Q.Obtain approximately the ratio of the nuclear radii of the gold isotope 79197Au and the silver isotope 47107Ag.
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Nuclear Density: Why All Nuclei Are Almost Equally Dense
Imagine you have a bag of marbles. If you pack them tightly, the density of the bag depends only on the marbles themselves — not on how many you put in. The nucleus behaves the same way. That's the core idea.
The Intuition
An atom's nucleus is made of protons and neutrons (collectively called nucleons). These nucleons are held together by the strong nuclear force, which is extremely short-ranged. Think of it like magnets: each nucleon only "feels" its immediate neighbours. So adding more nucleons doesn't compress the inner ones — it just adds a new layer on the outside.
This means the nucleus grows in volume proportionally to the number of nucleons. Double the number of nucleons, double the volume. And since mass also doubles, the density stays constant.
The Precise Statement
The nuclear radius R is experimentally found to follow:
R=R0A1/3
where:
- A = mass number (total protons + neutrons)
- R0≈1.2×10−15 m (a constant, about 1.2 femtometres)
R=R0A1/3
This is the nuclear radius formula. It's not a guess — it comes from scattering experiments where high-energy electrons or alpha particles bounce off nuclei.
Deriving the Density
The nucleus is roughly spherical, so its volume is:
V=34πR3=34π(R0A1/3)3=34πR03A
Notice: volume is directly proportional to A. The mass of the nucleus is approximately m≈A×(1.67×10−27 kg) (mass of one nucleon). So density:
ρ=volumemass=34πR03AA×mnucleon=34πR03mnucleon
The A cancels out completely. The density is a constant — independent of the nucleus size.
Nuclear density is independent of mass number A. All nuclei have approximately the same density.
The Numerical Value
Plug in the numbers:
- mnucleon≈1.67×10−27 kg
- R0≈1.2×10−15 m
ρ=34π(1.2×10−15)31.67×10−27≈2.3×1017 kg/m3
That's about 230 million tonnes per cubic centimetre. To put it in perspective: a sugar-cube-sized piece of nuclear matter would weigh as much as 230 million cars.
| Object | Density (kg/m³) |
|--------|-----------------|
| Water | 103 |
| Earth (average) | 5.5×103 |
| White dwarf star | 109 |
| Atomic nucleus | 2.3×1017 |
Why This Matters
This constancy of density tells us something profound: the strong nuclear force saturates. Each nucleon only interacts with its nearest neighbours, not with the whole nucleus. If the force were long-range (like gravity), density would increase with size. It doesn't — so the force is short-range. …
Why this formula?
Why Nuclear Density is Constant — The Reasoning
The most striking result about nuclear density is that it is roughly the same for all nuclei, regardless of size. This is not obvious — why wouldn't a larger nucleus be denser? The answer lies in how nuclear force works and how nucleons pack together.
Step 1: The nuclear volume formula
Experiments show that the radius of a nucleus is given by:
R=R0A1/3
where R0≈1.2×10−15 m (1.2 fm) and A is the mass number (total number of protons + neutrons).
The A1/3 dependence is the key. It means volume grows linearly with A, not faster.
Why A1/3? Because nucleons are packed as tightly as possible — like spheres in a close-packed arrangement. If you double the number of nucleons, you need to double the volume, so the radius must increase by 21/3.
Step 2: Volume from the radius
Assuming the nucleus is a sphere:
V=34πR3=34π(R0A1/3)3=34πR03A
Notice: the A1/3 cube gives A directly. So volume is proportional to A.
Step 3: Mass of the nucleus
The mass of the nucleus is approximately:
M≈A⋅mnucleon
where mnucleon≈1.67×10−27 kg (the average mass of a proton or neutron). The small mass defect from binding energy is negligible for this calculation.
Step 4: Density
Nuclear density ρ is mass divided by volume:
ρ=VM=34πR03AA⋅mnucleon=34πR03mnucleon
The A cancels completely. Nuclear density is independent of the nucleus size.
Step 5: The numerical value
Plugging in the numbers:
ρ=34π(1.2×10−15)31.67×10−27≈2.3×1017 kg/m3
ρnuclear≈2.3×1017 kg/m3 …
The key idea is that nuclear radius follows the empirical formula R=R0A1/3, where A is the mass number and R0 is a constant (~1.2 fm). This means the ratio of radii depends only on the cube root of the mass numbers.
Step 1: Write the radius for each nucleus:
RAu=R0(197)1/3, RAg=R0(107)1/3.
Step 2: Take the ratio: …
Nuclear radius scales as R∝A1/3, so the ratio of radii for gold (A=197) and silver (A=107) is 3197/107≈1.23.
The key idea is that nuclear density is roughly constant for all nuclei — a fact known from scattering experiments. Since mass number A is proportional to volume, and volume scales as R3, we get R∝A1/3. This is one of the most reliable scaling laws in nuclear physics.
Let’s work through it.
- The nuclear radius formula For any nucleus, the radius is given by
R=R0A1/3
where R0≈1.2×10−15m (a constant). The exact value of R0 cancels out when we take a ratio, so we don’t need it here.
