RuukkilabraUpper secondary physics

Inside ITER: the machine and fusion gain

Why is it so hard to get more energy out of a fusion plasma than you put into it?

Prior knowledge

  • $\text{D–T}$ fusion releases $17.6\ \text{MeV}$: $3.5\ \text{MeV}$ to the helium nucleus and $14.1\ \text{MeV}$ to the neutronchapter Fusion reactions: from the Sun to deuterium and tritium
  • A magnetic field exerts a force only on moving chargeschapter Charged particles and magnetic confinement
  • Why ITER is built by seven Memberschapter ITER: why, where and who

Core path: follow the steps in order. Tasks marked Optional give extra practice. Optional tasks: 1.

Think about it

Inside a steel chamber as tall as a four-storey house, a gas thinner than air will be heated to about 150 million degrees, ten times hotter than the centre of the Sun. A few metres away, the magnets that hold it are colder than $-269\ ^\circ\text{C}$. Heating the gas takes huge amounts of power, and the hot gas keeps losing its energy.

Can such a machine give out more energy than it takes in, and what would that mean for electricity?

Review: the D–T neutron

In $\text{D–T}$ fusion, $^{2}_{1}\text{H} + {}^{3}_{1}\text{H} \to {}^{4}_{2}\text{He}\ (3.5\ \text{MeV}) + \text{n}\ (14.1\ \text{MeV})$. Why can the magnetic field of a tokamak hold the helium nucleus in the plasma but not the neutron?

Predict

Make your predictions before investigating 2 questions

Prediction 1: the hottest surface

Which part of ITER do you think must survive the largest heat flow on each square metre of its surface?

Prediction 2: power out

ITER is designed to make $500\ \text{MW}$ of fusion power from $50\ \text{MW}$ of heating. Suppose ITER had turbines that turn one third of its $500\ \text{MW}$ of fusion heat into electricity.Would it send net electricity to the grid?

Investigate

Investigate: explore the machine

Explore the cross-section of ITER. Select every part, in the drawing or in the list of parts below the panel. For each part, note in your own words: what it does, one number, and why it is hard to build. Work in pairs: one of you reads the panel aloud, the other takes notes, then swap.

From your notes, explain to your partner, then write four or five sentences: how do the three kinds of magnets work together to hold the plasma, and why must they be so cold?

The parts of the machine

ITER is a tokamak. Its plasma, about $830\ \text{m}^3$ of deuterium and tritium at about $150$ million $^\circ\text{C}$, is held by magnetic fields inside a ring-shaped steel chamber.

  • Magnets. $18$ D-shaped toroidal field coils make the field that runs around the ring (up to $11.8\ \text{T}$). Six ring-shaped poloidal field coils shape the plasma and hold it in place. The central solenoid, a $13\ \text{m}$ tall stack of six modules, works like the primary coil of a transformer: a changing current in it drives a current of up to $15\ \text{MA}$ in the plasma. All the magnets are superconducting and are cooled with helium to about $4\ \text{K}$.
  • Vacuum vessel. A double-walled steel chamber, $19.4\ \text{m}$ wide, keeps the vacuum and is the first barrier that keeps tritium in.
  • Blanket. $440$ modules line the inside of the vessel. They take the heat and the fast neutrons and shield the vessel and the magnets.
  • Divertor. At the bottom, $54$ cassettes with tungsten targets catch the heat and the helium "ash" that flow out along the edge of the plasma. The heat flow there is up to about $10\text{–}20\ \text{MW}$ on each square metre, the highest in the machine.
  • Heating. Beams of fast neutral atoms and two kinds of radio waves heat the plasma with a planned $50\ \text{MW}$.
  • Cryostat. A vacuum chamber about $30\ \text{m}$ tall around everything insulates the cold magnets from the warm building.
Colour photograph of a very large ring-shaped magnet coil in a factory hall.
A poloidal field coil being built in the coil factory on the ITER site. These giant rings shape and position the plasma. Photo: Johannes Reimer, CC BY 4.0, via Wikimedia Commons
Colour photograph looking up in the ITER assembly hall: a huge curved steel vacuum-vessel sector hangs in a grey tooling frame next to pink-wrapped D-shaped magnet coils, with yellow cranes overhead and workers on scaffolding.
A sector of the ITER vacuum vessel in its assembly tooling, 26 March 2024, next to D-shaped toroidal field coils wrapped in pink protective film. The workers on the scaffolding show the scale: one sector is about as tall as a four-storey building. Photo: Lauri Hellsten

Words of the machine

Theory summary

Key idea

A fusion plasma loses energy all the time: hot particles escape across the magnetic field and the plasma radiates. To keep it hot, we heat it from outside. The fusion gain $Q$ compares the fusion power produced in the plasma with this heating power.

