Electrical Materials
Crystal structures, magnetic materials, dielectric properties, and insulating materials.
a) Crystal Structure
Atomic arrangements, unit cells, and packing efficiency
1. Crystal Structure: Fundamentals
Space Lattice$$ \text{Lattice} + \text{Basis} \rightarrow \text{Crystal structure} $$
Unit Cell Volume: $ V = \bar{a} \cdot \bar{b} \cdot \bar{c} $
2. Atom Counting in 3D Unit Cells
APF$$ N = N_c(\frac{1}{8}) + N_e(\frac{1}{4}) + N_f(\frac{1}{2}) + N_b(1) $$
$$ APF = \frac{N_{atoms} \times \frac{4}{3}\pi r^3}{a^3} \quad;\quad \text{Void} = 1 - APF $$
3. Simple Cubic (SC) Structure
Polonium$$ N = 1 \quad;\quad CN = 6 \quad;\quad r = \frac{a}{2} $$
$$ APF = \frac{\pi}{6} \approx 0.52 \quad (52\%) $$
4. Body Centred Cubic (BCC)
Na, Li, Cr$$ N = 2 \quad;\quad CN = 8 \quad;\quad r = \frac{\sqrt{3}}{4}a $$
$$ APF = \frac{\sqrt{3}\pi}{8} \approx 0.68 \quad (68\%) $$
5. Face Centred Cubic (FCC)
Al, Cu, Ag$$ N = 4 \quad;\quad CN = 12 \quad;\quad r = \frac{\sqrt{2}}{4}a $$
$$ APF = \frac{\sqrt{2}\pi}{6} \approx 0.74 \quad (74\%) $$
6. Unit Cell Properties Comparison
Diamond: 34% APF$$ DC(0.34) < SC(0.52) < BCC(0.68) < FCC(0.74) $$
Diamond Cubic (Ge, Si, C): $N=8$, $CN=4$, $r = \frac{\sqrt{3}}{8}a$
7. Miller Indices & Bragg's Law
Crystallographyd-spacing: $$ d_{hkl} = \frac{a}{\sqrt{h^2+k^2+l^2}} $$
Bragg's Law: $$ n\lambda = 2d\sin\theta $$
b) Magnetic Materials
Dipoles, domains, hysteresis, and magnetic classification
8. Magnetic Materials: Fundamentals
DipolesBiot-Savart: $ dB = \frac{\mu_0}{4\pi}\cdot\frac{Id\ell\sin\theta}{r^2} $
Ampere's Law: $ \oint \vec{H}\cdot d\vec{l} = I_{enc} $
Intensity: $ B = \mu_0(H + M) \quad;\quad M = \chi_m H $
9. Anisotropy & Magnetostriction
Physical ChangesMagnetostriction: $\Delta L/L$ vs applied $H$.
Villari Effect: Converse of magnetostriction (Stress $\rightarrow$ $\Delta B$).
10. Curie Temperature & Magnetic Laws
$T_c$ Phase TransitionParamagnetic (Curie's Law):
$$ \chi_m = \frac{C}{T} $$
Ferromagnetic ($T > T_C$):
$$ \chi_m = \frac{C}{T - \theta} $$
Anti-ferro ($T > T_N$):
$$ \chi_m = \frac{C}{T + \theta} $$
11. Types of Magnetic Materials
ClassificationDia ($\chi < 0$) | Para ($\chi > 0$) | Ferro ($\chi \gg 0$) | Anti-ferro ($\chi \approx 0$) | Ferri (large $\chi$)
12. Magnetization: Paramagnetic Materials
Langevin Function$$ M = N\mu_0\left(\coth\alpha - \frac{1}{\alpha}\right) = N\mu_0 L(\alpha) \quad;\quad \alpha = \frac{\mu_0 H}{k_B T} $$
Weak fields ($\alpha \ll 1$): $M = \frac{N\mu_0^2 H}{k_B T}$ | Strong fields ($\alpha \gg 1$): $M \rightarrow N\mu_0 = M_{sat}$
13. B-H Hysteresis Loop Terms
Energy Loss$$ B_r = \text{Retentivity} \quad;\quad H_C = \text{Coercivity} \quad;\quad W_{hyst} = \oint H\,dB $$
Steinmetz: $P_h = k_h f B_{max}^n$
c) Dielectric Materials
Polarization, permittivity, breakdown mechanisms, and dielectric loss
14. Internal Field in Solids & Liquids
Local FieldLorentz Field: $$ E_{int} = E + \frac{P}{3\varepsilon_0} $$
