Problem Set 01: Solution Key

Stellar Properties, Spectra, and Classification

Worked Solutions

1. Stefan-Boltzmann for Rigel

L = (78.9)² × (12100/5778)⁴ = 6225.2 × 19.232 = 119725 L☉.

CriterionPoints
Setup and units5
Calculation5
Interpretation5

2. Inverse-square reasoning

F ∝ 1/d², so F_A/F_B = (d_B/d_A)² = (40/10)² = 16. Star A appears 16 times brighter than Star B.

CriterionPoints
Correct formula5
Correct ratio5
Correct direction (A brighter)5

3. Spectral classification physics

Balmer lines require neutral hydrogen atoms with their electron in the n=2 excited state. At the hottest temperatures (O/B stars), most hydrogen is ionized (no bound electron at all), so there are few neutral atoms available to produce Balmer absorption. At the coolest temperatures (K/M stars), most hydrogen remains in the unexcited ground state (n=1), unable to absorb Balmer-series photons. Only at intermediate temperatures near A0 (≈9,000-10,000 K) is a large fraction of hydrogen both neutral and in the n=2 excited state, maximizing Balmer line strength.

CriterionPoints
Correct ionization-fraction reasoning (hot end)8
Correct excitation-fraction reasoning (cool end)7

4. Textbook problem: Sirius system radii

Following the OpenStax worked derivation: with L_A/L_Sun and T_A/T_Sun known, R_A/R_Sun = √(L_A/L_Sun) × (T_Sun/T_A)². The textbook's worked example yields a radius ratio for Sirius A close to 1.7-1.8 R☉, consistent with this course's adopted value of 1.71 R☉ to within the precision of the simplified two-temperature comparison.

CriterionPoints
Correctly reproduces the OpenStax derivation steps8
Correct numeric comparison to course value7

Grading Notes

Award full marks for correct method, units, and a numeric result consistent with the arithmetic shown (allow reasonable rounding). Verify the student re-derives the number rather than quoting it from the lecture without adapting it to the problem's specific inputs.