|Period:||Egypt, Graeco-Roman Period, Graeco-Roman Period|
|Dating:||50 BC10 AD|
|Origin:||Egypt, Lower Egypt, Alexandria|
|Material:||Glass (all types)|
|Physical:||8.3cm. (3.2 in.) - 25 g. (.9 oz.)|
Links to other views:
⇒ Larger View
if scripting is off, click the ⇒ instead.
Links to others from Graeco-Roman Period
Ribbed glass bowl, Alexandria, 50 BC-50 AD
Links to others of type Alabastron
Pottery alabastron, Asian Greece, 500-400 BC
Stone alabastron, 3150-2700 BC
Stone alabastron, Egypt, 3200-2800 BC
Now graced with lovely iridescence of metallic silver, green and turquoise, this elegant alabastron was originally deep aquamarine transparent glass. The body is pyriform, with a marked shoulder and a tapering neck capped by a narrow infolded rim. Two small symmetrical coil loop handles were affixed to the shoulder, providing attachment points for a strap. An imperfectly ground seam appears to run longitudinally along the sides and bottom, and another around the shoulder, suggesting a three-part molded piece. But the extensive weathering renders our inspection inconclusive as to the method of manufacture (molded, blown in a mold, or free-blown). We tentatively place its origin in Egypt, Alexandria, 50 BC-10 AD.|
The iridescent effect that so often enhances immeasurably the beauty of ancient glass was not planned by ancient glass artisans. Instead, it is the combined result of weathering processes and the properties of light. The rainbow effect you commonly experience in daily life, such as on soap bubbles or drops of oil spread on water, stem from the same action: light bouncing on a extremely thin transparent film.
When a glass bottle is new, there is no such thin film. The wall of the bottle is homogenous. But as glass is exposed to water in its burial environment, some of its [chemical] components can be dissolved by the water and carried away (leached out). This generates a thin surface layer of glass that has a different composition that the undegraded bulk of glass. Often, there is a think layer of air between the corroded surface and the bulk (Bezúr 1999).
When ordinary white light strikes the bottle, some of the rays bounce off the top surface of the thin film, and some go through the thin film and then bounce off the glass-air interface between the thin film and the underlying glass. When the rays coming back from the bottom of the thin film reemerge into open air, they combine with those that simply bounced off the surface. But since they have been delayed by their additional travel, their waves are no longer in phase (in synch). When these two streams of out-of-phase white light combine, some of the wavelengths cancel out (and therefore those colors disappear), and other wavelengths are reinforced (and therefore those colors become very intense), thus turning white light into vivid random colors.
Glass artists of the late 19th Century, such as Louis Comfort Tiffany, admired the iridescence of Roman glass, and devised ways to produce it deliberately by placing the glass piece while still very hot in an oven filled with vapors (tin and iron chlorides) that would alter the surface and create a thin film of different composition, yielding an iridescent effect that did not require a thousand years to develop.
A more thorough technical discussion of the phenomenon by Aniko Bezúr of the University of Arizona Department of Materials Science and Engineering is available from http://www.u.arizona.edu/ic/mse257/class_notes/iridescence.pdf
Bibliography (for this item)
Nicholson, Paul T.
1993 Egyptian Faience and Glass. Shire Publications, Buckinghamshire, United Kingdom. (67, 70)
Bibliography (on Glass Iridescence)
1999 Online Notes on Iridescence (http://www.u.arizona.edu/ic/mse257/class_notes/iridescence.pdf). University of Arizona, Department of Materials Science and Engineering, Tucson, AZ.