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Most beautiful equations
2 minutes
physics
maths
philosophy
aesthetics
Intermediate
anybody
Euler's identity
e
i
π
+
1
=
0
e^{i\pi} + 1 = 0
e
iπ
+
1
=
0
Einstein's mass-energy equivalence
E
=
m
c
2
E = mc^2
E
=
m
c
2
The general wave equation
∂
2
u
∂
x
2
−
1
c
2
∂
2
u
∂
t
2
=
0
\frac{\partial^2 u}{\partial x^2} - \frac{1}{c^2} \frac{\partial^2 u}{\partial t^2} = 0
∂
x
2
∂
2
u
−
c
2
1
∂
t
2
∂
2
u
=
0
Maxwell's equations
Gauss’s law for electricity
∇
⋅
E
=
ρ
ε
0
Gauss’s law for magnetism
∇
⋅
B
=
0
Faraday’s law of induction
∇
×
E
=
−
∂
B
∂
t
Ampere’s law with Maxwell’s addition
∇
×
B
=
μ
0
J
+
μ
0
ε
0
∂
E
∂
t
\begin{gather} \text{\footnotesize Gauss's law for electricity} \nonumber \\ \nabla \cdot \mathbb{E} = \frac{\rho}{\varepsilon_0} \nonumber \\ \text{\footnotesize Gauss's law for magnetism} \nonumber \\ \nabla \cdot \mathbb{B} = 0 \nonumber \\ \text{\footnotesize Faraday's law of induction} \nonumber \\ \nabla \times \mathbb{E} = -\dfrac{\partial \mathbb{B}}{\partial t} \nonumber \\ \text{\footnotesize Ampere's law with Maxwell's addition} \nonumber \\ \nabla \times \mathbb{B} = \mu_0 \mathbb{J} + \mu_0 \varepsilon_0 \dfrac{\partial \mathbb{E}}{\partial t} \nonumber \\ \end{gather}
Gauss’s law for electricity
∇
⋅
E
=
ε
0
ρ
Gauss’s law for magnetism
∇
⋅
B
=
0
Faraday’s law of induction
∇
×
E
=
−
∂
t
∂
B
Ampere’s law with Maxwell’s addition
∇
×
B
=
μ
0
J
+
μ
0
ε
0
∂
t
∂
E
Shrodinger' wave equation
−
ℏ
2
2
m
∂
2
ψ
∂
x
2
=
i
ℏ
∂
ψ
∂
t
-\dfrac{\hbar^2}{2m}\dfrac{\partial^2\psi}{\partial x^2 }= i\hbar\dfrac{\partial \psi}{\partial t}
−
2
m
ℏ
2
∂
x
2
∂
2
ψ
=
i
ℏ
∂
t
∂
ψ