フィックの第2法則(拡散方程式):
$$\frac{\partial C}{\partial t}= D \frac{\partial^2 C}{\partial x^2}$$半無限体解(erfc):
$$\frac{C - C_0}{C_s - C_0}= \text{erfc}\!\left(\frac{x}{2\sqrt{Dt}}\right)$$有限スラブ解(フーリエ級数):
$$\frac{C - C_0}{C_s - C_0}= 1 - \sum_{n=0}^{\infty}\frac{4(-1)^n}{(2n+1)\pi}\exp\!\left(-\frac{(2n+1)^2\pi^2 Dt}{4L^2}\right)\cos\!\left(\frac{(2n+1)\pi x}{2L}\right)$$表面フラックス:$J_0 = -D\left.\dfrac{\partial C}{\partial x}\right|_{x=0}= (C_s-C_0)\sqrt{\dfrac{D}{\pi t}}$