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The Evolution of Diamond Cutting
Wendi Clouse
Midterm
Math G
Due 03/18/02
Shrouded
in mystery, intrigue and controversy, the diamond may be one of the most
mysterious substances on earth. It
is believed that the first diamond was discovered as early as 500 B.C., but
geologists believe that the formation of diamonds occurred in the Earthís
mantle at least one hundred million years ago. The diamond as a gem didnít make an appearance in jewelry
until1074 A. D., and at that time it was used only in the natural crystalline
form. It wasnít until 1916 that a
systematic mathematical approach to diamond cutting was developed. The man who revolutionized the industry
is Marcel Tolkowsky and he single-handedly changed the world of diamonds
forever.
The natural crystalline form of a
diamond is cubic; manifesting itself in a shape called an octahedron,
which looks like two four sided pyramids stacked on
top of one another, base to base.
The cubic form has four distinct cleavage planes, each in a different
direction. The cleavage plane is a
weakness in the crystalline form where the crystal will break. Although a diamond is one of the
hardest substances on earth (10 on the MOHS scale) a small amount of pressure
at the proper point can separate a diamond crystal. Octahedron photo
provided by http://www.drostes.com/pavilion_depth.html
The
practice of cutting diamonds is a relatively new art form, only done within the
last century. Up until the
fifteenth century it was common practice to ìcleaveî a diamond by applying a
chisel to one of the four perfect cubic planes in the crystalline structure,
then striking it with a mallet.
Unfortunately this sometimes resulted in the destruction of the gem due
to miscalculation of the cleavage plane.
If the angle of the chisel was wrong, the pressure from the mallet
shattered the crystal. After
cleaving was complete the diamond was then placed into an egg shaped tin cup
and the edges were hit with another diamond until the desired shape was
achieved. The shaping process was
limited to the natural shape of the diamond crystal and was at best very
rudimentary, producing clumsy looking diamonds with very little sparkle.
At
the end of the fifteenth century, a diamond cutter in Antwerp named Lodewyk van
Berken invented a machine called a scaif.
The scaif was a manually operated polishing wheel, made of a large
bronze disc imbedded with diamond dust.
Using olive oil as a lubricant, the wheel was capable of grinding away
flat symmetrical shapes called facets on the cleaved diamond crystal. The scaif made the cutting process so
precise that the tradesman could now concentrate on the optics of the gem,
producing stones that were livelier.
Van Berkenís invention lured cutters from around Europe to Antwerp to
study this new method, and the products that they produced quickly became
popular with the aristocracy of Europe.
Although
the popularity and demand for diamonds increased as cutting methods became more
precise, there were no new innovations to the cutting world until the twentieth
century when the diamond saw was invented. The diamond saw was a circular steel blade continually
lubricated with diamond dust and oil, it was capable of cutting against the
natural grain of the crystal without causing damage. Although it took a longer period of time to saw through a
diamond, it was now possible to recut diamonds that had been damaged, and cut
rough stones that were irregular in shape. Sawing was more expensive than cleaving due to the time
constraints and the amount of diamond dust that it took to operate ìIt required
about 1/10th of a carat of diamond dust for every carat of diamond
sawed through. And it was also a
much slower process than cleaving a diamond with a single stroke. Indeed it took days to saw through a
two-carat diamond. Despite such disadvantages, the diamond saw became the
favored method of shaping diamondsÖ Since it was far easier to train workers to
saw rather than cleave diamonds, it quickly transformed diamond cutting Antwerp
from an esoteric craft to a semi-mechanized industryî[footnote 1]
Then
came the largest change yet in the cutting world. Marcel Tolkowsky was born in 1899. His family had an established name in the diamond cutting
and dealing industry. Educated
first, at the German School in Antwerp, he studied at the Lycee FranÁois, and
then later would receive a D. Sc in engineering from the University of London. In 1919 he published a book called Diamond
Design. The book, only 104
pages in length had a profound affect on the diamond industry. At the age of 21, Marcel had managed to
calculate a formula to maximize refracted light, with the least amount of
sacrifice of reflected light, in other words he had calculated the parameters
of cut proportion that would give a half and half ratio between brilliance and
dispersion. Tolkowsky had in
theory invented the modern round brilliant cut diamond, and his guidelines for
proportion would become the defining factor in what the world would label ìa perfect
cutî. Tolkowsky was not the first
cutter to use this idea to improve the product, but he was the only one at the
time that could provide the ìmathematical proofî for his work. For what others were attempting to do
in practice, Tolkowsky had managed to prove on paper.
