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Microbiology and Chemistry Study Notes

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1. Introduction

Nuclear chemistry is the branch of chemistry that deals with the composition, structure, properties and reactions of atomic nuclei.

Ordinary chemical reactions mainly involve the rearrangement of electrons surrounding the nucleus. Nuclear reactions involve changes in the nucleus itself.

Nuclear changes can release very large amounts of energy because nuclear binding energies are much greater than ordinary chemical bond energies.

Main topics in nuclear chemistry

  • Radioactivity
  • Nuclear decay
  • Alpha, beta and gamma radiation
  • Nuclear reactions
  • Nuclear stability
  • Mass defect
  • Binding energy
  • Nuclear fission
  • Nuclear fusion
  • Radioisotope applications

2. Atomic Nucleus

The nucleus is the small, dense central part of an atom. It contains protons and neutrons, collectively called nucleons.

Proton

A proton has a positive charge of +1 and approximately one atomic mass unit of mass.

Neutron

A neutron has no electrical charge and has a mass close to one atomic mass unit.

Atomic number

Z = Number of protons

Atomic number identifies the element.

Mass number

A = Number of protons + Number of neutrons

Therefore:

Number of neutrons = A − Z

Nuclear notation

ᴬZX

Here A is the mass number, Z is the atomic number and X represents the element.

Example

²³₁₁Na

Sodium-23 contains:

Protons = 11
Neutrons = 23 − 11 = 12

3. Isotopes, Isobars and Isotones

Isotopes

Isotopes are atoms of the same element having the same atomic number but different mass numbers.

Example:

¹²₆C, ¹³₆C, ¹⁴₆C

All have six protons but different numbers of neutrons.

Isobars

Isobars have the same mass number but different atomic numbers.

Example:

⁴⁰₁₈Ar and ⁴⁰₂₀Ca

Isotones

Isotones have the same number of neutrons but different atomic numbers.

Term Same Different
Isotopes Atomic number Mass number
Isobars Mass number Atomic number
Isotones Number of neutrons Atomic number

4. Nuclear Reaction

A nuclear reaction is a process in which the nucleus of an atom changes and one or more new nuclei or particles are produced.

In a nuclear reaction, conservation laws must be obeyed.

Important quantities that are conserved include total charge and total nucleon number.

Example

²³⁸₉₂U → ²³⁴₉₀Th + ⁴₂He

This is alpha decay.

Check the mass numbers:

238 = 234 + 4

Check atomic numbers:

92 = 90 + 2

5. Radioactivity

Radioactivity is the spontaneous disintegration of an unstable atomic nucleus with the emission of radiation.

The process is spontaneous because it does not require a continuous external supply of energy to cause each individual decay.

Natural radioactivity

Radioactivity shown naturally by unstable nuclides is called natural radioactivity.

Examples include radioactive isotopes of uranium, thorium and radium.

Artificial radioactivity

Some radioactive nuclides are produced artificially by nuclear reactions.

Important characteristics

  • Radioactive decay is spontaneous.
  • It is a nuclear process.
  • It is largely independent of ordinary chemical conditions.
  • The decay follows a statistical law.
  • Different radioactive nuclides have different half-lives.

6. Types of Radiation

The three commonly discussed radioactive emissions are:

  1. Alpha (α)
  2. Beta (β)
  3. Gamma (γ)

They differ in mass, charge, penetrating power and ionizing power.

7. Alpha Radiation

An alpha particle consists of two protons and two neutrons.

α = ⁴₂He

Therefore, an alpha particle has:

  • Mass number = 4
  • Charge = +2
  • Two protons
  • Two neutrons

Alpha decay

²³⁸₉₂U → ²³⁴₉₀Th + ⁴₂He

In alpha decay:

A → A − 4
Z → Z − 2

Properties

  • High ionizing power
  • Low penetrating power compared with beta and gamma
  • Deflected by electric and magnetic fields
  • Positive charge

8. Beta Radiation

Beta radiation consists of high-speed particles produced during nuclear transformations.

Beta-minus decay

In beta-minus decay, a neutron changes into a proton, producing an electron and an antineutrino.

n → p + e⁻ + ν̄

Therefore, at the nuclear level:

¹₄C → ¹⁴₇N + ⁰₋₁e

In beta-minus decay:

A remains unchanged
Z increases by 1

Beta-plus decay

In beta-plus decay, a proton changes into a neutron and a positron is emitted along with a neutrino.

p → n + e⁺ + ν

Therefore, the atomic number decreases by one while the mass number remains unchanged.