Clausius-Mossotti: $$ \frac{\varepsilon_r - 1}{\varepsilon_r + 2} = \frac{N\alpha}{3\varepsilon_0} \quad;\quad \varepsilon_r = n^2 $$
15. Types of Dielectric Materials
ClassificationTotal Polarizability: $$ \alpha_{total} = \alpha_e + \alpha_i + \alpha_d + \alpha_{space} $$
16. Piezoelectric, Ferroelectric & Pyroelectric
Active DielectricsPiezoelectric:
$$ P = dT \text{ (Direct)}, S = dE \text{ (Inverse)} $$
Ferroelectric:
$$ \varepsilon_r = \frac{C}{T - T_C} \text{ (Curie-Weiss)} $$
Pyroelectric: $$ \Delta P = \lambda \Delta T $$
17. Dielectric Properties Summary
Overview$$ \varepsilon_r = \frac{\varepsilon}{\varepsilon_0} \quad;\quad \chi_e = \varepsilon_r - 1 \quad;\quad P = \varepsilon_0\chi_e E $$
$$ D = \varepsilon_0 E + P = \varepsilon_0\varepsilon_r E $$
Loss Tangent: $$ \tan\delta = \frac{\varepsilon''}{\varepsilon'} \quad \rightarrow \quad \text{Loss} = \omega\varepsilon_0\varepsilon''\tan\delta\,E^2 $$
18. Anti-Ferroelectric & Breakdown in Gases
GasesAntiparallel alignment: $$ P_{net} = 0 $$ Examples: Lead zirconate, Sodium nitrate
Gas Mobility: $$ \bar{V} = \mu E $$ Townsend Criterion: $$ \gamma(e^{\alpha d}-1) = 1 $$
Paschen's Law: $$ V_{breakdown} = f(p \cdot d) $$
19. Dielectric Breakdown in Liquids
LiquidsBubble Theory: $$ E_b = \frac{3\varepsilon_L}{2\varepsilon_L+1}E_0 $$
Liquid Globule stability: $$ E = 487.7\sqrt{\frac{\sigma}{R\varepsilon_L}} \text{ V/cm} $$
20. Dielectric Breakdown in Solids
SolidsVon Hippel (Intrinsic): $$ E_c = \frac{2\pi\nu em}{h}\left(\frac{1}{n_c^2} - \frac{1}{\varepsilon}\right) $$
Thermal Power loss: $$ W = E^2 f \cdot \frac{\varepsilon_r\tan\delta}{1.8\times10^{10}} \text{ W/cm}^3 $$
21. Dielectric Loss & Complex Permittivity
LossesComplex Permittivity: $$ \varepsilon^* = \varepsilon' - j\varepsilon'' \quad;\quad \tan\delta = \frac{\varepsilon''}{\varepsilon'} $$
Power Loss: $$ P_{loss} = V^2\omega C\tan\delta \quad Q = \frac{1}{\tan\delta} $$
Debye: $$ \varepsilon' = \varepsilon_\infty + \frac{\varepsilon_s - \varepsilon_\infty}{1+\omega^2\tau^2} \quad \varepsilon'' = \frac{(\varepsilon_s - \varepsilon_\infty)\omega\tau}{1+\omega^2\tau^2} $$
22. Dielectric Strength & Energy Absorbed
StrengthEnergy Lost: $$ W(t) = \frac{\omega}{2}\varepsilon_0\varepsilon_r\tan\delta\,E_0^2 \text{ W/m}^3 $$
Dielectric Strength: $$ E_{bd} = \text{Max Field before Breakdown} $$ Mica: 200 kV/cm (Highest)
d) Insulating Materials
Properties, thermal classification, and material selection
23. Insulating Materials: Basics & Properties
InsulatorsNTC behavior: $$ dR/dT < 0 $$ (Resistance decreases as Temp increases)
Max Voltage: $$ V_{max} = E_{bd} \times d $$
24. Thermal Classification of Insulators
ThermalY (90ยฐ) < A,E (105ยฐ) < B (130ยฐ) < F (150ยฐ) < H (180ยฐ) < C (>180ยฐ)
Montsinger's Rule: $$ L_2 = L_1 \times 2^{-(T_2-T_1)/10} $$ (Life halves every 10ยฐC rise)
25. Classification of Insulating Materials
CategoriesSFโ (Sulphur Hexafluoride): $$ E_{bd} \approx 3 \times \text{Air} $$ (GIS Switchgear)
Organic/Inorganic | Natural/Synthetic | Solid, Liquid, Gas States