Paper 4, Section II, E

Partial Differential Equations | Part II, 2015

(a) Show that the Cauchy problem for u(x,t)u(x, t) satisfying

ut+u=uxxu_{t}+u=u_{x x}

with initial data u(x,0)=u0(x)u(x, 0)=u_{0}(x), which is a smooth 2π2 \pi-periodic function of xx, defines a strongly continuous one parameter semi-group of contractions on the Sobolev space Hper sH_{\text {per }}^{s} for any s{0,1,2,}s \in\{0,1,2, \ldots\}.

(b) Solve the Cauchy problem for the equation

utt+ut+14u=uxxu_{t t}+u_{t}+\frac{1}{4} u=u_{x x}

with u(x,0)=u0(x),ut(x,0)=u1(x)u(x, 0)=u_{0}(x), u_{t}(x, 0)=u_{1}(x), where u0,u1u_{0}, u_{1} are smooth 2π2 \pi-periodic functions of xx, and show that the solution is smooth. Prove from first principles that the solution satisfies the property of finite propagation speed.

[In this question all functions are real-valued, and

Hper s={u=mZu^(m)eimxL2:uHs2=mZ(1+m2)su^(m)2<}H_{\text {per }}^{s}=\left\{u=\sum_{m \in \mathbb{Z}} \hat{u}(m) e^{i m x} \in L^{2}:\|u\|_{H^{s}}^{2}=\sum_{m \in \mathbb{Z}}\left(1+m^{2}\right)^{s}|\hat{u}(m)|^{2}<\infty\right\}

are the Sobolev spaces of functions which are 2π2 \pi-periodic in xx, for s=0,1,2,]s=0,1,2, \ldots]

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