IAO 2011, Теория, Група β — Задача 4. Photo of Jupiter
XVI International Astronomy Olympiad. Almaty, Kazakhstan, 22 – 30. IX. 2011. Round Theo, Group β. Theoretical round. Problems to solve · 22 септември 2011 г. · 8 т.
Внимание: Бележка към темата
The shared five-page official solution is a preliminary jury sketch. Tops of scanned pages 2–5 are truncated in the source itself (MediaBox equals CropBox); missing passages are marked explicitly. No detailed grading rubric is present in the year inventory; the solution introduction says correct student solutions are worth 8 points. The Bear drawing for problem 3 and the promised sector/point drawings for problem 5 are not supplied. The ray diagram for problem 4 has a partly clipped lower label. Printed slips, including the solar-mass exponent, latitude inconsistency and planetarium inequality, are retained with notes where relevant.
Бележка
General note. Maybe not all problems have correct questions. Some questions (maybe the main question of the problem, maybe one of the subquestions) may make no real sense. In this case you have to write in your answer (in English or Russian): «impossible situation – ситуация невозможна». Of course, this answer has to be explained numerically or logically.
Data from the tables (Planetary data, stars, constants, etc.) may be used for solving every problem.
The answers «Да-Yes» or «Нет-No» has to be written in English or Russian.
Условие
In the photo of Jupiter that was taken on October 19, 2009, one of the Galilean moons and its shadow on the disc of the planet can be seen. Jupiter was near the middle of Capricornus constellation when the photo was taken.
Find the orbital distance from the moon to the surface of the planet. Determine the name of the moon. The solution should be illustrated by drawings. The name of the moon in the solution and in the drawings should be written (or duplicated) in English.

Отговори
- Europa; supplied sketch gives L/R = 9.64 from Jupiter’s centre (table: 9.39).
Решение
Внимание: Непълно решение
The opening of the source text is cut off, a ray-diagram label is partly clipped, and the sketch identifies Europa and gives centre-distance ratio L/R=9.64 but does not explicitly subtract Jupiter radius for the requested surface distance.
Theoretical round. Sketches for solutions. For preliminary work of Jury ONLY.
Note for jury and team leaders. The proposed sketches are not full; the team leaders have to give more detailed explanations for students. But the correct solutions in the students’ papers (enough for 8 pts) may be shorter.
Photo geometry and identification
Source gap: the opening of this solution is missing at the top edge of scanned page 4. The visible text starts mid-sentence:
… moon (to the left) and to the shadow of the moon (to the right) the distance from the center of the moon to the center of Jupiter can be calculated using formulas of rectangular triangle:
Where is the angle between the direction to the Sun (The Sun beams come a little from the left) and the direction to the Earth (from where the picture is made). We can estimate this angle in two ways.
Or we remember that the Capricorn is a zodiac constellation, and the center of this constellation (not zodiac sign, but zodiac constellation!) is passed by the Sun approximately in the end of January — the beginning of February. The angle between the Sun positions on October, 19th and, assume, on February, 3rd, is equal 3.6 months or .
Or to start with that fact that the picture is made on October, 19th (a direct ascension of the Sun 26 days after an equinox we will estimate as ), Jupiter was in the middle of Capricorn constellation (not zodiac sign, but constellation!) (right ascension of this point we will estimate to ), and both the Sun and Jupiter were close to the ecliptic, declination of both points nearby –. This data allow us to estimate the angle between Sun and Jupiter at the celestial sphere as about the difference in declinations, that is, or .
From the second drawing, knowing this angle , and distances to the Sun from Earth and from Jupiter , it is possible to calculate the angle corner necessary to us:
By measuring the values R, a and b (accordingly 48.5 mm, 59 mm and 18 mm on the author printed picture, on other scaled printed pictures other values may be obtained, but their absolute values are not important, important is only ratios that do not depend on scale) in the photo, and using the formula for a rectangular triangle, we can receive a value of equal to 9.64.
From the given tables it is possible to find that for Io this ratio equals to 5.90, for Europa — 9.39, for Ganimede — 14.97, for Callisto — 26.33. It is evident, that our calculations are made with some accuracy, and the proximity of values 9.64 and 9.39 (1.5% of accuracy) says that we see the moon Europa in the picture.
Transcription note: “difference in declinations” and “1.5%” follow the supplied sketch. The sketch reports distance from Jupiter's centre, while the question asks distance from its surface; a final subtraction of the radius is not explicitly supplied. The ray-diagram label at the bottom of scanned page 3 is partly cut off.


