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🔬 Stellarator Magnetic Confinement: 3D Cutaway

Inspect a fictional stellarator with non-planar coils, vacuum sections, cryogenic circuits, and interactive textbook plasma calculations.

Physics & Mechanics3DModerate60 FPS📱 Mobile-adapted🤖 ChatGPT
Stellarator Magnetic Confinement: 3D Cutaway ↗ Open standalone
⚙ Under the hood

Interactive educational 3D stellarator assembly with non-planar coils, vessel sectors, thermal shields, vacuum ports and textbook plasma readouts.

stellaratormagnetic confinementplasma physics

3D · Three.js / WebGL renderer · 60 FPS target · runs fully client-side, no install

About this simulation

Stellarator Magnetic Confinement: An Interactive 3D Cutaway

A Machine That Shapes a Magnetic Field in Three Dimensions

A stellarator is an experimental magnetic-confinement device designed to hold a very hot, electrically conducting gas called plasma away from surrounding material surfaces. Rather than relying principally on an induced toroidal plasma current to twist the magnetic field, a stellarator uses carefully shaped external coils. Their combined field has a three-dimensional structure. This distinction matters because the shape of the magnetic field, not simply its magnitude, strongly influences how charged particles move around the installation.

This interactive exhibit presents a fictional scientific machine named HELION V-5. The model is not a reproduction of any operating facility. It is an engineering-inspired reconstruction containing a contoured plasma vessel, non-planar coil bodies, trim coils, structural supports, cryogenic conduits, diagnostic access ports, first-wall protection, divertor representations, service cabinets, and removable outer enclosure panels. The construction illustrates why a stellarator is better understood as an interconnected laboratory infrastructure than as one smooth metal ring.

Select any component to learn its intended role. Switch to cutaway mode to see beneath the housing, increase the exploded distance to separate assemblies, or follow the dependency-guided build sequence. The operation view displays a stylized luminous plasma volume and moving particles. Those motion graphics explain concepts, not the results of a validated magnetic or plasma calculation.

What Is Actually Being Confined?

A plasma is a gas whose charged particles include free electrons and ions. In magnetic confinement, the Lorentz force changes the direction of their motion. A charged particle moving with velocity v in an electromagnetic field experiences a force F = q(E + v × B). Its motion generally contains a component along the magnetic field and a rotation about that field, modified by gradients, curvature, collisions, and electric fields. Understanding the complete behavior of a plasma requires far more than drawing a helical line.

The plasma in a stellarator is normally arranged around a toroidal, or doughnut-like, volume. A simple circular magnetic field is not sufficient for good confinement, because curvature and gradients can produce drifts. Carefully designed three-dimensional fields give magnetic field lines a rotational transform: as they go around the torus, they also wind around its smaller cross-section. This winding is essential to the underlying confinement concept.

The visible pink volume in the exhibit is a teaching aid. It does not provide an actual pressure profile, electron density distribution, equilibrium flux surface, temperature map, or fusion reaction rate. The field trajectories are likewise illustrative. A physically credible field-line plot for an actual design would require a magnetic equilibrium and field integration, both beyond this installation explorer.

The Contoured Plasma Vacuum Vessel

Inside the installation is the plasma vessel, a sealed chamber surrounding the hot plasma. Vacuum conditions help reduce collisions with unwanted neutral gas, and the inner vessel provides the mechanical boundary for devices placed close to the plasma. Real vessel engineering involves complex welded geometries, thermal loads, sealing requirements, port intersections, surface treatment, and alignment. The exact arrangement depends on the particular experimental design.

Our model represents the plasma vessel with multiple connected toroidal sectors rather than one empty cavity. Each sector follows a deliberately wavy central path and has a shaped cross-section. This makes the internal geometry recognizable when viewed through the cutaway. Weld bands and alignment details are included to show where engineering attention would be directed, although they must not be read as construction drawings.

Surrounding material also serves a safety and maintenance role. Vacuum tightness is only one design objective; engineers must consider accessibility, in-vessel hardware, diagnostics, cleaning, pressure differences, and how assemblies can be replaced. The model's sections can be selected independently so that the scientific vessel is not visually lost beneath the impressive magnet structure.

