Respuesta :
Answer:
69.358°
Explanation:
[tex]\theta_2[/tex] = Angle at the interface = [tex]90-52=38^{\circ}[/tex]
[tex]\theta_1[/tex] = Required angle
[tex]n_1[/tex] = Refractive index of air = 1
[tex]n_2[/tex] = Refractive index of liquid = 1.52
From Snell's law we have
[tex]n_1sin\theta_1=n_2sin\theta_2\\\Rightarrow theta_1=sin^{-1}\dfrac{n_2sin\theta_2}{n_1}\\\Rightarrow \theta_1=sin^{-1}\dfrac{1.52\times sin38}{1}\\\Rightarrow \theta_1=69.358^{\circ}[/tex]
The angle from the normal that the refracted ray exit into the air is 69.358°
The refracted ray exits into the air at an angle of 58° from the normal which is explained below.
Snell's Law:
Given information:
Light is incident from the liquid, which is a denser medium, on the liquid-air interface, and will emerge out of the liquid to the air, which is a rarer medium.
the angle of incidence of light, i = 90° - 56° = 34°
the refractive index of liquid, n₁ = 1.52
the refractive index of air, n₂ = 1
let the angle of refraction of light be r.
According to Snell's Law:
[tex]\frac{sin(i)}{sin(r)}=\frac{n_2}{n_1} \\\\r=sin^{-1}[\frac{n_1}{n_2}sin(i)] \\\\r=sin^{-1}[1.52\times sin34]\\\\r=sin^{-1}[0.85][/tex]
r = 58°
Learn more about Snell's Law:
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