k is the proportionality constant in Coulomb's law, and is sometimes known as Coulomb's constant.
ε 0 = 8.85 x 10 -12 C 2 / Nm 2
ε 0 is a constant known as the permittivity of free space, which is the absolute value of the dielectric permittivity of a vacuum.
ε 0 is a constant known as the permittivity of free space, which is the absolute value of the dielectric permittivity of a vacuum.
F 12 = (k Q 1 Q 2 )/ r 2 12
Coulomb force law, inverse square law between objects 1 and 2 with a given charge a s a function of distance squared. Can be both attractive and repulsive in nature.
Coulomb force law, inverse square law between objects 1 and 2 with a given charge a s a function of distance squared. Can be both attractive and repulsive in nature.
E = Q r / (4 π ε 0 r 2 )
Electric field due to a point charge, written with ε 0 as opposed to using constant k.
Electric field due to a point charge, written with ε 0 as opposed to using constant k.
Dipole field
E = [3 ( p . r ) r - p] / (4 π ε 0 r 3 ) - [p δ 3 (r)] / (3 ε 0 )
In one direction along or perpendicular to dipole axis
E = p / (2 π ε 0 x 3 )
Energy and Torque on a dipole in an external E-field
U = - p . E , τ = p x E
Electric field of infinite line of charge:
E = λ / (2 π ε 0 r)
Where λ is defined as the charge per unit length.
E = λ / (2 π ε 0 r)
Where λ is defined as the charge per unit length.
Electric field of infinite charged plane:
E = σ / (2 ε 0 )
Where σ is defined as the charge per unit area.
E = σ / (2 ε 0 )
Where σ is defined as the charge per unit area.
Electric field of ring along axis:
E = Q x / [ 2 π ε 0 r (x 2 + a 2 ) 3/2 ]
E = Q x / [ 2 π ε 0 r (x 2 + a 2 ) 3/2 ]
Electric field of disk along axis
E = σ / 2 ε 0 [ 1 - z / (z 2 + R 2 ) 1/2 ]
E = σ / 2 ε 0 [ 1 - z / (z 2 + R 2 ) 1/2 ]
Electric flux:
Φ = E . A ;
dΦ = E . dA ; Φ = ∫ E . dA
Φ = E . A ;
dΦ = E . dA ; Φ = ∫ E . dA
Gauss's Law:
§ E . dA = Q enc / ε 0
Potential energy
U ab = U b - U a = -W ab = - ∫ F . dl ;
V ab = V b - V a = - ∫ E . dl ; V = k Q / r ; V = k ∫ dq / r ; E l = - dV / dl
E x = - dV / dx
U 12 = k Q 1 Q 2 / r 12
V ab = V b - V a = - ∫ E . dl ; V = k Q / r ; V = k ∫ dq / r ; E l = - dV / dl
E x = - dV / dx
U 12 = k Q 1 Q 2 / r 12
Capacitors
Q = C V
Parallel plate
Q = ε 0 A / d
U = Q 2 / 2 C
C = K C 0
ε = K ε 0
C = C 1 + C 2
1/C = 1/C2 + 1/C3
U = Q 2 / 2 C
C = K C 0
ε = K ε 0
C = C 1 + C 2
1/C = 1/C2 + 1/C3
Ohm's law
I = V/R = Δ Q / Δ t
Resistivity
ρ = ρ 0 [ 1 + α (T - T 0 )]
Power
P = VI = V 2 / R = I 2 R
The basic relation P = VI was transformed to the other two states by using Ohm's law.
The basic relation P = VI was transformed to the other two states by using Ohm's law.
Alternating Current
V = V 0 sin ω t
P = V 2 0 sin 2 (ω t) / R
P avg = V 2 0 / (2 R)
P = V 2 0 sin 2 (ω t) / R
P avg = V 2 0 / (2 R)
Current density
j = I/A = n e v drift = E / ρ
e = -1.6 x 10 -19 C
e = -1.6 x 10 -19 C
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