Posts with tag: science project

Science Fair Project Ideas That Use Real Physics

A levitation project stands out at a science fair because nothing else on the table is doing it. The catch is that the best version needs liquid nitrogen, and the version that needs none is a different project with different physics. This page sorts out which one you can actually build, then covers the planning, safety and presentation that decide your score.

The short answer

Three projects, sorted by what you can get hold of

Start here: six ways to demonstrate levitation
An overview of the whole field — still magnets, ring magnets, DIY tracks and three superconductor demonstrations. Read this first if you have not settled on a project yet.

Maglev train — no liquid nitrogen
Permanent magnets and a guide-walled track. Buildable in any classroom with no cryogenics and no special safety approval. Best suited to demonstrating friction, load and the limits of magnetic stability.

Superconductor hoverboard — needs liquid nitrogen
A YBCO disc cooled to −196 °C locks above a magnetic track and stays there at any angle. This is true stable levitation and it wins fairs, but you need a supply of liquid nitrogen and an adult supervising.

Which one should you pick?

Start with the liquid nitrogen question, because it decides everything else. If you can get a few litres through a school lab, a university department or a local welding or medical supplier, build the superconductor project — it demonstrates a genuine quantum effect and there is no way for a judge to mistake it for a trick. Our liquid nitrogen guide covers where to buy it and how to transport it.

If you cannot, do not treat the magnet project as a consolation prize. It answers a real engineering question — why do trains have a speed ceiling, and what happens when you remove the wheels — and it gives you something the superconductor project does not: a quantity you can vary and measure repeatedly in an afternoon.

Planning it properly

Judges reward a question with an answer, not a demonstration. Before you build anything, write down the variable you are going to change, the quantity you are going to measure, and what you expect to happen. A project that measures levitation height against load and plots the curve beats a project that simply makes something float, every time.

Then plan the practical side:

  • The steps of the experiment, in the order you will run them
  • Every material and instrument, including the ruler or scale you will measure with
  • How many times you will repeat each measurement — three runs minimum, so you can show your results are not a fluke
  • How you will record results as you go, rather than reconstructing them afterwards
  • A realistic timeline, working backwards from the fair date

Do a literature review before you start, too. Knowing that Earnshaw’s theorem forbids stable levitation with permanent magnets alone, or that flux pinning is what holds the superconductor in place, turns a demonstration into an explanation — and judges ask exactly these questions.

Safety comes first

The magnet project has two hazards worth naming in your write-up: strong neodymium magnets can pinch badly when they snap together, and they will erase cards and damage phones and hard drives kept nearby.

Liquid nitrogen needs more care. It boils at −196 °C, so it causes cold burns on contact, and it displaces oxygen as it evaporates. Handle it with an adult present, in a ventilated room, wearing eye protection and insulated gloves, and never seal it in a closed container. The handling guide covers storage, transport and what to do if it spills. Schools running this as a class activity can also use our institutional ordering route, which includes a risk assessment template.

Presenting to the judges

If you want a worked example of a project built for judging criteria — research question, variables, field-cooling protocol, force measurement, uncertainty and the graphs — follow our complete flux-pinning force experiment method.

Lead with the question, not the apparatus. Show your data — a graph beats a photograph — and be straightforward about what your setup does not prove. If your maglev train relies on guide walls for stability, say so and explain why the physics requires them. Admitting a limitation and explaining it reads as understanding; hiding it reads as not knowing.

Practise the demonstration until it works reliably, and have a plan for when it does not. Judges will ask why it works, so rehearse that answer in plain language before you rehearse the technical version.

The physics behind it

If you want to understand what you are demonstrating, the Meissner effect versus flux pinning explains why a superconductor holds its position instead of sliding away — the two are routinely confused, and getting it right will distinguish your project. What superconducting levitation is covers the underlying mechanism, and The Physics collects the rest of our explanatory articles.

Magnetic Levitation Science Project

This project levitates a small train on permanent magnets alone — no liquid nitrogen, no cryogenic handling, no special safety kit. That makes it one of the few levitation projects you can build and demonstrate in an ordinary classroom. If you can get hold of liquid nitrogen, the superconductor hoverboard project shows genuinely stable levitation and tends to score higher with judges.

Why would anyone want a train that floats?

Moving anything takes energy. A train resists changes to its velocity in proportion to its mass, which is why a heavier train needs a bigger push to get going, and why that push costs more fuel. Getting up to speed is only half the problem, though. Once a train reaches cruising speed it still burns energy continuously, because resistance forces are constantly trying to slow it down.