In
order to understand Tolkowskyís formula, we must first be familiar with the
optical properties that affect a diamonds appearance. The Gemological Institute of America defines optical
properties as: characteristics of a gemstone that govern its interaction with
light. The most popular terms for these properties in relation to the diamond
are dispersion, brilliance, and scintillation.
Dispersion
is simply the metamorphoses of white light, as it breaks into the spectral hues
of color visible to the human eye.
Dispersion is achieved through a process called refraction. Because a diamond is very dense
atomically, it slows the velocity of traveling light. Andrew Cockburn in his recent National Geographic article, Diamonds The Real Story relates ìthey
(diamonds) are so dense that they slow the speed of light by two-thirdsî. This characteristic is the key in
understanding the basis for Tolkowskyís research. Refraction is what happens when light passes from one object
to another; the light will suddenly slow as it enters the second object, the
change in velocity causes the light to travel at a different angle thus
bending. The angle of the bend
depends on the angle of the light beam as it enters the denser object (angle of
incidence).
http://micro.magnet.fsu.edu/optics/timeline/people/snell.html
ìIn 1621 a mathematician named Willebrord Snell discovered a ratio between the
angle of incidence and the angle of refraction. Snellís law [footnote 2] shows that every object has a
bending ratio; this is called the index of refractionî. The RI for diamond is 2.417, which is
extremely high for a transparent substance. Light entering a diamond bends, the beam of light is then
separated, because light waves travel at different speeds. Separation in the white beam causes
minute flashes of color to travel back to the eye in the form of prismatic
flashes of color. The eye
perceives color because white light is a combination of all light wavelengths,
when the wavelengths separate as the light slows; the eye is able to see the
full range of spectral color from violet to red. The diamond is considered the most dispersive gems in
nature. Diagram to the
right is an example spectral separation at the exit from the stone. Provided by the GIA website
Brilliance
is the combination of white light reflecting from both the surface and the
interior of the diamond.
Brilliance is defined as the brightness that lightens the stone. This optical characteristic is the
result of reflection, or the action of white light bouncing off of the surface
of a diamond and traveling back to the eye intact (no color separation
occurring) [Footnote 3].
Brilliance also occurs in the interior of the diamond as light travels
in straight lines instead of bent lines, as it bounces off of the internal
facet pattern and returns to the eye as white light. Before Tolkowsky developed his formula it was thought that a
diamond had to be cut to show either dispersion (refracted light) or brilliance
(reflected light). Tolkowsky was the
first to realize that you could have an equal balance of both if you controlled
the proportions of the diamondís anatomy.
Scintillation
is the ìsparkleî of the diamond, or the tiny flashes of light viewed when the
diamond, observer or light source moves.
Scintillation is the result of small flashes of light that the diamond
collects and then distributes from the different light and dark values in the
environment. This optical property
is a source of great beauty in a diamond, but does not play a big role in
Tolkowskyís formula. This diagram is from the website- http://www.accurateappraisal.com/estimati.htm is a dissected anatomy of a modern
round brilliant. The diagram will help define the measurements discussed in
Tolkowskyís proportional guidelines.

The table is the flat surface
across the top of the diamond. The
crown is the set of facets that join the table to the girdle; the girdle is the
thin set of facets or continual facet that encircles the diameter of the
stone. The pavilion refers to the
facet pattern that originates from the lower edge of the girdle and terminates
at the point on the bottom. If the
point of pavilion termination is faceted, the facet is called the culet, if the
pavilion comes to a perfect point it is determined that the diamond has no
culet.