- Write the ratio For gold: RAu=R0(197)1/3 For silver: RAg=R0(107)1/3 Dividing:
RAgRAu=(107)1/3(197)1/3=(107197)1/3
- Approximate the fraction 197/107≈1.841. Now take the cube root. A quick mental check: 1.23=1.728, 1.253=1.953. So the cube root lies between 1.2 and 1.25. More precisely, 1.233=1.23×1.23×1.23=1.5129×1.23≈1.861 — very close to 1.841. So (107197)1/3≈1.23 …
Method: Using the Radius–Mass-Number Relation
The key idea is that nuclear radius depends only on the mass number A, not on the atomic number Z. The standard empirical formula is:
R=R0A1/3
where R0≈1.2×10−15 m is a constant (the same for all nuclei). This means the ratio of two nuclear radii depends only on the ratio of their mass numbers.
Steps
-
Write the radius for each nucleus
For gold: RAu=R0(197)1/3
For silver: RAg=R0(107)1/3
-
Take the ratio — the R0 cancels immediately:
RAgRAu=(107)1/3(197)1/3=(107197)1/3
-
Simplify the fraction
107197≈1.841
-
Take the cube root …
Common Mistakes in Nuclear Radius Ratio Problems
Students typically make the same few errors when calculating the ratio of nuclear radii from mass numbers. Here is what goes wrong and how to fix each.
Mistake 1: Forgetting the Cube Root
The most frequent error is treating the radius as directly proportional to the mass number A, rather than to A1/3.
The nuclear radius formula is:
R=R0A1/3
where R0 is a constant (about 1.2×10−15 m). So the ratio of radii is:
R2R1=(A2A1)1/3
Students often write R2R1=A2A1 instead, which gives a wildly wrong answer.
Never write R∝A. The correct proportionality is R∝A1/3. The cube root is non-negotiable.
How to avoid: Every time you see "nuclear radius" and "mass number" together, immediately write R=R0A1/3 before doing anything else. Then take the ratio — the R0 cancels, and you are left with the cube root of the mass number ratio.
Mistake 2: Confusing Mass Number with Atomic Number
The formula uses A (mass number = protons + neutrons), not Z (atomic number = protons only). For gold, A=197; for silver, A=107. The atomic numbers (79 and 47) are irrelevant here.
The nuclear radius depends on the total number of nucleons, not just protons. Ignore Z in this calculation.
How to avoid: Circle the mass numbers in the isotope notation. The superscript (top-left) is A; the subscript (bottom-left) is Z. Use only the superscript.
Mistake 3: Inverting the Ratio
Students sometimes write RAgRAu=(197107)1/3 instead of (107197)1/3. Gold has more nucleons, so its nucleus is larger — the ratio must be greater than 1.
How to avoid: Check your common sense. Gold (A=197) is heavier than silver (A=107), so its radius should be larger. If your ratio comes out less than 1, you have inverted it.
Mistake 4: Not Simplifying the Cube Root
Students often leave the answer as (107197)1/3 without approximating. The question asks for an approximate ratio — you need a numerical value. …
- KEAM 2025Set pha-2025-0424A4 marksMCQQ.If the volume of nucleus having mass number 2 is V, then that for the nucleus having mass number 8 is (A) 2V (B) 3V (C) 4V (D) 6V (E) 9V
›Reveal solutionSolution
Since nuclear radius R=R0A1/3, volume ∝A; A goes from 2 to 8, so volume ×4=4V.
The nuclear radius scales as R=R0A1/3, so the volume is
V∝R3∝A.
Thus volume is directly proportional to mass number. Taking the ratio: …
- KEAM 2024Set eng-2024-06084 marksMCQQ.Mass numbers of two nuclei are in the ratio 2:3. The ratio of the nuclear densities would be (A) 2:31/3 (B) 31/3:2 (C) 2:3 (D) 3:2 (E) 1:1
›Reveal solutionSolution
Because the nuclear radius scales as R=R0A1/3, nuclear volume is proportional to A and density is constant for all nuclei. Hence 1:1.
The radius of a nucleus is R=R0A1/3, so its volume is
V=34πR3=34πR03A ∝ A.
The mass of a nucleus is proportional to A as well. Therefore density …
- KEAM 2024Set pha-2024-06104 marksMCQQ.If nuclear radius of $^{125}{52}Te$ is 6 fermi, then the nuclear radius of $^{27}{13}Al$ in fermi is (A) $3.6$ (B) $5$ (C) $2.5$ (D) $1.7$ (E) $4.2$
›Reveal solutionSolution
Nuclear radius scales as the cube root of mass number.
Nuclear radius R=R0A1/3, so
RTeRAl=(12527)1/3=53.
Therefore …
- KEAM 2021Set eng-2021-P1-A14 marksMCQQ.If the mass numbers of two nuclei are in the ratio 3:2, then the ratio of their nuclear densities is : (A) 31/3:21/3 (B) 21/3:31/3 (C) 2:3 (D) 1:1 (E) 3:2
›Reveal solutionSolution
Nuclear density is the same for all nuclei, so the ratio is 1:1.
Concept and Intuition
Nucleons are packed at essentially constant density inside nuclei. Since R∝A1/3, the volume grows exactly in proportion to the number of nucleons, keeping density constant.
Step-by-Step Solution
- R=R0A1/3, so V=34πR3∝A.
- Mass ∝A, therefore density ρ=VmA∝AA=const. …
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