atoms disintegrates in a given time of interval ‘dt’, then
rate of disintegration is given by
∝ Nt
(Negative sign indicates that the number of atoms decreases with time).
= λ Nt ……………………….. (1)
λ proportionality constant and is called disintegration or decay or radioactive
constant.
The decay constant (λ) can be defined as,"the fraction of the total number of
atoms of radioactive element disintegrating per unit time.”
Rearranging the eqn
. (1) we get,
= - λ dt
Integrating above equation between the limits, N =N0 at t=0 & N=Nt at t=t, we
get,
∫ = - λ ∫
loge = - λ t ( ∫ = loge )
i.e. λ t = - loge
. λ t = loge
.
λ = loge
Thus, λ =
.
log ……………………………… (2)
Eqn
. (2) is the expression for disintegration constant (decay constant).
The exponential form of Eqn
. (2) is Nt = N0
It means that radioactive disintegration is an exponential process and can be
represented graphically as fallows,
Fig.:- Disintegration of radioactive element.
According to the exponential (disintegration) law, infinite time is required for the
complete disintegration of an element. That is, as time passes, amount of
radioactive element decreases, at infinite time very negligible amount remains but
the amount will not be reduced to zero.
Radioactive disintegration follows first order reaction.
Half Life and Average Life:-
A) Half life:-
Half life period is defined as, the time required for disintegration of half of the
original amount of the radioactive substance.
Relation between half-life period and decay constant:-
Decay constant (λ) is given by the equation,
λ =
.
log
Where, N0 = initial amount and Nt = amount at time t
At half-life period,
t = / and Nt = N0/2
Hence,
λ =
.
/
log
/
λ =
.
/
log2
λ =
. × .
/
λ =
.
/
/ =
.
……………………………….. (3)
Eqn
. (3) is the expression for Half Life.
Since, equation (3) does not contain any concentration term; the half-life period is
independent of initial concentration.
B) Average Life:-
Average or mean life is defined as, the time up to which the radioactivity
of the element can be appreciably recorded, within experimental limits.
Average life =
Alternatively,
Average life period (Τ) is nothing but the reciprocal of decay constant (λ)
Average life (Τ) =
We have, / =
.
i.e. λ =
.
/
Putting this value in above eqn
. we get,
Average life (Τ) = = /
.
= 1.44 × / ……………………. (4)
Thus
Average life (Τ) = 1.44 × Half Life period
Nuclear Stability, Mass Defect and Binding Energy, N/Z Ratio:-
Stability of nucleus is affected by the various factors as fallows.
1. Nuclear forces:-
Nucleus has a very small size (radius 10 m) in which positively
charged protons and neutral neutrons are packed together, but still nucleus is
stable. This is because some strong attractive forces must be holding these particles
together in the nucleus.
There are three types of forces viz.
1. proton-proton (p-p) force,
2. neutron-neutron(n-n)forceand
3.proton-neutron(p—n)force.
Collectively,theseforcesarecalled nuclearforces.
(p-p)and (n-n)forces are approximately equalwhile(p-n) forces isgreater
than these two.Nuclearforces areshort-range forces (acting within therange 10-15
m).
Nuclearforces arecalledexchange forces,because in the nucleus there is
constant interconversion amongst protons andneutrons through the formation of
mesons (π+
, π-
, π0
)
n P n P
Due to these exchange forces, the nucleons adjust themselves to form stable
nucleus of minimum potential energy.
2. Mass defect and Binding energy:-
A) Mass defect:-
“The difference between calculated mass and observed atomic mass
is called as mass defect.”
Mathematically it can be calculated by using eqn
Δm = [ZmH + (A-Z)mn] – M
Where,
Δm = mass defect, ZmH = mass Z proton or hydrogen atoms, A = mass number
(A-Z)mn = mass of (A-Z) neutrons, M = observed atomic mass.
+ π+
- π+
B) Binding energy (B.E.):-
"It is the energy released in binding the nucleons together in the
nucleus."
OR "it is the energy required to break the nucleus into its isolated nucleons."
This release of energy is due toloss ofsome mass andis given byEinstein's equation as,
E =Δmc2
Where,
Δm = mass defect or mass lost C = velocity of light.
If Δm is in grams and C is in cm/sec., then Binding Energy is in ergs.
