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LEEI-14 Van De Graaff Generator
LEEI-21 Electron Beam Demonstrator
LEEI-26 Work Function of Metal
LEEI-35 Hall Effect Experiment
LEEI-37 Helmholtz Coil Magnetic Field
LEEI-38 Solenoid Magnetic Field
LEEI-42 Magnetic Hysteresis Loop
LEEI-45 Magnetoresistive Effect
LEEI-47 Magnetoresistive Sensor
LEEI-50 PN Junction Characteristics
LEEI-55 Nonlinear Circuit Chaotic
LEEI-60 Transmission & Reception
LEEI-61 MW Experiment-Basic
LEEI-62 MW Experiment-Advanced

Structure of an ideal diode


Structure of magnetron tube

Derivation of work function


Derivation of work function

Derivation of charge-mass ratio


Derivation of charge-mass ratio


Apparatus of Work Function & Specific Charge of Electron

Metal Electron Escape Energy Apparatus
Measure work function of metal
Study V-I characteristics of diode
Demonstrate principle of magnetron tube
Measure specific charge of electron (e/m)

Free electrons can transfer from one atom to another within a metal but they normally cannot escape from the metal surface, because the electrons are attracted by the force of the positive nuclei in the metal, known as the surface barrier. However, if sufficient energy is given to free electrons, their kinetic energy increases and thus they can overcome the surface barrier to leave the metal.


The minimum energy required for an electron to leave a metal surface is called the work function, or escape energy of the metal. There are several energy sources that can be applied to a metal surface to cause electron emission, such as heat energy, electric field energy, light energy or kinetic energy of electric charges bombing the metal surface. Hence, the electron emission phenomena are called thermionic emission, field emission, photoelectric emission, and secondary emission, respectively.


This experimental apparatus is designed to study the work function of a metal based on the thermionic emission principle in a vacuum diode tube. In this method, the cathode metal is heated to a sufficiently high temperature to enable free electrons to escape from the metal surface. The number of electrons emitted depends upon the temperature. The higher the temperature, the greater the emission of electrons.


By placing an ideal diode tube in a magnetic field which is perpendicular to the electron field, the motion of electrons emitted from the cathode will be exerted by Lorentz force to form a spiral track. When the Lorentz force is strong enough, the electrons will not reach the anode, so no current is output from the diode. This way, the output of the diode is controlled by magnetization current. That is the principle of a magnetron tube. The charge-mass ratio (e/m), i.e. specific charge of electron, can be derived from parameters applied to the magnetron tube.


Using this apparatus, students can:


1. Understand the concept of thermionic electron emission and verify Schottky effect

2. Understand the concept of work function of a metal

3. Learn how to measure metal work function based on Richardson straight-line method

4. Understand magnetron principle and determine charge-mass ratio (e/m) by magnetron

Ideal diode pure Tungsten filament
filament current 0.400 ~ 0.800 A, accuracy 1.0 mA
anode voltage DC 0 ~120 V, accuracy 0.1 V
Coil parameters inner radius r1=24.0 mm
outer radius r2=36.0 mm
length L=18.0 mm
number of turns N=800
Magnetization current 0 ~ 0.800 A
Parts List
Main unit
Ideal diode
Diode housing
Magnetization coil


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