Dielectrics_2

K
Dielectrics 
Prof. V. Krishnakumar 
Professor and Head 
Department of Physics 
Periyar University 
Salem – 636 011
Introduction 
• Dielectric materials: high electrical resistivities, but 
an efficient supporter of electrostatic fields. 
• Can store energy/charge. 
• Able to support an electrostatic field while 
dissipating minimal energy in the form of heat. 
• The lower the dielectric loss (proportion of energy 
lost as heat), the more effective is a dielectric 
material. 
• Another consideration is the dielectric constant, 
the extent to which a substance concentrates the 
electrostatic lines of flux.
Capacitance 
• Two electrodes separated by a gap 
define a capacitor. 
• When a bias is applied across the 
capacitor plates, one charges positively, 
the other negatively. 
• The amount of charge that the capacitor 
can store (Q) is proportional to the bias 
(V) times how good the capacitor is, the 
‘capacitance’ (C). 
• The capacitance is related to the area of 
the plates (A), their separation (d), and 
the Dielectric Constant (εεo) of the 
dielectric between the plates 
• Dielectric constant of vacuum; εo = 
8.85x10-12 F/m=55.2 Me/(V*m) 
d 
A 
C o 
 
 
e 
 o  * 
V  
e 
 m 
m 
V 
d 
A 
Q V m 
* 2 
 *
Why does charge built up? 
There is generally not a built-in electric field between the 
plates of an unbiased capacitor. 
When an electric field is applied, any charged carriers or 
species within the material will respond. 
For a conductor or semiconductor, e- will flow to the + 
plate, and possibly also holes will flow to the - plate. 
Current is carried=no charge buildup. 
For an insulator, there aren’t a significant number of free 
carriers. There are highly ionic species, however, but they 
aren’t very mobile at low temperatures. No appreciable 
current is carried=charge buildup.
Polarization in Insulators 
Positively charged species in insulators shift/rotate/align toward the 
negative electrode and negatively charged species shift/rotate/align 
towards the positive electrode; creating dipoles. The dipole moment 
density is termed the Polarization (P) and has the units of C/m2. 
Electron Cloud Electron Cloud 
+ 
+ 
- 
E 
Electronic polarization, occurs 
in all insulators 
- 
- - 
+ - + 
- 
+ + 
+ + 
E 
Ionic polarization occurs 
in all ionic solids: NaCl, 
MgO… 
- 
- 
- 
+ + 
E 
Molecular polarization, occurs 
in all insulating molecules; 
oils, polymers, H2O… 
Electric Dipole Moment 
p  q x 
Polarization 
q 
A 
p 
P   
V
Dielectric Effects 
Metal plates 
Dielectric 
A 
d 
C 
 
 
What makes  different from 0? 
POLARIZATION 
  
  
  1 
 
 
0 
r 
r 
In electrostatics, the CONSTITUITIVE RELATION is 
D E E P 
    
 Polarization 
P E 
0 
0 
 
 
Susceptibility
Dielectric Effects 
POLARIZATION arises from charge shifts in the material— 
there is a macroscopic separation of positive charge (e.g., the 
ions) and negative charge (e.g., the BONDING ELECTRONS). 
Induced DIPOLE MOMENT 
POLARIZATION is then 
di  q  x0 
There are many sources of dipoles. 
Amount of charge shift 
P  Ndipolesdi
Definitions 
•Permittivity is a physical quantity 
that describes how an electric field 
affects and is affected by a dielectric 
medium and is determined by the 
ability of a material to polarize in 
response to an applied electric field, 
and thereby to cancel, partially, the 
field inside the material. Permittivity 
relates therefore to a material's ability 
to transmit (or "permit") an electric 
field…The permittivity of a material 
is usually given relative to that of 
vacuum, as a relative permittivity, 
(also called dielectric constant in 
some cases)….- Wikipedia 
Dk 
Df 
 ' 
 
" 
r r
Permittivity and Permeability Definitions 
(Dielectric Constant) 
' " 
 
Permittivity 
     
 
0 
r r r   j 
•interaction of a material in the 
presence of an external electric 
field.
Permittivity and Permeability Definitions 
(Dielectric Constant) 
' " 
 
Permittivity 
     
 
0 
r r r   j 
•interaction of a material in the 
presence of an external electric 
field. 
Dk
Permittivity and Permeability Definitions 
 
    '  " 
' " 
 
 
0 
r r r   j 
•interaction of a material in the 
presence of an external electric 
field. 
    