Tolkowsky determined that
the proportions for a ìwell madeî diamond would fall into a specific
range. If a diamond were cut
according to his parameters, light would both refract and reflect back to the
eye. At the time of his research,
he looked only at the
behavior of refracted light as it exited the
diamond. He did not take internal
dispersion into consideration.
Some experts in the gemological field consider his dismissal of internal
dispersion to be an error, but the finished product speaks for itself. Even today there are few diamonds that
can compare to those cut within the Tolkowsky proportions. Tolkowskyís theoretical model outlines
that a round brilliant should have 58 facets that are symmetrical, 53% table;
60-61% total depth that includes the girdle thickness of 0.7 to 1.7%; 16.2%
crown height; 43.1% pavilion depth, crown angle of 34 degrees 30 minutes and
the pavilion angle of 40degrees and 40 minutes. Four
diagrams of: Tolkowskyís Ideal, proper light behavior, shallow cut and deep cut
provided by: http://www.jewelry1.com/diamond/Diamcut.htm
The following formula is taken
directly from http://www.folds.net/diamond_design/index.html#brilliance_and_fire It is a simplified version taken
from Tolkowskyís book Diamond Design. His formula, in this simplified form is the best
mathematical explanation of light behavior in the modern round brilliant. Although I have a thorough
understanding of the cause and affect of different variables that affect a
diamondís dispersion and brilliance, I do not have the mathematical experience
to define this formula on my own:
Start.
We choose alpha.
We start with a guess for beta (say, 35ƒ).
Step 1. We look at the girdle:
DE = diameter of a
knife-edge diamond. (1 mm is easiest.)
Step 2. We find out what fraction of the oblique rays are effective, and their
average angle:
CriticalAngle
= arcsin(1 / 2.417) = 24ƒ 26'
23"
EffectiveAngle
= arcsin(sin (alpha - 24ƒ 26' 23") * 2.417)
EffectiveFraction
= [1/3 - sin(EffectiveAngle)] * 3 / (-2)
SPT = AverageRefractedAngle
= arcsin(( (1/3) + sin(EffectiveAngle) ) / 2 / 2.417)
Step 3. We calculate angles of rays:
QPT = alpha - 24ƒ 26' 23"
QRP =
90ƒ - 2 * alpha + QPT
Q2ED
= 90ƒ - 2 * alpha
+ AverageRefractedAngle
Step 4. We calculate angles of typical rays before they leave the crown.
The FirstAngle is the angle between R'S' and the vertical.
The SecondAngle is the angle between Q1R1 and
the vertical.
FirstAngle
= 180ƒ - 4 * alpha
SecondAngle
= 2 * alpha
- AverageRefractedAngle
Step 5. We calculate some ratios that make the calculations easier.
f = 1 +
(1 / tan QPT / tan alpha)
g = (1 /
tan QPT - tan QRP) / 2 / tan QRP
Step 6. The loop starts here.
We calculate the table ratio of a knife-edge diamond:
h = 1 +
tan beta / tan alpha
t = g *
h / (f + g * h)
Step 7. We calculate distances at the top of the diamond:
PM = (DE / 2) * t
AP = PM
* f / g
Step 8. We calculate distances along the pavilion edge:
TC = PM
/ cos alpha
SC = TC
+ AP * (tan SPT) / (tan SPT + 1 / tan alpha) / cos alpha
Q2C
= (DE / 2) / cos alpha * (tan alpha -
tan Q2ED) / (tan alpha + tan Q2ED)
Step 9. We calculate a new guess for beta (the crown angle).
FirstWeight
= (TC * TC)
SecondWeight
= EffectiveFraction
* (SC * SC - Q2C * Q2C)
beta = (FirstWeight * FirstAngle + SecondWeight * SecondAngle) / (FirstWeight + SecondWeight)
This gives us a new guess for beta.
