USAAAO 2023, II кръг — Задача 6. Medium 3 · Into the Wilds

2023 National Astronomy Competition · 25 т.

Внимание: Бележка към темата

The separately attributed physical-constants.pdf is an undated common USAAAO archive reference; its identity as the table supplied for this exam is unproven. Printed question/key inconsistencies are preserved, including Medium 3 P5 radius and graph slope, Long 1 cosine denominator, and Long 2 exit-coordinate term and proper-motion magnitude.

Instructions (Please Read Carefully)

2023 National Astronomy Competition

1 Instructions (Please Read Carefully)

The top 5 eligible scorers on the NAC will be invited to represent USA at the next IOAA. In order to qualify for the national team, you must be a high school student with US citizenship or permanent residency.

This exam consists of 3 parts: Short Questions, Medium Questions and Long Questions.

The maximum number of points is 240 points.

The test must be completed within 2.5 hours (150 minutes).

Please solve each problem on a blank piece of paper and mark the number of the problem at the top of the page. The contestant’s full name in capital letters should appear at the top of each solution page. If the contestant uses scratch papers, those should be labeled with the contestant’s name as well and marked as “scratch paper” at the top of the page. Scratch paper will not be graded. Partial credit will be available given that correct and legible work was displayed in the solution.

This is a written exam. Contestants can only use a scientific or graphing calculator for this exam. A table of physical constants will be provided. Discussing the problems with other people is strictly prohibited in any way until the end of the examination period on April 1st. Receiving any external help during the exam is strictly prohibited. This means that the only allowed items are: a calculator, the provided table of constants, a pencil (or pen), an eraser, blank sheets of papers, and the exam. No books or notes are allowed during the exam. Exam is proctored and recorded. You are expected to have your video on at all times.

We acknowledge the following people for their contributions to this year’s exam:

Wesley Antônio Machado Andrade de Aguiar, Erez Abrams, Lucas Pinheiro, Sahil Pontula, Joe McCarty, Hagan Hensley, Leo Yao, and Andrew Liu.

Undated common archive reference · Table of Physical Constants

Table of Physical Constants

QuantitySymbolValue
Electron rest massmem_e9.109×10−31 kg9.109\times10^{-31}\,\mathrm{kg}
Proton rest massMpM_p1.6726×10−27 kg1.6726\times10^{-27}\,\mathrm{kg}
Electronic chargeee1.6022×10−19 C1.6022\times10^{-19}\,\mathrm C
Speed of light in free spacecc2.9979×108 m s−12.9979\times10^8\,\mathrm{m\,s^{-1}}
Permeability of free spaceμ0\mu_04π×10−7 H m−14\pi\times10^{-7}\,\mathrm{H\,m^{-1}}
Permittivity of free spaceϵ0\epsilon_08.854×10−12 F m−18.854\times10^{-12}\,\mathrm{F\,m^{-1}}
Planck’s constanthh6.626×10−34 J s6.626\times10^{-34}\,\mathrm{J\,s}
Reduced Planck’s constantℏ=h/2π\hbar=h/2\pi1.0546×10−34 J s1.0546\times10^{-34}\,\mathrm{J\,s}
ℏc\hbar c197.33 MeV fm197.33\,\mathrm{MeV\,fm}
Boltzmann’s constantkBk_B1.3807×10−23 J K−11.3807\times10^{-23}\,\mathrm{J\,K^{-1}}
Gas constantR=kB/mH\mathcal R=k_B/m_H8.250×103 J kg−1 K−18.250\times10^3\,\mathrm{J\,kg^{-1}\,K^{-1}}
Molar gas constantRR8.315 J mol−1 K−18.315\,\mathrm{J\,mol^{-1}\,K^{-1}}
Avogadro’s numberNAN_A6.022×1023 mol−16.022\times10^{23}\,\mathrm{mol^{-1}}
Standard molar volume22.414×10−3 m3 mol−122.414\times10^{-3}\,\mathrm{m^3\,mol^{-1}}
Unified atomic mass unit (C12C\vphantom{C}^{12}\mathrm C scale)uu931.5 MeV/c2=1.660538×10−27 kg931.5\,\mathrm{MeV}/c^2=1.660538\times10^{-27}\,\mathrm{kg}
Mass of hydrogen atommHm_H1.0078u=1.6735×10−27 kg1.0078u=1.6735\times10^{-27}\,\mathrm{kg}
Bohr magnetonμB\mu_B9.274×10−24 A m29.274\times10^{-24}\,\mathrm{A\,m^2} or J T−1\mathrm{J\,T^{-1}}
Nuclear magnetonμN\mu_N5.051×10−27 A m25.051\times10^{-27}\,\mathrm{A\,m^2} or J T−1\mathrm{J\,T^{-1}}
Proton magnetic momentμp\mu_p2.7928μN2.7928\mu_N
Neutron magnetic momentμn\mu_n−1.9130μN-1.9130\mu_N
Bohr radiusa0a_05.292×10−11 m5.292\times10^{-11}\,\mathrm m
Fine structure constantα=e2/(4πϵ0ℏc)\alpha=e^2/(4\pi\epsilon_0\hbar c)(137.04)−1(137.04)^{-1}
Compton wavelength of electronλC=h/(mec)\lambda_C=h/(m_ec)2.4263×10−12 m2.4263\times10^{-12}\,\mathrm m
Rydberg’s constantR∞R_\infty1.0974×107 m−11.0974\times10^7\,\mathrm{m^{-1}}
R∞hcR_\infty hc13.606 eV13.606\,\mathrm{eV}
Stefan-Boltzmann constantσ\sigma5.671×10−8 W m−2 K−45.671\times10^{-8}\,\mathrm{W\,m^{-2}\,K^{-4}}
Radiation density constanta=4σ/ca=4\sigma/c7.561×10−16 J m−3 K−47.561\times10^{-16}\,\mathrm{J\,m^{-3}\,K^{-4}}
Gravitational constantGG6.673×10−11 N m2 kg−26.673\times10^{-11}\,\mathrm{N\,m^2\,kg^{-2}}

