Directly proportional to
Inversely proportional to
Directly proportional to the square of
Inversely proportional to the square of
C. Directly proportional to the square of
Maxwell
Gauss
At/Wb
Weber
Heinrich Rudolf Hertz
Wilhelm Rontgen
James Clerk Maxwell
Andre Ampere
Right hand rule
Helix rule
End rule
Cork screw rule
2 x 10^-5
2 x 10^-3
2 x 10^5
2 x 10^3
6366 A, t/Wb
6000 A, t/Wb
8x10^-3 A, t/Wb
0.8 A, t/Wb
Atom
Proton
Electron
Neutron
Flux times area of core
Flux times number of turns times area of core
Flux times number of turns times length of core
Flux times number of turns
8.854 F/m
8.854 × 10^-12 mF/m
8.854× 10^-12 F/m
8.854 × 10^-12 F/m
scalar
phasor
vector
variable
The magnetic flux can be changed.
Hysteresis can be decreased.
Magnetic materials can be used.
Abundance of ferromagnetic material that can be temporarily magnetized.
Hardened steel
Cobalt steel
Soft iron
Tungsten steel
Curie's Law
Child's Law
CR Law
Curie-Weiss Law
Soft magnetic materials
Hard magnetic materials
High hysteresis loss materials
Low hysteresis loss materials
Joule's law
Faraday's law
Volta's theorem
Ampere's theorem
Becomes weaker
Becomes stronger
Reverses in direction
is unchanged
electric bells
earphones
relays
dy namic loudspeakers
iron
nickel
soft steel
hardened steel
Aluminum
Silver
Air
Cobalt
directly proportional to
inversely proportional to
independent of
dependent of
Ionic
Covalent
Metallic
Van der Waals
1 coulomb/volt
1 newton/coulomb
1 newton-meter
1 volt/second/ampere
Magnetic Reluctivity
Magnetic Resistivity
Magnetic susceptibility
Magnetic conductivity
Diamagnetic
Permanent magnets
Paramagnetic
Electromagnetic
Air gap
Free space
Vacuum
Atmosphere
potential gradient
potential difference
dielectric constant
the force
Wb/m
Tesla
At/m
N/Wb
Dielectric strength
Electric intensity
Potential gradient
Dielectric constant
phasor
vector
scalar
variable
deficit of electrons
excess of neutrons
excess of electrons
deficit of protons