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For the scenarios in which total internal reflection is possible, rank the scenarios on the basis of the critical angle, the angle above which total internal reflection occurs. At this angle, the refracted ray is at 90 degrees from the normal. Rank from largest to smallest. To rank items as equivalent, overlap them.

ITEM A: n1benzene =1.50 n2water =1.33

ITEM B: n1diamond =2.42 n2water =1.33

ITEM C: n1diamond =2.42 n2air =1.00

ITEM D: n1water =1.33 n2air =1.00

Answer :

jacob193

Answer:

[tex]\rm A > D > B > C[/tex] (no overlap.)

Explanation:

Let

  • [tex]\theta_i[/tex] be the angle of incidence, and
  • [tex]\theta_r[/tex] be the angle of refraction.

Also:

  • Let [tex]n_i[/tex] be the index of refraction for the medium where the light comes from.  
  • Let [tex]n_r[/tex] be the index of refraction of the medium which the light enters after refraction.

Note that to achieve total internal reflection, [tex]\displaystyle \frac{n_r}{n_i} \le 1[/tex]. In other words, [tex]n_r \le n_i[/tex]. That's a hint for distinguishing between the two media.

By Snell's Law,

[tex]n_i\, \sin \theta_i = n_r\, \sin \theta_r[/tex].

Rearrange this equation to obtain:

[tex]\displaystyle \sin \theta_i = \frac{n_r\, \sin \theta_r}{n_i}[/tex].

At the smallest [tex]\theta_i[/tex] that ensures total internal reflection, [tex]\theta_r = 90^\circ[/tex].

Accordingly, [tex]\sin \theta_r = 1[/tex]. Hence, the equation from Snell's Law would become

[tex]\displaystyle \sin \theta_i = \frac{n_r\, \sin \theta_r}{n_i} = \frac{n_r}{n_i}[/tex].

The angle of incidence [tex]\theta_i[/tex] should be between [tex]0^\circ[/tex] and [tex]90^\circ[/tex]. On that range, [tex]\sin \theta_i[/tex] would be strictly increasing. To compare the

In this question,

  • Item A: [tex]\displaystyle \frac{n_r}{n_i} = \frac{1.33}{1.50} \approx 0.887[/tex].
  • Item B: [tex]\displaystyle \frac{n_r}{n_i} = \frac{1.33}{2.42} \approx 0.550[/tex].
  • Item C: [tex]\displaystyle \frac{n_r}{n_i} = \frac{1.00}{2.42} \approx 0.413[/tex].
  • Item D: [tex]\displaystyle \frac{n_r}{n_i} = \frac{1.00}{1.33} \approx 0.752[/tex].

Rank of [tex]\displaystyle \frac{n_r}{n_i}[/tex] from largest to smallest: [tex]\rm A > D > B > C[/tex].

[tex]\implies[/tex]Rank of [tex]\sin \theta_i[/tex] from largest to smallest [tex]\rm A > D > B > C[/tex].

[tex]\implies[/tex]Rank of [tex]\theta_i[/tex] from largest to smallest [tex]\rm A > D > B > C[/tex].

Answer:

(no overlap.)

Explanation:

Let

be the angle of incidence, and

be the angle of refraction.

Also:

Let  be the index of refraction for the medium where the light comes from.  

Let  be the index of refraction of the medium which the light enters after refraction.

Note that to achieve total internal reflection, . In other words, . That's a hint for distinguishing between the two media.

By Snell's Law,

.

Rearrange this equation to obtain:

.

At the smallest  that ensures total internal reflection, .

Accordingly, . Hence, the equation from Snell's Law would become

.

The angle of incidence  should be between  and . On that range,  would be strictly increasing. To compare the

In this question,

Item A: .

Item B: .

Item C: .

Item D: .

Rank of  from largest to smallest: .

Rank of  from largest to smallest .

Rank of  from largest to smallest .

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