Non-Planar Magnets and Rotational Transform

The distinctive feature of a modern stellarator is its non-axisymmetric coil system. A non-planar coil is shaped in three dimensions rather than lying in one plane. Several such coils, carrying electrical current, produce a combined magnetic field with a carefully optimized geometry. In some stellarator designs, additional planar or auxiliary coils help adjust particular field characteristics. The crucial point is not a single coil but the field resulting from the complete current distribution.

The large blue coil casings in this exhibit trace twisted paths around the torus. Copper-colored conductor accents make the winding direction easier to inspect, while separate auxiliary loops suggest correction and trim functions. These are visibly complex mechanical parts, with many points along each curved tube. They are nevertheless fictional educational shapes, not an optimized engineering layout or a field configuration that has been checked for confinement quality.

Superconducting magnets introduce another subsystem: thermal management. When operated in suitable cryogenic conditions, superconductors can carry current with extremely low electrical resistance. This does not remove the engineering challenges of mechanical stresses, current leads, quench protection, heat leaks, and refrigeration. The exhibit deliberately does not assign real current ratings, critical fields, or allowable stresses to its coils.

The Structural Skeleton and Load Path

Magnetic coils are not floating drawings. Their housings, support structures, bolts, load-transfer features, and foundations form a mechanical system. Electromagnetic forces can act between current-carrying conductors, while gravitational loads, assembly tolerances, vibrations, and temperature changes impose other demands. A realistic machine must maintain sufficient geometric accuracy as conditions change.

The model contains adjustable-looking supports beneath its ring, radial structural members, perimeter foundation rings, maintenance bridges, service gantries, and selected alignment surfaces. These components are presented as recognizable engineering functions rather than an approved support design. The visual hierarchy is intentional: the surrounding frame is darker, the vacuum-facing metal is brighter, and the magnet array uses distinctive blue tones so that the user can follow the main systems without confusing them.

The guided-assembly mode begins with foundations and advances through the vacuum vessel, internal surfaces, coils, shields, service lines, diagnostic access, outer enclosure, and plasma illustration. This dependency order helps explain which systems conceptually surround or support others. It is not a safe installation procedure and does not prescribe real lifting operations, weld sequences, or pressure testing.

Cooling Infrastructure, Insulation, and Electrical Feeds

Scientific devices with cryogenic magnets require separation between warmer surroundings and colder equipment. A cryostat is an enclosure designed to control heat transfer to its cold contents. Radiative thermal shields, insulating vacuum spaces, supports selected for thermal performance, cooling tubes, and electrical current leads all contribute to the engineering system. Heat may enter by radiation, conduction along supports, or conduction through connected service hardware.

The visible thermal panels in this exhibit are simplified shaped surfaces between the inner chamber and the external housing. Some can be hidden with the cutaway slider so the magnet casings are easier to see. Metallic tube routes represent illustrative helium supply lines; copper-colored feeds represent illustrative current distribution paths. The app does not calculate refrigerant mass flow, cooling capacity, pressure drop, or thermal contraction.

One useful distinction is that vacuum insulation is not the same as the plasma vacuum. The plasma vessel encloses the space in which the discharge occurs, while an outer insulating vacuum may surround cold magnet components. The two spaces can have different operational roles and requirements. Understanding this distinction is one reason the model uses multiple nested boundaries rather than a single polished shell.

Ports, Diagnostics, and the Problem of Access

A plasma experiment must be observed to be understood. Optical diagnostics, microwave systems, spectroscopy, magnetic probes, interferometry, and other instruments can provide information about plasma conditions. Ports through surrounding structures allow instruments and services to reach the appropriate region. An access opening must, however, coexist with thermal insulation, mechanical structure, vacuum boundaries, and shielding.

