IAO 2018, Теория, Група α — Задача 5. αβ-5. Облакът на Оорт
XXIII Международна астрономическа олимпиада — Теоретичен тур, група α, български · 6 октомври 2018 г. · 8 т.
Parameters of orbits and physical characteristics of Sun, planets, some dwarf planets and Moon
| Body, planet | Average distance to central body (astr. units) | Distance (mln. km) | Sidereal period (tropical years) | Period (days) | Eccentricity e | Equatorial diameter (km) | Mass (10²⁴ kg) | Average density (g/cm³) | Gravity at surface (m/s²) | Max. magnitude from Earth | Albedo |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Sun | 1.6·10⁹ | 2.5·10¹¹ | 2.2·10⁸ | 8·10¹⁰ | 1392000 | 1989000 | 1.409 | −26.8ᵐ | |||
| Mercury | 0.387 | 57.9 | 0.241 | 87.969 | 0.206 | 4879 | 0.3302 | 5.43 | 3.70 | −2.2ᵐ | 0.06 |
| Venus | 0.723 | 108.2 | 0.615 | 224.701 | 0.007 | 12104 | 4.8690 | 5.24 | 8.87 | −4.7ᵐ | 0.78 |
| Earth | 1.000 | 149.6 | 1.000 | 365.256 | 0.017 | 12756 | 5.9742 | 5.515 | 9.81 | 0.36 | |
| Moon | 0.00257 | 0.38440 | 0.0748 | 27.3217 | 0.055 | 3475 | 0.0735 | 3.34 | 1.62 | −12.7ᵐ | 0.07 |
| Mars | 1.524 | 227.9 | 1.880 | 686.980 | 0.093 | 6794 | 0.6419 | 3.94 | 3.71 | −2.0ᵐ | 0.15 |
| Ceres | 2.77 | 414 | 4.60 | 1681 | 0.077 | 963 | 0.0009 | 2.16 | 0.27 | 6.7ᵐ | 0.09 |
| Jupiter | 5.204 | 778.6 | 11.862 | 4332.59 | 0.048 | 142984 | 1899.8 | 1.33 | 24.86 | −2.7ᵐ | 0.66 |
| Saturn | 9.584 | 1433.7 | 29.458 | 10759.20 | 0.054 | 120536 | 568.50 | 0.70 | 10.41 | 0.7ᵐ | 0.68 |
| Uranus | 19.191 | 2871.0 | 84.015 | 30685.93 | 0.046 | 51118 | 86.625 | 1.30 | 8.44 | 5.5ᵐ | 0.74 |
| Neptune | 30.071 | 4498.6 | 164.778 | 60187.64 | 0.008 | 49532 | 102.78 | 1.76 | 11.20 | 7.8ᵐ | 0.58 |
| Pluto | 39.482 | 5906.4 | 248.09 | 90613 | 0.249 | 2374 | 0.0130 | 1.86 | 0.61 | 15.1ᵐ | 0.6 |
For outer planets and Moon — in mean opposition.
| Coordinates | Hotel | Seafront in the center |
|---|---|---|
| λ (E) | 79°52′ | 79°51′ |
| φ (N) | 07°00′ | 06°54′ |
| Timezone | UT+05:30 | UT+05:30 |
Some constants and formulae
| Quantity | Value |
|---|---|
| Speed of light in vacuum, c (m/s) | 299792458 |
| Constant of gravitation, G (N·m²/kg²) | 6.674·10⁻¹¹ |
| Solar constant, A (W/m²) | 1367 |
| Hubble parameter, H₀ (km/s/Mpc): mean value | 68 |
| Hubble parameter: diapason of values | 50–100 |
| Planck constant, h (J·s) | 6.626·10⁻³⁴ |
| Charge of electron, e (C) | 1.602·10⁻¹⁹ |
| Mass of electron, mₑ (kg) | 9.109·10⁻³¹ |
| Proton-to-electron mass ratio | 1836.15 |
| Faraday constant, F (C/mol) | 96485 |
| Magnetic constant, μ₀ (H/m) | 1.257·10⁻⁶ |
| Universal gas constant, R (J/mol/K) | 8.314 |
| Boltzmann constant, k (J/K) | 1.381·10⁻²³ |
| Stefan-Boltzmann constant, σ (W/m²/K⁴) | 5.670·10⁻⁸ |
| Wien’s displacement constant, b (m·K) | 0.002897 |
| Laboratory wavelength of Hα (Å) | 6563 |
| Laboratory wavelength of Hβ (Å) | 4861 |
| Tropical year length, T (days) | 365.242199 |
| Sidereal year length, T (days) | 365.25636 |
| Anomalistic year length, T (days) | 365.259636 |
| Nodal period of lunar orbit (years) | −18.6 |
| Standard pressure (Pa) | 101325 |
| Visible light extinction by the terrestrial atmosphere in zenith (minimum) | 19%, 0.23ᵐ |
| Height of homogeneous atmosphere (m) | 7991 |
| Refractive index of water for 20°C, n | 1.334 |
| Moment of inertia of solid ball | |
| Moment of inertia of sphere | |
| Volume of a ball | |
| Area of sphere | |
| π | 3.14159265 |
| e | 2.71828183 |
| Golden ratio, φ | 1.61803399 |
Theoretical round. Basic criteria. For work of Jury
Note. The given sketches of solutions are not full; the team leaders have to give more detailed explanations to students. The correct solutions in the students’ papers (enough for 8 pts) may be shorter.
