Interference from Thin Films — Question 4

Section 35-6 · Physics pages 5818–5819

Question 4 Oblique film interference depends on cosine of the internal angle A plane-parallel film has thickness t and index n. The external index is n0. Let i and r be incidence and internal angles, with n0 sin i = n sin r. For the two reflected rays compared on a common outgoing wavefront, use D = 2nt/ cos r −n0(2t tan r) sin i. n0 nf ns t i r Schematic; labels, not drawing lengths, specify the data. (a) Simplify D and explain why using only the internal round-trip length gives the wrong phase. (b) For a film in air with one relative reflection reversal, n = 1.50, i = 30◦, and λ0 = 600 nm, find the least thickness for constructive reflection.
Show solutionHide solution
Question 4 - Solution Oblique film interference depends on cosine of the internal angle n0 nf ns t i r (a) Method and calculation D = 2nt cos r −2nt tan r sin r = 2nt(1 −sin2 r) cos r . D = 2nt cos r ; the external wavefront correction is essential. (b) Interpretation and further calculation sin r = 1/3 =⇒cos r = 2 √ 2/3; 2nt cos r = λ0/2. t = λ0 4n cos r = 106.066 nm . Physical check The phase comparison must refer to the same outgoing wavefront. The increased internal geometric travel is partly offset by the external path difference.

Question 4

Oblique film interference depends on cosine of the internal angle

A plane-parallel film has thickness t and index n. The external index is n0n_0. Let i and r be incidence and internal angles, with n0sin⁡i=nsin⁡rn_0\sin i=n\sin r. For the two reflected rays compared on a common outgoing wavefront, use D=2nt/cos⁡r−n0(2ttan⁡r)sin⁡iD=2nt/\cos r-n_0(2t\tan r)\sin i.

Diagram shown in the original SVG worksheet.

  1. Simplify D and explain why using only the internal round-trip length gives the wrong phase.

  2. For a film in air with one relative reflection reversal, n=1.50n=1.50, i=30∘i=30^\circ, and λ0=600nm\lambda_0=600\,\mathrm{nm}, find the least thickness for constructive reflection.

Question 4 - Solution

Oblique film interference depends on cosine of the internal angle

Diagram shown in the original SVG worksheet.

(a) Method and calculation

D=2ntcos⁡r−2nttan⁡rsin⁡r=2nt(1−sin⁡2r)cos⁡r.D=\frac{2nt}{\cos r}-2nt\tan r\sin r=\frac{2nt(1-\sin^2r)}{\cos r}.D=2ntcos⁡r;the external wavefront correction is essential.\boxed{D=2nt\cos r};\quad\text{the external wavefront correction is essential}.

(b) Interpretation and further calculation

sin⁡r=1/3⇒cos⁡r=22/3;2ntcos⁡r=λ0/2.\sin r=1/3\Longrightarrow\cos r=2\sqrt2/3;\quad 2nt\cos r=\lambda_0/2.t=λ04ncos⁡r=106.066nm.\boxed{t=\frac{\lambda_0}{4n\cos r}=106.066\,\mathrm{nm}}.

Physical check

The phase comparison must refer to the same outgoing wavefront. The increased internal geometric travel is partly offset by the external path difference.