Photoelectric Effect and Planck's Constant
Obj: Determine Planck's Constant Using Stopping Potentials
Materials:
two multimeters, several LEDs of known wavelength, variable power source,
several wires
Procedures
1. Record the wavelength of each LED
in Table 1. Determine
the positive and negative sides of the LED.
Arrange the power source, LED, ammeter, and voltmeter as shown in the
schematic diagram. Be sure the
power source is set at zero volts before energizing.
The ammeter should be set to read in the mA range and set to the
200μ amp setting (or 200 m).
2.
Slowly increase the voltage from zero until the LED conducts current.
Adjust the voltage until the ammeter vacillates between 0.0 and 0.1
μA. Record this voltage as the stopping
potential Vo (and K.E. = qVo).
3. Repeat the procedure for several
other colors of LEDs.
Analysis
1.
Complete the table below.
Table
1
Color |
Wavelength(nm) |
Frequency
(Hz ) |
Stopping
Vo |
Kmax
Energy (J) |
Energy
(eV) |
infrared |
|
|
|
|
|
red |
|
|
|
|
|
orange |
|
|
|
|
|
yellow |
|
|
|
|
|
green |
|
|
|
|
|
blue |
|
|
|
|
|
3. Which LED has the highest work
function (Wo)? Explain
what this means.
4. Choose one of your LEDs,
then calculate the final velocity of an electron as it travels across the LED
point gap. How would this velocity
change with color? (Hint:
K.E.max = qVo = ½mv2)
5. If the point gap approximates 1.0
mm, calculate the acceleration (v2 = 2ad) of the electron and the
time t to cross the gap. What vector
field supplies the accelerating force?
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