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Field Work SheetLenzor, Gyrolla, Azurwake & Diagonix | 9 Pixel Art StickersSticker Sheet

Field Work Sticker Sheet – Lenzor, Gyrolla, Azurwake & Diagonix | 9 Pixel Art Stickers

Regular price $19.99 USD
Regular price Sale price $19.99 USD
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Shipping calculated at checkout. Free US shipping · $10 flat shipping outside the US.
Surface
White
Shape
Kiss-Cut
Size
5.83″ × 8.27″
Made
To order · shipping times

The Field Work sticker sheet gathers several Pixelated Physics characters on one page, each built on a real piece of physics. Nine kiss-cut pixel-art stickers on one A5 sheet: Lenzor (Lenz’s law), Gyrolla (cyclotron), Azurwake (Cherenkov), Diagonix (polarisers), plus props. Peel them off one at a time and stick them wherever the physics belongs.

Surface
Shape
Size

Details

What you getA5 sheet · 9 stickers

One A5 kiss-cut sheet (5.83″ × 8.27″) on white sticker paper with 9 stickers, made to order.

ShippingFree US

Free US shipping · $10 flat shipping outside the US.

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

Nine stickers on one sheet: four characters who do their work through fields, and the light that fields make.

Lenzor’s line is Change the Flux. I Push Back. Drop a magnet down a copper pipe and it sinks slowly. Its moving field induces eddy currents in the copper, and by Lenz’s law those currents oppose the change that made them, braking the fall to a steady terminal speed. That is the copper pipe marked SLOW.

Gyrolla’s line is Bigger Circle. Same Lap Time. A charge moving across a uniform magnetic field circles with radius r = mv/(qB), but its lap frequency qB/(2πm) does not depend on speed. Ernest Lawrence built the cyclotron on that fact in the early 1930s. That is the orbit in a field marked × (pointing into the page), where a positive charge goes round anticlockwise.

Azurwake’s line is Faster Than Light. In Water. Legally. Nothing outruns light in vacuum, but light in water travels at about c/1.33, and a charged particle can beat that. It then sheds a cone of blue light at cos θ = 1/(nβ), about 41° in water for β near 1, the glow Pavel Cherenkov saw in 1934. That is the cone on the H2O tag.

Diagonix’s line is Nothing Got Through. Then They Added Me. Two crossed polarisers block everything. Slip a third between them at 45° and an eighth of unpolarised light gets through: ½ × cos²45° × cos²45°. That is the three filters and the 1/8 tag.

Equations

\[\begin{gathered} \mathcal{E} = -\frac{d\Phi_B}{dt} \end{gathered}\]
\[\begin{gathered} q v B = \frac{m v^2}{r} \;\Rightarrow\; r = \frac{m v}{q B} \\ f_c = \frac{q B}{2\pi m} \end{gathered}\]
\[\begin{gathered} \cos\theta = \frac{1}{n\beta}, \qquad \beta > \frac{1}{n} \end{gathered}\]
\[\begin{gathered} I = I_0\cos^2\theta \\ I_{\text{out}} = \frac{I_0}{2}\cos^2 45^\circ\,\cos^2 45^\circ \\ I_{\text{out}} = \frac{I_0}{8} \end{gathered}\]
Symbols
SymbolMeaningUnit
\(\mathcal{E}\) EMF induced around one ring of the pipe \(\mathrm{V}\)
\(\Phi_B\) magnetic flux through that ring \(\mathrm{Wb}\)
\(t\) time \(\mathrm{s}\)
\(q\) charge of the particle \(\mathrm{C}\)
\(v\) speed perpendicular to the field \(\mathrm{m/s}\)
\(B\) magnetic flux density \(\mathrm{T}\)
\(m\) mass of the particle \(\mathrm{kg}\)
\(r\) radius of the circle \(\mathrm{m}\)
\(f_c\) cyclotron frequency, laps per second (non-relativistic; at high energy it falls by 1/γ) \(\mathrm{Hz}\)
\(\theta\) for Cherenkov light: angle between the emitted light and the particle’s path; for a polariser: angle between the light’s polarisation and the transmission axis \(\mathrm{rad}\)
\(n\) refractive index of the medium, about 1.33 for water \(\mathrm{1}\)
\(\beta\) particle speed as a fraction of c \(\mathrm{1}\)
\(I\) intensity after one ideal polariser \(\mathrm{W/m^2}\)
\(I_0\) intensity arriving (unpolarised for the three-polariser line) \(\mathrm{W/m^2}\)
\(I_{\text{out}}\) intensity after the vertical, 45° and horizontal polarisers in turn \(\mathrm{W/m^2}\)
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