IOAA 2023, Теория — Задача 9. Second eclipse
IOAA 2023 — Theoretical competition · 20 т.
Указания
- Do not touch envelopes until the start of the examination.
- The theoretical examination lasts for 5 hours and is worth a total of 250 marks.
- There are Answer Sheets for carrying out detailed work and Working Sheets for rough work, which are already marked with your student code and question number.
- Use only the answer sheets for a particular question for your answer. Please write only on the printed side of the sheet. Do not use the reverse side. If you have written something on any sheet which you do not want to be evaluated, cross it out.
- Use as many mathematical expressions as you think may help the evaluator to better understand your solutions. The evaluator may not understand your language. If it is necessary to explain something in words, please use short phrases (if possible in English).
- You are not allowed to leave your work desk without permission. If you need any assistance (malfunctioning calculator, need to visit a restroom, etc.), please draw the attention of the supervisor.
- The beginning and end of the examination will be indicated by the supervisor. The remaining time will be displayed on a clock.
- At the end of the examination you must stop writing immediately. Put everything back in the envelope and leave it on the table.
- Once all envelopes are collected, your student guide will escort you out of the examination room.
- A list of constants and useful relations are included in the envelope.
Table of Constants
Fundamental constants
| Constant | Symbol | Value |
|---|---|---|
| Speed of light in vacuum | ||
| Planck constant | ||
| Boltzmann constant | ||
| Stefan-Boltzmann constant | ||
| Elementary charge | ||
| Universal gravitational constant | ||
| Universal electric constant | ||
| Universal gas constant | ||
| Avogadro constant | ||
| Wien’s displacement constant | ||
| Mass of electron | ||
| Mass of proton | ||
| Mass of neutron | ||
| Mass of Helium nucleus | ||
| Atomic mass unit (a.m.u., Dalton) |
Astronomical data
| Data | Symbol | Value |
|---|---|---|
| Hubble constant | ||
| North Ecliptic Pole () | ||
| North Galactic Pole () | ||
| 1 jansky | ||
| 1 parsec | ||
| 1 astronomical unit (au) | ||
| 1 sidereal day | ||
| 1 tropical year | solar days | |
| 1 sidereal year | solar days |
Approximations and Gauss’s formulae
Approximations
Gauss’s formulae
Spherical law of cosines:
Spherical law of sines: .
The Sun, Earth and Moon
The Sun
| Data | Symbol | Value |
|---|---|---|
| Solar luminosity | ||
| Apparent angular diameter of Sun | ||
| Effective temperature of Sun | ||
| Apparent visual magnitude | ||
| Absolute visual magnitude | ||
| Apparent bolometric magnitude | ||
| Absolute bolometric magnitude | ||
| Distance of the Sun from the Galactic centre |
The Earth and Moon
| Data | Symbol | Value |
|---|---|---|
| Obliquity of the ecliptic (Earth) | ||
| Platonic year (period of precession of Earth’s axis) | years | |
| Apparent visual magnitude of full Moon | ||
| Apparent angular diameter of Moon | ||
| Inclination of the lunar orbit to the ecliptic | ||
| Inclination of the lunar equator to its orbital plane | ||
| Lunar sidereal month | ||
| Synodic month | ||
| Tropical month | ||
| Anomalistic month (the average time between two successive Moon’s perigees) | ||
| Draconic month (time between two successive transits of the Moon through the same node) |
The Solar System
| Object | Mean radius [km] | Mass [kg] | Semimajor axis [au] | Eccentricity |
|---|---|---|---|---|
| Sun | — | — | ||
| Mercury | ||||
| Venus | ||||
| Earth | ||||
| Moon | (range –) | |||
| Mars | ||||
| Jupiter | ||||
| Saturn | ||||
| Uranus | ||||
| Neptune |
General Marking Scheme
| Case | Marking |
|---|---|
| Using incorrect physical concept (despite correct answers) | No points given |
| Giving correct answer without detailed calculation | Deduct 50% of the marks for that part |
| Minor mistakes in the calculations, e.g., wrong signs, symbols, substitutions | Deduct 20% of the marks for that part |
| Units missing from final answers | Deduct 0.5 pts |
| Too few or too many significant figures in the final answer | Deduct 0.5 pts |
| Error resulting from another error in an earlier part for which the student already lost marks, if the answer is physically reasonable. | Full points (i.e., no deductions) |
| Error resulting from another error in an earlier part, where the student should have realised the answer was physically unreasonable. | Deduct 20% of the marks for that part |
For example, if due to an error in an earlier part, the student calculates the mass of a star as instead of , they will only lose marks for the earlier part. However, if, for the same reason, a student calculates the mass as , they should realize this is wrong (a few times the Earth’s mass) and thus should lose some marks for this part as well.
Условие
For each of two eclipsing binary systems, Bolek and Lolek, the primary eclipses were observed with very high cadence as depicted below:

Figure 1. Observed lightcurve for system Bolek.