Two forces dominate. Air drag grows sharply with speed. Rolling friction comes from the wheels themselves — steel wheels flexing against steel rails, bearings turning, and wheels slipping when the grip runs out. Wheel slip is the practical ceiling: past roughly 300 km/h, conventional wheeled trains start fighting their own contact patch more than the air.

Remove the wheels and you remove that ceiling. A train that never touches its track has no rolling friction and no wheel slip, leaving only air drag to overcome. That is the entire argument for magnetic levitation, and it is the argument your project is demonstrating.

Why magnets alone refuse to hold still

Magnets are the obvious way to lift something without touching it. Put two magnets close together with like poles facing and they push apart hard enough to carry real weight.

The catch is stability. Try balancing one magnet above another and it will not simply hover — it flips, slides sideways and falls. This is not a matter of technique. It is a result known as Earnshaw’s theorem: a stationary object cannot be held in stable equilibrium by permanent magnets alone. Every position that looks balanced is balanced the way a pencil is balanced on its tip.

Real maglev systems solve this with an active stabilising mechanism — sensors and electromagnets that strengthen the field when the train drops and weaken it when the train rises, thousands of times per second. A classroom project solves it mechanically instead, with guide walls that physically stop the train escaping sideways while the magnets carry its weight.

That distinction is worth stating plainly in your write-up, because it is the single point most projects get wrong. Your train is magnetically supported and mechanically guided. It is not freely levitating. The only tabletop way to get true stable levitation without contact is flux pinning in a superconductor, which is a different experiment and needs liquid nitrogen.

What you need

  • A magnetic steel plate, roughly 7.5 × 30 cm, to act as the track base
  • About 70 permanent cube magnets, 10 × 10 × 2 mm
  • A Perspex cube for the train body, with double-sided adhesive
  • Perspex spacers to set the width of the track channel
  • A ruler, adhesive tape and a few non-magnetic coins for the measurements

The magnetic train kit contains all of the above along with step-by-step assembly videos, if you would rather not source the magnets individually.

Building the track

  1. Lay the wider Perspex spacer along the centre of the steel plate. This sets the channel the train will run in.
  2. Fill one side of the spacer with cube magnets, all pointing the same way. The steel plate holds them in place while you work.
  3. Fill the other side the same way, keeping the polarity consistent along the whole run.
  4. Fit magnets to the underside of the Perspex train cube so that it faces the track with the same pole, producing repulsion.
  5. Add the guide walls either side of the channel, close enough to stop the train tipping out but not so close that they drag.
  6. Set the train down in the channel. It should float a few millimetres clear and glide with a light push.

One detail trips people up: magnets attract when stacked along the field direction, but two magnets placed side by side attract only when their polarities are opposed. If a section of your track keeps flipping magnets around as you lay them, the polarity of that row is fighting its neighbour — turn the row over rather than forcing individual pieces.

Experiments worth running

A track that floats a train is a demonstration, not an experiment. What turns it into a science fair project is measuring something and explaining the result.

  • How much can it carry? Tape coins to the top of the train one at a time until it settles onto the track. That load is your levitation capacity.
  • How does height vary with load? Measure the gap with a ruler after each coin, then plot height against weight. The line is not straight — can you explain why the force climbs so steeply as the gap closes?
  • Does magnet count matter? Compare four magnets under the train against two. Does twice the magnet give you twice the clearance?
  • Where does the energy go? Give the train a consistent push and time how far it travels. With rolling friction gone, what is actually slowing it down?

Presenting it well

Judges reward projects that answer a question rather than projects that perform a trick. Lead with the physics problem — friction limits how fast trains can go — then show your height-versus-load graph as evidence of how the magnetic force behaves. Be upfront that the guide walls are doing the stabilising work, and explain why Earnshaw’s theorem makes them necessary. That honesty reads as understanding, not as a shortcoming.

If you want to go further, flux pinning versus the Meissner effect explains how superconductors achieve the stability that permanent magnets cannot, and our science fair project ideas covers how to structure and present the finished board.

What Is Superconducting Levitation and How Does it Work? 

Published: December 6, 2022 в 4:48 pm

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Categories: Experiments,The Physics

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Ever wondered how Quantum levitation is possible? It’s all due to superconducting materials! These materials have special properties that allow them to conduct electricity without any resistance. When a magnet is placed near a superconducting material, the superconductor does two things at the same time – expel some of the magnetic field from its body (Meissner effect) and pin some of the field inside (flux pinning). This creates two effects: 
Magnetic repulsion – the superconductor “becomes” an opposite magnet and feels a repulsion force. 
Quantum Locking – locking of the superconductor in the surrounding magnetic field, preventing the pinned magnetic flux lines from moving inside the material.

