Properties of Electrical Materials Flashcards
conducting materials
allow the movement of charge with quantum states for free electrons and electrons that can be liberated with very little energy input
dielectric (insulating) medium
- an ideal dielectric medium contains no free charges
- all electrons are bonded to atoms
- the medium will not conduct electricity
- in reality, a dielectric medium can be overcome by a strong enough electric field (called a breakdown)
dielectric polarization
- the electric field polarizes the dielectric medium
- atoms and molecules are aligned and stretched in the direction of the field
- positive nuclei are pushed in one direction, electrons in the opposite direction
- directions depend on direction of the field
- this creates an induced electric dipole
semiconducting materials
materials though which charge easily flow more or less easily
hole
- a hole is positively charged atom that attracts electrons
- when voltage is applied, electrons are drawn to positive charge
- hole attracts an electron from a neighboring atom, most likely from direction of negative charge
- hole atom become neutral, neighboring atom becomes new hole
- hole migrates toward negative charge, though atoms do not move
- in this way, both electrons and holes carry current
p-type material
majority carrier: holes
valance electrons in dope atoms: 3 electrons (Al, B, ln, Ga)
no. of covalent bonds formed by dope atom: 3, resulting in one neighbor atom unbonded
dope atom charge: retains static negative charge, hole is free to move
dope atom name: acceptor
minority carrier: free electrons
n-type
majority carrier: electrons
valence electrons in dope atoms: 5 electrons ( Ph, As, Sb)
no. of covalent bonds formed by dope atom: 4, donates a free electron
dope atom charge: retains positive charge, electron is free to move
dope atom name: donor
minority carrier: holes
permeability, μ
- a property of a material
- measure how readily a magnetic field is created within the material when an external magnetic field is applied
- due to behavior of electrons in presence of external magnetic field
- examples of high permeability: iron and steel
- examples of low permeability: wood and water
nonmagnetic materials
negligibly affected by presence of magnetic field (i.e. have low permeability)
types include:
- diamagnetic
- paramagnetic
- antiferromagnetic
diamagentism
- due to electrons circulation in their orbits
- exhibited by all materials
- cancels due to random orientation of the spins
paramagnetism
- due to circulation of unpaired electrons in their orbitals
- spins align with magnetic field
antiferromagnetism
- leads to tiny increase in permeability
- due to magnetic dipole moments that align
- moment of one atom has the opposite orientation of its neighbor
magnetic materials
- significantly affected by presence of magnetic field
- cause circulating currents in plane perpendicular to magnetic field
types include:
- ferromagnetic
- ferrimagnetic
ferromagnetism
- leads to large increase in permeability
- due to magnetic domains with fully aligned magnetic dipole moments
- results in spinning electrons even without external magnetic field
ferrimagnetism
- leads to increase in permeability, but less so than ferromagnetism
- due to ordered spin structures that neither cancel fully (as in antiferromagnetism) nor add fully (as in ferromagnetism)
ferromagnetism
- fully aligned
- large increase in permeability
ferrimagnetism
- neither fully aligned nor fully canceling
- moderate increase in permeability
antiferromagnetism
- fully canceling
- tiny increase in permeability
coefficient of thermal expansion
- rate at which material expands and contracts as temperature increases and decreases α = E/delta T - engineering strain: E = delta L/ Lo -change in linear dimension: delta L = Lo α delta T
The coefficient of thermal expansion is a property of both electrical and magnetic materials
However, the change in dimensions is not considered in resistance, capacitance, and so on, because the change is so small
electric flux Φ
- measures electric field
- does not flow equally well through all materials
- units are volt-meters (V * m)
permittivity, ε
- determines the flux that passes through the medium
- total electric flux generated by a point charge is proportion to charge
ϕ = q/ E
Eo is permittivity of free space
for air E= Eo= 8.85x 10^-12 F/m
dielectric constant (or relative permittivity), k
- dimensionless comparison to permittivity of free space, Eo
E= k Eo - informal definition: ratio of flux in a medium to flux in a vacuum
- for a vacuum, k =1
- formal definition: ratio of capacitances for a given voltage and separation
k = C with dielectric/ C vacuum - The NCEES Handbook sometimes uses the symbol, Er for relative permittivity
electric flux density, D
- relationship between density and electric flux is
D= εE - E is electric field intensity in (N/C)
Capacitance, C
- measures of capacitor’s ability to store electric charge
- ratio of stored charge to applied voltage
C = q/V
-for a parallel plate capacitor,
C = εA/d