If Δm is in kg and C is in m/sec., then Binding Energy is in joules.
Generally, Binding Energy is expressed in electron volts (eV) or million electron
volts (MeV).
1 eV = 1.6 x 10-12
ergs = 1.6 x 10-19
joules
1 MeV = 1.6 x 10-6
ergs = 1.6 x 10-13
joules
If the masses are expressed in amu, then Binding Energy (B.E.) in MeV is
obtained directly by using the relation,
B.E. = Δm × 931 MeV (since, 1 amu = 931 MeV)
binding energy per nucleon i.e. average (mean) binding energy is calculated as,
B.E. per Nucleon =
×
MeV
C) Stability and instability of nuclei:-
It is found that nuclei with B.E. between 8 to 9 MeV are highly stable.
* Nuclei having lower mass and B.E. less than 8 MeV are unstable and have a
tendency forfusion.
* Nuclei having very high mass and B.E. less than 8 MeV are unstable and have a
tendency forfission.
From fig. It is clear that, as mass number increases, B.E. increases. The
maximum B.E. is 8.7 MeV near mass number about 60 and then it decreases
gradually.
Thus, nuclei of elements with very low and very high mass numbers are
unstable. Nuclei with mass numbers between 20 and 166 as well as B.E. between 8
to 9 MeV are highly stable.
3. Neutron / Proton (N/Z) Ratio:-
It is observed thatneutrons are partly responsible for the stability of
nucleus because except hydrogen isotope no nucleus contains only protons. If there
are more protons in the nucleus more neutrons are required per proton forstability
of nucleus.
This can be seen from a plot of N Vs. Z . A line drawn atan angle of
45° represents nuclei containing equal number of N and Z.
For light nuclei upto Z = 20, the ratio N/Z = 1. Forheavy nuclei this ratio is larger
than unity and increases with increase in Z because the number of neutrons
exceeds the number of protons.
All stable nuclei lie within a certain range of N/Z ratio of about 1 to 1.6.This
region is called the zone of stability or stability belt
In a plot of the number Neutron (N) Vs atomic number (Z) the stable nuclei fall in a
narrow bond referred as the band of stability.
* Nuclei with N/2>1 are unstable & radioactive
* Elements on LHS of stability zone have N/Z > 1and have a tendency to increase
protons.
* Elements on R.H.S.of stability zone have N/Z < 1 and have tendency to decrease
protons.
> 1
< 1
Application of Radioisotopes:-
A) As Tracers:-
1. In studying reaction mechanism:-
(i)When water enriched in O18
isotope is used in photosynthesis, itis found that the
oxygen evolved in the process comes entirely from waterwhile oxygen of CO2 is
retained in organic compound.Application of Radioisotopes:-
CO + H2O18
(C6H12O ) + O
(ii) In ester hydrolysis by using water enriched in O18
isotope, it is found that the
acid only contains excess O18
as,
R--CO—OR’
+ HO18
H R--CO—O18
H + R’—OH
This indicates that, -OR'bond is broken andO18
H from H2 O18
takes the place of —OR’
while H combine with—OR’
producing alcohol.
2. In medicine:-
(i) Strong-radiationsemittedby60
Ni,Co60
,Co,radiumetc.areusefulto prevent the
growth ofcancer.
(ii) 131
I isotopeisusedtodetectand tocure thedisordersorcancersof thyroidglands.
(iii) 32
Pisotope are used to detect cancers i.e. for treatment of Leukemia.
(iv) Radioisotopeofiodineisusedtodetectbraintumor,
(v) 24
Na to determine the efficiency of blood circulation as well as function ofheart.
(vi) 198
Au isotope is used forcuring some types of cancers.
(vii)- radiationsarealsousedtosterilizethe surgicalinstruments.
3. In agriculture: -
(i) Food grains exposed to -radiations, last longer.
(ii) Superior plant varieties can be obtained by inducing mutation by  -rays.
(iii) Potatoes and milk are preserved by  -rays.
(iv) Pests and insects on crops can be killed by  - radiations.
(v) Radioactive phosphorus is used to study the efficiency of fertilizers.
(vi)14
C isotope is used for the study ofphotosynthesis and biosynthesis.
(vii) 35
S isotope is helpful to study the advantages and disadvantages of fungicides.
