Leftover magnetism
Hysteresis
Residual magnetism
Coercivity
C. Residual magnetism
3.78 x 10^4
3.78 x 10^-5
3.78 x 10^-3
3.78 x 10^-6
Paramagnetic
Non- magnetic
Ferromagnetic
Diamagnetic
Skin effect
Walt effect
Hall effect
Edison effect
Paramagnetic
Non- magnetic
Ferromagnetic
Diamagnetic
Soft magnetic materials
Hard magnetic materials
High hysteresis loss materials
Low hysteresis loss materials
Ohms/m
Ohms-m
Siemens-m
Siemens/m
6366 A, t/Wb
6000 A, t/Wb
8x10^-3 A, t/Wb
0.8 A, t/Wb
Magnetic effect
Magnetic phenomenon
Magnetic induction
Electromagnetic induction
4 × 10^5 H/m
4 × 10^-12 H/m
4× 10^-2 H/m
4 × 10^7H/m
80 × 10^18
8.5 × 10^22
20 × 10^10
50 × 10^20
Joule's Law
Faraday's second law of electromagnetic induction
Faraday's first law of electromagnetic induction
Coulomb's Law
Paramagnetic
Non- magnetic
Ferromagnetic
Diamagnetic
Weber
Gauss
Gilbert
Tesla
Joule
Volt- coulomb
electron-volt
Walt- second
phasor
vector
scalar
variable
Range
Lattice
Domain
Crystal
Heinrich Rudolf Hertz
Wilhelm Rontgen
James Clerk Maxwell
Andre Ampere
Permalloy
Alnico
Constantan
M anganin
0.5 to 1
1 to 5
5 to 10
1.15 to 1.25
Radiation
Convection
Thermionic emission
Conduction
Phasor quantity
Physical quantity
Scalar quantity
Vector quantity
Conductance
Reluctance
Admittance
Resistance
Radio frequency
Audio frequency
Power supply
Power transformer
Silicon dioxide is a good
The current carriers in conductors are valence electrons
For conductorsa the valence electron are strongly attracted to the nucleus
The valence electrons are located in the nucleus of an atom
p ositive
negative
almost zero
i nfinite
protons and electrons
neutrons and electrons
neutrons and positrons
atoms
Magnetic field intensity
Electric field intensity
Electromagnetic field intensity
Intensity magnetization
Magnetic potential
Magnetic field intensity
Magnetic permeability
F lux density
Magnetism
Electromagnetism
Naturalism
Materialism