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HSC Physics
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Module 1: Kinematics1.1 Motion in a Straight Line
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1.2 Motion on a Plane
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Module 2: Dynamics2.1 Forces
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2.2 Forces, Acceleration and Energy
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2.3 Momentum, Energy and Simple Systems
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Module 3: Waves and Thermodynamics3.1 Wave Properties
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3.2 Wave Behaviour
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3.3 Sound Waves
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3.4 Ray Model of Light
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3.5 Thermodynamics
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Module 4: Electricity and Magnetism4.1 Electrostatics
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4.2 Electric Circuits
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4.3 Magnetism
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Module 5: Advanced Mechanics5.1 Projectile Motion
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5.2 Circular Motion
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5.3 Motion in Gravitational Fields2 Topics
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Module 6: Electromagnetism6.1 Charged Particles, Conductors and Electric and Magnetic Fields
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6.2 The Motor Effect1 Topic
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6.3 Electromagnetic Induction
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6.4 Applications of the Motor Effect1 Topic
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Module 7: The Nature of Light7.1 Electromagnetic Spectrum3 Topics
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7.2 Light: Wave Model
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7.3 Light: Quantum Model2 Topics
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7.4 Light and Special Relativity
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Module 8: From the Universe to the Atom8.1 Origins of the Elements5 Topics
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8.2 Structure of the Atom3 Topics
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8.3 Quantum Mechanical Nature of the Atom2 Topics
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8.4 Properties of the Nucleus2 Topics
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8.5 Deep Inside the Atom4 Topics
Lesson 26, Topic 1
In Progress
Evidence of the Electron
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Early Experiments with Cathode Rays
J. J. Thomson conducted a number of early experiments with cathode rays.
- Found that the cathode ray tube glowed more when the gas was at a lower pressure.
- Experimented with phosphorescent paint. The paint opposite the negatively charged cathode sparked and glowed.
- Use electric plates above and below the tube to deflect the cathode ray. This allowed Thomson to determine that the rays were negatively-charged.
Thomson’s Charge-to-Mass Experiment
Thomson was also measured the electron’s charge-to-mass ratio. He achieved this by creating perpendicular electric and magnetic fields around a cathode ray tube. The experiment involved two stages.
- The magnetic and electric fields were varied until their forces on the particles cancelled, causing no ray deflection. With no net force, the magnetic and electric forces could be equated and re-arranged to find the velocity of the electrons.
- The magnetic field was then applied alone to the tube, causing a circular deflection of the particles perpendicular to the field. The radius of curvature was measured.
Thomson combined the results of the two stages to calculate the charge-to-mass ratio for the electron.
Millikan’s Oil Drop Experiment
Millikan observed the behaviour of oil droplets to determine a value for the charge of the electron.
- Oil was atomised into tiny droplets. A beam of X-rays were passed through the oil so that some droplets became charged.
- The droplets fell through a gap in the higher of two parallel charged plates, entering a uniform electric field.
- The voltage was adjusted until some droplets were suspended, achieved when the force due to gravity was equally opposed by the force due to the electric field.
- Millikan calculated the mass of the suspended oil droplets by measuring their radii and using known values for the density of oil.
- The charge of the oil droplets could then be found be equating the electric and gravitational forces, and re-arranging to find q.
The experiment found that all charges on the droplets were multiples of a fundamental charge, the charge of an electron. This was calculated to be 1.6 \times 1-^{-19} \text C, known as the elementary charge.