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Sonoluminescence

Apparatus

Julio and apparatus

photo: Julio da Graca is making adjustments to the SBSL apparatus.  The cylindrical water-filled resonator is visible.

Our ultimate objective is to understand the light emission mechanisms of SBSL(single bubble sonoluminescence).  The presence of a noble gas in the trapped bubble is known to be important for strong emission of light. The question we are addressing currently is what happens if two noble gases are present in the bubble. In the presence of large temperature and pressure gradients, the two noble gases are expected to segregate according to the mass differences.  As we vary the mixing ratio and noble gas species(He, Ne, Ar, and Xe) in the bubble, we are measuring:

  • Emitted light intensity
  • Range of acoustic pressure which can produce SBSL
  • Time dependence of the bubble's radius R(t) as measured by Mie scattering
  • Dependence of all of the above on the water temperature
  • spectrum of emitted light

 

A schematic set up of our SBSL apparatus

The cylindrical cavity is made up by a quartz tube (75 mm inner diameter and 80 mm long) and two brass end plates.  A pair of piezoelectric transducers (PZT) are epoxied onto the end plates.  The PZTs excite a resonance in the cylindrical resonator at 17.3 kHz.  A mixture of noble gases has been dissolved into the water.  A gas bubble is created by passing a pulse of current into the heater wire.  The bubble can be levitated at the anti-node of the resonance if the acoustic amplitude is sufficiently high.  When the acoustic amplitude is increased further beyond certain threshold, light emission can be seen with naked eyes.  When the acoustic amplitude exceeds a second threshold, the bubble becomes unstable, breaks up and dissolves back into water.  The photodiode is used to monitor the light emission intesity.

 

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