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EXPERIMENTAL PROCEDURE

Hook up the light bulb in a circuit with an ammeter and voltmeter, as shown below. The bulb used (a type 44) is rated as 6.3 V at .25 A. It has a coiled filament and is gas filled. The gas filling increases the life of the bulb, but introduces a complication in the analysis.

Measure the current in the lamp and the voltage across it for voltages up to about 6 V. Don't exceed 6.3 V. Make several measurements in the range between zero and 0.1 V in order determine the room-temperature resistance.

From your data calculate the resistance of the filament from Ohm's Law. Plot the low-current resistance versus current (it should be a straight line) and extrapolate the data points to zero current. The resistance at zero current will be the room temperature value . Once is determined, use Eqn. (2) to calculate the temperature of the filament for each resistance value. From the current and voltage also calculate the power delivered to the filament at each point.

From Eqn. (1) for Stefan's Law, taking the natural logarithm of both sides gives

A plot of versus will yield a straight line with a slope of 4 and an intercept at . From your data make such a plot and you will probably notice that the lower end of the plot is not a straight line. This is because the gas in the bulb cools the filament by convection and so radiation is not the only mechanism for heat loss. However, at higher power, radiation overwhelms the convection cooling and the log plot should be quite linear. From the high temperature data determine the slope of your line and compare it to the value predicted by Stefan's Law.

If a value for the emissivity is between 1/3 and 1/2, can you estimate the surface area of the filament?



next up previous contents
Next: Electron Diffraction Up: Stefan's Law Previous: Stefan's Law



Nick Tufillaro
Mon Jul 31 18:04:31 PDT 1995