How Does Superconducting Levitation or Quantum Levitation Work?

Superconducting levitation requires two conditions to be met in order for it to happen. First, the material itself must be cooled to temperatures well below room temperatures (around -163°C / -261°F). This is because all the superconductors we know of today, become superconductive only at low temperatures. Second, a powerful magnet must be placed near the superconductor. Initially, this causes electron pairs (Cooper pairs) within the material to start moving, and produce a magnetic field opposite to the external field, and as a result create magnetic repulsion. This is called the Meissner effect

Meissner effect
A small magnetic ball is dropped above a superconductor. Its magnetic field is being expelled from the superconductor and as a result the ball is repelled from the superconductor.

If the magnetic field is strong enough and the superconductor is of the right type (called Type II), the field will overcome the Meissner expulsion and penetrate the body of the superconductor. The magnetic field will enter the body in the form of discrete magnetic tubes or fluxons. The fluxons may get stuck in pinning centers – areas where superconductivity is relatively weaker, such as defects, grain boundaries, etc. This effect is called Flux Pinning. Any movement of the fluxons outside the pinning centers will cause the energy of the system to increase and will thus be followed by a force the tries to negate it. This is similar to a ball at the bottom of a bowl where any movement of the ball will increase its potential energy and will thus be encountered with a returning force towards the center. 

Fluxons pinned inside superconductor
Discrete flux line (fluxons) shown from above as they enter a superconductor and get stuck in an array of pinning centers.
Ball rolling inside a bowl
A ball feels a returning force inside a potential wall

When the flux is pinned inside the material it locks the superconductor in place and we get the 3D locking effect. The superconductor can be frozen mid-air in any orientation and even be suspended below the magnet. We can distinguish between the Meissner repulsion and flux pinning with an easy-to-do experiment:

Flux pinning force measrument
Flux pinning forces can be both negative and positive
Meissner effect force measrument
Meissner effect repulsion force is always positive

Read more about these here

What determines the strength of the locking?

Superconducting Critical Current – Superconductors have one “card” in its sleeve – the ability to transfer currents without resistance. These supercurrents produce a magnetic field that interacts with the external field and are the source of the levitation and suspension forces. 
The maximal levitation force depends strongly on the maximal internal current a superconductor can transfer or critical current, I. A typical value of Ic in modern high-Tc superconductors is ~500A for a 1cm wide tape at liquid nitrogen temperatures (77K). The higher the critical current the stronger the levitation force.

External magnetic Field strength & gradient – Another parameter that affects the levitation force is the strength of the external magnetic field and its spatial gradient. The levitation forces stem from the energy changes when fluxons move inside the superconductor and in/out of pinning centers. The stronger the magnetic field the more fluxons are and the overall force needed to move them. Also, if the external field changes rapidly in space, having a strong spatial gradient, the fluxons will try to move when the superconductor is moved which will require a stronger force. 

Quantum locking changing angle2
A superconductor is locked mid-air in different orientations above a permanent magnet.

Superconductor Hoverboard Science Fair Project: Build It and Measure It

Published: September 19, 2022 в 1:36 pm

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Categories: Science fair,The Physics

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A superconductor cooled in liquid nitrogen will hang in mid-air above a magnetic track and glide along it with almost no friction — a real hoverboard, at desk scale. It also makes an unusually strong science fair project, because unlike most levitation demonstrations you can measure it, not just admire it.

A levitating superconductor gliding along a magnetic track, the hoverboard effect

What you are actually demonstrating

This is the part most projects get wrong, and getting it right is what separates a good board from an average one.

Two different effects are at work, and they are not the same thing:

  • The Meissner effect is the superconductor expelling magnetic field from its interior. On its own it produces repulsion — and repulsion alone is unstable. A magnet floating purely by repulsion slides off sideways almost immediately.
  • Flux pinning is what actually holds the disc in place. YBCO is a type-II superconductor, which means magnetic field does not get expelled completely. Instead it threads through the material in thousands of discrete quantised tubes, or vortices, and defects in the ceramic trap those vortices where they are. The disc is effectively pinned to the field pattern it was cooled in.

That distinction is why the disc will hang below a magnet, or sit locked at an angle, and stay there. Pure repulsion cannot do that. If your write-up says “the Meissner effect makes it float”, it is not quite right — and a physics teacher will notice.