4. In industry:-
(i) To study self diffusion of metals, mechanism of friction and effectiveness of
lubricants.
(ii)  -rays from radioisotopes are used to detect the flaws and leaks in moulds, welding
and gas systems.
(iii) To measure level of liquids in closed tanks and to trace movement of oil in the
pipes of a refinery.
(iv) α and  rays are used to measure thickness of metallic and plastic sheets.
(v) To study wear and tear of machinery parts by using radioactive tracers.
B. As radiotherapy:-
(i) 60
Co emits  -rays are used for testing deeply separated cancer growths.
(ii) Radioisotope of phosphorus is used for treatment of Leukemia.
(iii) Radioisotope iodine for treatment of hyperthyroidism.
(iv) 24
Na is used to check the blood circulation and to study the functioning of
heart.
(C) In mutation of crops:-
Radioisotopes are used in mutation of crops. Mutations are induced in
plants to get crops with higher yield, resistant to disease and better adaptability
to the environments.
(D) Carbon dating: - (W. F. Libby (1960) first developed this technique.)
The process of determining the age of historic and archaeological organic
samples by comparing the ratio of 14
C to 12
C is called 14
C dating or carbon
dating.
The isotope 14
C is radioactive. The 14
C atom is produced in upper atmosphere
by the bombardment of neutron on Nitrogen atom.
N + n C + H
The atmospheric carbon dioxide a mixture of 14
CO2 and 12
CO2 present in a
fixed ratio. Plants absorb CO2 from the atmosphere and prepare cellulose
(wood) by photosynthesis. As long as the plant is alive the ratio of 14
C to 12
C
atoms in the wood is the same as in the atmosphere.
When the tree is cut, this cycle stops and the ratio 14
C to 12
C begins to
decrease because the 14
C atoms are constantly disintegrating. The concentration of
14
C can be measured by counting its radioactivity.
Consider, N0 concentration of 14
C in fresh (living) tree
Nt concentration of 14
C at particular time t (after cutting),
The age of the wood or old geological specimen (i.e. time, t), can be determined
by using disintegration law, as
λ =
.
log where, λ = 0.693/ /
here, / Half life period of radioactive carbon (14
C)

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Nuclear chemistry

  • 1. Nuclear Chemistry Prof. Jadhav S.S. MSc.BEd. Introduction:- Nuclear Chemistry is sub discipline of chemistry. i.e. concerned with changes in the nucleus of atom. Nuclear changes are source of radioactivity & nuclear power. That’s why nuclear chemistry is very important branch of chemistry. Atom of the element consists of three fundamental particles proton, electron and neutron which are called sub-atomic particles. These particles are mainly responsible for physical, chemical and also nuclear behavior of atoms of all the elements. Out of them protons and neutrons are jointly called nucleon. Nuclear reaction can be brought about by the interaction of two nuclei or under the impact of a subatomic particle on the nucleus. Nuclear chemistry deals with the study of nuclear particles, nuclear forces and nuclear reactions. Comparison of Chemical and Nuclear Reactions Chemical Reactions Nuclear Reactions One substance is converted into another, but atoms never change identity. Atoms of one element typically are converted into atoms of another element. Only Electrons take part in chemical reaction Nucleus of element takes part in nuclear reaction. Small amount energy evolved during chemical reaction Large amount energy evolved during nuclear reaction Reaction rates are influenced by temperature, concentration and catalyst. Reaction rates are depend on concentration of element, but not influenced by temperature, catalyst.
  • 2. Types of Nuclear Radiation:- Radioactivity:- Radioactivity is a phenomenon of spontaneous and uncontrollable disintegration occurs by emission of active radiations from an unstable atomic nucleus. On the basis of effect of electric and magnetic field the radiations emitted by naturally occurring radioactive elements are classified into three types viz., α,  and  –radiations. When these radiations are given out by radioactive element, the process is called α -decay,  –decay and  -decay respectively. α –decay:- "Whenever the element emits an α-particle, the mass number decreases by 4 units and atomic number decreases by 2 units." This is known as α -decay. ℎ + + α –decay involve emission of Helium nucleus.
