The "Diamond Design" by Tolkowsky. A Study of the Reflection and Refraction of Light in Diamond

Back of the Brilliant

Let us now pass to the consideration of the other alternative, i.e. where the top surface is a horizontal plane AB and where the bottom surface AC is inclined at an angle (to the horizontal (fig. 1). As before, we have to introduce a third plane BC to have a symmetrical section.

First Reflection

Fig. 1

Let a vertical ray PQ strike AB. As the angle of incidence is zero, it passes into the stone without refraction and meets plane AC at R. Let RN be the normal at that point, then, for total reflection to occur, angle NRQ = 24°26'. But, angle NRQ = angle QAR - a as AQ and QR, AR and RN are perpendicular. Therefore, for total reflection of a vertical ray, a = 24°26'. Let us now incline the ray PQ so that it gradually changes from a vertical to a horizontal direction, and let P'Q' be such a ray. Upon passing into the diamond it is refracted, and strikes AC at an angle Q'R'N' where R'N' is the normal to AC. When P'Q' becomes horizontal, the angle of refraction T'Q'R' becomes equal to 24°26'. This is the extreme value attainable by that angle; also, for total reflection, angle Q'R'N' must not be less than 24°26'. If we draw R'V, vertical angle VR'Q' = R'Q'T' = 24°26', and angle VR'N' = VR'Q' + Q'R'N' =24°26' + 24°26' = 48°52' as before, a = angle VR'N', and therefore a = 48°52.

For absolute total reflection to occur at the first facet, the inclined facets must make an angle of not less that 48°52' with the horizontal.

Second Reflection

Fig. 2

When the tray of light is reflected from the first inclined facet AC (fig. 2), it strikes the opposite one BC. Here too the light must be totally reflected, for otherwise there would be a leakage of light through the back of gem stone. Let us consider, in the first instance, a ray of light vertically incident upon the stone. The path of the ray will be PQRST. If RN and SN' are the normals at R and S respectively, then for total reflection, angle N'SR = 24°26'. Let us find the value of a to fulfil that condition: angle QRN = angle QAR = a as having perpendicular sides. angle SRN = angle QRN as angles of incidence and reflection. Therefore angle NRS = a. Now let angle N'SR = c. Then, in triangle RSC,

angle SRC = 90° - a

angle RSC = 90° - c

angle RCS = 2 x angle RCM = 2 x ARQ = 2 (90° - a).

The sum of these three angles equals two right angles,

90° - a + 90° - c + 180° - 2a = 180°, or

3a+ c = 180° 3a = 180° - c.

Fig. 3

Now, c is not less than 24°26', therefore a is not greater than a = (180 - 24°26')/3 = 51°51'. Let us again incline PQ from the vertical until it becomes horizontal, but in this case in the other direction, to obtain the inferior limit. Then (fig.3) the path will be PQRS. Let QT, RN, SN' be the normals at Q, R, and S respectively. At the extreme case, TQR will be 24°26'. Draw RV vertical at R.

Then

angle QRV = angle TQR = 24°26' angle VRN = a.

As before, in triangle RSC,

angle SRC = 90° - NRS = 90° - a - 24°26'

angle RCS = 2 a (90° - a)

angle RSC = 90° - c.

Then

90 - a - 24°26' + 180° - 2a + 90° - c = 180°

3a + x = 180° - 24°26' = 155°34'

3a = 155°34' - c.

In the case now considered,

c = 24°26'.

Then

3a = 155°34' - 24°26' = 131° 8'

a = 43°43' (10)

For absolute total reflection at the second facet, the inclined facets must make an angle of not more than 43°43' with the horizontal.

We will note here that this condition and the one arrived at on "First Reflection" are in opposition. We will discuss this later, and will pass now to considerations of refraction.


Author: Marcel TOLKOWSKY.
This material is a part of "Diamond Design" book,
was published E & F.N. Spon, Ltd., London, 1919.