Parameters of orbits. Physical characteristics of Sun, some planets, Moon and Galilean moons of Jupiter
Элементы орбит. Физические характеристики Солнца, некоторых планет, Луны и Галилеевых спутников Юпитера
Parameters of orbits. Physical characteristics of Sun, some planets, Moon and Galilean moons of Jupiter
| Небесное тело, планета | Среднее расстояние от центрального тела в астр. ед. | Среднее расстояние от центрального тела в млн. км | Сидерический (или аналогичный) период обращения в тропич. годах | Сидерический (или аналогичный) период обращения в средних сутках | Эксцентриситет, | Экваториальн. диаметр км | Масса кг | Средняя плотность г/см | Ускор. своб. пад. у пов. м/с | Наклон оси | Альбедо |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Body, planet | Average distance to central body in astr. units | Average distance to central body in mln. km | Sidereal (or analogous) period in troph. years | Sidereal (or analogous) period in days | Eccentricity | Equat. diameter km | Mass kg | Av. density g/cm | Grav. acceler. at surf. m/s | Axial tilt | Albedo |
| Солнце Sun | 1392000 | 1989000 | 1,409 | ||||||||
| Меркурий Mercury | 0,387 | 57,9 | 0,241 | 87,97 | 0,206 | 4 879 | 0,3302 | 5,43 | 3,70 | 0,01° | 0,06 |
| Венера Venus | 0,723 | 108,2 | 0,615 | 224,70 | 0,007 | 12 104 | 4,8690 | 5,24 | 8,87 | 177,36 | 0,78 |
| Земля Earth | 1,000 | 149,6 | 1,000 | 365,26 | 0,017 | 12 756 | 5,9742 | 5,515 | 9,81 | 23,44 | 0,36 |
| Луна Moon | 0,00257 | 0,38440 | 0,0748 | 27,3217 | 0,055 | 3 475 | 0,0735 | 3,34 | 1,62 | 6,7 | 0,07 |
| Марс Mars | 1,524 | 227,9 | 1,880 | 686,98 | 0,093 | 6 794 | 0,6419 | 3,94 | 3,71 | 25,19 | 0,15 |
| Юпитер Jupiter | 5,204 | 778,6 | 11,862 | 4 332,59 | 0,048 | 142 984 | 1899,8 | 1,33 | 24,86 | 3,13 | 0,66 |
| Сатурн Saturn | 9,584 | 1433,7 | 29,458 | 10 759,20 | 0,054 | 120 536 | 568,50 | 0,70 | 10,41 | 26,73 | 0,68 |
| Спутник | Среднее расстояние от центра планеты в астр. ед. | Среднее расстояние от центра планеты в тыс. км | Сидерич. период обращения в средних сутках | Наклонение орбиты (°) | Эксцентриситет, | Диаметр км | Масса кг | Средняя плотность г/см | Ускор. своб. пад. у пов. м/с | Макс. блеск, вид. с Земли *) | Геом Альбедо |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Moon | Average distance to planet center in astr. units | Average distance to planet center in thous. km | Sidereal period in days | Orbit inclination (°) | Eccentricity | Diameter km | Mass kg | Av. density g/cm | Grav. acceler. at surf. m/s | Max. magn. From Earth *) | Geom Albedo |
| Ио Io | 0,00282 | 421,70 | 1,769137 | 0,050° | 0,0041 | 3 643 | 89,31 | 3,53 | 1,80 | 0,63 | |
| Европа Europa | 0,00449 | 671,03 | 3,551181 | 0,471° | 0,0094 | 3 122 | 48,00 | 3,01 | 1,32 | 0,67 | |
| Ганимед Ganymede | 0,00716 | 1070,41 | 7,154553 | 0,204° | 0,0011 | 5 262 | 148,19 | 1,94 | 1,43 | 0,43 | |
| Каллисто Callisto | 0,01259 | 1882,71 | 16,689018 | 0,205° | 0,0074 | 4 821 | 107,59 | 1,83 | 1,23 | 0,20 |
*) В среднем противостоянии. *) In mean opposition.
Some constants and formulae
Некоторые константы и формулы
Some constants and formulae
| Русский | English | |
|---|---|---|
| Скорость света в вакууме, c (м/с) | 299 792 458 | Speed of light in vacuum, c (m/s) |
| Гравитационная постоянная, G (Н·м/кг) | Constant of gravitation, G (N·m/kg) | |
| Солнечная постоянная, A (Вт/м) | 1367 | Solar constant, A (W/m) |
| Параметр Хаббла, H (км/с/МПк): среднее значение; диапазон значений | 71; 50-100 | mean value; diapason of values: Hubble parameter, H (km/s/Mpc) |
| Постоянная Планка, h (Дж·с) | Plank constant, h (J·s) | |
| Заряд электрона, e (Кл) | Charge of electron, e (C) | |
| Масса электрона, m (кг) | Mass of electron, m (kg) | |
| Соотношение масс протона и электрона | 1836.15 | Proton-to-electron ratio |
| Постоянная Фарадея, F (Кл/моль) | 96 485 | Faraday constant, F (C/mol) |
| Магнитная постоянная, μ (Гн/м) | Magnetic constant, μ (H/m) | |
| Универсальная газовая постоянная, R (Дж/моль/K) | 8.314 | Universal gas constant, R (J/mol/K) |
| Постоянная Больцмана, k (Дж/K) | Boltzmann constant, k (J/K) | |
| Стандартная атмосфера (Па) | 101 325 | Standard atmosphere (Pa) |
| Постоянная Стефана-Больцмана, σ (Вт/м/K) | Stefan-Boltzmann constant, σ (W/m/K) | |
| Константа смещения Вина, b (м·K) | 0.002897 | Wien’s displacement constant, b (m·K) |
| Лабораторная длина волны Hα (Å) | 6562.81 | Laboratory wavelength of Hα (Å) |
| Длина тропического года, T (сут) | 365.242199 | Tropical year length, T (days) |
| Показатель преломления воды при 20°C, n | 1.334 | Refractive index of water for 20°C, n |
| Момент инерции шара | Moment of inertia of a solid ball | |
| Площадь сферы | Area of sphere | |
| π | 3.14159265 | π |
| e | 2.71828183 | e |
| Золотое сечение, φ | 1.61803399 | Golden ratio, φ |
Оригинал в Архива: betatheo.pdf · официални решения: theosol.pdf