0 
r jr 
 
interaction of a material in the 
presence of an external magnetic field. 
Permittivity 
(Dielectric Constant) 
Permeability 
Dk
Permittivity and Permeability Definitions 
 
    '  " 
' " 
 
 
0 
r r r   j 
•interaction of a material in the 
presence of an external electric 
field. 
    
0 
r jr 
 
interaction of a material in the 
presence of an external magnetic field. 
Permittivity 
(Dielectric Constant) 
Permeability 
Dk
STORAGE 
Electric Magnetic 
Fields Fields 
Permittivity Permeability 
' " 
Electromagnetic Field Interaction 
MUT 
r r  jr ' " 
 r  r  j r 
STORAGE
STORAGE 
Electric Magnetic 
Fields Fields 
LOSS 
Permittivity Permeability 
' " 
Electromagnetic Field Interaction 
MUT 
r r  jr ' " 
 r  r  j r 
STORAGE 
LOSS
Loss Tangent 
" 
 
r 
 
' 
tan 
r 
  
r  
' 
r  
'' 
r  
Energy Lost perCycle 
Energy Stored perCycle 
1 
 D   
Q 
tan 
Dissipation Factor D Quality Factor Q 
Df
Relaxation Constant t 
t = Time required 
for 1/e of an aligned 
system to return to 
equilibrium or 
random state, in 
seconds. 
1 1 
c fc 
t 
2 
  
100 
1 
1 
10 
Water at 20o C 
10 100 
f, 
GHz 
most energy is lost at 1/t 
' 
r  
" 
 r 
  
t 
   
j 
s 
 
 
   
 1 
Debye equation : ( )
Dielectric Effects 
 s  static 
   optical 
0 ln()  
P LO 
30-50 meV 10-15 eV 
visible 
infrared 
Major source of POLARIZATION 
is distortion of the bonding 
electrons around atoms. This 
leads to the normal 
semiconductor dielectric 
constant. 
In POLAR materials, like 
GaAs and SiC, the different 
charge on the A and B atoms 
can be polarized as well, 
leading to a difference 
between the optical and the 
static dielectric constants. 
In Appendix C, the two values for GaAs are reversed!
Dielectrics_2
Dielectrics_2
Definition: 
A photonic crystal is a periodic arrangement 
of a dielectric material 
that exhibits strong interaction with light
Dielectrics_2
Dielectrics_2
Piezoelectric Effect 
In materials with NO REFLECTION SYMMETRY (like GaAs or 
many molecular species) the applied electric field produces a 
DISTORTION OF THE LATTICE (size change) and vice versa. 
FORCE 
ELECTRIC FIELD 
A common piezoelectric is Poly-Vinylidene Flouride, which is 
used in a variety of stereo headsets. The most common is 
crystalline quartz used as frequency control crystals—pressure 
applied to the quartz has a resonance which can be used in a 
feedback loop to create a highly-stable oscillator—the quartz 
crystal oscillator.
Dielectrics_2
Dielectrics_2
Phase sensitive multimeter interfaced 
with impendence analyzer for dielectric 
measurements
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Dielectrics_2