The exhibit includes radial bellows-like port tubes, thick bolted flanges, contrasting viewport elements, and repeated fasteners. The decorative glass surfaces indicate places where optical access might be required, but the program does not calculate a view cone or certify a vacuum window. Separate instrument cabinets represent supporting data-acquisition systems. No manufacturer hardware, facility labels, or proprietary trade dress has been replicated.

Try selecting a viewport, then isolating its subsystem. The surrounding shell disappears and the port architecture becomes visually apparent. Next, return to cutaway mode to see how the selected part relates to the vessel and nearby coils. This approach turns a visually dense scientific machine into a sequence of understandable spatial relationships.

Divertors, First-Wall Protection, and Exhaust

Even a well-confined plasma can exchange energy and particles with its surroundings. Plasma-facing components must withstand loads while supporting particle and impurity control. A divertor is a specially designed part of the edge-plasma interaction system, directing exhaust to protected surfaces. Its geometry and performance depend on magnetic topology, particle transport, heat flux, material choices, and active cooling.

Our internal section includes discrete armour-like tiles, target cassette shapes, and cooling manifolds. The pieces are meaningful as subsystem illustrations: they show that the machine contains important internal structures beneath its vacuum wall and magnet system. They do not predict strike-point locations, material erosion, peak thermal loading, or target lifetime. In particular, the positioning of these elements is illustrative and not an experimentally determined divertor layout.

The difference between magnetically confined central plasma and surfaces that manage exhaust is essential. Magnetic confinement reduces direct contact of the hot core with material walls; it does not make engineering at the plasma boundary optional. Selecting the in-vessel layer reveals these components in an otherwise visually crowded installation.

Reading the Live Physics Instruments

The interactive control panel contains an illustrative local magnetic field B, an illustrative proton temperature T, and an illustrative particle number density n. These values are teaching inputs. They are not measured characteristics of HELION V-5, and they should never be interpreted as its predicted operating point. The equations are basic textbook relationships evaluated in SI units.

Magnetic pressure is represented by pB = B²/(2μ₀), where μ₀ is the permeability of free space in the commonly used textbook approximation. It is also an expression for magnetic-field energy density in vacuum. The displayed result uses megapascals. Doubling field strength increases this quantity by a factor of four, illustrating why strong magnetic fields can have substantial engineering implications.

A characteristic proton speed is calculated with v = √(2kBT/mp), corresponding to equating kinetic energy with kBT for an illustrative particle. This is not the mean or root-mean-square speed of a complete three-dimensional Maxwellian velocity distribution. The associated uniform-field Larmor radius is ρL = mpv/(eB). It is a local textbook approximation, not a prediction of real particle confinement in the three-dimensional stellarator field.

The panel also evaluates p = nkBT for one ideal-gas species and f = eB/(2πmp) for the proton cyclotron frequency in a uniform magnetic field. The independent frequency check uses the angular cyclotron frequency and a separate conversion to cycles per second. The visible comparison is a numerical consistency check, not a validation against laboratory data. Changing any of the teaching controls updates relevant calculations immediately.

Modes, Visibility, and How to Explore

Start in cutaway mode to see the arrangement of coils, ports, shielding, and the shaped vessel. Increase the reveal slider to remove more front-facing enclosure panels. Return to exterior mode for an assembled housing view. The component isolation mode displays only the selected part's subsystem. Use the part search box to find an individual magnet, port, latch, support, or armour tile; each selected part has its own name and a short educational explanation.

Exploded mode translates components away from the center. This shows the assembly hierarchy but does not represent actual removal paths, safe clearances, or lifting trajectories. The Fit all camera action uses the translated component locations, so even at the largest separation every part remains inside the projected field of view. Orbit the camera to understand paths that overlap when viewed from only one direction.

Operation mode turns on animated tracers and a luminous toroidal volume. These lines and moving points are explanatory artwork. They are not field-line integration, charged-particle orbit following, or magnetohydrodynamics. All rendering and calculations are performed locally in the browser without analytics, external libraries, or a network dependency after the included files have loaded.

