The Speed of Light - The University of Utahbelz/phys3719/presentations/ramirez.pdf · determine the...
Transcript of The Speed of Light - The University of Utahbelz/phys3719/presentations/ramirez.pdf · determine the...
The Speed of Light
Foucault Method
Daniel Ramirez April 11 2011
We have used the Foucault Method to measure the speed of light. Our best value calculated from the collected data is
The accepted value of the speed of light as defined by the 2006 CODATA recommended value is
The error in our value places our calculated result within two standard deviations of the accepted value.
Abstract
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c = (3.05 ± 0.3)x108 ms
History I
• Light traveled from eyes to object then back to eyes
• If stars appeared when eyes were opened, then the speed of light must be infinite.
The ancient Greek, Heron of Alexandria argued:
History II
• The idea of an infinite speed of light lasted for centuries
• 1729 - James Bradley used starlight aberration to get the first accepted measurement of c
Starlight Aberration
Due to the velocity of the earth, light appears to arrive at an angle.
The Foucault Method
• 1862 - Foucault’s method for measuring the speed of light directed a beam of light at a rotating mirror.
Experimental Setup
Experimental Method
• Optical alignment is the true challenge of the experiment
• Data collection is straightforward. Increase the speed of the rotating mirror to
~1500 rpm cw and record the displacement of S with the micrometer. Repeat the measurement using
~1500 rpm ccw.
Data
c Calculated for 10 runs
Discussion
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c = (3.05 ± 0.03)x108 ms
Our calculated value of c for 10 runs was
With 2% relative uncertainty
This places our value within two standard deviations of the accepted value.
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c2006CODATA = 2.99792458x108 ms
Conclusion • We have tested the Foucault method for reliability in measuring the speed of
light.
• Our result of
successfully demonstrates that this method is an adequate means to determine the speed of light.
• For this particular experiment, the accuracy and precision could be refined by increasing the length, D, as well as by increasing the speed, ω, of the rotating mirror. – High quality laser, optically processed to reduced aberrations – D= 1 km – ω=20,000 rpm
-with these parameters a of ~2cm is possible
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c = (3.05 ± 0.03)x108 ms
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ΔS