| 0309 Effect of air/water coolant on Nd:YAG laser fiber surface temperature | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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D. GEKELMAN1, A. YAMAMOTO1, M.G. OTO1, C. LARES2, and J.M. WHITE1, 1University of California San Francisco, USA, 2Lares Research, Chico, CA, USA Objective: the purpose of this investigation was to measure, in vitro, the maximum temperature at the Nd:YAG laser fiber optic tip, with and without air/water coolant. Methods: a pulsed free running Nd:YAG laser, emission wavelength 1064nm, pulse duration 110 m s, was used varying parameters of power (W) and repetition rate (Hz) and energy per pulse (mJ/pulse) for 30s, with a 300m m diameter fiber, under 4 settings of air/water coolant at 15 psi: none (NN); minimum (MN) (4ml/min); medium (MU) (8ml/min); and maximum (MX) (12ml/min). The maximum temperature at the fiber tip was measured, 4 repetitions each (n=144), using an infra-red camera, with a speed of 1 scan every 45 ms. A two-factor ANOVA was used for statistical analysis (p≤0.05). Results: the effect of laser parameters on surface temperature is shown in the following table: Means table for Maximum Temperature (OC) ±1SD
The effect of coolant on surface temperature was NN>MN=MU=MX. Conclusions: laser parameters affect the fiberoptic surface temperature, which is directly related to energy per pulse. The addition of an air/water coolant significantly lowered surface temperature on the fiberoptic tip for all laser parameters tested. Supported by Lares Research. | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| Seq #47 - Clinical Techniques in Fixed and Implant Prosthodontics 11:00 AM-12:15 PM, Thursday, 7 March 2002 San Diego Convention Center Exhibit Hall C | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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