Back to Topic 5.4 — Fission
5.4.1Physics15 flashcards

Mass-energy equivalence and binding energy

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Card 1 of 155.4.1
5.4.1
Question

What is the 'mass defect' of a nucleus?

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All 15 Flashcards — Mass-energy equivalence and binding energy

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Card 1definition

Question

What is the 'mass defect' of a nucleus?

Answer

(Mass of the separate protons + neutrons) − (mass of the bound nucleus). The nucleus is the **lighter** one.

Card 2definition

Question

What is the 'binding energy' of a nucleus?

Answer

The energy equivalent of the mass defect (E = mc²) — the energy needed to **pull the nucleus apart** into separate nucleons.

Card 3definition

Question

What is 'binding energy per nucleon'?

Answer

Binding energy ÷ number of nucleons (A). It lets you **compare the stability** of different nuclei fairly.

Card 4formula

Question

Which equation links the mass defect to the binding energy?

Answer

$E = mc^{2}$ — mass-energy equivalence (given in the data booklet). Here m is the mass defect.

Card 5formula

Question

Fast way to convert a mass defect in u into energy in MeV?

Answer

Multiply Δm (in u) by **931.5**, because 1 u = 931.5 MeV c⁻².

Card 6concept

Question

On the binding-energy-per-nucleon curve, what does 'higher' mean?

Answer

**More tightly bound = more stable.** The curve peaks near iron (A ≈ 56), the most stable nuclei.

Card 7concept

Question

Why does fusion of light nuclei release energy?

Answer

It moves **up** the steep left side of the curve — the product is more tightly bound — so energy is released.

Card 8concept

Question

Why does fission of heavy nuclei release energy?

Answer

It moves **up** the gentle right side of the curve toward iron — the products are more tightly bound — so energy is released.

Card 9concept

Question

Which nucleus sits at the peak of the curve?

Answer

Iron (around **A ≈ 56**) — the most tightly bound, most stable nucleus.

Card 10comparison

Question

Fusion vs fission — which releases more energy per unit mass of fuel?

Answer

**Fusion** — it climbs the steep light-nuclei side, giving several times more MeV per nucleon than fission.

Card 11example

Question

A nucleus has Δm = 0.030 u and 4 nucleons. Binding energy per nucleon?

Answer

E = 0.030 × 931.5 ≈ 28 MeV total, then 28 ÷ 4 ≈ **7 MeV per nucleon**.

Card 12definition

Question

What is the strong nuclear force?

Answer

An **attractive**, **short-range** (≈ 1–3 fm) force between nucleons that holds the nucleus together against the protons' electric repulsion.

Card 13concept

Question

Why does the strong force not pull nucleons into one point?

Answer

Below about 0.5 fm it becomes strongly **repulsive**.

Card 14process

Question

How do you turn a mass given in MeV c⁻² into an energy?

Answer

Drop the c⁻²: a mass defect of 2.0 MeV c⁻² is a binding energy of **2.0 MeV**.

Card 15concept

Question

Why is the binding energy per nucleon roughly constant above A ≈ 60?

Answer

The strong force is **short-range**: each nucleon is bound only by its nearest neighbours, however big the nucleus.

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