Lab 05: Jeans Mass, Jeans Length, and Free-Fall Time

Compute and compare gravitational-instability and collapse-timescale criteria for two real dense cores.

Apparatus and Setup

This lab computes Jeans mass, Jeans length, and free-fall time for the OMC-1 dense core and Barnard 68 side by side, and evaluates each against its own observed (or, for OMC-1, representative) mass.

Materials and Data

Coren(H2) (cm^-3)T (K)Observed mass (Msun)
OMC-1 dense core1.0e+0520(representative dense-core values; not individually mass-measured in this course's dataset)
Barnard 688.0e+04102.1

Standard published values, level 2 (Bergin & Tafalla 2007 for the representative dense-core values; Alves, Lada & Lada 2001 for Barnard 68's real measured mass, radius, and density).

Procedure

  1. Compute the Jeans length and Jeans mass for both cores using Lecture 09's formulas.
  2. Compute the free-fall time for both cores using Lecture 10's formula.
  3. For Barnard 68, compare the computed Jeans mass to its real observed mass (2.1 Msun) and state whether it is above, below, or comparable to the instability threshold.
  4. Using the observed star-formation efficiency per free-fall time (epsilon_ff~1-2%, Lecture 10), estimate an effective star-formation timescale for the OMC-1 core, and compare it to the core's own free-fall time.

Analysis and Uncertainty

Discuss explicitly why the simple Jeans criterion's idealized assumptions (uniform density, no turbulence, no magnetic support, no rotation) mean Barnard 68's near-critical Jeans-mass result should be read as "consistent with marginal instability," not as a precise, exact prediction of imminent collapse.

Deliverables

Assessment Criteria

References and Provenance