9. Gamma Radiation

Gamma radiation consists of high-energy electromagnetic radiation emitted by an excited nucleus.

ᵃX* → ᵃX + γ

Gamma emission does not change the atomic number or mass number.

ΔA = 0
ΔZ = 0

Properties

  • No mass charge
  • No electric charge
  • Very high penetrating power
  • Lower ionizing power than alpha particles
  • Not deflected by electric or magnetic fields

10. Comparison of Alpha, Beta and Gamma Radiation

Property Alpha Beta Gamma
Nature Helium nucleus Electron/positron Electromagnetic radiation
Charge +2 −1 for β⁻ 0
Mass High Very small Zero rest mass
Ionizing power Very high Moderate Low compared with α
Penetrating power Low Moderate Very high
Electric field Deflected Deflected strongly Not deflected

A common exam point is:

Ionizing power: α > β > γ
Penetrating power: γ > β > α

11. Nuclear Equations

A nuclear equation must be balanced with respect to nuclear charge and nucleon number.

Alpha decay

ᴬZX → ᴬ⁻⁴Z⁻²Y + ⁴₂He

Beta-minus decay

ᴬZX → ᴬZ+1Y + ⁰₋₁e

Beta-plus decay

ᴬZX → ᴬZ−1Y + ⁰₊₁e

Gamma emission

ᴬZX* → ᴬZX + γ

Worked example

Complete the following alpha decay:

²²⁶₈₈Ra → ?

Alpha emission decreases mass number by 4:

226 − 4 = 222

Atomic number decreases by 2:

88 − 2 = 86

Element 86 is radon.

²²⁶₈₈Ra → ²²²₈₆Rn + ⁴₂He

12. Radioactive Decay Law

Radioactive decay follows first-order kinetics.

If N is the number of radioactive nuclei remaining at time t, the rate of decay is proportional to N.

−dN/dt = λN

where λ is the decay constant.

On integration:

ln(N₀/N) = λt

Therefore:

N = N₀e−λt

Common logarithm form

log(N₀/N) = λt / 2.303

Therefore:

λ = 2.303/t × log(N₀/N)

This equation is very important for numerical problems.

13. Decay Constant

Decay constant is the probability per unit time that a particular radioactive nucleus will decay.

It is represented by λ.

λ = −(1/N)(dN/dt)

The unit of λ is inverse time, such as s⁻¹ or yr⁻¹.

A larger λ means faster radioactive decay.

14. Half-Life

Half-life is the time required for half of the original radioactive nuclei to decay.

If the initial amount is N₀, after one half-life:

N = N₀/2

The relationship between half-life and decay constant is:

t₁/₂ = 0.693/λ

Therefore:

λ = 0.693/t₁/₂

After multiple half-lives

After n half-lives:

N = N₀(1/2)ⁿ

For example, after three half-lives:

N = N₀/8

So 12.5% of the original radioactive nuclei remain.

15. Mean Life

Mean life is the average lifetime of radioactive nuclei.

It is represented by τ.

τ = 1/λ

Since:

t₁/₂ = 0.693/λ

We get:

t₁/₂ = 0.693τ

Or:

τ = t₁/₂ / 0.693

Therefore, mean life is longer than half-life.

16. Activity

Activity is the number of radioactive disintegrations occurring per unit time.

A = −dN/dt

From the decay law:

A = λN

At the beginning:

A₀ = λN₀

As the number of radioactive nuclei decreases, activity also decreases.

A = A₀e−λt

17. Units of Radioactivity

Becquerel

The SI unit of activity is the becquerel (Bq).

1 Bq = 1 disintegration per second

Curie

The curie (Ci) is an older unit of radioactivity.

1 Ci = 3.7 × 10¹⁰ Bq

Therefore:

1 mCi = 3.7 × 10⁷ Bq

18. Radioactive Dating

Radioactive isotopes can be used to estimate the age of certain materials because radioactive decay occurs at a predictable statistical rate.

Carbon-14 dating

Carbon-14 is used to estimate the age of once-living materials.

The basic principle is that after an organism dies, the amount of carbon-14 decreases by radioactive decay.

t = 2.303/λ × log(N₀/N)

The same equation can be written using activity because activity is proportional to the number of radioactive nuclei.

t = 2.303/λ × log(A₀/A)

Radioactive dating is based on measured decay and appropriate assumptions about the system being dated.

19. Nuclear Stability

Not all nuclei are stable. Nuclear stability depends on the balance between attractive nuclear forces and electrostatic repulsion between protons.

