Tag Archives: curve

Some special solutions to curve shortening flow

Consider {\boldsymbol{\gamma}(p,t)} is a closed curve in {\mathbb{R}^2} which moves by its curvature. More preciesly, let

\displaystyle \partial_t\boldsymbol{\gamma}(p,t)=\kappa \mathbf{N}

where {\mathbf{N}} is the unit normal pointing to the inside of the region inscribed by the curve. Such a flow is curve shortening flow. We are interested in some particular (convex, graphical) solutions of the flow.

Suppose {\boldsymbol{\gamma}} locally can written as a graph, say {\boldsymbol{\gamma}=(x,u(x,t))}. Then the flow equation means

\displaystyle u_t=\frac{u_{xx}}{1+u_x^2}

Consider {u(x,t)=g(\lambda t+f(x))} in particular, where {\lambda} is a constant. Then we can decouple the equation into two differential equations.

\displaystyle f''+\mu f'^2-\lambda=0,

\displaystyle g''-\lambda g'^3-\mu g'=0.

where {\mu} is a constant. Depending on the values of {\lambda} and {\mu}, one can have the following four cases

(1) {\lambda=0}, {\mu=0}. Then {u(x,t)=ax} and {\boldsymbol{\gamma}} is actually a static line.

(2) {\lambda\neq 0}, {\mu=0}. Then one can choose {f=\frac{1}{2}\lambda x^2} and {g(x)=\frac{1}{2}\sqrt{\frac{x}{-2\lambda}}}. In this case

\displaystyle u^2+\frac{1}{4}x^2=-\frac{1}{2}t

{\boldsymbol{\gamma}} is a circle.

(3) {\lambda\mu<0}. Say {\lambda=-1} and {\mu=1}. Then one can solve the ODE to get {f(x)=\log\cos x} and {g(x)=const}, {\sinh^{-1}(e^x)}, {\pm \cosh^{-1}(e^x)}. They corresponds to grim reaper, hair clip and paper clip (Angenent oval) respectively.

u=\log\cos x-t

\sinh u=e^{-t}\cos x,\quad \cosh u=e^{-t}\cos x

(4) {\lambda\mu>0}. This can be reduced to (3) by writing 

\displaystyle y=u(x,t),\quad v(y,t)=f^{-1}(-\lambda t+g^{-1}(y)).

K. Nakayama, T. Iizuka, M. Wadati, Curve Lengthing equation and its solutions, J. Phys. Soc. Japan. 63 (1994) 1311-1321.

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