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HSC Physics
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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
Participants2
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EduKits Education
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Michael
Lesson 3, Topic 1
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The Motor Effect
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Current-carrying conductors in magnetic fields experience a force. This is known as the motor effect.
This force results from the induced magnetic fields of the moving charges interacting with the external magnetic field surrounding the conductor.

The force on a conductor (length L) at angle θ from perpendicular to a magnetic field is given by the following:
F=LI_\perp B = LIB\sin\theta
The right-hand push rule (see right) should be used to determine the direction of the applied force.
- Max. force is produced where the conductor is perpendicular to the magnetic field
- There is NO force when the conductor is parallel with the magnetic field, i.e. aligned in the direction of its field lines