Total Internal Reflection of quartz

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To determine the maximum refractive index (n) of the surrounding fluid for total internal reflection at point Po in a quartz slab, Snell's law must be applied twice due to the light ray crossing the interface twice. The first application helps find the angle of refraction (θ2) when the light enters the quartz, using the known incident angle (θ1 = 34°) and the refractive index of quartz (n2 = 1.544). The second application of Snell's law at the exiting surface relates θ2 to the critical angle, allowing for the derivation of a condition that must be met for total internal reflection to occur. The critical angle can be expressed using the formula θc = sin⁻¹(n2/n1), where n1 is the refractive index of the fluid. This process ultimately leads to an algebraic expression that defines the maximum value of n for total internal reflection.
runfast220
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Homework Statement


The drawing shows a crystalline quartz slab with a rectangular cross-section. A ray
of light strikes the slab at an incident angle of 1=34o, enters the quartz and travels to
point Po (Figure2). This slab is surrounded by a fluid with a refractive index n. What
is the maximum value of n such that total internal reflection occurs at point Po?

@1= 34deg n2= 1.544




Homework Equations



n1sin@1 = n2sin@2
@c = sin-1 (n2/n1)

The Attempt at a Solution


Well I know in order to find n1 I need to know the critical angle, but I don't know how to find the critical angle without n1. My only idea was to use Snell's law of refraction to find n1 by setting @1 at 90deg?
 

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Hi runfast220,

The ray of light crosses an interface twice: once on the way into the quartz, and once while exiting it (unless, of course, it is totally internally reflected!).

This means that you need to apply Snell's law twice: once for each crossing. The first crossing, on the way into the quartz, tells you what \theta_2 is. Granted, you can't solve for a numerical value for it just yet, but you can assume that the parameters you need (the refractive index of quartz, the refractive index of the fluid, n, and the incident angle \theta_1) are known, and can therefore include them algebraically (as symbols) in Snell's law. You will therefore end up with an algebraic expression for \theta_2 in terms of these three known quantities.

Now, because the light ray enters the quartz at this angle (\theta_2), the angle of incidence upon the second (exiting) surface will be closely related to \theta_2 (can you see how)? At that point, applying Snell's law for the exiting light ray, you can figure out what condition (on the known parameters) must be satisfied in order for this incident angle to be greater than or equal to the critical angle.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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