The second bright source doubles the screen position with the same geometry. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Second order needs a second-order path source

The source path difference is 4 m, exactly two wavelengths. That source order must match the screen order.

Δ=4 m=2λ\Delta=4\ \text{m}=2\lambda
Second-order path sourceThe path ledger supplies the order used on the screen.path Apath B

The second row is twice the first

With the same geometry, the second row lands at twice the first screen position. The third row keeps the same scale visible.

mλLdy12 m6 m3 m4 m22 m6 m3 m8 m32 m6 m3 m12 m\begin{array}{c|c|c|c|c}m&\lambda&L&d&y\\1&2\ \text{m}&6\ \text{m}&3\ \text{m}&4\ \text{m}\\2&2\ \text{m}&6\ \text{m}&3\ \text{m}&8\ \text{m}\\3&2\ \text{m}&6\ \text{m}&3\ \text{m}&12\ \text{m}\\\end{array}

Doubling the order doubles the position

The second-order source has path difference 4 m, so the screen position doubles with the same slit and screen distance.

y=2λLd=8 m;Δ=4 my=2\frac{\lambda L}{d}=8\ \text{m};\quad \Delta=4\ \text{m}
Young second-order ledgerThe second-order fringe cites the matching path source.path Apath Bfringe ypathSource=boundwavelength=2 mslitSeparation=3 mscreenDistance=6 morder=2 countfringePosition=8 m