IOAA 2017, Анализ на данни — Задача 2. The search for dark matter

Data Analysis Examination · 75 т.

Указания
  1. The data analysis examination lasts for 4 hours and is worth a total of 150 marks.
  2. Dedicated IOAA Summary Answer Sheets are provided for writing your answers. Enter the final answers into the appropriate boxes in the corresponding Summary Answer Sheet. On each Answer Sheet, please fill in
    • Student Code (Country Code and 1 digit)
  3. Graph Papers are required for your solutions. On each Graph Paper, please fill in
    • Student Code (Country Code and 1 digit)
    • Question no.
    • Graph no. and total number of graph papers used.
  4. There are Answer Sheets for carrying out detailed work/rough work. On each Answer Sheet, please fill in
    • Student Code (Country Code and 1 digit)
    • Question no.
    • Page no. and total number of pages.
  5. Start each problem on a separate Answer Sheet. 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.
  6. Use as many mathematical expressions as you think that 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).
  7. You are not allowed to leave your working desk without permission. If you need any assistance (malfunctioning calculator, need to visit a restroom, need more Answer Sheets, etc.), please draw the attention of the invigilator using the sign card.
  8. The beginning and end of the examination will be indicated by a long sound signal. Additionally, there will be a buzzer sound, fifteen minutes before the end of the examination (before the final sound signal).
  9. At the end of the examination you must stop writing immediately. Sort and put your Summary Answer Sheets, Graph Papers, and Answer Sheets for each part (D1 and D2) in separate stack. You are not allowed to take any sheet of paper out of the examination area.
  10. Wait at your table until your envelope is collected. Once all envelopes are collected, your student guide will escort you out of the examination area.
  11. A list of constants is given on the next page.
Table of constants
Mass (M⊕M_{\oplus})5.98×10245.98 \times 10^{24} kgEarth
Radius (R⊕R_{\oplus})6.38×1066.38 \times 10^{6} m
Acceleration of gravity (gg)9.8 m s−2^{-2}
Obliquity of Ecliptic23°27’
Length of Tropical Year365.2422 mean solar days
Length of Sidereal Year365.2564 mean solar days
Albedo0.39
Mass(M☾)7.35×10227.35 \times 10^{22} kgMoon
Radius (R☾)1.74×1061.74 \times 10^{6} m
Mean distance from Earth3.84×1083.84 \times 10^{8} m
Orbital inclination with the Ecliptic5.14°
Albedo0.14
Apparent magnitude (mean full moon)-12.74
Mass (M⊙M_{\odot})1.99×10301.99 \times 10^{30} kgSun
Radius (R⊙R_{\odot})6.96×1086.96 \times 10^{8} m
Luminosity (L⊙L_{\odot})3.83×10263.83 \times 10^{26} W
Absolute Magnitude (M⊙\mathcal{M}_{\odot})4.80 mag
Angular diameter0.5 degrees
1 au1.50×10111.50 \times 10^{11} mPhysical constants
1 pc206,265 au
Distance from Sun to Barnard’s Star1.83 pc
Gravitational constant (GG)6.67×10−11 N⋅m2⋅kg−26.67 \times 10^{-11}\ \mathrm{N \cdot m^{2} \cdot kg^{-2}}
Planck constant (hh)6.62×10−34 J⋅s6.62 \times 10^{-34}\ \mathrm{J \cdot s}
Boltzmann constant (kBk_{\mathrm{B}})1.38×10−23 J⋅K−11.38 \times 10^{-23}\ \mathrm{J \cdot K^{-1}}
Stefan-Boltzmann constant (σ\sigma)5.67×10−8 W⋅m−2⋅K−45.67 \times 10^{-8}\ \mathrm{W \cdot m^{-2} \cdot K^{-4}}
Hubble constant (H0H_0)72 km s−1^{-1} Mpc−1^{-1}
Speed of light in vacuum (cc)299,792,458 m s−1^{-1}
Proton mass938.27 MeV ⋅\cdot c−2^{-2}
Deuterium mass1875.60 MeV ⋅\cdot c−2^{-2}
Neutron mass939.56 MeV ⋅\cdot c−2^{-2}
Helium-3 mass2808.30 MeV ⋅\cdot c−2^{-2}
Helium-4 mass3727.40 MeV ⋅\cdot c−2^{-2}

Условие

A low surface brightness galaxy (LSB) is a diffuse galaxy with a surface brightness that, when viewed from the Earth, is at least one magnitude lower than the ambient night sky.

Some of its matter is in the form of “baryonic” matter such as neutral hydrogen gas and stars. However, most of its matter is in the form of invisible mass – so called “dark matter”. In this question, we will investigate the mass of dark matter in a galaxy, the effect of dark matter on the rotation curves of the galaxy, and the distribution of dark matter in the galaxy.

The table below provides the data of a LSB galaxy named UGC4325. The galaxy is assumed to be edge-on. At every distance rr from the centre of the galaxy, we measure

  1. λobs\lambda_{\mathrm{obs}}, the observed wavelength of the Hα\alpha emission line. The Hubble expansion of the Universe has already been excluded from the data.
  2. VgasV_{\mathrm{gas}}, the contribution of the gas component to the rotation due to MgasM_{\mathrm{gas}}, derived from HI surface densities.
  3. V∗V_*, the contribution of the stellar component to the rotation due to M∗M_*, derived from RR-band photometry.