The loop ends here. We can repeat steps 6-9 until the guess for beta
stops changing.
Step 10. Because Tolkowsky uses a knife-edge girdle, we do NOT need to adjust
the diameter and table ratio.
Step 11. Tolkowsky says that:
Modern diamonds have longer lower girdle facets, so
these angles are slightly different.
Step 12. The diamond total depth contains the crown
and the pavilion. Because it has a knife-edge girdle, there is no girdle
thickness:
CrownHeight = diameter / 2 * (1 - t) * tan beta
PavilionDepth = diameter / 2 * tan alpha
-(CuletHeight)
=-((culet / 2) *
cos(22ƒ 30') * tan alpha)
TotalDepth = CrownHeight + PavilionDepth - CuletHeight
Shallow Cut:
If the
diameter becomes to large for the depth of the stone, both reflected light and
refracted light will exit the diamond via the pavilion, returning a very small
amount of light to the eye. When
this happens the affect is called a fish eye, and the value of the diamond is
decreased because its ìcorrected carat weightî[Footnote 5] is much smaller that
the actual carat weight purchased. Photos of
fisheye (right) and deep cut below are provided by www.pricescope.com
Deep Cut:
When the
diameter of the stone is too small for its total depth, light is thrown out of
the pavilion at odd angles instead of being reflected back to the eye. A deep cut is a very poor value because
the diameter of the stone is smaller than the cut should carry; therefore the
total weight of the diamond is heavier than its appearance. Because diamonds are priced according
to weight, jewelers can make a greater amount of profit selling stones that
have a deep cut. They buy the
poorly cut stones at discounted rates, and then sell them, because of the
higher carat weight at the same price as a diamond that is cut to proper
proportions. Take for example two
diamonds that weigh 1 carat each, and are the same color and clarity- one is
cut to proper proportions and one is cut deep. The one that is cut well will measure approximately 6.5 mm
in diameter, however the diamond that is cut poorly will only measure 5.75mm in
diameter. Three quarters of a
millimeter may not seem like much difference, but the diamond that measures
smaller will look the same as a .75-carat stone. If you had purchased a .75 ct instead of 1 carat you could
have saved as much a $4,000.00 in todayís market. Not to mention that the .75ct that is cut well will be more
beautiful than the one carat with poor proportions. Compare the behavior of light in the following diagrams:


The diagrams above is how
light should behave in a diamond cut properly. Photo above
provided by GIA

The
diagram above is an example of a shallow cut.
This
diagram is an example of a deep cut.
When examining the
different examples of cut proportion, you can easily visualize why diamonds cut
close to Tolkowskyís proportions manage to return a large amount of light to
the eye, but it should also raise a question. If Tolkowskyís proportions are best for light return, why
arenít all diamonds cut in this fashion?
In order to answer this question we need to consider several
factors: the diamond industry is
profit driven, diamonds are a commodity priced according to weight and rarity,
the industry itself can not agree on terminology for categorizing cut, most
jewelry purchases are based on emotion instead of logic, and most sales people
do not take the time to educate the consumer properly on this grading aspect.
The diamond industry
(cutters, designers, manufacturers) buys diamonds by the carat [Footnote 4] and
sells by the carat. If a cutter
buys 100 carats of rough crystal, but only yields 40 carats of finished goods
his profit is much lower than if he yields 60 carats of finished goods. Due to the natural shape of the diamond
crystal (octahedron) it is more profitable for a cutter to produce a diamond
with a deep cut because they realize higher yield from their initial
investment.
Retail establishments want a high profit margin;
therefore they purchase diamonds at the lowest cost they can find. Often their inventory is purchased
sight unseen, with cost being the driving factor. Low employment cost usually accompanies a higher profit margin
so employee-training courses are substandard; most employees are trained only
marginally about proportion and given none of the mathematics involved. The diamond industry itself cannot
agree on a specific grading policy for cut. The industry relies on profit, and if profit decreases
because the end customer demands a better product, the company coffers
diminish. The consumer has very
few educational tools available, and in all honesty most consumers make their
diamond purchases on a whim.
