Problem Sets
Problem Set 1 (due Sep. 12)
- Chapter 1, Prob 1a, 1b.
- Chapter 1, Prob 2b, 2d, 2e.
- Express the general solution of
$(\dfrac{d^{3}}{dx^{3}}-)y=e^{-e^{x}}$
with incomplete Gamma fuctions.
Problem Set 2 (due Sep. 19)
-
Consider the wave equation for an electron
$i\dfrac{\partial\Psi}{\partial t}-\dfrac{\partial^{2}\Psi}{\partial x^{2}}=U\Psi,$
where $\Psi=\Psi(x,t)$ is the wavefunction of the electron and $U=U(x,t)$ is the potential.
Let the initial condition be
$\Psi(x,0)=f(x).$
Use the Green function method to convert the wave equation into an integral equation.
-
Let $y$ satisfy the equation
$y"+x^{2}y=0$
and the initial conditions $y(x_{0})=1,$ $y^{\prime}(x_{0})=0$
where $x_{0}>0.$
- Find the WKB approximation of $y(x)$ for $x>x_{0}$. For what values of $x$ do you expect it be a good approximation?
- Use the computor to obtain the numerical values of $y(x)$ as a function of $x$ for $x_{0}=1,5,10.$ Compute also the numerical values of the WKB approximation of $y(x)$. Compare the computor result with the approximate result.
Problem Set 3 (due Sep. 26)
- Problem 4 in Chapter 7.
Problem Set 4 (due Oct. 3)
- Problem 10 in Chapter 7.
-
Find the leading term for the following integrals for $\lambda>>1$:
- $\int_{0}^{\pi/2}e^{-\lambda\cos t}dt,$
- $\int_{-1}^{1}e^{\lambda t^{5}}dt,$
- $\int_{-\infty}^{\infty}e^{\lambda(x^{2}-x^{4})}dx.$
Use the computer to evalaute the numerical values of these integrals and compare them with the numerical values of their leading terms as a function of $\lambda.$
Problem Set 5 (due Oct. 12)
Compute the leading asymptotic term of the following integrals:
- $I(\lambda)=\int_{0}^{\infty}e^{-\lambda x}e^{-1/x^{3}}dx,$
- $I(\lambda)=\int_{0}^{\infty}e^{-\lambda\sqrt{1+x}}xdx,$
where $\lambda$ is very large.
Find the leading term for each of the following integrals when $\lambda>>1:$
- $\int_{0}^{\pi}e^{i\lambda\sin x}dx,$
- $\int_{-2}^{2}e^{i\lambda/(1+x^{2})}dx,$
Problem Set 6 (due Oct. 19)
-
- Determine the unshaded regions of $f(z)=e^{iz^{5}}$ in the infinity of which $f(z)$ vanishes.
- Express $J\equiv\int_{-\infty}^{\infty}e^{ix^{5}}dx$ by Gamma functions.
- Find the values of $\int_{-\infty}^{\infty}\cos x^{5}$ $dx$ and $\int_{-\infty}^{\infty}\sin x^{5}$ $dx.$
- Problem 4a in Chapter 2.
Problem Set 7 (due Oct. 24)
- Problem 4a in Chapter 2.
- Evaluate $I=\int_{0}^{\infty}\dfrac{\cos x}{1+x^{2}}dx.$
-
Find the leading asymptotic form of the integral
$I(\lambda)=\int_{-\infty}^{\infty}e^{i\lambda x}e^{ix^{3}/3}dx,$ $\ \lambda>>1.$
Compare this asymptotic form with the numerical value of the integral.
Problem Set 8 (due Oct. 31)
-
Find the leading asymptotic form of the integral
$I(\lambda)=\int_{-\infty}^{\infty}e^{i\lambda(x-x^{5}/5)}dx,$
$\lambda>>1.$
-
Find the leading asymptotic form of the integral
$I(\lambda)=\int_{-\infty}^{\infty}e^{i\lambda(x+x^{5}/5)}dx,$
$\lambda>>1.$
- Prob 1 of Chapter 8.
Problem Set 9 (due Nov. 7)
-
Let $I(\lambda)=\int_{0}^{\infty}\dfrac{e^{i\lambda x-1/x}}{1+x}dx,$ $ \lambda>>1.$
- Calculate the leading term of this integral by evaluating the contribution from the relevant saddle point.
- Justify your result by deforming the contour of integration into one on which the integrand is the largest at the saddle point.
-
Find both $y_{in}$ and $y_{out}$ for the equation
$\epsilon y^{"}-y^{\prime}+(1+x^{3})y=0,$ $0$<$x$<$1,$ $y(0)=1,$ $y(1)=3.$
It is assumed that $\epsilon$<<$1.$ Where is the boundary layer and what is its width?
- Find the next-order term for the problem above.
Problem Set 10 (due Nov. 21)
-
Solve approximately $\epsilon y^{\prime\prime}+(3\sin x)y^{\prime}+(\cos x)y=0,0$ < $x$ < $1$. The boundary conditions are
$y(0)=1,y(1)=3.$
-
Solve the differential equation in Problem 1 which holds for $-1$ < $x$ < $1$. The boundary conditions are
$y(-1)=1,y(1)=3.$
-
Solve approximately $\epsilon y^{\prime\prime}-2xy^{\prime}+(1+x^{4})y=0,0$ < $x$ < $1$. The boundary conditions are
$y(0)=1,y(1)=3.$
-
Solve approximately the differential equation in Problem 3 which holds for $-2$ < $x$ < $1.$ The boundary conditions are
$y(-2)=1,y(1)=3.$
Problem Set 11 (due Dec. 5 - turn into grader's office 2-333C by the end of the day)
-
Consider the equations
$\overset{\cdot\cdot}{x}+\omega_{0}^{2}x=-\dfrac{\epsilon}{3}(x+y)^{3},$
$\overset{\cdot\cdot}{y}+W_{0}^{2}y=-\dfrac{\epsilon}{3}(x+y)^{3}.$
The initial conditions are $x(0)=2a,$ $y(0)=2A,$ $\overset{\cdot}{x}(0)=\overset{\cdot}{y}(0)=0.$
Find an approximate solution of this problem valid for $t$ much less than $O(\epsilon^{-2})$.