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in (figure 1) shown a rectangular glass block that has a metal reflecto…

Question

in (figure 1) shown a rectangular glass block that has a metal reflector on one face and water on an adjoining face. a light beam strikes the reflector as shown. you gradually increase the angle \\( \theta \\) of the light beam. if \\( \theta \geq 51.2^{\circ} \\), no light enters the water. what is the speed of light in this glass?

part b
the target variable is the speed of light \\( v \\) in the glass, which you can determine from the index of refraction \\( n \\) of the glass. which equations will you use to find \\( n \\) and \\( v \\)? check all that apply.
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\\( \sin \theta_a = n_b \sin \theta_b \\)
\\( \sin \theta_{\text{crit}} = \frac{n_b}{n_a} \\)
\\( v = \frac{c}{n} \\)
\\( \lambda = \frac{\lambda_0}{n} \\)
\\( \theta_r = \theta_a \\)
\\( \tan \theta_p = \frac{n_b}{n_a} \\)
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Explanation:

Brief Explanations

To find \( n \) (refractive index of glass) and \( v \) (speed of light in glass), we analyze each equation:

  1. \(\boldsymbol{\sin\theta_a = n_b \sin\theta_b}\): This is Snell’s Law, relating angles of incidence (\(\theta_a\)) and refraction (\(\theta_b\)) to refractive indices (\(n_a, n_b\)) of two media. Applicable for refraction at the glass - water interface (or other interfaces here).
  2. \(\boldsymbol{\sin\theta_{\text{crit}} = \frac{n_b}{n_a}}\): This is the critical angle formula for total internal reflection, which may apply if total internal reflection occurs at the glass - water boundary (relevant to the problem’s context of light entering water).
  3. \(\boldsymbol{v=\frac{c}{n}}\): Relates the speed of light in a medium (\(v\)) to the speed of light in vacuum (\(c\)) and the refractive index (\(n\)) of the medium. Directly gives \( v \) once \( n \) is known.

The other equations are not relevant:

  • \(\lambda=\frac{\lambda_0}{n}\): Relates wavelength in medium to vacuum wavelength, not needed for \( n \) or \( v \) here.
  • \(\theta_r=\theta_a\): Describes reflection (angle of reflection = angle of incidence), not refraction or speed.
  • \(\tan\theta_p=\frac{n_b}{n_a}\): Relates to Brewster’s angle (polarization), not needed for \( n \) or \( v \) in this context.

Answer:

\(\sin\theta_a = n_b \sin\theta_b\), \(\sin\theta_{\text{crit}} = \frac{n_b}{n_a}\), \(v=\frac{c}{n}\)