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Magnetic field around a long straight conductor
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Magnetic field in long straight coil
B
=
μ
r
μ
0
N
⋅
I
l
B=\frac{\mu_r\mu_0N\cdot I}{l}
B
=
l
μ
r
μ
0
N
⋅
I
Induced Voltage
u
i
n
d
=
−
d
Φ
m
d
t
u_{ind}=-\frac{d\Phi_m}{dt}
u
in
d
=
−
d
t
d
Φ
m
Self induction in coil
u
i
n
d
=
−
L
⋅
d
i
d
t
u_{ind}=-L\cdot\frac{di}{dt}
u
in
d
=
−
L
⋅
d
t
d
i
Energy in coil
w
=
L
⋅
I
2
2
w=\frac{L\cdot I^2}{2}
w
=
2
L
⋅
I
2
Angular frequency
ω
=
2
π
⋅
f
=
2
π
T
\omega=2\pi\cdot f=\frac{2\pi}{T}
ω
=
2
π
⋅
f
=
T
2
π
Instantaneous value, alternating voltage
u
=
u
^
⋅
s
i
n
(
ω
t
+
α
)
u=\hat{u}\cdot sin(\omega t +\alpha)
u
=
u
^
⋅
s
in
(
ω
t
+
α
)