PASCO h/e Apparatus Instruction Manual

Includes
Teacher's Notes
and
Typical
Experiment Results
Instruction Manual and Experiment Guide
012-04049J
h/e Apparatus
and
h/e Apparatus Accessory Kit
08/98
© 1989 PASCO scientific $5.00
012-04049J h/e Apparatus and h/e Apparatus Accessory Kit
Table of Contents
Section Page
Copyright, Warranty, and Equipment Return.................................................. ii
Introduction ..................................................................................................... 1
Background Theory ......................................................................................... 2
Equipment and Setup ....................................................................................... 3
Equipment List .......................................................................................... 3
Installing the Batteries ...............................................................................3
Battery Voltage Check............................................................................... 3
Equipment Setup ....................................................................................... 4
Using the Accessory Kit Filters ................................................................. 6
Experiments:
Experiment 1: Wave Model vs Quantum Model................................. 7
Experiment 2: The Relationship of Energy, Wavelength
and Frequency............................................................ 11
Technical Information .................................................................................... 13
Theory of Operation ................................................................................. 13
Schematic Diagram................................................................................... 14
Teacher’s Guide.............................................................................................. 15
Technical Support ................................................................. Inside Back Cover
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h/e Apparatus and h/e Apparatus Accessory Kit 012-04049J
Copyright, Warranty, and Equipment Return
Please—Feel free to duplicate this manual subject to the copyright restrictions below.
Copyright Notice
The PASCO scientific 012-04049J h/e Apparatus and h/e Apparatus Accessory Kit manual is copyrighted and all rights reserved. However, permission is granted to non-profit educational institutions for reproduction of any part of the manual providing the reproductions are used only for their laboratories and are not sold for profit. Reproduction under any other circumstances, without the written consent of PASCO scientific, is prohibited.
Limited Warranty
PASCO scientific warrants the product to be free from defects in materials and workmanship for a period of one year from the date of shipment to the customer. PASCO will repair or replace at its option any part of the product which is deemed to be defective in material or workmanship. The warranty does not cover damage to the product caused by abuse or improper use. Determination of whether a product failure is the result of a manufacturing defect or improper use by the customer shall be made solely by PASCO scientific. Responsibility for the return of equipment for warranty repair belongs to the customer. Equipment must be properly packed to prevent damage and shipped postage or freight prepaid. (Damage caused by im­proper packing of the equipment for return shipment will not be covered by the warranty.) Shipping costs for returning the equipment after repair will be paid by PASCO scientific.
Equipment Return
Should the product have to be returned to PASCO scientific for any reason, notify PASCO scientific by letter, phone, or fax BEFORE returning the product. Upon notification, the return authorization and ship­ping instructions will be promptly issued.
NOTE: NO EQUIPMENT WILL BE
ACCEPTED FOR RETURN WITHOUT AN AUTHORIZATION FROM PASCO.
When returning equipment for repair, the units must be packed properly. Carriers will not accept responsibility for damage caused by improper packing. To be certain the unit will not be damaged in shipment, observe the following rules:
The packing carton must be strong enough for the
item shipped.
Make certain there are at least two inches of pack-
ing material between any point on the apparatus and the inside walls of the carton.
Make certain that the packing material cannot shift
in the box or become compressed, allowing the instrument come in contact with the packing carton.
Address: PASCO scientific
10101 Foothills Blvd. Roseville, CA 95747-7100
Phone: (916) 786-3800 FAX: (916) 786-3292 email: techsupp@pasco.com web: www.pasco.com
Credits
This manual edited by: Dave Griffith
Teacher’s guide written by: Eric Ayar
ii
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012-04049J h/e Apparatus and h/e Apparatus Accessory Kit
Introduction
The emission and absorption of light was an early subject for investigation by German physicist Max Planck. As Planck attempted to formulate a theory to explain the spectral distribution of emitted light based on a classical wave model, he ran into considerable difficulty. Classical theory (Rayleigh-Jeans Law) predicted that the amount of light emitted from a black body would increase dramati­cally as the wavelength decreased, whereas experiment showed that it approached zero. This discrepancy became known as the ultraviolet catastrophe.
Experimental data for the radiation of light by a hot, glowing body showed that the maximum intensity of emitted light also departed dramatically from the clas­sically predicted values (Wien's Law). In order to rec­oncile theory with laboratory results, Planck was forced to develop a new model for light called the quantum model. In this model, light is emitted in small, discrete bundles or quanta.
The relationship between the classical and quantum theo­ries for the emission of light can be investigated using the PASCO scientific h/e Apparatus. Using the Apparatus in combination with the PASCO Mercury Vapor Light Source (Model OS-9286) allows an accurate determina­tion of the h/e ratio and thus a determination of h, Planck's constant.
Figure 1. The h/e Apparatus Shown With the Accessory Kit and Mercury Vapor Light Source
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h/e Apparatus and h/e Apparatus Accessory Kit 012-04049J
Background Theory
Planck's Quantum Theory
By the late 1800's many physicists thought they had ex­plained all the main principles of the universe and discov­ered all the natural laws. But as scientists continued work­ing, inconsistencies that couldn't easily be explained be­gan showing up in some areas of study.