Neutron-proton ratio

For lighter stable nuclei, the number of neutrons and protons is often similar.

For heavier stable nuclei, more neutrons are needed to help offset the increasing proton-proton repulsion.

Magic numbers

Certain numbers of protons or neutrons are associated with unusually stable nuclear arrangements.

Common magic numbers include:

2, 8, 20, 28, 50, 82, 126

General idea

Nuclei far from the band of stability tend to undergo radioactive transformations that move them toward a more stable neutron-proton arrangement.

20. Mass Defect

The mass of a stable nucleus is slightly less than the sum of the masses of its individual free nucleons.

The difference is called mass defect.

Δm = [Z mp + N mn] − mnucleus

The missing mass has been converted into energy during formation of the nucleus.

Einstein's mass-energy relationship is:

E = mc²

Therefore:

Binding energy = Δm c²

21. Binding Energy

Binding energy is the energy required to separate a nucleus completely into its individual protons and neutrons.

It is also equal to the energy released when the free nucleons combine to form the nucleus.

Using mass defect

E = Δm c²

When mass defect is in atomic mass units

A useful conversion is:

1 u ≈ 931.5 MeV

Therefore:

Binding energy (MeV) = Δm (u) × 931.5

Binding energy per nucleon

Binding energy per nucleon = Total binding energy / A

A larger binding energy per nucleon generally indicates greater nuclear stability.

22. Packing Fraction

Packing fraction is a quantity used in nuclear chemistry to describe the difference between the isotopic mass and its mass number on an appropriate atomic mass scale.

It can be expressed as:

Packing fraction = [(isotopic mass − mass number) / mass number] × 10⁴

Depending on the convention used in a particular textbook, the exact presentation may differ. Therefore, the definition and formula given in the course text should be followed in numerical problems.

In an examination, always write the definition and the exact formula before substituting values for packing fraction.

23. Nuclear Fission

Nuclear fission is the splitting of a heavy nucleus into two or more smaller nuclei with the release of energy.

Example

A simplified representation is:

²³⁵₉₂U + ¹₀n → fission fragments + neutrons + energy

The exact fission products can vary.

Chain reaction

Neutrons released during one fission event can cause additional fission events.

This produces a chain reaction.

Controlled chain reaction

In a nuclear reactor, the chain reaction is controlled so that energy is released at a manageable rate.

Why energy is released

The fission products have, on average, greater binding energy per nucleon than the original heavy nucleus. The difference appears as released energy.

24. Nuclear Fusion

Nuclear fusion is the combination of light nuclei to form a heavier nucleus with the release of energy.

Example

²₁H + ³₁H → ⁴₂He + ¹₀n + energy

Deuterium and tritium are hydrogen isotopes.

Why fusion requires high temperature

Positively charged nuclei repel each other. Therefore, very high temperature and suitable conditions are required to bring nuclei close enough for the strong nuclear force to act effectively.

Sun and stars

Nuclear fusion is the main source of energy in the Sun and other stars.

25. Nuclear Reactor

A nuclear reactor is a device in which a controlled nuclear chain reaction is maintained to produce useful energy.

Main parts

  • Fuel: Contains fissionable material.
  • Moderator: Slows down fast neutrons in reactor designs that use thermal neutrons.
  • Control rods: Absorb neutrons and regulate the chain reaction.
  • Coolant: Transfers heat away from the reactor core.
  • Shielding: Reduces radiation exposure outside the reactor.

Basic energy sequence

Nuclear fission → heat → steam → turbine → generator → electricity

26. Applications of Nuclear Chemistry

Medical applications

  • Diagnosis using radioactive tracers
  • Nuclear medicine imaging
  • Treatment of certain cancers
  • Sterilization of medical equipment

Industrial applications

  • Thickness measurement
  • Leak detection
  • Tracer studies
  • Examination of welds and materials

Agriculture

  • Tracer studies of nutrient uptake
  • Investigation of plant metabolism
  • Mutation breeding under controlled conditions

Archaeology and geology

Radioactive dating methods can help estimate the age of suitable materials.

Scientific research

Radioisotopes can be used as tracers to follow chemical and biological processes.

27. Radiation Hazards

Ionizing radiation can damage biological molecules and living tissues.

Possible biological effects

  • Damage to DNA
  • Cell injury
  • Tissue damage
  • Increased risk of cancer
  • Acute radiation injury at sufficiently high exposure

Basic radiation protection principles

Radiation exposure is commonly reduced by considering:

  • Time
  • Distance
  • Shielding

Exposure should be minimized by using appropriate procedures, monitoring and shielding.

