Posts with tag: Quantum levitation

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.

A small Perspex maglev train carriage floating a few millimetres above a magnet-lined track, seen at an angle
The finished project: a carriage held clear of the rail by permanent magnets alone, no cryogenics involved.

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.

Side view of the carriage floating above the magnet rail with clear Perspex guide walls on either side holding it in the channel
Supported by magnets, guided by walls. The magnets carry the weight; the Perspex sides stop it sliding out.

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
Flat lay of the project parts: Perspex track pieces and end caps, two rows of cube magnets, and a block of spare cube magnets
Everything the track needs: the Perspex channel and end caps, two magnet rails, and the cube magnets for the carriage.

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.

Watch the build, step by step

These clips show the kit version being assembled. The sequence is the same if you are sourcing the parts yourself — lay the magnets in matched rows, box the channel in, then magnetise the carriage last.

Step 1
Step 2
Step 3a
Step 3b
Step 3c
Step 4
Step 5
Step 6
Step 7

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. Check every coin against a spare magnet first and set aside any that stick: a lot of modern coinage is steel under a thin copper or nickel plating, and a coin the track can pull on is no longer measuring weight alone. Copper, aluminium and cupronickel coins are all safe. Weigh one on a kitchen scale so you can report the capacity in grams rather than in coins.
  • 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.

The maglev track on a dark reflective desk, the carriage floating above the rail with its reflection below
Built once, it keeps working. The track needs no power and no consumables, so it can sit on a desk and still be demonstrated a year later.

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.

Related: Quantum locking explained — why a superconductor stays frozen in a magnetic field, and how to demonstrate it.

What Is Superconducting Levitation and How Does it Work? 

Published: December 6, 2022 в 4:48 pm

Author:

Categories: Experiments,The Physics

Tags: ,,,,,,

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

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. 

Discrete flux line (fluxons) shown from above as they enter a superconductor and get stuck in an array of pinning centers.
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 forces can be both negative and positive
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. 

A superconductor is locked mid-air in different orientations above a permanent magnet.

Related: Quantum locking explained — why a superconductor stays frozen in a magnetic field, and how to demonstrate it.

Hands-on Quantum Physics

Published: February 24, 2019 в 9:17 am

Author:

Categories: Experiments

Tags: ,,,,,,

Quantum Levitation has dazzled millions of people via major TV networks, the TED conference live and online, and in universities and schools around the world. But we haven’t just created a sophisticated demo for audiences to view; we developed our kits to be simple-to-use and highly engaging educational tools.  

You Can Experiment with Quantum Levitation

It’s time to take quantum phenomena into your own hands! We designed our mini-maglev kit for whole classrooms to be able to explore circular motion. Your students can operate the kit themselves, conducting meaningful experiments like:

  1. Circular motion – polar vs. cartesian coordinates
  2. Circular motion – constant velocity
  3. Harmonic motion I 
  4. Harmonic motion II – tuneable harmonic oscillator 
  5. Conservation of mechanical energy
  6. Linear momentum conservation I
  7. Linear momentum conservation II – plastic collisions

Each involves three straightforward steps:

1. Perform the experiment

Position the maglev track (horizontal / tilted), then lock the levitator/s on the track and prepare your smartphone camera. Record several videos of the experiment using different parameters.  

2. Extract the data

Export your videos to Tracker software. Examine the recorded motion of the levitators with your students, and have them identify the relevant parameter involved (coordinates, velocity, angle, etc). 

 

3. Analyze the data

Use Tracker, Excel, or a similar software to analyze the data you’ve collected. You can perform linear fitting, calculate energies, etc. Discuss the results with your students and enjoy a lively Q&A session about the experiment!