In 1901 Planck published his law of radiation. In it he stated that an oscillator, or any similar physical system, has a discrete set of possible energy values or levels; en­ergies between these values never occur.
Planck went on to state that the emission and absorption of radiation is associated with transitions or jumps be­tween two energy levels. The energy lost or gained by the oscillator is emitted or absorbed as a quantum of radiant energy, the magnitude of which is expressed by the equa­tion:
E = h
ν
where E equals the radiant energy, ν is the frequency of the radiation, and h is a fundamental constant of nature. The constant, h, became known as Planck's constant.
Planck's constant was found to have significance beyond relating the frequency and energy of light, and became a cornerstone of the quantum mechanical view of the suba­tomic world. In 1918, Planck was awarded a Nobel prize for introducing the quantum theory of light.
The Photoelectric Effect
In photoelectric emission, light strikes a material, causing electrons to be emitted. The classical wave model pre­dicted that as the intensity of incident light was increased, the amplitude and thus the energy of the wave would in­crease. This would then cause more energetic photoelec­trons to be emitted. The new quantum model, however, predicted that higher frequency light would produce higher energy photoelectrons, independent of intensity, while increased intensity would only increase the number of electrons emitted (or photoelectric current). In the early 1900s several investigators found that the kinetic energy of the photoelectrons was dependent on the wave­length, or frequency, and independent of intensity, while the magnitude of the photoelectric current, or number of electrons was dependent on the intensity as predicted by the quantum model. Einstein applied Planck's theory and explained the photoelectric effect in terms of the quantum model using his famous equation for which he received the Nobel prize in 1921:
E = h
ν
= KE
max
+ W
O
where KE ted photoelectrons, and W move them from the surface of the material (the work
is the maximum kinetic energy of the emit-
max
is the energy needed to re-
O
function). E is the energy supplied by the quantum of light known as a photon.
The h/e Experiment
A light photon with energy hν is incident upon an elec­tron in the cathode of a vacuum tube. The electron uses a minimum WO of its energy to escape the cathode, leaving it with a maximum energy of KE energy. Normally the emitted electrons reach the anode of the tube, and can be measured as a photoelectric current. However, by applying a reverse potential V between the anode and the cathode, the photoelectric current can be stopped. KE
can be determined by measuring the mini-
max
mum reverse potential needed to stop the photoelectrons and reduce the photoelectric current to zero.* Relating kinetic energy to stopping potential gives the equation:
KE
max
Therefore, using Einstein's equation,
ν
= Ve + W
h
When solved for V, the equation becomes:
V = (h/e)
If we plot V vs ν for different frequencies of light, the graph will look like Figure 2. The V intercept is equal to -
W
/e and the slope is h/e. Coupling our experimental de-
O
termination of the ratio h/e with the accepted value for e, 1.602 x 10
-19
coulombs, we can determine Planck's
constant, h.
Stopping
Potential
V
Figure 2. The graph of V vs.
*NOTE: In experiments with the PASCO h/e Ap­paratus the stopping potential is measured directly, rather than by monitoring the photoelectric current. See the Theory of Operation in the Technical Infor­mation section of the manual for details.
in the form of kinetic
max
= Ve
O
ν
- (WO/e)
Slope = h/e
Frequency ν
νν
ν
νν
2
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012-04049J h/e Apparatus and h/e Apparatus Accessory Kit
Equipment and Setup
Equipment Required:
Lens/Grating Assembly
Filters
h/e Apparatus AP-9368
Mercury Vapor light
Source OS-9286
Light Aperture Assembly
– Digital voltmeter (SE-9589) – h/e Apparatus, (AP-9368*) – h/e Apparatus Accessory Kit, (AP-9369*) – Mercury Vapor Light Source, (OS- 9286*)
Installing the Batteries
The h/e Apparatus requires two 9-volt batteries (supplied but not installed). The battery compartment is accessed by loosening the thumbscrew on the rear end panel, and re­moving the cover plate.
NOTE: The h/e Apparatus can also be powered
using a ±9 V dual power supply. Just remove the batteries and connect +9 V to the "+6 V MIN" bat­tery test terminal and -9 V to the "-6 V MIN" bat­tery test terminal.
Battery Voltage Check
Although the h/e Apparatus draws only a small amount of current and batteries normally last a long time, it's a good idea to check the output voltage before each use. Battery test points are located on the side panel of the Apparatus near the ON/OFF switch. Batteries functioning below the recommended minimum operating level of 6 volts may cause erroneous results in your experiments.
Support Base Assembly
Light Block (for Light Source)
Coupling Bar Assembly
h/e Apparatus Accessory Kit AP-9369
Figure 3. h/e Equipment Identification
*These items may be purchased separately from PASCO
scientific, or together as an AP-9370 h/e System.
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To check the batteries, use a voltmeter to measure be­tween the OUTPUT ground terminal and each BATTERY TEST terminal (-6V MIN and +6V MIN). If either battery tests below its minimum rating, it should be replaced before running experiments.
Battery Test Terminals
ON/OFF Switch
Ground Te rm i na l
Figure 4. Battery Test Points
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