At $Q = 1$, called scientific breakeven, the plasma produces as much fusion power as it receives. No magnetic fusion experiment has reached it yet with real $\text{D–T}$ fuel: JET's record from 1997 was $16\ \text{MW}$ of fusion power from $24\ \text{MW}$ of heating, $Q \approx 0.67$. ITER's goal is $Q = 10$: $500\ \text{MW}$ of fusion power from $50\ \text{MW}$ of heating, in pulses of $400\text{–}600\ \text{s}$. In D–T fusion, $3.5\ \text{MeV}$ of the $17.6\ \text{MeV}$ goes to the helium nucleus, which is charged and stays in the plasma. At $Q = 10$ these helium nuclei heat the plasma about twice as much as the external heating does: a burning plasma.

Fusion gain

$$Q = \frac{P_\text{fusion}}{P_\text{heating}}$$

Here $P_\text{fusion}$ is the fusion power produced in the plasma and $P_\text{heating}$ is the heating power that reaches the plasma from outside. Both are in watts, so $Q$ has no unit.

$200$
$400$
$600$
$0$
$P\ (\text{MW})$
$50$
$\alpha\text{: }100$
$\text{n: }400$
$500$
$110$
$620$
$\text{peaks}$
$\text{heating}$
$\text{into plasma}$
$\text{fusion}$
$\text{in plasma}$
$\text{grid}$
$\text{electricity in}$

Gain is not electricity. $Q$ describes the plasma only. ITER has no turbines and will not produce any electricity. During a pulse the whole plant (heating systems, cooling water, cryogenics, magnets) draws far more electricity than the $50\ \text{MW}$ that reaches the plasma. According to ITER, it needs $110\ \text{MW}$ at the least and up to $620\ \text{MW}$ in peaks of $30\ \text{s}$; the cooling water and the cryogenic systems take about $80\ \%$ of it. A power plant would turn the heat into electricity with steam turbines, typically about one third of it. Even then, $500\ \text{MW}$ of heat would give only about $170\ \text{MW}$ of electricity: far less than ITER's peak demand of $620\ \text{MW}$.

Scientific gain is not commercial viability. A power plant must also produce more electricity than the whole plant uses, run for months instead of minutes, breed its own tritium, survive years of neutron damage and sell its electricity at a price people will pay. ITER is built to test the physics and the technology for that, not to show that fusion electricity is cheap.

Word bank

fusion power · heating power · gain · breakeven · burning plasma · to produce · to consume · to convert (heat into electricity) · a turbine · an experiment · a power plant · commercially viable

Sentence starters

  • The gain $Q$ compares … with …
  • This does not mean that …, because …
  • ITER is an experiment, whereas a power plant …
  • A limitation of ITER is …
  • The evidence suggests that …

Pair discussion: gain and electricity

Discuss with a partner, using the word bank and the sentence starters, then each write three or four sentences: what is the difference between the gain of the plasma and the electricity a power plant produces? Use the bar chart.

Back to your predictions

Compare your predictions with the explorer and the text. Then answer the opening question in one or two sentences: why is it so hard to get more energy out of a fusion plasma than you put in?

    Would you change your prediction?

    Apply

    Worked example

    Problem

    ITER's goal is a pulse with $P_\text{heating} = 50\ \text{MW}$ and $P_\text{fusion} = 500\ \text{MW}$. Calculate the fusion gain $Q$ and the power carried by the helium nuclei. Do the helium nuclei heat the plasma more than the external heating does?

    Step 1/7

    Given: heating power ${P_\text{heating} = 50\ \text{MW}}$, fusion power ${P_\text{fusion} = 500\ \text{MW}}$. In one $\text{D–T}$ reaction, ${E_\text{total} = 17.6\ \text{MeV}}$ is released and the helium nucleus carries ${E_\alpha = 3.5\ \text{MeV}}$. Find: $Q$ and the helium power $P_\alpha$.

    Step 2/7

    Principle: $Q$ is the ratio of the two powers. Every reaction gives the same share of its energy to the helium nucleus, so the helium nuclei carry the same share of the fusion power.

    Step 3/7

    Formula: $$\begin{aligned} Q &= \frac{P_\text{fusion}}{P_\text{heating}} \\ P_\alpha &= \frac{E_\alpha}{E_\text{total}} \cdot P_\text{fusion} \end{aligned}$$

    Step 4/7

    Unit conversions: None are needed. Both powers are in megawatts and both energies in megaelectronvolts, so the units cancel in each ratio.

