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Chapter 22. Electromagnetism. contents. Force on a current-carrying conductor Force on beam of charged particles Fleming’s Left-hand rule Turning effect of a current-carrying coil in a magnetic field The D.C. Motor Chapter Review. Force on a current-carrying conductor.
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Chapter 22 Electromagnetism
contents Force on a current-carrying conductor Force on beam of charged particles Fleming’s Left-hand rule Turning effect of a current-carrying coil in a magnetic field The D.C. Motor Chapter Review
Force on a current-carrying conductor Apparatus to demonstrates force on a current-current conductor in an external magnetic field
Force on a current-carrying conductor After Switch ON Before Switch ON
Force on a current-carrying conductor After Switch ON Before Switch ON
Force on a current-carrying conductor ▪ Current-carrying conductor placed in a magnetic field will experience a force (known as Lorentz force) (Note: Current is not parallel to magnetic field) F = BILsin θ F: Lorentz Force on current- carrying conductor B: Magnetic Field Stength I: Current in conductor L: Length of conductor Θ: Angle between B & I
Action = Force B= Magnetic Field C= Current Fleming’s Left-hand rule ▪ Fleming’s left-hand rule is used to find the directions of force, magnetic field and conventional current when any of the other two quantities are known
Force on a current-carrying conductor Example: Current DOWN Current UP Current OFF
Force on a current-carrying conductor Application: Moving Coil loudspeaker
Force on beam of charged particles Positive Charged Particles
Force on beam of charged particles Negative Charged Particles F V
Force on beam of charged particles • Used in Cathode Ray tube for • TV screen • computer monitors • Oscilloscope to • study waveforms
Force on beam of charged particles F = qvBsin θ F: Force on charged particls B: Magnetic Field Stength q: Charge of the particles (Charge of 1 proton = 1.6 x 10-19C) (Charge of 1 electron = -1.6 x 10-19C) v: velocity of the charged particles Θ: Angle between B & charged particles
Turning Effect of a current-carrying coil in a magnetic field Carbon Brushes Commutator
Turning Effect of a current-carrying coil in a magnetic field • Purpose of the commutator: • To reverse the direction of the current in the loop whenever • the commutator changes contact from one brush to the other • This ensures that the loop will always be turning in one • direction
Turning Effect of a current-carrying coil in a magnetic field
Turning Effect of a current-carrying coil in a magnetic field
Turning Effect of a current-carrying coil in a magnetic field
Turning Effect of a current-carrying coil in a magnetic field • The current-carrying coil in a magnetic • field on the whole experiences a turning • effect • Turning force (or turning effect) can be • increased by either (or both): • - increasing the number of turns on the coil • - increasing the current in the coil • - place a soft-iron core within the field Application: Electric Motors like electric fans, hair dryers
Turning Effect of a current-carrying coil in a magnetic field
Turning Effect of a current-carrying coil in a magnetic field
Turning Effect of a current-carrying coil in a magnetic field
Turning Effect of a current-carrying coil in a magnetic field
Force between two parallel Current-Carrying Wires Unlike currents repel
Force between two parallel Current-Carrying Wires Like currents attract
A Cyclotron – Charged Particles Accelerator
A Cyclotron – Charged Particles Accelerator
A Cyclotron – Charged Particles Accelerator
A Cyclotron – Charged Particles Accelerator
A Cyclotron – Charged Particles Accelerator
A Cyclotron – Charged Particles Accelerator