thermionic emission

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Thermionic emission If a tungsten filament is heated to about 2000 o C, some of the electrons have sufficient kinetic energy to escape from the surface of the wire. This effect is called thermionic emission. It is quite easy to imagine this if we think about a metal wire as a lattice of ions in a

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Thermionic emission. If a tungsten filament is heated to about 2000 o C, some of the electrons have sufficient kinetic energy to escape from the surface of the wire. This effect is called thermionic emission . - PowerPoint PPT Presentation

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Page 1: Thermionic emission

Thermionic emission

• If a tungsten filament is heated to about 2000 o C, some of the electrons have sufficient kinetic energy to escape from the surface of the wire.

• This effect is called thermionic emission.

• It is quite easy to imagine this if we think about a metal wire as a lattice of ions in a sea of free electrons. In effect we are boiling the electrons off.

Page 2: Thermionic emission

Thermionic Diode• In the vacuum tube there are

two electrodes• Cathode -ve Anode

+ve • When the filament is

switched on electrons start to flow from the cathode the tungsten filament and are attracted to the anode

• You need a vacuum as the electrons would collide with the gas particles. Also the filament would burn up

• Thermionic_diode

Page 3: Thermionic emission

Deflection tube

• The electron gun consists of a heated filament/cathode and an anode with a hole in it.

• This produces a narrow beam of electrons

• The screen is coated with a fluorescent material which glow when electrons strike it.

Page 4: Thermionic emission

Deflection Tube

Page 5: Thermionic emission

Defection by an electric field

• The negatively charged electrons are attracted towards the positive plate.

Page 6: Thermionic emission

Deflection tube

• In a magnetic field the electron is deflected depending on the direction of the magnetic field - Use Lenz’s left hand rule.

Page 7: Thermionic emission

Cathode Ray Tubes

Thermionic emission was the starting point for Joseph John Thomson to produce his cathode ray tube (CRT) in 1897, the descendants of which we used to see every day, before TFT (thin film transistor) TV sets became more common.

• Now do question 1 page 243

Page 8: Thermionic emission

Using an Oscilloscope

Page 9: Thermionic emission

Learning Objectives

To know what an oscilloscope is and how it works.

The job description of the oscilloscope’s main parts

How the oscilloscope shows Direct Current DC and Alternating Current AC

No calculations are required in the exam for the voltage, time period or frequency

Page 10: Thermionic emission

Cathode Ray Oscilloscope

Page 11: Thermionic emission

Definition

From the specification book:-

An oscilloscope consists of a specially made electron tube and associated control circuits.

The electron gun emits electrons towards a fluorescent screen light is emitted when electrons hit the screen this is what we see.

Page 12: Thermionic emission

Tube Photograph

Page 13: Thermionic emission

Electron Gun Photograph

Page 14: Thermionic emission

Tube Diagram

H.T. supply

heater supply

y plates - amplifier

+-fluorescent screen

anode

x plates - timebase

Page 15: Thermionic emission

Cathode Ray Oscilloscope (CRO)

Display

Channel1 Channel 2

Time base

Y-gain

My tie

Page 16: Thermionic emission

How does it work?

An oscilloscope consists of a specially made electron tube and associated control circuits.

An electron gun at one end of the glass tube emits electrons in a beam towards a fluorescent screen at the other end of the tube.

Light is emitted from the spot on the screen where the beam hits the screen.

Page 17: Thermionic emission

How does it work?

When no p.d. is applied across the plates the spot on the screen is stationary.

If a pd is applied across the X-plates the beam of electrons is deflected horizontally and the spot moves across.

pd across Y-plates spot moves up and down.

Page 18: Thermionic emission

Time Period (ms)

Peak-to-Peak voltage

Reading the CRO 1

To get the time period you need to measure this distance and convert it to time by multiplying by the time base setting

Page 19: Thermionic emission

Oscilloscope Controls

The x-plates are connected to a time base circuit which is designed to make the spot move across the screen in a given time then back again much faster. a bit like a trace on a heart monitor.

The y-plates are connected to the Y-input and this causes the spot to move up or down depending on the input pd.

Page 20: Thermionic emission

summary

H.T. supply

heater supply

y plates

+-phosphor screen

anode

electron gun produces a beam

of electronslight produced on

the screen by electron beam

a p.d. across the y plates deflects the

trace vertically

a p.d. across the x plates deflects the trace horizontally

x plates

Page 21: Thermionic emission

Displaying a waveform1. The time base

• The X-plates are connected to the oscilloscope’s time base circuit.

• This makes the spot move across the screen, from left to right, at a constant speed.

• Once the spot reaches the right hand side of the screen it is returned to the left hand side almost instantaneously.

• The X-scale opposite is set so that the spot takes two milliseconds to move one centimetre to the right. (2 ms cm-1).

NTNU Oscilloscope Simulation

KT Oscilloscope Simulation

Page 22: Thermionic emission

Gain and Time-Base Controls

Page 23: Thermionic emission

Displaying a waveform2. Y-sensitivity or Y-gain

• The Y-plates are connected to the oscilloscope’s Y-input.

• This input is usually amplified and when connected to the Y-plates it makes the spot move vertically up and down the screen.

• The Y-sensitivity opposite is set so that the spot moves vertically by one centimetre for a pd of five volts (5 V cm-1).

• The trace shown appears when an alternating pd of 16V peak-to-peak and period 7.2 ms is connected to the Y-input with the settings as shown.

NTNU Oscilloscope Simulation

KT Oscilloscope Simulation

Page 24: Thermionic emission

Peak Voltage

Peak p.d. = 3 Divisions x 1.0 mV/div = 3.0 mV

Page 25: Thermionic emission

Period & Frequency

period = 4.0 divisions x 1.0 ms/div = 4.0 msfrequency = 1 / periodfrequency = 1 / 0.004 sfrequency = 250 Hz

Page 26: Thermionic emission

Measuring d.c. potential difference

Diagram a shows the trace for pd = 0V.Diagram b shows the trace for pd = +4VDiagram c shows the trace for pd = -3V.

NTNU Oscilloscope Simulation

KT Oscilloscope Simulation

All three diagrams below show the trace with the time base on and the Y-gain set at 2V cm-1.

Page 27: Thermionic emission

Self Test

Page 28: Thermionic emission

Internet Links• Oscilloscope - basic display function -

NTNU • Oscilloscope Simulation - by KT • Lissajous figures - Explore Science • Lissajous figures - by KT