USAPhO 1997, Полуфинал — Задача 1. A1

United States Physics Team — 1997 Exam 2

Указания

Entia non multiplicanda sunt praeter necessitatem

DO NOT OPEN THIS TEST UNTIL YOU ARE TOLD TO BEGIN

  1. Please show all work, and do not hesitate to use explanatory words in addition to equations. Partial credit will be awarded.

  2. Begin each problem on a fresh sheet of paper. In the upper right-hand corner of each page, write your name, problem number, and the page number/total number of pages for this problem (e.g., "A2, 3/4" for "Problem A2, page 3 of four").

  3. You may use a non-programmable calculator, but may not use any tables, books, notes, or collections of formulas.

  4. Work Part A first. You have ninety minutes to complete all four problems.

  5. After you have completed Part A, you may take a break.

  6. Then work Part B. You have 90 minutes to complete both problems.

Possibly useful information:

Gravitational field on Earth’s surface: g=9.8 N/kgg = 9.8\ \mathrm{N/kg}

Gravitational constant: G=6.67×10−11 N-m2/kg2G = 6.67\times10^{-11}\ \mathrm{N\text{-}m^2 / kg^2}

Coulomb constant: k=1/4πϵo=8.99×109 N-m2/C2k = 1 / 4\pi\epsilon_o = 8.99\times10^{9}\ \mathrm{N\text{-}m^2 / C^2}

Speed of light in vacuum: c=3.00×108 m/sc = 3.00\times10^{8}\ \mathrm{m/s}

Permeability of empty space: μo\mu_o, where μoϵo=1/c2\mu_o\epsilon_o = 1/c^2

Ideal gas constant R=8.31 J/mol-KR = 8.31\ \mathrm{J / mol\text{-}K}

Boltzmann’s constant: kB=1.38×10−23 J/Kk_B = 1.38\times10^{-23}\ \mathrm{J/K}

Avagadro’s number: NA=6.02×1023N_A = 6.02\times10^{23}

1 electron volt = 1 eV=1.60×10−19 J1\ \mathrm{eV} = 1.60\times10^{-19}\ \mathrm{J}

Planck’s constant: h=6.63×10−34 J-s=4.14×10−15 eV-sh = 6.63\times10^{-34}\ \mathrm{J\text{-}s} = 4.14\times10^{-15}\ \mathrm{eV\text{-}s}

(1−x)−1=1+x+x2+x3+…(1 - x)^{-1} = 1 + x + x^2 + x^3 + \ldots for ∣x∣<1|x| < 1 \qquad cos⁡θ≈1−θ2/2\cos\theta \approx 1 - \theta^2/2 for θ≪1\theta \ll 1

(1+x)n=1+nx+(1/2!)n(n−1)x2+…(1 + x)^n = 1 + nx + (1/2!)n(n-1)x^2 + \ldots for ∣x∣<1|x| < 1 \qquad sin⁡θ≈θ\sin\theta \approx \theta for θ≪1\theta \ll 1

Условие

A laser may be constructed from two main components: a resonant cavity of length LL formed from two highly reflecting flat mirrors, and a gas-filled tube that emits light when excited by a high voltage. Placed inside the otherwise evacuated cavity, the tube creates light which bounces back and forth between the mirrors such that standing light waves are produced within the cavity. (The radiation can be let out through a tiny window in one of the mirrors, but in this problem we are interested in what goes inside the cavity.)

Two vertical flat mirrors, each labelled Mirror, a distance L apart (arrow labelled L between them); between them a horizontal gas tube labelled ACME TUBES INC.

(a) What are the frequencies possible for the standing light waves in the cavity? Express your answer in terms of the cavity length LL and the speed of light in vacuum, cc. [5 т.]

(b) Suppose the plasma tube emits light of a pure frequency fo=5×1014f_o = 5\times10^{14} Hz. Which standing wave mode (specified by an integer non_o) is excited in the cavity if L=1.5L = 1.5 m? [5 т.]

(c) Suppose the plasma tube emits light not of a pure frequency, but emits light having all the frequencies in the range fo±Δff_o \pm \Delta f, where fo=5×1014f_o = 5\times10^{14} Hz, and Δf=1×109\Delta f = 1\times10^{9} Hz. How many standing wave modes are excited in the cavity if L=1.5L = 1.5 m? [5 т.]

(d) Using the fof_o and Δf\Delta f of part (c), what is the largest value of LL such that only one standing wave mode will be excited in the cavity, thereby giving the laser only one output frequency? [5 т.]

(Adapted from A.P. French, Vibrations and Waves, Norton, NY, 1971).

Отговори

Решение


Оригинал в Архива: Semifinal 1997.pdf · официални решения: Semifinal 1997 Solutions.pdf