What the Exhibit Does Not Claim

The mechanical complexity of this model is intended to support scientific understanding. It does not verify magnet topology, fusion output, pressure loading, superconducting stability, vessel integrity, neutron shielding, radiation protection, or operational safety. Its units and equations describe local idealized relationships, not an end-to-end experiment. No manufacturing drawing or genuine device specification is supplied.

The fictional identity, colours, and arrangement are original to this digital exhibit. Some features are genuine scientific concepts, such as rotational transform and the use of non-planar coils. Others are engineering-inspired reconstructions or simplified educational representations. The animated plasma and stylized field paths belong specifically in the latter category. Recognizing these distinctions is part of reading a good scientific visualization responsibly.

Illustrative design, not affiliated with any real institution or manufacturer.

Frequently Asked Questions

1. What is the main difference between a stellarator and a tokamak?

Both use magnetic fields to confine toroidal plasma. A tokamak typically uses substantial induced plasma current as part of its confinement configuration, while a stellarator relies more heavily on externally shaped three-dimensional coils to produce rotational transform. There are multiple designs within both families, so this is a useful architectural distinction rather than a complete comparison of performance.

2. Why do stellarator coils have such unusual shapes?

Their three-dimensional shape helps produce the twisting magnetic geometry needed for confinement. A carefully selected winding system changes the field-line structure throughout the torus. Actual coil design is an optimization problem involving plasma equilibrium, particle transport, conductor manufacture, support loads, diagnostic access, and engineering constraints. The paths shown here express the principle rather than reproduce a real optimized solution.

3. Does the animated field show a real solution of Maxwell's equations?

No. The illustrated curves and particles are designed to communicate the idea of winding field geometry. They are not derived from the coil geometry by a Biot–Savart calculation, nor from a validated three-dimensional equilibrium solver. A real magnetic analysis requires current distributions, boundary assumptions, an appropriate field model, and independent validation.

4. Why does the plasma need a vacuum vessel?

A controlled low-background-gas environment helps experiments manage impurities, collisions, and the creation of the intended discharge. The vessel also acts as a mechanical boundary and supports diagnostic and plasma-facing systems. Vacuum engineering remains important even when the plasma is magnetically confined away from most material surfaces.

5. What are the large copper-coloured paths around the coils?

They are conductor accents, trim-coil illustrations, and electrical distribution routes. Their colour is a visual teaching convention. The app does not specify the electrical current, resistive losses, inductance, or actual superconducting conductor composition. Real conductor systems require separate electromagnetic, cryogenic, and structural analysis.

6. What purpose do thermal shields and cryogenic lines serve?

They are components of the thermal-control infrastructure around cold magnet systems. Insulating boundaries reduce unwanted heat flow, and cooling circuits remove heat from the appropriate structures. Exactly how a real system is cooled depends on its design. The illustrated lines are not an operational flow schematic or a certified thermal design.

7. What is a divertor in magnetic-confinement research?

A divertor helps manage particles and energy leaving the plasma edge by guiding exhaust to protected surfaces. It can support impurity control and removal of heat. The model's target-like internal cassettes are simplified illustrations; real divertor geometry and expected heat flux require a detailed magnetic and plasma-edge calculation.

8. Is magnetic pressure the same as plasma pressure?

No. The displayed magnetic-pressure expression, B²/(2μ₀), relates to the energy density of a magnetic field in the stated approximation. The displayed idealized particle pressure, nkBT, relates number density and temperature for one species. Magnetic confinement involves a balance of field geometry and plasma behaviour, not numerical equality of these two readouts under all circumstances.

9. Can this model predict fusion power or plasma stability?

No. Fusion power, confinement time, stability, collisional transport, radiation losses, heating, and exhaust require detailed scientific models and experimental inputs. This exhibit offers component inspection and textbook local calculations. Its aesthetic realism and interactive animation do not establish physical predictive accuracy.

10. Can I use the exploded view to plan a real assembly?

No. The separation paths and dependency stages are a conceptual explanation of subsystem order, not installation instructions. Real devices require verified design documents, engineering tolerances, specialized handling equipment, safety procedures, and manufacturer-specific information. The exploded mode is intended for science communication and spatial learning only.

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