Index力と場Sticker

Diagonix

Malus’s Law / Three-Polarizer Effect Physics

\[I = I_0\cos^2\theta\]
通常価格 $4.99 USD
通常価格 セール価格 $4.99 USD
セール 売り切れ
Size
Surface

Diagonix is a Pixelated Physics law character, one of our forces designs. Two crossed polarisers block all light, but a third at 45° between them lets an eighth through. Malus’s law, I = I₀cos²θ. This is a 3" × 3" pixel-art sticker. The physics panel below gives the equation, what each symbol means and the sources.

Shipping calculated at checkout by destinationMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Shipping calculated at checkout by destination. Printed to order for you.

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

A polarizer passes the fraction cos²θ of already-polarized light. Two crossed polarizers block everything, but slip a third one between them at 45° and one-eighth of the original unpolarized light gets through.

Diagonix is a diplomat, and her trick is getting in the way.

Light’s electric field can oscillate in any direction across the beam. A polariser passes only the part of the oscillation along its transmission axis. Ordinary unpolarised light loses half its intensity at the first polariser and comes out vertical. Put a horizontal polariser after it and nothing gets through at all, because vertical light has no horizontal part. Two feuding border guards, one admitting only vertical travellers and one only horizontal, and nobody crosses.

Now Diagonix steps in between, tilted at 45°. The rule for light meeting a polariser at angle θ is the first line on this page, Malus’s law: the intensity drops by cos²θ. At 45° that is one half. So she lets half of the vertical travellers through, re-stamped diagonal. The horizontal guard then sees diagonal light, also 45° away, and lets half of those through. Half, then half, then half: one eighth of the original unpolarised light emerges, where before there was none. The bars on her clipboard read ½, ¼, ⅛, the last two lines.

Étienne-Louis Malus, an officer in the French corps of engineers who had served on Napoleon’s expedition to Egypt, published his discovery that reflected light is polarised in 1809. The cosine-squared rule carries his name.

The surprise is not that the middle filter adds light. It doesn’t; it only removes some. What it changes is the question the last filter gets to ask. Light that has just answered “diagonal” has a fresh, even chance of answering “horizontal”, whatever it said before.

Nothing got through. Then they added me.

Equations

\[I = I_0\cos^2\theta\]
\[I_{\text{out}} = \frac{I_0}{2}\cos^2 45^\circ\,\cos^2 45^\circ\]
\[I_{\text{out}} = \frac{I_0}{8}\]
Symbols
SymbolMeaningUnit
\(I\) intensity after one ideal polariser \(\mathrm{W/m^2}\)
\(I_0\) intensity arriving (unpolarised for the three-polariser line) \(\mathrm{W/m^2}\)
\(\theta\) angle between the light's polarisation and the polariser's transmission axis \(\mathrm{rad}\)
\(I_{\text{out}}\) intensity after the vertical, 45° and horizontal polarisers in turn \(\mathrm{W/m^2}\)

Source Malus, É.-L. (1809). Sur une propriété de la lumière réfléchie. Mémoires de physique et de chimie de la Société d'Arcueil, 2, 145–158.