Radioactive materials must be handled only under appropriate laboratory, medical or industrial radiation safety procedures.

28. Solved Numericals

Numerical 1: Number of neutrons

Calculate the number of neutrons in ²³₁₁Na.

Given:

A = 23
Z = 11

Formula:

Number of neutrons = A − Z

Substitution:

Neutrons = 23 − 11
= 12

Answer: ¹¹Na²³ contains 12 neutrons.

Numerical 2: Half-life from decay constant

A radioactive substance has a decay constant of 0.231 min⁻¹. Calculate its half-life.

Given:

λ = 0.231 min⁻¹

Formula:

t₁/₂ = 0.693/λ

Substitution:

t₁/₂ = 0.693 / 0.231
t₁/₂ = 3.00 min

Answer: Half-life = 3.00 min.

Numerical 3: Decay constant from half-life

The half-life of a radioactive isotope is 10 hours. Calculate its decay constant.

Given:

t₁/₂ = 10 h

Formula:

λ = 0.693/t₁/₂

Substitution:

λ = 0.693/10
λ = 0.0693 h⁻¹

Answer: λ = 0.0693 h⁻¹.

Numerical 4: Amount remaining after three half-lives

A radioactive sample initially contains 80 g of material. How much remains after three half-lives?

Given:

N₀ = 80 g
n = 3

Formula:

N = N₀(1/2)ⁿ

Substitution:

N = 80(1/2)³
N = 80/8
N = 10 g

Answer: 10 g remains.

Numerical 5: Fraction remaining after four half-lives

What fraction of a radioactive sample remains after four half-lives?

Formula:

N/N₀ = (1/2)ⁿ

Substitution:

N/N₀ = (1/2)⁴
= 1/16

Therefore:

Percentage remaining = (1/16) × 100
= 6.25%

Answer: 1/16, or 6.25%, remains.

Numerical 6: Time required for decay

A radioactive sample decreases from 1000 nuclei to 250 nuclei. If its half-life is 5 hours, calculate the time required.

Initial amount:

N₀ = 1000

Final amount:

N = 250

First determine how many half-lives have passed.

1000 → 500 → 250

Therefore, two half-lives have passed.

t = 2 × 5
t = 10 h

Answer: 10 hours.

Numerical 7: Mean life

Calculate the mean life of a radioactive substance whose half-life is 20 years.

Given:

t₁/₂ = 20 years

Formula:

τ = t₁/₂ / 0.693

Substitution:

τ = 20/0.693
τ ≈ 28.86 years

Answer: Mean life ≈ 28.9 years.

Numerical 8: Activity

A sample contains 2.0 × 10¹⁰ radioactive nuclei and has a decay constant of 0.002 s⁻¹. Calculate its activity.

Given:

N = 2.0 × 10¹⁰
λ = 0.002 s⁻¹

Formula:

A = λN

Substitution:

A = (0.002)(2.0 × 10¹⁰)
A = 4.0 × 10⁷ s⁻¹

Since 1 Bq = 1 s⁻¹:

A = 4.0 × 10⁷ Bq

Answer: Activity = 4.0 × 10⁷ Bq.

Numerical 9: Binding energy from mass defect

Calculate the binding energy of a nucleus if its mass defect is 0.010 u.

Given:

Δm = 0.010 u

Formula:

E = Δm × 931.5 MeV

Substitution:

E = 0.010 × 931.5
E = 9.315 MeV

Answer: Binding energy = 9.315 MeV.

Numerical 10: Binding energy per nucleon

A nucleus has total binding energy of 56 MeV and mass number 7. Calculate its binding energy per nucleon.

Given:

Total binding energy = 56 MeV
A = 7

Formula:

BE per nucleon = Total BE/A

Substitution:

BE per nucleon = 56/7
= 8 MeV

Answer: Binding energy per nucleon = 8 MeV.

Numerical 11: Decay constant using the decay equation

A radioactive sample decreases from 800 mg to 200 mg in 12 hours. Calculate its decay constant.

Given:

N₀ = 800 mg
N = 200 mg
t = 12 h

Formula:

λ = (2.303/t) log(N₀/N)

Substitution:

λ = (2.303/12) log(800/200)
λ = (2.303/12) log 4

Since:

log 4 ≈ 0.6021
λ ≈ (2.303 × 0.6021)/12
λ ≈ 0.1156 h⁻¹

Answer: λ ≈ 0.116 h⁻¹.