    Step 5/7

    Substitution: $$\begin{aligned} Q &= \frac{500\ \text{MW}}{50\ \text{MW}} = 10 \\[6pt] P_\alpha &= \frac{3.5\ \text{MeV}}{17.6\ \text{MeV}} \cdot 500\ \text{MW} \\ &= 0.1989 \cdot 500\ \text{MW} \\ &= 99.4\ \text{MW} \end{aligned}$$

    Step 6/7

    Answer: $Q = 10$ and $P_\alpha \approx 99\ \text{MW}$, two significant figures as in $3.5\ \text{MeV}$. The helium nuclei heat the plasma with about $99\ \text{MW}$, about twice the external $50\ \text{MW}$: about two thirds of the heating comes from fusion itself.

    Step 7/7

    Reasonableness: The helium nucleus is about four times heavier than the neutron, so by conservation of momentum it gets about one fifth of the energy: one fifth of $500\ \text{MW}$ is $100\ \text{MW}$. The other, about $400\ \text{MW}$, leaves with the neutrons and heats the blanket. $Q = 10$ is far above JET's $0.67$, which is why ITER is so much larger.

    Fuel, blankets and radiation

    Tritium fuel cycle. Only a small fraction of the fuel, about one per cent according to ITER, fuses on its way through the plasma. Cryopumps pump the exhaust out of the vessel, and the tritium plant separates the hydrogen isotopes and sends deuterium and tritium back to the fuelling system. Tritium is radioactive (half-life $12.3$ years, a weak beta emitter), so detritiation systems take it out of air and water.

    Breeding. Tritium is very rare; today it comes mainly from heavy-water fission reactors. A power plant must make its own from lithium: $^{6}_{3}\text{Li} + \text{n} \to {}^{4}_{2}\text{He} + {}^{3}_{1}\text{H} + 4.8\ \text{MeV}$. In ITER, a few test blanket modules will try out ways to do this.

    Radiation protection. The fast neutrons make the vessel and the blanket radioactive (activation), so parts inside the vessel are changed by remote-handling robots. A thick concrete bioshield surrounds the machine. The fuel leaves no long-lived high-level waste, and the reaction stops by itself if anything fails, but tritium, activated parts, the strong magnets and the heat are real hazards. ITER obtained the licence of a French nuclear installation in 2012.

    How much tritium burns in one pulse?

    During one planned pulse ITER produces $500\ \text{MW}$ of fusion power for $400\ \text{s}$. Each $\text{D–T}$ reaction releases $17.6\ \text{MeV}$ and uses one tritium atom, mass $3.016\ \text{u}$.

    How many grams of tritium fuse during the pulse? ($1\ \text{MeV} = 1.602 \cdot 10^{-13}\ \text{J}$, $1\ \text{u} = 1.661 \cdot 10^{-27}\ \text{kg}$)

    g
    Hint 1: a guiding question

    First find the fusion energy of the whole pulse, $E_\text{pulse} = Pt$, in joules.

    Hint 2: what is the connection

    The number of reactions is $N = E_\text{pulse} / E$, with $E = 17.6\ \text{MeV}$ in joules.

    Hint 3: an intermediate step

    $N \approx 7.09 \cdot 10^{22}$. Multiply by the mass of one tritium atom in kilograms, then change to grams.

    Show the solution

    Given

    fusion power $P = 500\ \text{MW} = 5.00 \cdot 10^{8}\ \text{W}$, pulse length $t = 400\ \text{s}$, energy of one $\text{D–T}$ reaction $E = 17.6\ \text{MeV}$, mass of a tritium atom $m_\text{T} = 3.016\ \text{u}$, $1\ \text{u} = 1.661 \cdot 10^{-27}\ \text{kg}$, $1\ \text{MeV} = 1.602 \cdot 10^{-13}\ \text{J}$

    Find

    the mass $m$ of tritium that fuses during the pulse

    Principle

    Each reaction uses one tritium nucleus and releases $17.6\ \text{MeV}$. The number of reactions is the fusion energy of the pulse divided by the energy of one reaction, and the mass is that number times the mass of one atom.

