O que dizer sobre.
i ℏ ∂ ψ ∂ t = − ℏ 2 2 m ∂ 2 ψ ∂ x 2 {\displaystyle i\hbar {\partial \psi \over \partial t}={\frac {-\hbar ^{2}}{2m}}{\partial ^{2}\psi \over \partial x^{2}}}
i ℏ ∂ ψ ∂ t = − ℏ 2 2 m ∂ 2 ψ ∂ x 2 + V ψ {\displaystyle i\hbar {\partial \psi \over \partial t}={\frac {-\hbar ^{2}}{2m}}{\partial ^{2}\psi \over \partial x^{2}}+V\psi }
F = m a = m d 2 x d t 2 = − ∂ V ∂ x {\displaystyle F=ma=m{d^{2}x \over dt^{2}}=-{\partial V \over \partial x}}
