Q.Given the mass of iron nucleus as 55.85 u and A=56, find the nuclear density.
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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 density is nearly constant for all nuclei because the nuclear volume scales linearly with mass number A.
Step 1 – Find the nuclear radius.
Using the empirical formula R=R0A1/3, where R0=1.2×10−15 m:
R=1.2×10−15×(56)1/3 m.
Since 561/3≈3.83,
R≈4.60×10−15 m.
Step 2 – Compute the nuclear volume.
V=34πR3=34π(4.60×10−15)3≈4.07×10−43 m3.
Step 3 – Convert mass to kg and find density. …
Nuclear density is nearly constant for all nuclei because the nuclear volume scales linearly with mass number A. Using the iron nucleus (A=56, mass =55.85 u) and the empirical radius formula R=R0A1/3 with R0=1.2 fm, the density comes out to about 2.3×1017 kg/m3.
The idea behind nuclear density is beautiful in its simplicity. Unlike ordinary matter, where density varies wildly from gas to solid, nuclear matter has an almost constant density. Why? Because a nucleus is a tightly packed sphere of protons and neutrons. If you add more nucleons, the volume increases proportionally — the radius follows R=R0A1/3, so volume ∝A. Mass also ∝A (since each nucleon has roughly 1 u). So density ≈ constant, independent of A.
We’ll now calculate it for iron, step by step.
- Convert the mass to kilograms. The mass of the iron nucleus is given as 55.85 u. One atomic mass unit is 1 u=1.660539×10−27 kg. So:
m=55.85×1.660539×10−27 kg≈9.27×10−26 kg.
- Find the nuclear radius. The empirical formula for nuclear radius is:
R=R0A1/3,
where R0≈1.2 fm (1 femtometre = 10−15 m).
For iron, A=56, so:
R=1.2×10−15×561/3 m.
Now 561/3 is about 3.825 (since 3.83=54.9, close enough).
Thus:
R≈1.2×10−15×3.825≈4.59×10−15 m.
- Compute the volume. The nucleus is spherical, so:
V=34πR3.
First cube the radius:
R3≈(4.59×10−15)3=4.593×10−45≈96.7×10−45=9.67×10−44 m3.
Then:
V=34π×9.67×10−44≈4.1888×9.67×10−44≈4.05×10−43 m3.
- Calculate density. Density ρ=Vm: …
Method: Direct Application of the Nuclear Density Formula
This problem uses the fact that nuclear density is nearly constant for all nuclei. The method is straightforward: find the nuclear volume from the radius formula, then divide mass by volume.
Step 1: Write the nuclear radius formula
The radius of a nucleus is given by:
R=R0A1/3
where R0=1.2×10−15 m (a constant) and A is the mass number.
Step 2: Convert the given mass to kilograms
Mass of iron nucleus = 55.85 u.
Recall: 1 u=1.66×10−27 kg.
So:
m=55.85×1.66×10−27=9.27×10−26 kg
The mass number A=56 is close to the mass in u (55.85). This is because 1 u ≈ mass of one nucleon. For density calculations, using either value gives nearly the same result.
Step 3: Calculate the nuclear radius
R=(1.2×10−15)×(56)1/3
561/3≈3.83 (since 3.833=56.2).
R=1.2×10−15×3.83=4.60×10−15 m
Step 4: Calculate the nuclear volume
The nucleus is spherical:
V=34πR3
First find R3:
R3=(4.60×10−15)3=97.3×10−45=9.73×10−44 m3
Then:
V=34×3.14×9.73×10−44 …
The most common mistake here is treating the mass number A as the mass of the nucleus in kilograms. A is just the number of nucleons — it has no units. The mass in kilograms must be calculated separately.
Mistake 1: Using A directly as mass in kg
A student writes ρ=34πR356 and gets a wildly wrong answer. The mass number 56 is dimensionless, not a mass. You must convert the given mass from atomic mass units (u) to kg first: 1 u=1.66×10−27 kg.
Never plug A into the density formula as if it were the mass. A only tells you the number of nucleons, not the mass in SI units.
Mistake 2: Forgetting the nuclear radius formula
The radius of a nucleus is R=R0A1/3, where R0≈1.2×10−15 m. Some students use the atomic radius (of the order 10−10 m) instead, which makes the density off by a factor of 1015. The nucleus is tiny — always use the nuclear radius formula.
Mistake 3: Using the atomic mass instead of nuclear mass
The problem gives the mass of the iron nucleus as 55.85 u, so this is already correct. But if a question gives the atomic mass, remember that the mass of electrons is included. For iron (Z=26), that’s about 26×9.1×10−31 kg — negligible for most exam purposes, but conceptually you should know the difference.
Mistake 4: Unit mismatch in the final answer
Nuclear density comes out around 2.3×1017 kg/m3. A common slip is reporting it in g/cm3 without converting, or forgetting that 1 u=1.66×10−27 kg and 1 fm=10−15 m.
Work entirely in SI units (kg, m) from the start. Convert u to kg and fm to m before plugging into any formula. This avoids unit errors at the end. …
- CBSE 2026Set A1 markMCQQ.The nuclear density is approximately (A) independent of mass number (B) directly proportional to mass number (C) inversely proportional to mass number (D) directly proportional to A^(1/3)
›Reveal solutionSolution
Nuclear radius R = R₀A^(1/3), so volume ∝ A and mass ∝ A, making density independent of A.
The nuclear radius follows the empirical relation R=R0A1/3, where R0≈1.2 fm and A is the mass number.
Volume of the nucleus: V=34πR3=34πR03A, so V∝A.
Mass of the nucleus: M≈A×mnucleon, so M∝A.
