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Physics Resonance: Problem set 23 -->

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Thursday, 10 November 2016

Problem set 23

  1. A diode D as shown in the circuit has an i-V relation that can be approximated by \begin{align*} i_{_D}=\begin{cases} v^2_{_D}+2v_{_D},&\text{for }v_{_D}>0\\ 0,&\text{for }v_{_D}\leq 0 \end{cases} \end{align*}
    The value of v_{_D} in the circuit is
    1. (-1+\sqrt{11})
    2. 8V
    3. 5V
    4. 2V
  2. The Taylor expansion of the function \ln{(\cosh x)}, where x is real, about the point x= 0 starts with the following terms:
    1. -\frac{1}{2}x^2+\frac{1}{12}x^4+\cdots
    2. \frac{1}{2}x^2-\frac{1}{12}x^4+\cdots
    3. -\frac{1}{2}x^2+\frac{1}{6}x^4+\cdots
    4. \frac{1}{2}x^2+\frac{1}{6}x^4+\cdots
  3. Given 2\times2 unitary matrix U satisfying U^\dagger U=UU^\dagger = 1 with \det U = e^{i\phi}, one can construct a unitary matrix V \:( V^\dagger V = VV^\dagger= 1) with \det V=1 from it by
    1. multiplying U by e^{i\phi/2}
    2. multiplying any single element of U by e^{i\phi}
    3. multiplying any row or column of U by e^{i\phi/2}
    4. multiplying U by e^{i\phi}
  4. The value of the integral \int_C \frac{z^3dz}{z^2-5z+6}, where C is a closed contour defined by the equation 2|z|- 5 = 0, traversed in the anti-clockwise direction, is
    1. -16\pi i
    2. 16\pi i
    3. 8\pi i
    4. 2\pi i
  5. The function f(x) obeys the differential equation \frac{d^2f}{dx^2}-(3 - 2i)f = 0 and satisfies the conditions f(0) = 1 and f(x)\rightarrow \infty as x\rightarrow 0. The value of f(\pi) is
    1. e^{2\pi}
    2. e^{-2\pi}
    3. -e^{-2\pi}
    4. -e^{2\pi i}

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