• Pixel-art sticker of Hallway, personifying Hall Effect, with the caption "Current? Step Aside."

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Hallway

Hall Effect Physics

\[V_H = \frac{I B}{n q t}\]
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Meet Hallway the hall monitor, who waves the current aside: a magnetic field pushes moving charges to one side of a conductor and builds a transverse voltage, VH = IB/(nqt). The sign of the voltage shows whether the carriers are positive or negative. Pixel-art kiss-cut sticker in 2, 3, 4 and 6 inches; equation, symbols and sources in the physics panel below.

Size
Surface

Flat $6 shipping worldwideMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Flat $6 shipping on every order, worldwide, whatever's in it.

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

Meet Hallway, a strip of conductor who builds a sideways voltage whenever a magnetic field pushes on her current.

Charges moving through a conductor in a magnetic field feel a sideways magnetic force. They drift to one edge until the electric field from the piled-up charge balances the magnetic push. The voltage across the strip is the Hall voltage, discovered by Edwin Hall in 1879. It is IB/(nqt): it grows with current and field, and is smaller when there are more carriers to share the current.

The sign of the Hall voltage reveals the sign of the carriers. In most metals they are electrons, but in some semiconductors the current behaves as if it is carried by positive 'holes'.

Hall sensors are cheap and everywhere: they measure magnetic fields, detect wheel and shaft rotation in cars, and sense the lid closing on many laptops.

Metals have huge carrier densities, so their Hall voltages are tiny. Semiconductors, with far fewer carriers, give much larger signals, which is why sensors use them.

Equations

\[V_H = \frac{I B}{n q t}\]
Symbols
SymbolMeaningUnit
\(V_H\) Hall voltage across the strip \(\mathrm{V}\)
\(I\) current \(\mathrm{A}\)
\(B\) magnetic flux density \(\mathrm{T}\)
\(n\) number density of charge carriers \(\mathrm{m⁻³}\)
\(q\) charge of each carrier \(\mathrm{C}\)
\(t\) thickness of the strip along B \(\mathrm{m}\)