Light as a Wave — Question 7

Section 35-1 · Physics pages 5724–5725

Question 7 Huygens wavelets recover the refraction angle A plane wave crosses a plane boundary from index n1 = 1.00 into n2 = 1.50. During a common time interval ∆t, its wavefront advances distances v1∆t and v2∆t. With angles measured from the normal, the construction gives sin θ1 = v1∆t/AB and sin θ2 = v2∆t/AB. Let θ1 = 30◦. n1, v1 n2, v2 Schematic; labels, not drawing lengths, specify the data. (a) Eliminate the construction length AB and time interval to derive the refraction law. (b) Find the refracted angle and the wavelength ratio across the boundary.
Show solutionHide solution
Question 7 - Solution Huygens wavelets recover the refraction angle n1, v1 n2, v2 (a) Method and calculation sin θ1 sin θ2 = v1 v2 = n2 n1 . n1 sin θ1 = n2 sin θ2 . (b) Interpretation and further calculation θ2 = sin−1(1/3) = 19.471◦. f2 = f1, λ2/λ1 = v2/v1 = n1/n2 = 2/3 . Physical check The same time interval is essential: the wavefront construction compares simultaneous phase surfaces, while frequency remains continuous at a stationary boundary.

Question 7

Huygens wavelets recover the refraction angle

A plane wave crosses a plane boundary from index n1=1.00n_1=1.00 into n2=1.50n_2=1.50. During a common time interval Δt\Delta t, its wavefront advances distances v1Δtv_1\Delta t and v2Δtv_2\Delta t. With angles measured from the normal, the construction gives sin⁡θ1=v1Δt/AB\sin\theta_1=v_1\Delta t/AB and sin⁡θ2=v2Δt/AB\sin\theta_2=v_2\Delta t/AB. Let θ1=30∘\theta_1=30^\circ.

Diagram shown in the original SVG worksheet.

  1. Eliminate the construction length AB and time interval to derive the refraction law.

  2. Find the refracted angle and the wavelength ratio across the boundary.

Question 7 - Solution

Huygens wavelets recover the refraction angle

Diagram shown in the original SVG worksheet.

(a) Method and calculation

sin⁡θ1sin⁡θ2=v1v2=n2n1.\frac{\sin\theta_1}{\sin\theta_2}=\frac{v_1}{v_2}=\frac{n_2}{n_1}.n1sin⁡θ1=n2sin⁡θ2.\boxed{n_1\sin\theta_1=n_2\sin\theta_2}.

(b) Interpretation and further calculation

θ2=sin⁡−1(1/3)=19.471∘.\boxed{\theta_2=\sin^{-1}(1/3)=19.471^\circ}.f2=f1,λ2/λ1=v2/v1=n1/n2=2/3.f_2=f_1,\quad\boxed{\lambda_2/\lambda_1=v_2/v_1=n_1/n_2=2/3}.

Physical check

The same time interval is essential: the wavefront construction compares simultaneous phase surfaces, while frequency remains continuous at a stationary boundary.