类别 全部 - current - magnetic - force

作者:peter hill 14 年以前

673

M&G

The text discusses various concepts related to motors and electromagnetism. It explains the motor effect where a current-carrying conductor in a magnetic field experiences a force and how this principle is utilized in DC motors to produce torque.

M&G

M&G

References

UNSW
HSC online

AC Motors

  • Universal - all coils - with core opposing outer
  • Induction - Outer field drives eddy current in core rather than from slip rings
  • Transformers

  • Electricity > Mag Field > Electricity
  • Transformers - An electrically powered electricity generator
  • More turns more volts
  • Laminations to hold field but stop current
  • Power

  • DC Generator is reverse DC motor
  • AC Generator has windings on outside
  • 3 phase has constant torque
  • Powerline insulation and lightening wires
  • Insulation

    Generators

  • Faraday Effect: Motor Effect separate + from -
  • Moving conductor in a field is a Battery
  • Lenz's Law - eddy currents maintain field and applies a drag force
  • Lenz's Law

    Motors

  • Motor Effect
  • A current in a field has a palm push
  • Ampere's law
  • DC Motors have constant switched force, Maximum torque at max distance flat to field
  • Comutators make Coil always the wrong way
  • Motor Effect

    Current creates a force

    Applications

    loudspeaker

    Radial Field (Push up down)

    Spring

    Galvanometer

    Axial Field (B is not a function of angle)

    Force prop Current

    Spring means deflection = current

    DC Motor

    Through Field

    Comutator to change current

    External Magnet

    Electromagnet

    Perminant

    Commutator

    Loop

    Coil

    t = BAincos(q)

    n = turns

    B = Field in tesla T

    A = area x m times y m

    i = current A

    q= angle to mag field

    One wire

    t = Fd

    Torque has units Newton meters

    Vectors do not have to known

    1nm clockwise

    Wire

    Two wires

    F Force N newtons attractive

    l Length m meters length of parallel wire

    k 2E-7 magnetic constant

    d separation m meters

    I current A amps

    The force of 1 N is read off the apparatus, defining the amp and thus also the coulomb

    F/l = KII/D

    Parallel Pull together

    Anti Parallel = anti

    Single wire

    F = BIlSin(q)


    - Field Strength (tesla T)

    - I Current (amps A)

    - l Length (m)

    - Sin(q) angle

    Magfields
    Worked solutions
    Drawing

    in x Out .

    Solenoid Loop

    N -> S

    Handrules

    Solenoid finger flow in current , thumb points north

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    Finger field, thumb up current, palm push

    Grip wire