  • 1. Dielectrics Prof. V. Krishnakumar Professor and Head Department of Physics Periyar University Salem – 636 011
  • 2. Introduction • Dielectric materials: high electrical resistivities, but an efficient supporter of electrostatic fields. • Can store energy/charge. • Able to support an electrostatic field while dissipating minimal energy in the form of heat. • The lower the dielectric loss (proportion of energy lost as heat), the more effective is a dielectric material. • Another consideration is the dielectric constant, the extent to which a substance concentrates the electrostatic lines of flux.
  • 3. Capacitance • Two electrodes separated by a gap define a capacitor. • When a bias is applied across the capacitor plates, one charges positively, the other negatively. • The amount of charge that the capacitor can store (Q) is proportional to the bias (V) times how good the capacitor is, the ‘capacitance’ (C). • The capacitance is related to the area of the plates (A), their separation (d), and the Dielectric Constant (εεo) of the dielectric between the plates • Dielectric constant of vacuum; εo = 8.85x10-12 F/m=55.2 Me/(V*m) d A C o   e  o  * V  e  m m V d A Q V m * 2  *
  • 4. Why does charge built up? There is generally not a built-in electric field between the plates of an unbiased capacitor. When an electric field is applied, any charged carriers or species within the material will respond. For a conductor or semiconductor, e- will flow to the + plate, and possibly also holes will flow to the - plate. Current is carried=no charge buildup. For an insulator, there aren’t a significant number of free carriers. There are highly ionic species, however, but they aren’t very mobile at low temperatures. No appreciable current is carried=charge buildup.
  • 5. Polarization in Insulators Positively charged species in insulators shift/rotate/align toward the negative electrode and negatively charged species shift/rotate/align towards the positive electrode; creating dipoles. The dipole moment density is termed the Polarization (P) and has the units of C/m2. Electron Cloud Electron Cloud + + - E Electronic polarization, occurs in all insulators - - - + - + - + + + + E Ionic polarization occurs in all ionic solids: NaCl, MgO… - - - + + E Molecular polarization, occurs in all insulating molecules; oils, polymers, H2O… Electric Dipole Moment p  q x Polarization q A p P   V
  • 6. Dielectric Effects Metal plates Dielectric A d C   What makes  different from 0? POLARIZATION       1   0 r r In electrostatics, the CONSTITUITIVE RELATION is D E E P      Polarization P E 0 0   Susceptibility
  • 7. Dielectric Effects POLARIZATION arises from charge shifts in the material— there is a macroscopic separation of positive charge (e.g., the ions) and negative charge (e.g., the BONDING ELECTRONS). Induced DIPOLE MOMENT POLARIZATION is then di  q  x0 There are many sources of dipoles. Amount of charge shift P  Ndipolesdi
  • 8. Definitions •Permittivity is a physical quantity that describes how an electric field affects and is affected by a dielectric medium and is determined by the ability of a material to polarize in response to an applied electric field, and thereby to cancel, partially, the field inside the material. Permittivity relates therefore to a material's ability to transmit (or "permit") an electric field…The permittivity of a material is usually given relative to that of vacuum, as a relative permittivity, (also called dielectric constant in some cases)….- Wikipedia Dk Df  '  " r r
  • 9. Permittivity and Permeability Definitions (Dielectric Constant) ' "  Permittivity       0 r r r   j •interaction of a material in the presence of an external electric field.
  • 10. Permittivity and Permeability Definitions (Dielectric Constant) ' "  Permittivity       0 r r r   j •interaction of a material in the presence of an external electric field. Dk
  • 11. Permittivity and Permeability Definitions      '  " ' "   0 r r r   j •interaction of a material in the presence of an external electric field.     0 r jr  interaction of a material in the presence of an external magnetic field. Permittivity (Dielectric Constant) Permeability Dk
  • 12. Permittivity and Permeability Definitions      '  " ' "   0 r r r   j •interaction of a material in the presence of an external electric field.     0 r jr  interaction of a material in the presence of an external magnetic field. Permittivity (Dielectric Constant) Permeability Dk
  • 13. STORAGE Electric Magnetic Fields Fields Permittivity Permeability ' " Electromagnetic Field Interaction MUT r r  jr ' "  r  r  j r STORAGE
  • 14. STORAGE Electric Magnetic Fields Fields LOSS Permittivity Permeability ' " Electromagnetic Field Interaction MUT r r  jr ' "  r  r  j r STORAGE LOSS
  • 15. Loss Tangent "  r  ' tan r   r  ' r  '' r  Energy Lost perCycle Energy Stored perCycle 1  D   Q tan Dissipation Factor D Quality Factor Q Df
  • 16. Relaxation Constant t t = Time required for 1/e of an aligned system to return to equilibrium or random state, in seconds. 1 1 c fc t 2   100 1 1 10 Water at 20o C 10 100 f, GHz most energy is lost at 1/t ' r  "  r   t    j s       1 Debye equation : ( )
  • 17. Dielectric Effects  s  static    optical 0 ln()  P LO 30-50 meV 10-15 eV visible infrared Major source of POLARIZATION is distortion of the bonding electrons around atoms. This leads to the normal semiconductor dielectric constant. In POLAR materials, like GaAs and SiC, the different charge on the A and B atoms can be polarized as well, leading to a difference between the optical and the static dielectric constants. In Appendix C, the two values for GaAs are reversed!
  • 20. Definition: A photonic crystal is a periodic arrangement of a dielectric material that exhibits strong interaction with light
  • 23. Piezoelectric Effect In materials with NO REFLECTION SYMMETRY (like GaAs or many molecular species) the applied electric field produces a DISTORTION OF THE LATTICE (size change) and vice versa. FORCE ELECTRIC FIELD A common piezoelectric is Poly-Vinylidene Flouride, which is used in a variety of stereo headsets. The most common is crystalline quartz used as frequency control crystals—pressure applied to the quartz has a resonance which can be used in a feedback loop to create a highly-stable oscillator—the quartz crystal oscillator.
  • 26. Phase sensitive multimeter interfaced with impendence analyzer for dielectric measurements

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