Rest masses of some leptons and hadrons in MeV/c2\mathrm{MeV}/c^2:

e±e^\pm 0.5110, μ±\mu^\pm 105.66, τ±\tau^\pm 1777, π0\pi^0 134.98, π±\pi^\pm 139.57, K±\mathrm K^\pm 493.7, K0\mathrm K^0 497.7, η\eta 547, D0\mathrm D^0 1865, D±\mathrm D^\pm 1869, p 938.3, n 939.6, Λ0\Lambda^0 1115.7, Σ+\Sigma^+ 1189, Σ0\Sigma^0 1193, Σ−\Sigma^- 1197, Ξ0\Xi^0 1315, Ξ−\Xi^- 1321, Ω−\Omega^- 1672, Z0\mathrm Z^0 91.187×10391.187\times10^3, W±\mathrm W^\pm 80.41×10380.41\times10^3.

QuarkChargeI3I_3SSCCBBTTMass (GeV/c2\mathrm{GeV}/c^2)
u+23+\frac2312\frac120000∼0.003\sim0.003
d−13-\frac13−12-\frac120000∼0.006\sim0.006
c+23+\frac2300+100∼1.25\sim1.25
s−13-\frac130-1000∼0.11\sim0.11
t+23+\frac230000+1174.3
b−13-\frac13000-104.2
Undated common archive reference · Astrophysical Data and Conversion Factors

Astrophysical Data

QuantitySymbolValue
1 astronomical unitAU1.496×1011 m1.496\times10^{11}\,\mathrm m
1 parsecpc3.086×1016 m3.086\times10^{16}\,\mathrm m
Luminosity of SunL⊙L_\odot3.85×1026 W3.85\times10^{26}\,\mathrm W
Mass of SunM⊙M_\odot1.989×1030 kg1.989\times10^{30}\,\mathrm{kg}
Radius of SunR⊙R_\odot6.96×108 m6.96\times10^8\,\mathrm m
Mass of EarthMEM_E5.9742×1024 kg5.9742\times10^{24}\,\mathrm{kg}
Radius of EarthRER_E6.3781×106 m6.3781\times10^6\,\mathrm m

Other data and conversion factors

QuantitySymbolValue
1 ångstromÅ10−10 m10^{-10}\,\mathrm m
1 fermifm10−15 m10^{-15}\,\mathrm m
1 barnb10−28 m210^{-28}\,\mathrm{m^2}
1 pascalPa1 N m−21\,\mathrm{N\,m^{-2}}
1 standard atmosphere1.0132×105 Pa1.0132\times10^5\,\mathrm{Pa}
Standard acceleration due to gravitygg9.807 m s−29.807\,\mathrm{m\,s^{-2}}
1 electron volteV1.6022×10−19 J1.6022\times10^{-19}\,\mathrm J
eV/hc\mathrm{eV}/hc8.065×105 m−18.065\times10^5\,\mathrm{m^{-1}}
eV/kB\mathrm{eV}/k_B1.1604×104 K1.1604\times10^4\,\mathrm K
Wavelength of 1 eV photon1.2399×10−6 m1.2399\times10^{-6}\,\mathrm m

