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Transcript
Determining Planck’s constant Using
LEDs
PH1130: Modern Physics Lab
Shahil Kantesaria, Worcester Polytechnic Institute, Worcester, MA
Historical Perspective and Physics Theory
Max Planck (1858-1947) was born in Kiel Germany and attended schools in Munich and Berlin.
Planck was an early pioneer in the field of quantum physics. Around 1900 Planck developed the concept
of a fundamental unit of energy, a quantum, to explain the spectral distribution of blackbody radiation.
This idea of a basic quantum of energy is fundamental to quantum mechanics of modern physics. Planck
received a Nobel Prize for his work in the early development of quantum mechanics in 1918.
Interestingly, Planck himself remained skeptical of practical applications for quantum theory for many
years.
In order to explain blackbody radiation, Planck proposed that atoms absorb and emit radiation
in discrete quantities given by
E = nhf
where:
 n is an integer known as a quantum number
 f is the frequency of vibration of the molecule, and
 h is a constant, Planck's constant.
Planck named these discrete units of energy quanta. The smallest discrete amount of energy radiated or
absorbed by a system results from a change in state whereby the quantum number, n, of the system
changes by one.
In 1905 Albert Einstein (1879-1955) published a paper in which he used Planck's quantization of
energy principle to explain the photoelectric effect. The photoelectric effect involves the emission of
electrons from certain materials when exposed to light and could not be explained by classical models.
For this work Einstein received the Nobel Prize in Physics in 1921.
Niels Bohr (1885-1962) used Planck’s ideas on quantization of energy as a starting point in
developing the modern theory for the hydrogen atom. Robert Millikan made the first measurement of
Planck’s constant in 1916. The best current value for Planck's constant is 6.62607554 x 10-34 J · s.
In this experiment, you will use light emitting diodes (LED’s) to measure Planck's constant. You
should be familiar with semiconductors and diodes from Modern Physics. To review: LED’s are
semiconductors that emit electromagnetic radiation in optical and near optical frequencies when a
voltage is applied to them. LED’s emit light only when the voltage is forward biased and above a
minimum threshold value. This combination of conditions creates an electron hole pair in a diode.
Electron hole pairs are charge carriers and move when placed in an electrical potential. Thus many
electron hole pairs produce a current when placed in an electric field. Above the threshold value the
current increases exponentially with voltage.
A quanta of energy is required to create an electron hole pair and this energy is released when
an electron and a hole recombine. In most diodes this energy is absorbed by the semiconductor as heat,
but in LED’s this quanta of energy produces a photon of discreet energy E = hf. Because multiple states
may be excited by increasing the voltage across a diode, photons of increasing energies will be emitted
with increasing voltage. Thus the light emitted by an LED may span a range of discrete wavelengths that
decrease with increasing voltage above the threshold voltage (shorter wavelength = higher energy). We
are interested in the maximum wavelength that is determined by the minimum energy needed to just to
create an electron hole pair. It is numerically equal to the turn on voltage of the LED. The relation
between the maximum wavelength, l, and the turn on voltage, V0 , is
𝐸 = ℎ𝑓 =
where:




ℎ𝑐
= 𝑒𝑉0
λ
f is the frequency of the emitted photons,
c is the velocity of light,
e is the electronic charge, and
h is Planck's constant.
If the turn on voltage, 𝑉0 , is measured for several diodes of different color (and different maximum
wavelength, l), a graph of 𝑉0 vs. 1/ λ should be linear with a slope of hc/e. An experimental value of
Planck's constant may then be determined by using the known values of the speed of light, c, and the
charge of an electron, e, and computing h.
Procedure
Equipment:
Vernier
Voltage probe
Breadboard
100Ω resister
10KΩ potentiometer
LEDs
Wires
Adjustable Power Supply
The circuit that will be used for this experiment to determine Planck’s constant is shown below:
1) Connect the power supply leads to the breadboard. Use the convention red (+) and black (-).
2) Attach a wire from the breadboard’s positive terminal to the first pin of the 10KΩ potentiometer
labeled 1.
3) Attach a wire from the breadboard’s negative terminal to the third pin of the 10KΩ
potentiometer labeled 3.
4) Connect one end of the 100Ω resistor to the second pin on the potentiometer (middle pin) and
the other end of the resistor to an empty slot in the breadboard.
5) Select an LED which has been provided to you to insert into the breadboard. Connect the longer
lead of the LED to the same pin column as the 100Ω resistor. (end of the resistor not connected
to the potentiometer) Connect the other lead of the led to an empty slot.
6) Attach a wire from the shorter lead of the LED to the third pin of the potentiometer.
7) Connect the positive end of the voltage probe to the longer lead of the LED and vice versa for
the negative end.
The final circuit setup should resemble the figure below:
8) Open the given lab template in Logger Pro.
9) Switch on the power supply and adjust the voltage so that it outputs 6V.
10) Click the collect button on the template. Check the 10KΩ potentiometer to see that it is turned
fully counterclockwise, the LED should be fully lit.
11) Turn the potentiometer knob clockwise till the LED has shut off, adjust the knob until you find
the point at which the LED is barely on. Press the keep button on the template and enter in the
LED’s Frequency (THz). You will see that the template has gone ahead and calculated the energy
and Planck’s constant for the particular LED.
12) Repeat steps 9 through 11 for the different LEDs given to you in lab. Remember each time to
switch out the LED and to let Logger Pro run. (Do not end collecting till all LEDs have been
recorded)
Calculations
Now that you have found the minimum turn on voltages for the various LEDs given to you in lab, the
next step will be to determine a value for Planck’s constant.
1) Click on the X-axis label on the graph in the Logger Pro template and select “adjusted freq”, Next
click on the Y-axis label and select “E”.
2)
Find the best fit for the curve on the Frequency vs. Energy plot. (Generally a linear fit will work
well) The slope of your best fit line will be the value for Planck ’s constant (h).
Questions
1) What was the value of h in your experiment and what is the percent error from the true value of
h?
2) What could some of the factors of error in this experiment be and how could you eliminate
them to achieve a better result?
TA Section
1) Expected results: 5.77 * 10−34 to 7.67 *10−34 for the five LEDs
2) Manufacture listed frequencies could differ from actual LEDs, use a spectrometer to determine
actual frequency for each LED.
References
1. J. O’Connor and L. O’Connor, “Measuring Planck’s constant using a light emitting diode,” Phys. Teach.
12, 423–425 (Oct. 1974).
2. J.W. Jewett Jr., “Get the LED out,” Phys. Teach. 29, 530–534 (Nov. 1991).
3. Hackworth Martin, M. H. (2012, May 1). Measuring planck’s constant. Retrieved from
http://www.physics.isu.edu/~hackmart/planck's.PDF