  • 3.  –decay :- "Whenever the element emits a -particle, the mass number remains unchanged and atomic number increases by 1 units." This is known as  -decay. + ( ) + Actually, the emission of -particle results due to transformation of a neutron into proton and electron. (The electron is ejected from the nucleus while the proton is retained by it and thus the atomic number of nucleus increases by one unit) +  -decay:- "Whenever the element emits a -rays, there is no change either in mass number or in atomic number." This is known as  -decay.  - decay involve radiation of high energy photon. Metastable Krypton-81 decays by  emission. This process simply results in lower energy form of the nucleus. + 
  • 4. Properties of α ,  and  -rays:- Properties of α -rays:- 1. These rays consist of +vely chargedparticlescalled α -particles. 2. α -particles have +2 charge and mass of 4 unitsi.e.they arehelium nucleus. 3. They have lower velocity about 1/10th that of the light. 4. They have highest ionizing power due to their considerable kinetic energy. 5. They possess least penetrating power due to their larger size and lowervelocity. 6. They produce luminosity in ZnS due tohighest kinetic energy. 7.They are deflectedinelectric and magnetic field to the smaller extent. 8. They affectphotographicplate tolesser extent. Properties of  -rays:- 1. These rays consist of -vely chargedparticlescalled  -particles. 2.  -particles have -1 charge and negligible mass i.e.they areelectrons. 3. They have higher velocity about 9/10th that of the light. 4. They have lower ionizing power due to their lower kinetic energy. 5. They have higher penetrating power due to their small size and higher velocity. 6. They produce lower luminosity in ZnS due tolower kinetic energy. 7.They are highlydeflected inelectric and magnetic field. 8. They affectphotographic plate to larger extent. Properties of  -rays:- 1. These rays consist of electromagnetic radiations like -rays. 2.  -rays do not carry any charge. 3. They have highest velocity equal to that of the light. 4. They have least ionizing power due to their least kinetic energy. 5. They have highest penetrating power due to their non-material nature and higher velocity. 6. They produce least luminosity in ZnS due to negligible kinetic energy. 7. They remain undeflected in electric and magnetic field. 8. They affect photographic plate to greater extent.
  • 5. Rate of Radioactive Decay and Decay Constant:- The number of radioactive atoms disintegrating per unit time is called rate of radioactive decay or rate of radioactive disintegration. It is proportional to the number of radioactive atoms present at the given instant. Rate Expression (Expression for decay constant):- Rate of radioactive disintegration varies with the concentration of radioactive element. Let N0 be the number of radioactive atoms present initially (i.e. when t=0). Nt be the number of radioactive atoms present after time t. If ‘dNt’ number of atoms disintegrates in a given time of interval ‘dt’, then rate of disintegration is given by ∝ Nt (Negative sign indicates that the number of atoms decreases with time). = λ Nt ……………………….. (1) λ proportionality constant and is called disintegration or decay or radioactive constant. The decay constant (λ) can be defined as,"the fraction of the total number of atoms of radioactive element disintegrating per unit time.” Rearranging the eqn . (1) we get, = - λ dt Integrating above equation between the limits, N =N0 at t=0 & N=Nt at t=t, we get, ∫ = - λ ∫ loge = - λ t ( ∫ = loge )
  • 6. i.e. λ t = - loge . λ t = loge . λ = loge Thus, λ = . log ……………………………… (2) Eqn . (2) is the expression for disintegration constant (decay constant). The exponential form of Eqn . (2) is Nt = N0 It means that radioactive disintegration is an exponential process and can be represented graphically as fallows, Fig.:- Disintegration of radioactive element. According to the exponential (disintegration) law, infinite time is required for the complete disintegration of an element. That is, as time passes, amount of radioactive element decreases, at infinite time very negligible amount remains but the amount will not be reduced to zero. Radioactive disintegration follows first order reaction.
  • 7. Half Life and Average Life:- A) Half life:- Half life period is defined as, the time required for disintegration of half of the original amount of the radioactive substance. Relation between half-life period and decay constant:- Decay constant (λ) is given by the equation, λ = . log Where, N0 = initial amount and Nt = amount at time t At half-life period, t = / and Nt = N0/2 Hence, λ = . / log / λ = . / log2 λ = . × . / λ = . / / = . ……………………………….. (3) Eqn . (3) is the expression for Half Life. Since, equation (3) does not contain any concentration term; the half-life period is independent of initial concentration.