Note. Jury members should evaluate the student’s solutions in essence, and not by looking on formal existence the mentioned sentences or formulae. The formal presence of the mentioned positions in the text is not necessary to give the respective points. Points should be done if the following steps de facto using these positions.
Note. Jury members should elaborate more detailed criteria, and also create criteria for other correct ways of the student’s solutions.
Printed source discrepancies
The galaxy key prints nm for the wavelengths 6563 and 4861, while the constants sheet gives Å. The Martian key reverses the question’s subpart order, prints a lunar-radius term 0.17·10⁵ km, and reuses L₂ for the semimajor axis. The satellite key calls R a diameter and prints 10h20m after subtracting 62 minutes from 11h12m. Printed formulas and labels are retained rather than silently corrected. The satellite key refers to a drawing absent from the supplied solution packet.
Език на решенията
Приложени са съответните официални решения и критерии на английски език от архива. Българският ръкопис съдържа задачи α-1, α-2 и общите αβ-3–5. Допълнението 1.2 към α-1 е записано на следващата страница и е включено към същата задача.
Условие
Понастоящем се счита, че като източник на дългопериодични и непериодични комети се явява външният облак на Оорт, чийто вътрешен и външен радиус се оценяват съответно като 0,2 и 0,8 светлинни години. Кометните тела в този облак се движат хаотично и понякога се сблъскват едно с друго. В резултат на това всяко столетие земните жители наблюдават от 10 до 20 ярки комети, долитащи в централните области на Слънчевата система. Характерният размер на ядрата на такива комети е около 2–3 километра. Оценете по порядък (грубо) общия брой на такива кометни тела във външния облак на Оорт, средното разстояние между тях, а също тяхната сумарна маса. С какви разстояния в Слънчевата система и с масите на какви тела могат да се сравнят получените резултати?
Решение
The fact that every century we observe from 10 to 20 bright comets means that approximately once every 6 years 8 months () two comet bodies collide in the outer Oort cloud, resulting in one of them rushes into the inner regions of the solar system. Collisions occur because all these bodies move chaotically with typical velocities less than the second cosmic velocity (otherwise they would leave this area) and more than half of the first cosmic velocity (otherwise they would move into the inner cloud areas). To estimate the average their velocities, we take the first cosmic velocity for the average distance :
where is the mass of the Sun, and are the outer and inner radii of the cloud. (One can also use the formula , 0.5 ly is about 30,000 times larger than the distance from the Earth to the Sun, therefore, the speed of the Earth in its orbit should be divided by the square root of 30,000. So we obtain .
Let us find how the frequency of collisions is related to the number of comet bodies in the Oort cloud. If there are comet bodies in total, then their concentration in space is
(The fact was taken into account). We will use the collision model in which each comet body moves relative to the others with the same average velocity . During the time , the comet body will cover the distance and in its movement will capture the volume
where is the average diameter of the comet body, we will consider it equal to 2.5 km. If another comet body appears in this volume, then a collision occurs, and the probability of such an event is equal to
Since any of the comet bodies can collide, the total number of collisions will be equal to:
Each collision leads to the fact that with some probability our body will be sent to the inner regions of the Solar System. This probability can be estimated from different models, let us estimate it as an approximate ratio of solid angles:
Thus, in order that one body goes to the inner regions of the solar system, it is necessary to fulfill the condition
Calculations give: ,
with an accuracy of one significant digit: .
If the concentration of the comet bodies is (bodies per ), then each body has a volume of space , and, respectively, the average distance will .
This is roughly the minimum distance between the Earth and Venus.
To estimate the total mass of the comet bodies, we assume that their average density is equal to the density of ice (), and the average volume is . Thus, the average mass of one comet body is:
and the sum of the mass of all the bodies:
This is one hundred masses of Jupiter or one-tenth of the mass of the Sun.
Basic criteria
The problem may have many approaches to be solved. For each way of solution necessary own plan how to estimate the partial solutions. Below is criteria for the author's solution.
| Item | Points |
|---|---|
| Idea how the process is going | 1 |
| Calculation of the average velocities | 1 |
| Step by step formulae and calculations | 4 in total |
| Calculation average distance. Comparing with distances in Solar system | 1 |
| Calculation the total mass. Comparing with masses in Solar system | 1 |
Оригинал в Архива: iao2018_alpha.pdf · официални решения: theosol.pdf · допълнителни данни: theo.pdf