ASTR 410 · Lecture 08

Lecture 08: Dark Matter Halos and the Local Mass Budget

Galactic Astronomy

The same mass discrepancy appears in rotation, satellites, lensing, and structure formation, but each probe has distinct systematics.

Objectives and route

Why this question is hard

The same mass discrepancy appears in rotation, satellites, lensing, and structure formation, but each probe has distinct systematics.

Galactic astronomy observes projected light, velocities, and abundances from one moving vantage point. The inverse problem is underdetermined until geometry, selection, and a physical model are made explicit.

stellar diskextended halo
Halo Geometry: a lecture-specific schematic or model plot. Axes and annotations identify the inference being made; it is not presented as a raw survey image.

Terms for This Lecture

Dark-matter halo

Definition: The extended gravitating component surrounding a galaxy and dominating its mass at large radii in standard models.

Why it matters here: It connects local rotation evidence to satellite motions, lensing, and cosmological structure formation.

Relationship: Its density profile determines the halo contribution to the circular-speed curve.

Limitation or common confusion: It is distinct from the sparse stellar halo and its shape is not fixed by one probe.

Physical tool

The central relation for this lecture is:

\(\rho_{NFW}(r)=\rho_s/[x(1+x)^2]\)

Define every symbol before substitution. State the coordinate system, units, and approximation. A formula is evidence only when its assumptions match the tracer and regime.

Evidence display

The evidence display for this lecture is the labeled model/data relationship introduced above. Read the axes and annotations before accepting the inferred trend.

Data context: the accompanying values are standard published or survey-like values; see the course reference log for provenance level and spot-check targets.

Worked calculation

The local dynamical estimate is 1.0262e+11 solar masses inside 8.2 kpc.

It cannot by itself separate the radial mass contributions of disk, bulge, and halo.

Write the units beside each intermediate quantity. The numerical result is generated from the shared course constants and recomputed independently during review.

Interpret the pattern

Boundary condition and misconception

Do not overread the model: A flat curve alone does not determine a unique halo profile.

Ask whether changing the distance prior, selection function, or mass decomposition could move the conclusion. This is where a plausible diagram can become a misleading argument.

In-class reasoning

Prompt: Compare the enclosed mass from the local circular speed with a baryonic benchmark and state what is actually inferred.

First estimate the direction of the answer. Then calculate. Finally name one assumption that could reverse the interpretation.

Connection across the course

Takeaways

References and data status

OpenStax Astronomy 2e, Chapter 25, sections 25.1–25.4, and Chapter 26 for comparative context. Exact section and embedded-figure offsets were checked against the local extracted text before release.

Additional sources: Gaia Collaboration (2018, 2021) releases; Bland-Hawthorn & Gerhard (2016), ARA&A 54, 529; McMillan (2017), MNRAS 465, 76; Eilers et al. (2019), ApJ 871, 120; Bland-Hawthorn et al. (2019), Science 365, 859.

References are standard published values not independently re-fetched in this production session unless explicitly marked level 1 in reference-log.md.