Exam
Written Qualifying Examination in APPLIED MATHEMATICS September 11, 1995
Fall 1995 · 12 questions in this exam.
Questions in This Exam
Ordered by the question sequence in the original exam.
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Question A1
Let \(A\) be a real \(m\times n\) matrix with adjoint \(A^*\).
- Prove that if \(R(A)\) and \(N(A)\) denote the range and nullspace of \(A\) respectively, then \[ R(A)\oplus N(A^*)=\mathbb {R}^m. \] (\(\oplus \) means orthogonal direct sum.)
- Using the result of (a), state and prove Fredholm’s Alternative Theorem.
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Question A2
Let \(A\) be a real \(m\times n\) matrix.
- Define the Least Square Pseudo-Inverse \(A'\).
- Show how Gaussian Elimination can be used to compute \(A'\).
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Question A3
Let \(S=\{\phi _1,\phi _2,\ldots ,\phi _n,\ldots \}\) be a countable orthonormal set in a Hilbert space \(\mathcal {H}\). Prove that \(S\) is a complete orthonormal set if and only if it is a maximal orthonormal set; i.e., there exists no unit vector \(\psi \) such that \(\{\psi ,\phi _1,\phi _2,\ldots ,\phi _n,\ldots \}\) is an orthonormal set.
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Question A4
Consider the integral equation \[ u(x)-\lambda\int_{-1}^{1}\sum_{j=0}^{2}P_j(x)P_j(t)u(t)\,dt=f(x), \qquad\text{for } -1\le x\le 1, \] where \(P_j(x)\) is the \(j\)th Legendre function. **(a)** For which values of \(\lambda\) does the integral equation have a unique solution? **(b)** Calculate this solution for the case that \(f(x)=x^2+1\).
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Question B1
Let \(f(x)\) be in the Hilbert space \(L^2(-\infty ,\infty )\). Construct and use a Green’s function to find the solution in \(L^2(-\infty ,\infty )\) of the equation \[ u''-\alpha ^2u=f(x),\qquad (\alpha >0). \]
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Question B2
Liouville’s theorem states that a bounded entire function \(f(z)\) must be a constant.
- Prove Liouville’s theorem.
- Use Liouville’s theorem to prove the Fundamental Theorem of Algebra: every polynomial \(P_n(z)\) of degree \(n\ge 1\) has a root.
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Question B3
- State and prove Jordan’s Lemma of complex function theory.
- Use Jordan’s Lemma and the residue theorem to prove the equation \[ \int _0^\infty \frac {\cos (x)}{x^2+a^2}\,dx=\frac {\pi e^{-a}}{2a} \] where \(a>0\).
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Question B4
Find the spectral representation of the delta function for the selfadjoint operator \(L\) in the Hilbert space \(L^2(0,1)\) defined by \[ Lu=-u'',\quad\text{for }0\le x\le 1 \] \[ u(0)=0,\qquad\text{and}\qquad u(1)+u'(1)=0. \] **Part C** Do two of the four problems.
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Question C1
The (generalized) Hilbert transform \(H\) of a periodic function \(f\) can be defined as follows: For any simply connected two-dimensional domain \(\Omega \), let \(\phi \) satisfy \(\nabla ^2\phi =0\) with \(\nabla \phi \cdot \mathbf {n}=f\) on \(\partial \Omega \). Then \(Hf=\nabla \phi \cdot \mathbf {t}\) on \(\partial \Omega \). (\(\mathbf {n}\) is the exterior unit normal, \(\mathbf {t}\) is the unit tangent vector.)
- Prove that \(H(Hf)=-f\).
- Find a relationship between the Fourier transform and the Hilbert transform, using a unit circle as the domain \(\Omega \).
- What is the Hilbert transform of \(f(x)=a\sin (x)+b\cos (2x)\)?
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Question C2
Using an integral representation for the \(n\)-th order Bessel function \(J_n(x)\), find the leading order asymptotic representation of \(J_n(x)\) for large positive \(x\).
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Question C3
The \(z\)-transform is defined on sequences in \(\ell ^2\) by \[ U(z)=\sum _{-\infty }^{\infty }u_nz^n, \] \[ u_n=\frac {1}{2\pi i}\int _C U(z)z^{-n-1}\,dz \] where the contour \(C\) is a closed contour enclosing the origin, and integration is counterclockwise. If \(z\) is restricted to lie on the unit circle then \(U(z)=U(e^{i\theta })=f(\theta )\).
- Find the relationship between the \(z\)-transform and the Fourier series representation of \(f(\theta )\).
- Use the \(z\)-transform to solve the system of equations \[ \frac {du_n}{dt}=\frac {1}{2h}(u_{n+1}-u_{n-1}) \] with \(u_n(0)=\delta _{n0}\).
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Question C4
The flux \(q\) of dilute chemicals in a solute is usually assumed to be governed by Fick's law, \(q=-D\nabla c\), where \(c\) is the concentration. In an electric field, if the chemical species is ionic, then the flux is given by the Nernst-Planck equation \(q=-D\nabla c-\mu c\nabla\phi\) where \(\phi\) is the potential of the electric field. **a)** Assuming the field \(\nabla\phi\) is constant, and is independent of the concentration of the ionic species, find an evolution equation governing the concentration \(c\) as a function of time. **b)** Suppose the concentrations at the two ends of a one dimensional domain are held fixed. Find the concentration as a function of time, starting from arbitrary initial conditions. Caution: The spatial operator is not self-adjoint! A transformation of the form \(c(x,t)=e^{\alpha x}u(x,t)\) is helpful.