Авторы

  • B.A. Kholkhodjayev
    Dots Tashkent State Technical University,
  • J.J. Dilmurodov
    Student. Tashkent State Technical University,
  • D.B. Asatullayeva
    Student Uzbekistan State Word Languages University

DOI:

https://doi.org/10.71337/inlibrary.uz.arims.84792

Ключевые слова:

Radioactive decay alpha decay beta decay gamma decay half-life electron capture exponential functions differential equation radiocarbon method C-14 isotope nuclear physics radiation ionizing radiation mass reduction.

Аннотация

The term 'radioactive decay' is used in the Uzbek language, although its core terminology originates from international scientific nomenclature. This article explains the fundamental concepts and calculations related to radioactive decay.


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RADIOACTIVE DECAY

Kholkhodjayev B.A.

Dots.

Dilmurodov J.J.

Student.

Tashkent State Technical University,

Asatullayeva D.B.

Student

Uzbekistan State Word Languages University

Tel.: +998 90 082 81 73

https://doi.org/10.5281/zenodo.15344042

Annotation.

The term 'radioactive decay' is used in the Uzbek language, although its

core terminology originates from international scientific nomenclature. This
article explains the fundamental concepts and calculations related to radioactive
decay.

Keywords.

Radioactive decay, alpha decay, beta decay, gamma decay, half-life, electron

capture, exponential functions, differential equation, radiocarbon method, C-14
isotope, nuclear physics, radiation, ionizing radiation, mass reduction.

Introduction.

To analyze the origin of this term, attention must be given to its

components:

Radioactive:

This

word

derives

from

the

Latin

'radius,'

meaning

'ray.'

The phenomenon of radioactivity was discovered at the end of the 19th century
and the term became widely used in scientific literature of that time.

Decay:

This is an Uzbek word meaning 'fragmentation' or 'disintegration.'
It is used to describe the process of atomic nuclei of radioactive substances
breaking apart.

Radioactive decay is the process by which unstable atomic nuclei break

down into smaller nuclei or other particles, emitting ionizing radiation. This
process can occur naturally or be induced artificially.

Main Part. Types of Radioactive Decay
1.

Alpha Decay

An alpha particle (²⁴He, composed of 2 protons and 2 neutrons) is emitted

from the nucleus.


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As a result, the atomic number decreases by 2 units, and the mass number

decreases by 4 units.

Example:
2.

Beta Decay

A neutron transforms into a proton, emitting a beta particle (electron).

The atomic number increases by 1 unit, but the mass number remains
unchanged.
Example:

3.

Gamma Decay

The nucleus releases excess energy in the form of gamma radiation.

The

mass

number

and

atomic

number

remain

unchanged.

Gamma decay often occurs after alpha or beta decay.

4. Positron Emission
A proton transforms into a neutron, emitting a positron (e⁺).

The atomic number decreases by 1 unit, while the mass number remains
unchanged.

4.

Electron Capture

The nucleus captures an electron from the surrounding electron cloud,

converting a proton into a neutron.

The atomic number decreases by 1 unit, and the mass number remains

unchanged.

Applications
In Medicine: Radiotherapy, X-ray diagnostics.
In

Energy:

Power

generation

at

nuclear

power

plants.

In

Archaeology:

Dating

using

the

radiocarbon

(¹⁴C)

method.

In Military: Nuclear weapons.

Radioactive Decay Equation
Let m(t) represent the mass of a radioactive substance at time t. It is known

from physics that the rate of radioactive decay is proportional to the remaining
mass of the substance, that is:

m' = -km (1)
where k = const > 0 is the proportionality coefficient.

Thus, m = m(t) satisfies the separable differential equation (1). Solving it yields
the general solution:

m = ce^(-kt)
If the initial mass at time t = 0 is m₀ > 0, then c = m₀, and the mass changes

according to:


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m = m₀e^(-kt) (2)
Over time, the mass decreases exponentially towards zero.
Half-Life
The half-life T is the time required for half of the initial radioactive

substance to decay.

Setting m(T) = m₀/2 gives:
m₀/2 = m₀e^(-kT)
which leads to:
T = (ln2)/k or k = (ln2)/T.
This formula allows determining k if T is known (which is relatively easy to

measure).

Application to Radiocarbon Dating
It is known that living organisms absorb C-14 isotopes from the

atmosphere along with stable C-12 carbon. During the life of an organism, the
ratio of C-14 to C-12 remains constant at some value m₀. Upon death, the intake
of C-14 stops, and its amount begins to decrease.

The half-life of C-14 is approximately 5570 years. Therefore:
k = ln2/5570 ≈ 1.24 × 10⁻⁴ year⁻¹.
Thus, the mass of C-14 at time t after death is:
m(t) = m₀e^(-t/8000).
If m(t) is determined (for instance, by measuring the emitted particles),

then the time elapsed since the death of the organism can be calculated by:
t = 8000 × ln(m₀/m(t)).

This formula allows determining the age of ancient organic materials.

References:

1. Shokhamidov Sh.Sh. “Elements of Applied Mathematics,” Tashkent,
Uzbekistan, 1997.
2. Fikhtengolts G.M. Fundamentals of Mathematical Analysis.
3. Azlarov T., Mansurov H. Fundamentals of Mathematical Analysis, 2005.
4. Berman: Problem Book in Mathematical Analysis, 1989

Библиографические ссылки

Shokhamidov Sh.Sh. “Elements of Applied Mathematics,” Tashkent, Uzbekistan, 1997.

Fikhtengolts G.M. Fundamentals of Mathematical Analysis.

Azlarov T., Mansurov H. Fundamentals of Mathematical Analysis, 2005.

Berman: Problem Book in Mathematical Analysis, 1989