    Formula

    $$N = \frac{Pt}{E}, \qquad m = N m_\text{T} = \frac{Pt}{E}\,m_\text{T}$$

    Unit conversions

    $E$$= 17.6\ \text{MeV}$
    $= 17.6 \cdot 1.602 \cdot 10^{-13}\ \text{J}$
    $= 2.820 \cdot 10^{-12}\ \text{J}$
    $m_\text{T}$$= 3.016 \cdot 1.661 \cdot 10^{-27}\ \text{kg}$
    $= 5.010 \cdot 10^{-27}\ \text{kg}$

    Substitution

    $$\begin{aligned} N &= \frac{5.00 \cdot 10^{8}\ \text{W} \cdot 400\ \text{s}}{2.820 \cdot 10^{-12}\ \text{J}} \\ &= 7.093 \cdot 10^{22} \\[6pt] m &= 7.093 \cdot 10^{22} \cdot 5.010 \cdot 10^{-27}\ \text{kg} \\ &= 3.554 \cdot 10^{-4}\ \text{kg} \end{aligned}$$

    Answer

    $m \approx 0.36\ \text{g}$

    This is the tritium burned in one $400$-second pulse; two significant figures, because the fusion power and the pulse length are planned, rounded values.

    Reasonableness

    One gram of tritium has about $2 \cdot 10^{23}$ atoms, and the pulse needs about $7 \cdot 10^{22}$ reactions, about a third of that. The pulse releases $200\ \text{GJ}$ of fusion energy from less than half a gram of tritium (and about a quarter of a gram of deuterium): the huge energy density that makes fusion attractive. Because only about one per cent of the fuel burns on one pass, far more tritium is pumped through the plasma and recycled.

    Find the error

    A student writes: "JET reached $Q = 0.67$ in 1997, so JET produced $67\ \%$ of the electricity it used." What is wrong?
    Optional Find the parts

    Test yourself: the explorer asks you to find six parts from their descriptions.

    Common misconception

    "$Q = 10$ means that ITER gives ten times more electricity than it uses." $Q$ compares two powers in the plasma: the fusion power and the heating that reaches the plasma. ITER produces no electricity at all, and the whole plant draws far more from the grid than the $50\ \text{MW}$ that reaches the plasma.

    A second mistake is "the plasma is $150$ million degrees, so the machine must be extremely hot everywhere". The plasma is hundreds of thousands of times less dense than air, and the magnetic field holds it away from the walls. A few metres away, the magnets are at about $4\ \text{K}$.

    Check your understanding

    1. Concept: breakeven

    What does $Q = 1$ mean?

    Suggestion: one answer does not show everything you can do, but review the theory summary.

    2. Calculation: a record

    In 1997 JET produced $16\ \text{MW}$ of fusion power while $24\ \text{MW}$ of heating reached the plasma. What was its fusion gain?

    Suggestion: one answer does not show everything you can do, but review the theory summary.

    3. Gain and viability

    A laboratory reports that its plasma reached $Q = 1.5$ for a few seconds. Which conclusion is justified by this result alone?

    Suggestion: one answer does not show everything you can do, but review the theory summary.

    4. Explain and argue

    Your friend says: "ITER makes $500\ \text{MW}$. That is enough for a city, so why don't they connect it to the grid?" Answer your friend in four or five sentences. Use $Q$, numbers and at least one reason why a power plant needs more than ITER can show.

    Word bank

    fusion power · heat · turbine · gain $Q$ · experiment · to draw power from the grid · to breed · pulse

    Sentence starters

    • That is a good question, but …
    • The $500\ \text{MW}$ is …, not …
    • ITER is built to …, whereas a power plant …
    • Even if …, it would still …

    Summary

    • ITER's superconducting magnets (toroidal field coils, poloidal field coils, central solenoid) hold and shape the plasma; the vacuum vessel, the blanket and the divertor surround it; beams and waves heat it.
    • Fusion gain: $Q = P_\text{fusion} / P_\text{heating}$. $Q = 1$ is scientific breakeven; JET reached $0.67$ in 1997; ITER aims at $Q = 10$, $500\ \text{MW}$ from $50\ \text{MW}$.
    • At $Q = 10$ the helium nuclei carry about $100\ \text{MW}$ and heat the plasma more than the external heating: a burning plasma.
    • $Q$ is a plasma gain, not electricity. ITER produces no electricity, and a power plant needs much more than a high $Q$.
    • Tritium is recycled in a closed loop and must later be bred from lithium; neutrons activate the structure, so ITER is a licensed nuclear installation.

    Le coin français

    The French name of the tokamak is the same word, le tokamak, and many words of the machine look like English ones. Listen, repeat, and say the last sentence to your partner.

    Photographs and videos

    • ITER poloidal field coil factory. Johannes Reimer. source, CC BY 4.0
    • An ITER vacuum-vessel sector in the assembly hall, March 2024. Lauri Hellsten. Photograph supplied by the author (2026-11-03), © Lauri Hellsten, all rights reserved; used with the author's permission