Jewelry purchases are luxury items, purely emotional, very few people
who are purchasing that tenth anniversary gift want to explore ìmathematicsî
when they are shopping. Weight diagram provided by http://www.drostes.com/pavilion_depth.html
In conclusion there are
many factors that can change both the value and esthetics of a diamond. Tolkowskyís formula is one way to
define beauty in mathematical language.
However, as with art many people interpret beauty in different
ways. A mathematical proof may
provide us with the understanding of the scientific behavior, but it does not
provide the only definition of beauty.
Ultimately beauty is in the eye of the beholder.
Footnote 1-The Rise and
Fall of Diamonds the Shattering of a Brilliant Illusion
Edward Jay Epstein, Simon and
Schuster, copyright 1982 by EJE Publications LTD.
Page 105, paragraph 1.
Footnote 2- the formula for
the law of refraction is as follows:
The ratio of the sine of the
angle of incidence i to the sine of the angle of refraction r is equal to the ratio of the speed of light
in the original medium,V; to the speed
of light in the medium, Vr. Or sin i/sin r = Vi/Vr. Snellís law is often related in refractive indexes instead
of the speed of light in the two mediums.
Footnote
3- Reflection according to the GIA Diamond Dictionary is the bouncing back of
light when it strikes a polished surface.
Approximately 17 percent of the light striking the external surface of a
polished diamond vertically is reflected back into the air; the greater part
enters the stone. Light striking an internal surface of a polished diamond at
an angle greater than the critical angle (24 degrees 26 minutes) is reflected
back into the diamond (total internal reflection).
Footnote
4- Carat is a weight measurement equaling 200 milligrams. The carat is broken into 100 units of
measure called points, thus a 50 pointer equals ‡ carat.
Footnote
5- Corrected carat weight is the weight a diamond would have been if cut to
correct proportions.
Bibliography
The Rise and Fall of
Diamonds the Shattering of a Brilliant Illusion
Edward Jay Epstein, Simon and
Schuster, copyright 1982 by EJE Publications LTD.
National Geographic
Periodical, March 2002, Diamonds The Real Story, written by Andrew
Cockburn. Page 2-35
A.N. Wilson. Copyright 1982 by The Gemological
Institute of America
GIA Diamond Dictionary, 3rd Edition, copyright 1988
Gemological Institute of America
http://mineral.galleries.com/minerals/elements/diamond/diamond.htm
http://www.factmonster.com/ce6/sci/A0860657.html
http://www.factmonster.com/ce6/sci/A0846218.html
http://www.gia.org/giaresearch/diamond-cut5.cfm
http://www-groups.dcs.st-and.ac.uk/~history/Mathematicians/Snell.html
http://micro.magnet.fsu.edu/optics/timeline/people/snell.html
http://guest:guest@www.giaonline.gia.edu/public/cgi/as_web.exe?dia_dic.ask+D+419851
http://guest:guest@www.giaonline.gia.edu/public/cgi/as_web.exe?dia_dic.ask+D+511488
http://www.jewelry1.com/diamond/Diamcut.htm
http://www.folds.net/diamond_design/index.html#brilliance_and_fire
http://www.pricescope.com/tutor_fisheye.asp
http://www.agsdiamonds.com/AGSDiamondsHomePage.html
http://mineral.galleries.com/minerals/elements/diamond/diamond.htm
http://www.jewelry1.com/diamond/Diamcut.htm
http://www.amnh.org/exhibitions/diamonds/refraction.html
http://www.accurateappraisal.com/gabi_tolkowsky.htm
http://www.gia.org/giaresearch/diamond-cut8.cfm
http://micro.magnet.fsu.edu/optics/timeline/people/snell.html
http://www.cutstudy.com/cut/english/model_1.htm
http://www.pricescope.com/tutor_brill.asp
http://www.drostes.com/pavilion_depth.html
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