Accumulate the Nectar and Wait for Blossoming
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∇×B⃗−1c∂E⃗∂t=4πcj⃗∇⋅E⃗=4πρ∇×E⃗+1c∂B⃗∂t=0⃗∇⋅B⃗=0\begin{array}{c} \nabla \times \vec{\mathbf{B}} -\, \frac1c\, \frac{\partial\vec{\mathbf{E}}}{\partial t} & = \frac{4\pi}{c}\vec{\mathbf{j}} \nabla \cdot \vec{\mathbf{E}} & = 4 \pi \rho \\ \nabla \times \vec{\mathbf{E}}\, +\, \frac1c\, \frac{\partial\vec{\mathbf{B}}}{\partial t} & = \vec{\mathbf{0}} \\ \nabla \cdot \vec{\mathbf{B}} & = 0 \end{array}∇×B⃗−c1∂t∂E⃗∇×E⃗+c1∂t∂B⃗∇⋅B⃗=c4πj⃗∇⋅E⃗=0⃗=0=4πρ
