Bouncing Light Beam
refraction - gradient of index (GRIN) of refraction - periodic defocusing/focusing
What it shows:
As a simulation of atmospheric refraction, this demonstration shows the gradual
and continuous bending of light due to a gradient in the optical density of the
medium. In this case the variable refracting medium is a tank of sugar water
with a vertical gradient in the concentration of sugar and a HeNe laser provides
the light beam. It can be used as a model of mirage formation (except that the
direction of increasing refractive index is in the opposite direction) or even
as a representation of the refraction of seismic waves through the Earth's mantle.
Total internal reflection, total internal refraction, as well as periodic beam
defocusing and refocusing are also shown.
How it works:
A long, narrow, plastic tank
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is filled two-thirds full of warm water adulterated with a light-scattering
substance. Sugar cubes are added to the tank and allowed to dissolve
undisturbed. This establishes a strong gradient in the index of refraction
ranging from n=1.50 (84% sugar at the bottom of the tank) to n=1.33 (pure water,
a few centimeters off the bottom). A laser beam, directed horizontally down the
length of the tank, will be refracted downward in an arc and "bounce" by total
internal reflection at the plastic-air interface at the outside surface of the
bottom of the tank. Following the bounce, the beam will arc upward and back down
by "total internal refraction" and so on. Depending on the gradient that has been
established and the angle and height at which the beam enters the tank, the beam
may bounce anywhere from once to several times in the length of the tank.
A closer observation reveals another interesting effect: a defocusing (divergence)
of the beam as it arcs downward toward the higher refractive sugar water and a
refocusing as it arcs upward. This effect is only in the vertical direction
(direction of the gradient) and not in the horizontal, and is periodic with every
bounce. Thus this demo can also be used as a model of long-distance laser beam
transmission (periodic focusing and defocusing with gas lenses) and possibly as an
analogy to accelerator strong focusing.
Setting it up:
The tank of sugar water must be prepared at least 24 hrs before intended
use to allow enough time for all the sugar to completely dissolve. Fill the tank
to about two-thirds full of warm water and stir in a few drops of milk to make
the laser beam visible by scattering.
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A good rule-of-thumb is, if the water looks cloudy (milky) you've added way too
much milk and the beam will become attenuated (scattered out of the path) before
it reaches the end of the tank (that's bad). If you don't have a feel for what
looks too cloudy, look down the length of the tank...if you can't see the other
end of the tank, the laser beam won't make it that far either (for the same reason).
Having satisfied yourself on the proper concentration of milk, drop sugar cubes in
so that 50% of the bottom area of the tank is evenly covered with cubes.
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Of course they'll start dissolving immediately but it takes a long time to dissolve
completely and you don't want any undissolved sugar remaining on the bottom as this
will spoil the "bounce" of the beam.
Once the gradient has been established it will be quite stable and the tank can be
moved into the lecture hall, albeit very carefully so as not slosh out the
water. Best results are obtained 24 to 30 hrs after preparation, but the demo will
still work even after two to three days. However, expect fewer bounces with
increasing time as the sugar diffuses upwards and slowly degrades the gradient.
Also, the sugar water will begin to reek after a few days as the milk begins to spoil.
In an emergency (short time notice), you can use Karo™ light corn syrup or prepare
a concentrated sugar solution in a beaker of water
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and add it to the tank by gently pouring it down a stirring rod to minimize mixing
with the water. However, this results in too strong a gradient and it's best to
still wait a few hours for diffusion to take its course and "soften" the interface
between sugar solution and pure water.
Set the tank on the lecture bench supported by a block of wood on each end. Setting
directly on the lecture bench may result in frustrated total internal reflection,
especially if some spilled water allows for intimate optical contact between tank
and bench-top. As for which laser to use, the more power the better: 2 mW is fine
for a classroom but lecture halls require 10 mW and upward for good visibility. The
35 mW HeNe and the 125 mW Argon work brilliantly. The Argon laser is a bit unwieldy
and noisy, however and requires warmup/cooldown time.
Comments:
Originally conceived by William M. Strouse,
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we have modified it only in scale. If you happen to use corn syrup and the Argon
laser combination, you will be in for a surprise. It turns out that corn syrup
fluoresces yellow when excited by the blue/green laser light. As the Argon beam
arcs downward, it appears to turn yellow in color, bounces off the bottom and becomes
blue/green again as it arcs upward. And this happens with every bounce! This would
be an interesting puzzler to present to the class. Rating ***
1
It measures 36" × 5" × 1.5" (91.4cm × 12.7cm × 3.8cm). The side walls are made from
1/4" thick acrylic, the end walls from 3/8", and the bottom from 1/8". Size is, of
course, not important to the demonstration except that the thickness of the bottom
of the tank should be kept to a minimum; no more that 1/8". This is because one gets
a partial internal reflection off the inside surface as well as the total internal
reflection off the outside surface; if the distance between these reflections becomes
much larger than 1/8", the double reflection becomes noticeable and degrades the effect.
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Rather than milk, you can of course use other scattering substances. For example,
Edmund Scientific Co. sells a "Scatter Liquid Concentrate" (Cat. No. 38,938) which
is a concentrate of polystyrene spheres. Mix 5 drops per 2 liters of water. We
have also used DuPont "Ludox", which is a colloidal silica; mix 10 ml per 2 liters
of water.
3
The tank size and water volume is irrelevant. 50% coverage (as measured by eye) is
what counts...if you overdue it you'll find that the excess sugar won't dissolve.
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Use about 800 g of sugar to 500 ml of water. Continuously stir and heat to 40-50°C;
let cool before adding to tank.
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W. M. Strouse, Am J Phys 40, 913 (1972) "Bouncing Light Beam"
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