Figure 2. Observed lightcurve for system Lolek.
In the figures, is the time in hours relative to the moment of minimum and is the brightness in the (visible) band in magnitudes. The points are the measurements and the line is the fitted model of the shape of the eclipse.
You can assume that in both cases the eclipses are central () and last for a very small fraction of the orbital period, limb darkening is negligible, and the orbits have low eccentricity.
On the Answer Sheet, draw the predicted shape of the light curve for each of the secondary eclipses. Write down the equations and calculations leading to your predictions.
Вторинні затемнення — T.9 (20 pt)

Передбачувана крива блиску для системи Болек

Передбачувана крива блиску для системи Льолек
Решение

Figure 1: Observed lightcurve for system Bolek.

Figure 2: Observed lightcurve for system Lolek.
Answer Sheet

Figure 3: Predicted lightcurve for the second eclipse for system Bolek.

Figure 4: Predicted lightcurve for the second eclipse for system Lolek.
Solution
For each of the systems, since the eclipses are short we can assume that the angle swept along the orbit during the eclipse is negligibly small, which means that the tangential velocity in relative orbital motion is constant.
System A
A sharp peak minimum in a central eclipse implies that . Therefore, both eclipses will be total, with minima of brightnesses and , respectively.
| Marking criterion | Points |
|---|---|
| Noticing that | 1 point |
| Brightnesses at the two minima are and | 1 point |
Define the magnitude at minimum as and the baseline magnitude as . From Pogson’s law applied to the two cases: and . For the first case, with simple operations we obtain: . Plugging this into the second case: .
| Marking criterion | Points |
|---|---|
| Correct application of Pogson’s law | 1 point |
| Obtaining the luminosity ratio | 1 point |
| Final formula for the depth of the minimum | 1 point |
As the orbits are near-circular, timescales will be the same for both eclipses. Therefore it is sufficient to ‘copy’ the shape of the primary one while scaling down the depth to . Reading off and from the plot, we arrive at , , and the following figure:

Figure 5: Predicted lightcurve for the second eclipse for system A – correct answer.
| Marking criterion | Points |
|---|---|
| Correct depth of the second eclipse | 2 points |
| Overall correct shape (sharp peak and symmetry not broken) | 1 point |
| All contact times matching the first eclipse | 1 point |
Note about marking: Reproducing the exact shape of the eclipse (concave/convex, smooth descent, etc.) is not subject to grading as it requires mm-level precision, and the focus is on the thought process instead.
System B
For the second system, we follow a generally similar scheme, but we see that the minimum is flat. is the time of the descent from the baseline brightness to the lowest point, i.e., between contacts I and II, while is the time between contacts II and III during which the lightcurve remains at its lowest point:

From this, we obtain and, after rearranging, .
| Marking criterion | Points |
|---|---|
| Noticing that and can be calculated from the contact times | 1 point |
| Calculating, or giving the correct formula for, | 1 point |
Here is the radius of the smaller star and there are two solutions – it could either be (partially) eclipsing or (entirely) eclipsed. Let us first assume that it was eclipsed. After measuring for the eclipse and for the baseline we again (just like for system A) assume and write down: .
| Marking criterion | Points |
|---|---|
| Calculating, or giving the correct formula for, | 1 point |
Reading off and from the plot, we arrive at , .
, where stands for the surface brightness of each star.
(or ).
| Marking criterion | Points |
|---|---|
| Relation between , ratios and (or ) ratios | 1 point |
| Concluding that (or ) | 2 points |
In such a case, it does not matter if star 2 is eclipsing or eclipsed. During the baseline, we always see two disks with a total brightness of , while during the eclipse, we see one disk of radius and total brightness .
Note about marking: This solution can be independently verified by assuming that the smaller component was eclipsing and cutting out a disk of surface and brightness contribution in the star of surface and surface brightness . Instead of of star 1, we would have measured of a combination of the two, with a brightness . The same conclusion will follow. Any solution correctly arriving at this conclusion and the correct figure – no matter the order of steps taken – should be scored equally. For the maximum number of points, however, the student should make a convincing point that this is the only solution, i.e. lifting the previously made assumption (or exploring both cases).
| Marking criterion | Points |
|---|---|
| Solution showing there is only one possible shape of the secondary eclipse | 1 point |
To draw the second eclipse, one must simply copy the shape of the first one:

Figure 6: Predicted lightcurve for the second eclipse for system B – correct answer.
| Marking criterion | Points |
|---|---|
| Correct depth of the second eclipse | 2 points |
| Overall correct shape (flat minimum and symmetry not broken) | 1 point |
| All contact times matching the first eclipse | 1 point |
Original PDF comments
The original solution PDF contains two comments attributed to IOAA on this page:
“In previuos erratic version it was "... - 1".”
“In previous erratic version it was L_2/L_1 = ...”
Бележки за изданието
The English question packet includes a Ukrainian answer form for problem 9. The constants table prints Earth’s obliquity as 23.5′ and the Moon’s semimajor axis in km under an au heading. In the eclipse key, the magnitude addition and luminosity-ratio labels differ from its derivation and results; the original PDF correction comments are retained. Aldebaran’s key prints 4412 km/h and then uses 4416 in the angular-speed numerator. The X-ray question and key allocate points to parts (c) and (d) differently. DART’s alternative calculation prints both 0.17622 and 0.17662 m/s. The LISA key labels the component-mass calculation Part (b), repeats one algebra line and prints the period factor with a positive square. These printed discrepancies remain literal.
Оригинал в Архива: theory.pdf · официални решения: th_solutions.pdf