  • 8. B) Average Life:- Average or mean life is defined as, the time up to which the radioactivity of the element can be appreciably recorded, within experimental limits. Average life = Alternatively, Average life period (Τ) is nothing but the reciprocal of decay constant (λ) Average life (Τ) = We have, / = . i.e. λ = . / Putting this value in above eqn . we get, Average life (Τ) = = / . = 1.44 × / ……………………. (4) Thus Average life (Τ) = 1.44 × Half Life period
  • 9. Nuclear Stability, Mass Defect and Binding Energy, N/Z Ratio:- Stability of nucleus is affected by the various factors as fallows. 1. Nuclear forces:- Nucleus has a very small size (radius 10 m) in which positively charged protons and neutral neutrons are packed together, but still nucleus is stable. This is because some strong attractive forces must be holding these particles together in the nucleus. There are three types of forces viz. 1. proton-proton (p-p) force, 2. neutron-neutron(n-n)forceand 3.proton-neutron(p—n)force. Collectively,theseforcesarecalled nuclearforces. (p-p)and (n-n)forces are approximately equalwhile(p-n) forces isgreater than these two.Nuclearforces areshort-range forces (acting within therange 10-15 m). Nuclearforces arecalledexchange forces,because in the nucleus there is constant interconversion amongst protons andneutrons through the formation of mesons (π+ , π- , π0 ) n P n P Due to these exchange forces, the nucleons adjust themselves to form stable nucleus of minimum potential energy. 2. Mass defect and Binding energy:- A) Mass defect:- “The difference between calculated mass and observed atomic mass is called as mass defect.” Mathematically it can be calculated by using eqn Δm = [ZmH + (A-Z)mn] – M Where, Δm = mass defect, ZmH = mass Z proton or hydrogen atoms, A = mass number (A-Z)mn = mass of (A-Z) neutrons, M = observed atomic mass. + π+ - π+
  • 10. B) Binding energy (B.E.):- "It is the energy released in binding the nucleons together in the nucleus." OR "it is the energy required to break the nucleus into its isolated nucleons." This release of energy is due toloss ofsome mass andis given byEinstein's equation as, E =Δmc2 Where, Δm = mass defect or mass lost C = velocity of light. If Δm is in grams and C is in cm/sec., then Binding Energy is in ergs. If Δm is in kg and C is in m/sec., then Binding Energy is in joules. Generally, Binding Energy is expressed in electron volts (eV) or million electron volts (MeV). 1 eV = 1.6 x 10-12 ergs = 1.6 x 10-19 joules 1 MeV = 1.6 x 10-6 ergs = 1.6 x 10-13 joules If the masses are expressed in amu, then Binding Energy (B.E.) in MeV is obtained directly by using the relation, B.E. = Δm × 931 MeV (since, 1 amu = 931 MeV) binding energy per nucleon i.e. average (mean) binding energy is calculated as, B.E. per Nucleon = × MeV
  • 11. C) Stability and instability of nuclei:- It is found that nuclei with B.E. between 8 to 9 MeV are highly stable. * Nuclei having lower mass and B.E. less than 8 MeV are unstable and have a tendency forfusion. * Nuclei having very high mass and B.E. less than 8 MeV are unstable and have a tendency forfission. From fig. It is clear that, as mass number increases, B.E. increases. The maximum B.E. is 8.7 MeV near mass number about 60 and then it decreases gradually. Thus, nuclei of elements with very low and very high mass numbers are unstable. Nuclei with mass numbers between 20 and 166 as well as B.E. between 8 to 9 MeV are highly stable.
