Skip to product information
1 of 3
Regular price $6.99 USD
Regular price Sale price $6.99 USD
Sale Sold out
Shipping calculated at checkout. Free US shipping · $10 flat shipping outside the US.
Size
3" × 3"
Surface
White
Made
To order · shipping times

Expulsieur is a Pixelated Physics law character, one of our quantum designs. Meissner effect: below its critical point a type-I superconductor pushes out a weak magnetic field, even field already in. This is a 3" × 3" pixel-art sticker. The physics panel below gives the equation, what each symbol means and the sources.

Size
Surface

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Free US shipping · $10 flat shipping outside the US, whatever's in your order.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

Full refund & replacement policy

The physics

Expulsieur is the maître d’ of a restaurant made of lead, and magnetic fields do not get a table.

A superconductor loses all electrical resistance when it is cold enough. A merely perfect conductor would freeze in whatever magnetic field it held at that moment. In 1933 Walther Meissner and Robert Ochsenfeld cooled cylinders of tin and lead in a weak magnetic field and measured the field around them. As the metal turned superconducting, the field inside was pushed out, including field that was already there. That is the Meissner effect: a superconductor is not just a perfect conductor but a perfect diamagnet, the first line on this page.

Lead turns superconducting below about 7.2 K. Above that, field lines wander through the dining room like any customer. Below it, Expulsieur shows them out. They bend round the building and crowd at the edges, continuous, never ending inside.

Two years later the brothers Fritz and Heinz London wrote equations for it. The field does not stop dead at the surface; it fades exponentially over a short distance, the London penetration depth, the second and third lines. Lines may lean in at the doorway, but not far.

He has limits. Lead is a type-I superconductor, and the expulsion works only for applied fields below its critical field, about 80 mT near absolute zero; above that, superconductivity collapses. And in real samples, cooling in a field often expels the flux only partly, a caveat he would rather you didn’t mention.

Still, once the room is cold, the rule at his door is simple.

Your field waits outside.

Equations

\[\mathbf{B}_{\text{inside}} = 0\]
\[B(x) = B_0\,e^{-x/\lambda_L}\]
\[\lambda_L = \sqrt{\frac{m}{\mu_0 n_s e^2}}\]
Symbols
SymbolMeaningUnit
\(\mathbf{B}_{\text{inside}}\) magnetic field in the bulk of the superconductor (applied field below the critical field) \(\mathrm{T}\)
\(B(x)\) field at depth x below the surface \(\mathrm{T}\)
\(B_0\) field at the surface \(\mathrm{T}\)
\(x\) depth below the surface \(\mathrm{m}\)
\(\lambda_L\) London penetration depth \(\mathrm{m}\)
\(m\) electron mass \(\mathrm{kg}\)
\(\mu_0\) vacuum magnetic permeability \(\mathrm{N/A^2}\)
\(n_s\) density of superconducting electrons (conventions differ by a factor of 2) \(\mathrm{m^{-3}}\)
\(e\) elementary charge \(\mathrm{C}\)
View full details