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Andromeda galaxy is the closest large galaxy and is visible to the naked eye. Estimate its brightness relative to the Sun, assuming it has luminosity\({\rm{1}}{{\rm{0}}^{{\rm{12}}}}\)times that of the Sun and lies\({\rm{2 Mly}}\)away.

Short Answer

Expert verified

The brightness related to the sun is obtained as: \(\eta = {\rm{ 6}}{\rm{.2 \times 1}}{{\rm{0}}^{{\rm{ - 11\;}}}}\).

Step by step solution

01

Relative brightness.

The relative brightness is given by,

\({\rm{Relative}}\,{\rm{Brightness}} = {\rm{luminosity}} \times \frac{{4\pi r_{sun}^2}}{{4\pi R_{Andromeda}^2}}\)

Here\({r_{sun}}\)is the radius of the sun,\({r_{Andromeda}}\)is the radius of the Andromeda galaxy.

02

Evaluating the brightness

A star's luminosity is a measurement of the overall amount of light it emits. If we know the star's luminosity, we can use the formula to compute its apparent brightness as:

\(F = \frac{L}{{4\pi {d^2}}}\)

The value of\(L\)is the brightness of the star.

The value of\(d\)is the distance to the star.

Using the formula to evaluate the ratio of apparent brightness for the sun and the Andromeda as:

\(\begin{array}{c}\eta = \frac{{{F_A}}}{{{F_S}}}\\ = \frac{{{L_A}d_S^2}}{{{L_S}d_A^2}}\end{array}\)

Values are then corresponding to Andromeda which is then denoted by the value of\({\rm{A}}\).

The value of\({\rm{S}}\)denoted for the sun.

Putting the values and then we obtain:

\(\begin{array}{c}\eta {\rm{ }} = {\rm{ }}\frac{{{\rm{(1}}{{\rm{0}}^{{\rm{12}}}}{\rm{ \times }}{{\rm{L}}_{\rm{S}}}{\rm{)(1}}{\rm{.58 \times 1}}{{\rm{0}}^{{\rm{ - 5}}}}{\rm{ly}}{{\rm{)}}^{\rm{2}}}}}{{{{\rm{L}}_{\rm{S}}}{{{\rm{(2 \times 1}}{{\rm{0}}^{\rm{6}}}{\rm{ly}} \times {\rm{9}}{\rm{.46}} \times {\rm{1}}{{\rm{0}}^{15}}\,{\rm{m/ly)}}}^{\rm{2}}}}}\\ = {\rm{ 6}}{\rm{.2 \times 1}}{{\rm{0}}^{{\rm{ - 11}}}}\end{array}\)

Therefore, the relative brightness of the Andromeda galaxy with respect to the sun is \({\rm{6}}{\rm{.2 \times 1}}{{\rm{0}}^{{\rm{ - 11}}}}\).

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Most popular questions from this chapter

Consider a star moving in a circular orbit at the edge of a galaxy. Construct a problem in which you calculate the mass of that galaxy in kg and in multiples of the solar mass based on the velocity of the star and its distance from the center of the galaxy.

(a) Use the Heisenberg uncertainty principle to calculate the uncertainty in energy for a corresponding time interval of\({\rm{1}}{{\rm{0}}^{{\rm{ - 43}}}}{\rm{ s}}\). (b) Compare this energy with the\({\rm{1}}{{\rm{0}}^{{\rm{19}}}}{\rm{ GeV}}\)unification-of-forces energy and discuss why they are similar.

(a) Estimate the mass of the luminous matter in the known universe, given there are\({\rm{1}}{{\rm{0}}^{{\rm{11}}}}\)galaxies, each containing\({\rm{1}}{{\rm{0}}^{{\rm{11}}}}\)stars of average mass\({\rm{1}}{\rm{.5}}\)times that of our Sun. (b) How many protons (the most abundant nuclide) are there in this mass? (c) Estimate the total number of particles in the observable universe by multiplying the answer to (b) by two, since there is an electron for each proton, and then by\({\rm{1}}{{\rm{0}}^{\rm{9}}}\), since there are far more particles (such as photons and neutrinos) in space than in luminous matter.

Lacking direct evidence of WIMPs as dark matter, why must we eliminate all other possible explanations based on the known forms of matter before we invoke their existence?

If neutrino oscillations do occur, will they violate conservation of the various lepton family numbers (\({{\rm{L}}_{\rm{e}}}\),\({{\rm{L}}_{\rm{\mu }}}\), and \({{\rm{L}}_{\rm{T}}}\))? Will neutrino oscillations violate conservation of the total number of leptons?

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