Numerical 12: Half-life from the previous result

Using λ = 0.1156 h⁻¹, calculate the half-life.

Formula:

t₁/₂ = 0.693/λ

Substitution:

t₁/₂ = 0.693/0.1156
t₁/₂ ≈ 5.99 h

Answer: Half-life ≈ 6.0 hours.

29. Practice Questions

1. Define radioactivity.
2. Differentiate between isotopes, isobars and isotones.
3. Explain alpha, beta and gamma radiation.
4. Write the general equation for alpha decay.
5. Explain radioactive decay law.
6. Derive the relation: t₁/₂ = 0.693/λ
7. Define decay constant and mean life.
8. Explain mass defect and binding energy.
9. Explain nuclear fission with a suitable example.
10. Explain nuclear fusion and its importance in stars.
11. Describe the main components of a nuclear reactor.
12. Explain medical and industrial applications of radioisotopes.

30. Common Mistakes

  • Do not confuse mass number with atomic number.
  • In alpha decay, both A and Z decrease.
  • In beta-minus decay, A remains the same and Z increases by one.
  • In beta-plus decay, A remains the same and Z decreases by one.
  • Gamma emission changes neither A nor Z.
  • Half-life is not the time required for all nuclei to decay.
  • After each half-life, half of the nuclei present at the beginning of that interval remain.
  • The decay constant is not the same thing as half-life.
  • Activity depends on both decay constant and the number of radioactive nuclei.
  • Binding energy is not the same as mass defect. Mass defect is converted into binding energy.
  • Fission involves splitting heavy nuclei, whereas fusion involves combining light nuclei.
  • Do not write a nuclear equation without checking both mass number and atomic number.

31. TU Examination Preparation

Important 2-mark questions

  1. Define radioactivity.
  2. What are isotopes?
  3. Define half-life.
  4. Define decay constant.
  5. What is mean life?
  6. What is activity?
  7. Define mass defect.
  8. Define binding energy.
  9. What is nuclear fission?
  10. What is nuclear fusion?
  11. What is a nuclear reactor?
  12. What is a radioisotope?

Important 5-mark questions

  1. Explain the properties of alpha, beta and gamma radiations.
  2. Derive the radioactive decay equation.
  3. Explain half-life and mean life and derive their relationship.
  4. Explain mass defect and binding energy.
  5. Explain nuclear fission.
  6. Explain nuclear fusion.
  7. Explain the applications of radioisotopes.

Important 10-mark questions

  1. Explain radioactivity in detail. Discuss alpha, beta and gamma radiations with their properties and differences.
  2. Derive the radioactive decay law and obtain the expressions for decay constant, half-life and mean life.
  3. Explain mass defect, binding energy and nuclear stability.
  4. Discuss nuclear fission, chain reaction and the working principle of a nuclear reactor.
  5. Explain nuclear fusion and compare it with nuclear fission.

Numericals to prepare

  • Number of protons and neutrons
  • Half-life
  • Decay constant
  • Mean life
  • Amount remaining after several half-lives
  • Activity
  • Radioactive dating
  • Mass defect
  • Binding energy
  • Binding energy per nucleon

32. Quick Revision

Nuclear notation

ᴬZX
Neutrons = A − Z

Alpha decay

ᴬZX → ᴬ⁻⁴Z⁻²Y + ⁴₂He

Beta-minus decay

ᴬZX → ᴬZ+1Y + ⁰₋₁e

Beta-plus decay

ᴬZX → ᴬZ−1Y + ⁰₊₁e

Gamma emission

ᴬZX* → ᴬZX + γ

Decay law

N = N₀e−λt
ln(N₀/N) = λt

Half-life

t₁/₂ = 0.693/λ

Mean life

τ = 1/λ
τ = t₁/₂/0.693

Activity

A = λN

Mass-energy relation

E = mc²

Binding energy

BE = Δm × 931.5 MeV

Binding energy per nucleon

BE/A

Radiation comparison

Ionizing power: α > β > γ
Penetrating power: γ > β > α

Nuclear processes

Fission → heavy nucleus splits
Fusion → light nuclei combine

33. Quick Check

1. What is the charge of an alpha particle?

2. Which radiation has the greatest penetrating power?

3. What happens to atomic number during beta-minus decay?

4. What is the relation between half-life and decay constant?

5. What is the SI unit of activity?

6. Which process involves splitting a heavy nucleus?

7. Which equation represents binding energy from mass defect?

8. What remains unchanged during gamma emission?