Trigonometrical identities

sin⁡(θ+ϕ)=sin⁡(θ)cos⁡(ϕ)+cos⁡(θ)sin⁡(ϕ)\sin(\theta+\phi)=\sin(\theta)\cos(\phi)+\cos(\theta)\sin(\phi)
cos⁡(θ+ϕ)=cos⁡(θ)cos⁡(ϕ)−sin⁡(θ)sin⁡(ϕ)\cos(\theta+\phi)=\cos(\theta)\cos(\phi)-\sin(\theta)\sin(\phi)
sin⁡α+sin⁡β=2sin⁡12(α+β)cos⁡12(α−β)\sin\alpha+\sin\beta=2\sin\frac12(\alpha+\beta)\cos\frac12(\alpha-\beta)
cos⁡α+cos⁡β=2cos⁡12(α+β)cos⁡12(α−β)\cos\alpha+\cos\beta=2\cos\frac12(\alpha+\beta)\cos\frac12(\alpha-\beta)
cos⁡α−cos⁡β=2sin⁡12(α+β)sin⁡12(β−α)\cos\alpha-\cos\beta=2\sin\frac12(\alpha+\beta)\sin\frac12(\beta-\alpha)

In a triangle ABC, a/sin⁡A=b/sin⁡B=c/sin⁡Ca/\sin A=b/\sin B=c/\sin C

and a2=b2+c2−2bccos⁡Aa^2=b^2+c^2-2bc\cos A

Prefixes

T = tera = 101210^{12}c = centi = 10−210^{-2}
G = giga = 10910^9m = milli = 10−310^{-3}
M = mega = 10610^6μ\mu = micro = 10−610^{-6}
k = kilo = 10310^3n = nano = 10−910^{-9}
p = pico = 10−1210^{-12}
f = femto = 10−1510^{-15}

Условие

(25 points) Into the Wilds

You are an astronaut exploring uncharted parts of space in your trusty spaceship, when you suddenly fall into a magical portal to another universe!

Looking for a way back home, you fly to the nearest solar system. Just like normal solar systems, it is home to several planets in orbit around a star - except with one minor difference: it’s miniature! The star is only 4 kilometers in diameter, and the whole solar system could fit within a small country back home on Earth.

You know your astrophysics well enough to know that this should be impossible! The only explanation is that some law of physics works differently in this universe. Since you’re still alive, chemistry must be unchanged, so quantum mechanics and electromagnetism must work the same as you’re used to. Therefore, the only thing that can be different is gravity.

You decide to do some experiments around the solar system to figure out exactly what is different about gravity here.

(a) (10 points) First you measure the orbital periods tit_i and orbital semi-major axes aia_i of the planets in the solar system. You name the planets P1P_1 through P5P_5, because you are incredibly unoriginal. Your data is as follows:

Planetaa (km)tt (minutes)
P1P_15.11:51
P2P_29.04:10
P3P_312.16:38
P4P_417.011:02
P5P_520.314:46

Based on this data, do you think that gravity here follows an inverse square law? Justify your answer with calculations and/or drawing an appropriate plot. (You needn’t be too formal with statistics here, any well-reasoned argument will get full credit.)

(b) (3 points) If the mass of the star is MM and the gravitational constant in this universe is G′G', then what is G′MG'M?

This is a good start! Unfortunately, without a known mass, you can’t determine the gravitational constant G′G'. You decide to give the planets a closer look to see what else you can find out. You’ll start from the outermost and work your way in.

(c) (5 points) After narrowly escaping being eaten by P5P_5’s local fauna, you penetrate the stormy atmosphere of P4P_4 to find that it’s made almost entirely of water (ρ=997 kg/m3)(\rho=997\ \mathrm{kg/m^3}) with a radius of 500 m. While standing in your ship floating on the water’s surface, you experience a heavy gravitational pull - 2 times what you’re used to on Earth.

What is the gravitational constant in this universe?

(d) (2 points) What is the mass of this solar system’s star?

(e) (5 points) You notice that this star looks yellowish-orange, suggesting its surface temperature is a little lower than that of the Sun. Taking a spectrum, you measure that this star’s spectral radiance peaks at a wavelength of 916 nm.

The lifetime of a star can be roughly estimated based on its luminosity and the mass of fuel it has available to burn*. Use a simple scaling argument to roughly estimate the lifetime of this solar system’s sun. Explain your reasoning.

(Hint: use our Sun’s lifetime of 101010^{10} years as a reference point.)

*A more careful calculation shows that the temperature at the core of the star wouldn’t actually be enough to ignite fusion, so nuclear physics must work differently here in order for fusion to be possible. Let’s ignore that for the sake of this question, though.

Решение


Оригинал в Архива: second_exam_2023-1.pdf · официални решения: second_exam_2023_sols-1.pdf · допълнителни данни: physical-constants.pdf