IAO 2013, Практически тур, α/β — Задача 8. Jupiter. Analysis of observational data of Jupiter and its moons

XVIII Международная астрономическая олимпиада / XVIII International Astronomy Olympiad, Литва, Вильнюс, 6–14.IX.2013 / Vilnius, Lithuania — Practical round. Problems to solve · 6 септември 2013 г.

Условие

Observational data of Jupiter and its moons are given on separate sheets.
Your answers (measured values, results of calculations, used formulas) must be written in corresponding tables.

A. Group α — supplied rotational velocity

The separate sheet for group α supplies vr=12.6 km/sv_r=12.6\ \mathrm{km/s}.

Group α Part A: Jupiter rotation diagram and supplied speed 12.6 km/s

A. Group β — rotational velocity

Spectrum of Jupiter (Fig. 1) was obtained when the slit of a spectrograph was aligned along the planet’s equator. Wavelengths (λ\boldsymbol{\lambda}) of several recognized lines are shown. Due to Jupiter rotation the reflected Sunlight was affected by the Doppler effect. The spectral lines become inclined, because the spectrum of light reflected from the receding part of Jupiter is red-shifted, and of light reflected from the approaching part is blue-shifted. Non-inclined lines, which are visible in the spectrum, were formed in the Earth atmosphere.

Fig. 1. Jupiter spectrum, labelled wavelengths in nm and inclined spectral lines

Table A

N [nm/mm] = ______

λ\lambda (nm)dx (mm)dλd\lambda (nm)vrv_r (km/s)

vr_avgv_{r\_avg} [km/s] = ______

Formulae

vrv_r [km/s] = ______

A.1. Evaluate the mean scale of the given spectral interval (N), in nm per mm.

A.2. Measure the difference between the uppermost and the lowermost end of an inclined spectral line in mm (dx) and convert it into nm (dλ\mathbf{d}\boldsymbol{\lambda}). Do this for 3 lines independently.

A.3. Calculate the equatorial rotational velocity of Jupiter (vr\mathbf{v_r}) for each measured line and the final averaged value (vr_avg\mathbf{v_r\_avg}).

B. Equatorial rotational period and radius

Two CCD images of Jupiter are shown in Figs. 2 and 3. The vertical lines in figures marks the position of the projection of Jupiter‘s rotation axis (we assume it is perpendicular to the line of sight). The rotation period can be obtained from horizontal shifts of stable atmospheric features located relatively close to the equator.

Fig. 2. Jupiter on 2011-11-20 at 21:37:01 UTC, axis and feature 1 marked
Fig. 3. Jupiter on 2011-11-20 at 23:28:36 UTC, axis and feature 1 marked

Table B

dt [s] = ______

Featurex1x_1 (mm)x2x_2 (mm)LxL_x (mm)ϕ\phi (°)
1
2
3

ϕavg\phi_{\mathrm{avg}} = ______

PJeP_{Je} [h] = ______

RJeR_{Je} [km] = ______

Formulae

ϕ\phi [°] = ______

PJeP_{Je} [h] = ______

RJeR_{Je} [km] = ______

B.1. What time interval in seconds (dtdt) separate these images?

B.2. One feature useful for measurements is already marked “1”. Select and mark two additional features as “2” and “3” in both pictures.

B.3. Measure distances from the central vertical line to the marked features in both images (x1x_1 and x2x_2, respectively) and to the Jupiter limb at the feature’s latitude (LxL_x).

B.4. Calculate the rotational angle (ϕ\phi) for each feature.

B.5. Calculate the averaged value of rotational angle (ϕ_avg\phi\_avg).

B.6. Calculate the rotational period (PJeP_{Je}), in hours.

B.7. Calculate Jupiter‘s equatorial radius (RJeR_{Je}), in km.

C. Mass and density

Figs. 4-6 display observations of three Jupiter moons obtained during five successive nights in September 2011. Abscissa in those figures is time of observation measured in hours from the beginning of the observing session. Ordinate is the angular distance (in angular minutes) of the moon from the center of Jupiter at the moment of observation. The equatorial radius of Jupiter in the angular seconds is also given for some moments.

Fig. 4. Moon 1: angular distance from Jupiter versus time, with Jupiter angular-radius values
Fig. 5. Moon 2: angular distance from Jupiter versus time, with Jupiter angular-radius values
Fig. 6. Moon 3: angular distance from Jupiter versus time, with Jupiter angular-radius values

Table C

MoonPmP_m (h)aJea_{Je}a (m)MJM_J (kg)
1
2
3

MJ_avgM_{J\_avg} [kg] = ______

Rp/ReR_p/R_e = ______

RJ_avgR_{J\_avg} [km] = ______

V [m³] = ______

ρJ\rho_J [kg/m³] = ______

Formulae

MJM_J [kg] = ______

RJ_avgR_{J\_avg} [km] = ______

C.1. Estimate the period of revolution of each Jupiter‘s moon (PmP_m), in hours.

C.2. Estimate the semimajor axis of the orbit of each Jupiter‘s moon expressed in Jupiter‘s equatorial radii (a_Jea\_Je) and convert it into meters (aa).

C.3. Use your mesurements of each moon to calculate the mass of Jupiter (MJM_J) independently.

C.4. Calculate the averaged value of Jupiter mass (MJ_avgM_{J\_avg}).

C.5. From Jupiter image estimate the ratio of Jupiter‘s polar and equatorial radii (Rp/ReR_p/R_e).

C.6. Calculate the mean radius of Jupiter (RJ_avgR_{J\_avg}).

C.7. Calculate the density of Jupiter (ρJ\rho_J).

Решение


Оригинал в Архива: pract8.pdf · официални решения: ab8sol1.png · допълнителни данни: ab8sol2.png · допълнителни данни: ab8sol3.png · допълнителни данни: alphapract8data.pdf · допълнителни данни: betapract8data.pdf · допълнителни данни: jupiter.pdf · допълнителни данни: moons.pdf · допълнителни данни: table_a.png · допълнителни данни: table_b.png · допълнителни данни: table_c.png · допълнителни данни: betapract8.pdf