Turning a demonstration into an experiment

A levitating disc is a spectacle. A science project needs a question with a measurable answer. The demonstration becomes an experiment the moment you introduce something you can change and something you can measure.

Workable questions, in rough order of difficulty:

  1. How does levitation height depend on the field strength below the disc? Change the number of magnet layers; measure the gap.
  2. How long does levitation last, and what determines it? Time from removal of coolant to the disc touching down, against ambient temperature or disc thickness.
  3. How does track spacing affect how freely the disc moves? Vary the gap between magnet rows; measure how far a single push carries the disc.
  4. Does the cooling height change the pinning? Cool the disc at 3 mm above the track, then at 10 mm, and compare where it comes to rest. This one surprises people, and it is the most direct evidence of flux pinning there is.

Question 4 is the strongest project of the four, because the result is counter-intuitive and it tests the actual mechanism rather than just the outcome.

What you need

  • A YBCO superconductor disc (a “levitator”)
  • Neodymium magnets, 10 × 10 × 2 mm
  • A steel sheet to build the track on
  • Track spacers
  • Plastic tongs — never handle a cooled disc with bare fingers
  • Liquid nitrogen, roughly half a litre, and a shallow foam tray
  • A ruler or calipers, and a phone that can shoot slow motion

Everything except the liquid nitrogen is in the superconductivity kitsthe two-minute kit guide will tell you which one fits. Liquid nitrogen has to be sourced locally — the liquid nitrogen guide covers where to buy it and how to handle it safely.

Build 1 — the magnet matrix

Magnets arranged in a matrix with alternating polarity for quantum locking

Lay the magnets on the steel sheet in a square — 2 × 2, then 3 × 3, then 4 × 4. Orient them so that neighbours attract side by side, which means adjacent magnets point in opposite directions. This alternating arrangement produces a strong, sharply varying field just above the surface, which is exactly what gives the vortices something to pin to.

Cool the disc in the tray for about a minute, until the vigorous bubbling settles down. Lift it with the tongs and place it a few millimetres above the matrix.

A superconductor locked in place above a four-magnet array

Push it gently sideways, then downwards, then try to rotate it. It resists in every direction — not just upwards. That is the observation worth recording, because it is what rules out simple magnetic repulsion.

Build 2 — the straight track

Rearrange the magnets into two parallel rows: neighbours across the track attract, magnets along the track repel. Push them as close together as they will sit. You want the field to be uniform along the track and strongly varying across it.

A superconductor moving freely along a straight magnetic track with almost no friction

Cool the disc, set it on the track, and give it the lightest possible push. It is locked across the track but free along it, so it keeps going until air resistance and small field irregularities stop it. Time how long a single push lasts, and repeat it five times — the spread between runs is itself a result worth reporting.

Build 3 — introduce your variable

Now change one thing at a time and measure. Insert a spacer to widen the gap between the two magnet rows and repeat the timed push. Or cool the disc at two different heights above the same track and mark where it settles in each case.

Take five readings per condition, not one. Superconductor demonstrations vary between runs — how much they vary is a genuine finding, and showing that you know to repeat measurements is worth more to a judge than a single dramatic result.

Observe and think

  • Why is the disc stable sideways as well as vertically? What would happen if only the Meissner effect were involved?
  • Why does the disc return to the height at which it was cooled, rather than to the closest approach?
  • What is actually stopping the disc on a straight track, if there is no contact friction?
  • Why does the effect end abruptly rather than fading away gradually?

Safety

Liquid nitrogen boils at −196 °C and causes cold burns on contact. Work in a ventilated room, wear eye protection and insulating gloves, never seal it in a closed container, and have an adult present. The disc stays dangerously cold for a while after it leaves the bath — always move it with tongs. Full guidance and a downloadable risk-assessment template are in the liquid nitrogen guide.

Common mistakes

  • Not cooling for long enough. Wait until the bubbling calms. A partly cooled disc will levitate weakly and drop early.
  • Magnets all facing the same way. The field then barely varies above the surface and there is little for the vortices to pin to.
  • Handling the disc warm-side down. Frost forms quickly; keep the cooled face towards the track.
  • Reporting one run. Repeat everything five times and report the spread.
  • Calling it anti-gravity. Gravity is unchanged throughout. The disc is held by pinned magnetic flux, and saying so correctly is free marks.

Where to go next

If the project goes well, the natural extension is to measure the transition itself: cool the disc while monitoring its resistance and find the temperature at which it drops to zero. That needs a four-point probe setup and turns a visual demonstration into a quantitative one.