iGCSE Physics (0625) 3.2.4 Dispersion of light Paper 4 -Exam Style Questions- New Syllabus
Question

(ii) On Fig. 5.1, carefully draw the refracted light ray in the soap film and label the angle of refraction.
(i) Define monochromatic.
(ii) Calculate the frequency of the light.
Most-appropriate topic codes (Cambridge IGCSE Physics 0625):
• Topic $3.2.2$ — Refraction of light (Parts $\mathrm{(a)}$, $\mathrm{(b)}$)
• Topic $3.2.4$ — Dispersion of light (Part $\mathrm{(c)(i)}$)
• Topic $3.1$ — General properties of waves (Part $\mathrm{(c)(ii)}$)
• Topic $3.3$ — Electromagnetic spectrum (Part $\mathrm{(c)(ii)}$)
▶️ Answer/Explanation
Part (a)
Correct Answer: The ratio of the speed of light in air (or vacuum) to the speed of light in the soap film.
The refractive index ($n$) is a dimensionless measure that describes how fast light travels through a material. It is formally defined as the ratio of the speed of light in a vacuum (approximated as the speed of light in air) to the speed of light in the specified medium: $n = \frac{c}{v}$.
Part (b)(i)
Correct Answer: $i = 60^{\circ}$, $1.28 = \frac{\sin 60^{\circ}}{\sin r}$, $r = 42.6^{\circ} \approx 43^{\circ}$
First, find the angle of incidence ($i$), which is measured from the normal. Since the ray makes a $30^{\circ}$ angle with the boundary, $i = 90^{\circ} – 30^{\circ} = 60^{\circ}$. Applying Snell’s Law, $n = \frac{\sin i}{\sin r}$, we rearrange to find $\sin r = \frac{\sin 60^{\circ}}{1.28}$. Calculating this gives $r \approx 42.6^{\circ}$, which rounds to $43^{\circ}$.
Part (b)(ii)
Correct Answer: A normal drawn at the incidence point; a refracted ray drawn bending towards the normal with the angle $r$ labeled.
Draw a dashed normal line perpendicular to the surface. The refracted ray should be drawn inside the film, bending toward the normal (since $r < i$).
Part (c)(i)
Correct Answer: Light of a single frequency.
Monochromatic light consists of waves with a single frequency (or wavelength), resulting in a single pure color.
Part (c)(ii)
Correct Answer: $4.4 \times 10^{14}\text{ Hz}$
Using $v = f\lambda$, where $v = 3.0 \times 10^8\text{ m/s}$ and $\lambda = 680 \times 10^{-9}\text{ m}$. Rearranging for frequency: $f = \frac{v}{\lambda} = \frac{3.0 \times 10^8}{680 \times 10^{-9}} \approx 4.4 \times 10^{14}\text{ Hz}$.
