USAAAO 2024, II кръг — Short 2
2024 National Astronomy Competition · 10 т.
Внимание: Бележка към темата
All eight whole original problems, their native sections, lettered parts, three roman subparts of Long 1(f), full official worked keys and original marking/acceptance notes are retained. Printed scientific discrepancies are preserved in local source notes. The official key adds a Friedmann-variable clarification and a solar apparent magnitude assumption absent from the question booklet, and changes Long1(f)(iii) from a factor to a percentage; these source variants are explicitly attributed. A separate undated common archive constants/reference table is included with its own source identity; its use as the exact 2024 provided attachment is not established, and its constants are not substituted into the printed key. The native cover specifies blank paper rather than a designated answer sheet. April 13th is the end of the examination period, not an established single sitting date.
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 225 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 13th. 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:
Abhay Bestrapalli, Orion Foo, Hagan Hensley, David Lee, Sandesh Kalantre, Andrew Liu, Joe McCarty, Leo Yao
Common archive reference — Table of Physical Constants
This separate common USAAAO archive reference is undated in the catalogue. Its use as the exact 2024 exam attachment is not established.
| Quantity | Symbol | Value |
|---|---|---|
| Electron rest mass | ||
| Proton rest mass | ||
| Electronic charge | ||
| Speed of light in free space | ||
| Permeability of free space | ||
| Permittivity of free space | ||
| Planck’s constant | ||
| Reduced Planck’s constant | ||
| Boltzmann’s constant | ||
| Gas constant | ||
| Molar gas constant | ||
| Avogadro’s number | ||
| Standard molar volume | ||
| Unified atomic mass unit ( scale) | ||
| Mass of hydrogen atom | ||
| Bohr magneton | or | |
| Nuclear magneton | or | |
| Proton magnetic moment | ||
| Neutron magnetic moment | ||
| Bohr radius | ||
| Fine structure constant | ||
| Compton wavelength of electron | ||
| Rydberg’s constant | ||
| Stefan-Boltzmann constant | ||
| Radiation density constant | ||
| Gravitational constant |
Rest masses of some leptons and hadrons in :
0.5110, 105.66, 1777, 134.98, 139.57, 493.7, 497.7, 547, 1865, 1869, p 938.3, n 939.6, 1115.7, 1189, 1193, 1197, 1315, 1321, 1672, , .
| Quark | Charge | Mass () | |||||
|---|---|---|---|---|---|---|---|
| u | 0 | 0 | 0 | 0 | |||
| d | 0 | 0 | 0 | 0 | |||
| c | 0 | 0 | +1 | 0 | 0 | ||
| s | 0 | -1 | 0 | 0 | 0 | ||
| t | 0 | 0 | 0 | 0 | +1 | 174.3 | |
| b | 0 | 0 | 0 | -1 | 0 | 4.2 |
Common archive reference — Astrophysical Data and identities
Astrophysical Data
| Quantity | Symbol | Value |
|---|---|---|
| 1 astronomical unit | AU | |
| 1 parsec | pc | |
| Luminosity of Sun | ||
| Mass of Sun | ||
| Radius of Sun | ||
| Mass of Earth | ||
| Radius of Earth |
Other data and conversion factors
| Quantity | Symbol | Value |
|---|---|---|
| 1 ångstrom | Å | |
| 1 fermi | fm | |
| 1 barn | b | |
| 1 pascal | Pa | |
| 1 standard atmosphere | ||
| Standard acceleration due to gravity | ||
| 1 electron volt | eV | |
| Wavelength of 1 eV photon |
Trigonometrical identities
In a triangle ABC,
and
Prefixes
| Prefix | Name | Factor |
|---|---|---|
| T | tera | |
| G | giga | |
| M | mega | |
| k | kilo | |
| c | centi | |
| m | milli | |
| micro | ||
| n | nano | |
| p | pico | |
| f | femto |
Source note: This undated common table prints , and . The 2024 eclipse key instead uses , Earth mass and Earth radius . Both original sets of values are preserved separately; this reference is not an established exact dated 2024 attachment.
Условие
David the astronomy enthusiast loves looking at stars! Specifically, he particularly enjoys looking at stars on the ecliptic. One day, he is out stargazing at midnight (local solar time) and looks at the antisolar point (the point on the celestial sphere exactly opposite to the Sun). He notices a faint glow of magnitude , and after some research he concludes that this is caused by a phenomenon known as gegenschien, where Solar System dust is lit up by the Sun and reflects some light back towards Earth. These particles are in an orbit of 2.06 AU around the Sun. Assuming the radii of these particles are around 1 cm and their albedo is 0.14, estimate the density of these particles. Express your answer in particles per square arcsecond.
Отговори
particles/arcsec²
The official key also accepts half this value and other reasonable scattering assumptions for full credit.
Решение
We can find the total luminosity from one square arcsecond of this source by using
From this we get
where we used since the particles are directly opposite to the Sun.
Now, let’s calculate how much luminosity one particle reflects. To do this, we simply calculate the flux from the Sun and multiply by the cross sectional area of the particle and it’s albedo. This gives
Finally, all that is left to do is divide these two numbers to get an answer of
Note: one reasonable thing to do is to divide this number by two because the light emitted by these particles is not isotropic, it is mostly scattered back towards the direction of the Earth. This and other reasonable assumptions should be accepted for full credit.
Теми и трудност
Оценена трудност: 3/5.
Светлина и астрономически измервания · Слънчева система · Звездни величини · Поток и светимост · Астероиди, комети и метеори
Предпоставки: Гимназиална подготовка, Разширена олимпиадна подготовка
Оригинал в Архива: second_exam_2024.pdf · официални решения: second_exam_2024-solutions.pdf · допълнителни данни: physical-constants.pdf