  • 12. 3. Neutron / Proton (N/Z) Ratio:- It is observed thatneutrons are partly responsible for the stability of nucleus because except hydrogen isotope no nucleus contains only protons. If there are more protons in the nucleus more neutrons are required per proton forstability of nucleus. This can be seen from a plot of N Vs. Z . A line drawn atan angle of 45° represents nuclei containing equal number of N and Z. For light nuclei upto Z = 20, the ratio N/Z = 1. Forheavy nuclei this ratio is larger than unity and increases with increase in Z because the number of neutrons exceeds the number of protons. All stable nuclei lie within a certain range of N/Z ratio of about 1 to 1.6.This region is called the zone of stability or stability belt In a plot of the number Neutron (N) Vs atomic number (Z) the stable nuclei fall in a narrow bond referred as the band of stability. * Nuclei with N/2>1 are unstable & radioactive * Elements on LHS of stability zone have N/Z > 1and have a tendency to increase protons. * Elements on R.H.S.of stability zone have N/Z < 1 and have tendency to decrease protons. > 1 < 1
  • 13. Application of Radioisotopes:- A) As Tracers:- 1. In studying reaction mechanism:- (i)When water enriched in O18 isotope is used in photosynthesis, itis found that the oxygen evolved in the process comes entirely from waterwhile oxygen of CO2 is retained in organic compound.Application of Radioisotopes:- CO + H2O18 (C6H12O ) + O (ii) In ester hydrolysis by using water enriched in O18 isotope, it is found that the acid only contains excess O18 as, R--CO—OR’ + HO18 H R--CO—O18 H + R’—OH This indicates that, -OR'bond is broken andO18 H from H2 O18 takes the place of —OR’ while H combine with—OR’ producing alcohol. 2. In medicine:- (i) Strong-radiationsemittedby60 Ni,Co60 ,Co,radiumetc.areusefulto prevent the growth ofcancer. (ii) 131 I isotopeisusedtodetectand tocure thedisordersorcancersof thyroidglands. (iii) 32 Pisotope are used to detect cancers i.e. for treatment of Leukemia. (iv) Radioisotopeofiodineisusedtodetectbraintumor, (v) 24 Na to determine the efficiency of blood circulation as well as function ofheart. (vi) 198 Au isotope is used forcuring some types of cancers. (vii)- radiationsarealsousedtosterilizethe surgicalinstruments.
  • 14. 3. In agriculture: - (i) Food grains exposed to -radiations, last longer. (ii) Superior plant varieties can be obtained by inducing mutation by  -rays. (iii) Potatoes and milk are preserved by  -rays. (iv) Pests and insects on crops can be killed by  - radiations. (v) Radioactive phosphorus is used to study the efficiency of fertilizers. (vi)14 C isotope is used for the study ofphotosynthesis and biosynthesis. (vii) 35 S isotope is helpful to study the advantages and disadvantages of fungicides. 4. In industry:- (i) To study self diffusion of metals, mechanism of friction and effectiveness of lubricants. (ii)  -rays from radioisotopes are used to detect the flaws and leaks in moulds, welding and gas systems. (iii) To measure level of liquids in closed tanks and to trace movement of oil in the pipes of a refinery. (iv) α and  rays are used to measure thickness of metallic and plastic sheets. (v) To study wear and tear of machinery parts by using radioactive tracers. B. As radiotherapy:- (i) 60 Co emits  -rays are used for testing deeply separated cancer growths. (ii) Radioisotope of phosphorus is used for treatment of Leukemia. (iii) Radioisotope iodine for treatment of hyperthyroidism. (iv) 24 Na is used to check the blood circulation and to study the functioning of heart.
  • 15. (C) In mutation of crops:- Radioisotopes are used in mutation of crops. Mutations are induced in plants to get crops with higher yield, resistant to disease and better adaptability to the environments. (D) Carbon dating: - (W. F. Libby (1960) first developed this technique.) The process of determining the age of historic and archaeological organic samples by comparing the ratio of 14 C to 12 C is called 14 C dating or carbon dating. The isotope 14 C is radioactive. The 14 C atom is produced in upper atmosphere by the bombardment of neutron on Nitrogen atom. N + n C + H The atmospheric carbon dioxide a mixture of 14 CO2 and 12 CO2 present in a fixed ratio. Plants absorb CO2 from the atmosphere and prepare cellulose (wood) by photosynthesis. As long as the plant is alive the ratio of 14 C to 12 C atoms in the wood is the same as in the atmosphere. When the tree is cut, this cycle stops and the ratio 14 C to 12 C begins to decrease because the 14 C atoms are constantly disintegrating. The concentration of 14 C can be measured by counting its radioactivity. Consider, N0 concentration of 14 C in fresh (living) tree Nt concentration of 14 C at particular time t (after cutting), The age of the wood or old geological specimen (i.e. time, t), can be determined by using disintegration law, as λ = . log where, λ = 0.693/ / here, / Half life period of radioactive carbon (14 C)