LECTURE 17. Electrical properties - Welcome to AML 883 -...
Transcript of LECTURE 17. Electrical properties - Welcome to AML 883 -...
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AML 883 Properties and selection of engineering materials
LECTURE 17. Electrical properties
M P GururajanEmail: [email protected]
Room No. MS 207/A3 Phone: 1340
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Types of electric behaviour
● Conduction● Insulation
● Dielectrics – insulators; what we are talking about is the behaviour in an electric field
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Dipole moment
+ +
Permanent dipole moment of water molecule
Image courtesy: wiki
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Dielectrics
● Dielectric constant – relative permittivity: how much does a material polarize (acquires dipole moment)
● Dielectric loss factor: Energy dissipated when radiofrequency waves pass through the material (energy appears as heat, of course)
● Dielectric breakdown potential: damage due to dielectric losing its insulating properties
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Resistivity and conductivity
Current, i
Pot
entia
l diff
eren
ce, V
R=V/i
L
Area, A
Current, i+
V
Resistivity, = (A/L) R
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Resistivity
● Electrical resistance: ohms ()● Ohm's law: Electrical resistance in a material is
the potential drop V across it, divided by the current i passing through it
● Potential drop: volts● Current: amps● Material property: electrical resistivity (get rid of
the effects of geometry)●Ohmm
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Georg Simon Ohm
Image courtesy: wiki
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Count Alessandro Antanio Anastasio Volta
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AndreMarie Ampere
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Electrical resistivity
● A quantity of immense range● Conductors: little more than
● Best insulators:
● Electrical conductivity: reciprocal of electrical resistivity!
● Units of conductivity: siemens per m
10−8m
1016m
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Ernest Werner von Siemens
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Dielectric properties
Potential difference, V
Cha
rge,
Q
C=Q/V
t
Area, A
Current, i+
V
Dielectric constant, =
Breakdown
Dielectric material
C (with dielectric)C (without dielectric)
Charge, Q
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Field
● Region of space in which objects experience forces
● Provided of course they are of the right type● Electric field: field created by charges● Electric field strength between two oppositely
charged plates separated by a distance t with potential difference V between them is E = V/t
● E is independent of position (except near the edges of the plate)
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Capacitor
● Two conducting plates separated by a dielectric● Capacitors (or, condensers) store charge● Charge Q (coulombs) is directly proportional to
the potential difference between the plates V (volts): Q = C V
● C – capacitance (farads)
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CharlesAugustin de Coulomb
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Michael Faraday
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Permittivity
● The capacitance of a parallel plate capacitor of area A, separated by empty space isc= A/t
● is the permittivity of free space (farad metre)● Replace the empty space by a dielectric,
capacitance increases. Why?
0
0
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Permittivity
● Dielectric polarizes● The field created by polarization opposes the
field E● So, the voltage difference needed to support
the charge is reduced● Thus, the capacity of the condenser is
increased● C = A/t● is the permittivity of the dielectric
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Dielectric constant
● Relative permittivity – dielectric cosntant:● = C(with dielectric)/C(without didlectric) = /● Ct● Dielectric constant is dimensionless (ratio)● Dielectric constant for air is unity (as well as
gases, for all practical purposes); for most dielectrics it lies between 2 and 20; for ferroelectrics, it could be as high as 20,000
r 0
r 0
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Capacitors
● Time constant for charging or discharging a capacitor in series with a resistor is = RC; R is the resistance of the circuit
● When charged, the energy stored in a capacitor is (½) Q V = (½) C V
● The energy stored can be large; supercapactiors store enough energy to power a hybrid car
● Small capacitors are used in circuits to tune oscillations and give controlled time delays
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Breakdown potential or dielectric strength
● Units V/m (Typically, MV/m)● The electrical gradient at which an insulator
breaks down and a damaging surge of current flows through it
● Measured by increasing, at a uniform rate, a 60 Hz alternating potential applied across the faces of a plate of the material until breakdown occurs
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Dielectric properties
Time
Vol
tage
, V a
nd C
urre
nt, i
Oscillating Charge, + Qh
f
i
V
Dielectric loss tangent: tan
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Loss tangent or loss factor
● Polarization involves the small displacement of charge (either of electrons or of ions) or molecules that carry a dipole moment when an electric field is applied to the material
● Alternating field – drives the charge between two alternating configurations
● Charge motion – like an electric current which is out of phase with the voltage – by 90 degrees if there were no losses
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Loss tangent● In real dielectric, current dissipates energy –
giving it a small phase shift ● The loss tangent, tan (or the dissipation factor,
D) is the tangent of the loss angle● The power factor is the sine of the loss angle● When the angle is small, all three, namely,
dissipation factor, power factor, and loss angle are the same
● Loss factor – loss tangent times the dielectric constant
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Loss factor● Loss factor – loss tangent times the dielectric
constant● Measure of energy dissipated in a dielectric
when in an oscillating field● Selection of materials that extremise dielectric
loss – L = tan is the measure r
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Power dissipation● Place a dielectric in a cycle of electric field of
amplitude E and frequency f● A power P is dissipated and the field is
correspondingly attenuated● Power dissipated per unit volume (P) is f E L● This power appears as heat and is generated
uniformly throughout the material● Higher the frequency or field strength, higher
the heating● Radiofrequency welding of polymers
2
0
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Electrostriction and piezoelectricity
● All dielectrics change shape in an electric field; consequence of the small shift in charge that allows them to polarize
● Electrostriction – one sided relationship between electric field and deformation
● Piezoelectric materials – twosided: electric field causes deformation and deformation induces charge differences between its surfaces, thus creating a field
● Piezoelectric – a true, linear effect
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Pyroelectric materials
● Contain molecules with permanent dipole moments that, in a single crystal, are aligned, giving the crystal permanent polarization
● With temperature, polarization changes – creating surface charges, or, if surfaces are connected, a pyorelectric current
● Principle of intruder detection systems and of thermal imaging
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Ferroelectric materials
● Materials with natural dipole moment● Dipole moment align – like magnetic moments
in a magnet● Direction of polarisation can be changed with
the application of electric fields● This change leads to a change of shape!