…
- CBSE 2025Set ANNUAL1 markMCQQ.The nuclei have their mass numbers in the ratio of 1:3. The ratio of their nuclear densities would be(a) (3)^(1/3) : 1(b) 1:1(c) 1:3(d) 3:1
›Reveal solutionSolution
Because the nuclear radius scales as R = R0 A^(1/3), the nuclear volume scales exactly as A, so density = mass/volume comes out essentially the same constant for every nucleus, regardless of A.
Nuclear radius: R = R0 A^(1/3), where R0 approx 1.2 fm is a constant.
Nuclear volume: V = (4/3) pi R^3 = (4/3) pi R0^3 A
Since nuclear mass is approximately proportional to A (mass number, roughly A times the nucleon mass), density:
rho = mass / volume is proportional to A / A = constant
…
- CBSE 2025Set ANNUAL1 markQ.The density of nuclear matter is independent of the size of the nucleus. (T/F)
›Reveal solutionSolution
This statement is True — nuclear density is essentially the same for all nuclei, independent of the mass number (size) of the nucleus.
The radius of a nucleus with mass number A is given empirically by R=R0A1/3, where R0≈1.2 fm is a constant. The nuclear volume is then V∝R3∝A, and since the nuclear mass is also proportional to A (each nucleon has roughly the same mass), the density …
- CBSE 2024Set ANNUAL1 markQ.What is the ratio of nuclear densities of two nuclei having mass number 1:4?
›Reveal solutionSolution
Nuclear density is (almost exactly) the same for all nuclei, regardless of mass number.
Nuclear density is given by ρ=volumemass=34πR3mA, where the nuclear radius scales as R=R0A1/3. Substituting:
ρ=34π(R0A1/3)3mA=34πR03AmA=34πR03m
…
- CBSE 2024Set ANNUAL1 markMCQQ.Two nuclei have mass numbers in the ratio 1:3, the ratio of the nuclear densities are(a) 3:1(b) 1:1(c) 1:9(d) 1:3
›Reveal solutionSolution
Nuclear density ρ=mass/volume∝A/A3⋅3= constant, since the nuclear radius R∝A1/3 makes volume ∝A — so it does not depend on mass number at all.
The empirical nuclear radius formula is R=R0A1/3, where R0≈1.2fm is a constant and A is the mass number. The nuclear volume is
V=34πR3=34πR03A
which is directly proportional to A. The nuclear mass is also (to good approximation) proportional to A, since M≈Au (each nucleon contributes roughly one atomic mass unit).
So the nuclear density is …
- CBSE 2023Set 55/1/11 markMCQQ.The mass density of a nucleus of mass number A is :(a) proportional to A1/3(b) proportional to A2/3(c) proportional to A3(d) independent of A
›Reveal solutionSolution
The mass density of a nucleus is roughly constant for all nuclei because both the mass and the volume scale with the mass number A, making the density independent of A. The correct option is (d).
The key idea here is that a nucleus behaves like a tiny, incompressible drop of nuclear matter. Its volume is proportional to the number of nucleons (protons and neutrons), and its mass is also proportional to that number. When you take the ratio, the A cancels out.
Let’s see why this is true step by step.
-
What is mass number A?
A is the total number of nucleons in the nucleus. The mass of a single nucleon is roughly mn≈1.67×10−27 kg. So the mass of the nucleus is approximately M≈A⋅mn. This is a direct proportionality: M∝A.
-
How does the size of a nucleus scale with A?
Experiments (like Rutherford scattering) show that the radius R of a nucleus follows the empirical formula:
R=R0A1/3
where R0≈1.2×10−15 m (about 1.2 femtometers). This is a well-established result — the nuclear volume grows with the number of nucleons.
- What is the volume of the nucleus? Treating the nucleus as a sphere:
V=34πR3=34π(R0A1/3)3=34πR03A
So V∝A. The volume is directly proportional to the number of nucleons.
- Now compute the density: …
-
- CBSE 2022Set ANNUAL1 markQ.Two nuclei have mass numbers in the ratio 1 : 27. What is the ratio of nuclear density?
›Reveal solutionSolution
Nuclear density is the same for all nuclei, so the ratio is 1 : 1.
The nuclear radius is R=R0A1/3, so the nuclear volume is
V=34πR3=34πR03A.
The nuclear mass is proportional to the mass number, m≈Amnucleon. Hence the density is
ρ=Vm=34πR03AAmnucleon=34πR03mnucleon, …
- CBSE 2020Set 55/1/11 markQ.The nuclear radius of 1327Al is 3⋅6 fermi. Find the nuclear radius of 2964Cu.(OR)A proton and an electron have equal speeds. Find the ratio of de Broglie wavelengths associated with them.
›Reveal solutionSolution
Part (a): Since R∝A1/3, RCu=RAl(64/27)1/3=3.6×34=4.8 fermi.
Part (b): With equal speeds λ∝1/m, so λp/λe=me/mp≈1/1836.
Part (a)
The nucleus behaves like a constant-density drop, so its volume ∝A and its radius follows
R=R0A1/3,R0≈1.2 fm.
Taking a ratio removes R0:
RAlRCu=(AAlACu)1/3=(2764)1/3=34.
With RAl=3.6 fm:
RCu=3.6×34=4.8 fm. …
- CBSE 2020Set ANNUAL1 markMCQQ.The nucleus is approximately spherical in shape. Then the surface area of nucleus having mass number A varies as :(a) A5/3(b) A2/3(c) A4/3(d) A1/3
›Reveal solutionSolution
Since the nuclear radius scales as A1/3, the surface area of the (spherical) nucleus scales as (A1/3)2=A2/3.
Working
The empirical nuclear radius formula is
R=R0A1/3,R0≈1.2 fm
Treating the nucleus as a sphere, its surface area is …
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