The rotational velocities of the test particle due to the gas component, VgasV_{\mathrm{gas}}, and the star component, V∗V_*, are defined as the velocities in the plane of the galaxy that would result from the corresponding components without any external influences. These velocities are calculated from the observed baryonic mass density distributions.

rr (kpc)λobs\lambda_{\mathrm{obs}} (nm)VgasV_{\mathrm{gas}} (km/s)V∗V_* (km/s)
0.70656.3712.8720.97
1.40656.4316.7532.22
2.09656.46414.1440.91
2.79656.47520.1846.75
3.49656.47824.0850.10
4.89656.48428.0847.94
6.25656.48129.2545.47
7.10656.48127.0347.78
9.03656.48225.9045.32
12.05656.48221.0342.30

The mass of dark matter MDM(r)M_{\mathrm{DM}}(r) within a volume of radius rr can be defined in terms of the rotational velocity due to dark matter VDMV_{\mathrm{DM}}, the radius rr and gravitational constant GG,

MDM(r)=rVDM2G.(1)M_{\mathrm{DM}}(r) = \frac{rV_{\mathrm{DM}}^2}{G}. \qquad (1)

To a good approximation, the observed rotational velocity VobsV_{\mathrm{obs}} can be modelled as

Vobs2=Vgas2+V∗2+VDM2.(2)V_{\mathrm{obs}}^2 = V_{\mathrm{gas}}^2 + V_*^2 + V_{\mathrm{DM}}^2. \qquad (2)

The observed rotational velocity VobsV_{\mathrm{obs}} depends on the mass of the galaxy M(r)M(r) within a volume of radius rr measured from the galaxy’s centre.

The mass density ρDM(r)\rho_{\mathrm{DM}}(r) of dark matter within a volume of radius rr can be modelled by a galaxy density profile,

ρDM(r)=ρ01+(rrC)2(3)\rho_{\mathrm{DM}}(r) = \frac{\rho_0}{1 + \left(\dfrac{r}{r_{\mathrm{C}}}\right)^2} \qquad (3)

where ρ0\rho_0 and rCr_{\mathrm{C}} are the central density and the core radius of the galaxy, respectively. According to the density profile, the mass of dark matter MDM(r)M_{\mathrm{DM}}(r) within a volume of a radius rr can be described by

MDM(r)=4πρ0rC2[r−rCarctan⁡(r/rC)].(4)M_{\mathrm{DM}}(r) = 4\pi\rho_0 r_{\mathrm{C}}^2\left[r - r_C \arctan(r/r_C)\right]. \qquad (4)

Part 1 The mass of dark matter and rotation curves of the galaxy

(D2.1) In laboratories on Earth, Hα\alpha has an emitted wavelength λemit\lambda_{\mathrm{emit}} of 656.281 nm. Compute the observed rotational velocities of the galaxy VobsV_{\mathrm{obs}} and the rotational velocities due to the dark matter VDMV_{\mathrm{DM}} at distance rr in units of km s−1^{-1}.

For the different values of rr given in the table, compute the dynamical mass M(r)M(r) and the mass of dark matter MDM(r)M_{\mathrm{DM}}(r) in solar masses. [21 т.]

(D2.2) Create rotation curves of the galaxy on graph paper by plotting the points of VobsV_{\mathrm{obs}}, VDMV_{\mathrm{DM}}, VgasV_{\mathrm{gas}}, V∗V_* versus the radius rr and draw smooth curves through the points (mark your graph as “D2.2”).

Order the contribution of the different components to the observed velocity in descending order. [16 т.]

Part 2 Dark matter distribution

(D2.3) Take a data point at small rr and large rr to estimate ρ0\rho_0 and rCr_C. Note that for large values of xx, arctan⁡(x)≈π/2\arctan(x) \approx \pi/2 and at small xx, arctan⁡(x)≈x−x3/3\arctan(x) \approx x - x^3/3. [7 т.]

(D2.4) By comparing Equation (4) to a linear function, the central density ρ0\rho_0 could also be found by a linear fit. Plot an appropriate graph so that a linear fit can be used to find another value of ρ0\rho_0. Evaluate ρ0\rho_0 in units of M⊙_{\odot} kpc−3^{-3}. (Mark your graph as “D2.4”). If you cannot find the value of rCr_C from the previous part, use rC=r_{\mathrm{C}} = 3.2 kpc as an estimate for this part. [19 т.]

(D2.5) Compute logarithmic values of the dark matter density, ln⁡[ρDM(r)]\ln[\rho_{\mathrm{DM}}(r)], and plot the distribution of dark matter in the galaxy as a function of radius rr on graph paper. (Mark your graph as “D2.5”). [12 т.]

Отговори

Решение


Оригинал в Архива: DataAnalysis.pdf · официални решения: DataAnalysis_Solution.pdf