Terms Developed in Context
free-fall time
The collapse timescale of an ideal pressureless, uniform-density sphere under its own gravity. In this lecture, the term is not an isolated label: This concept is needed to reason about gravitational collapse: free-fall time and the star-formation efficiency problem. For a uniform sphere of density rho collapsing purely under its own gravity from rest, integrating the equation of motion for a test particle at the sphere’s edge (using the shell theorem to justify treating only the interior mass) gives a closed-form collapse time to the center, the free-fall time t_ff = sqrt(3 pi/(32 G rho)) -- a classical result depending only on the initial density, not on the cloud’s total mass or size individually.
It is tied to the lecture’s observables or evidence in this way: If self-gravity is the only force acting (idealized, pressureless collapse), a uniform sphere collapses to a point in a finite time, the free-fall time, that depends only on the initial density -- a classical result of Newtonian gravity applicable to any self-gravitating fluid, from stellar interiors to molecular-cloud cores. A second connection is important for using the term in physical reasoning: This is a strict lower bound on the true collapse time for any cloud with additional support (thermal pressure, turbulence, magnetic fields, or rotation), since those all act to slow collapse relative to the pure free-fall rate; comparing a cloud’s actual observed lifetime or star-formation timescale to t_ff quantifies how much slower real collapse is than the idealized free-fall rate. The observational interpretation is constrained by If every Jeans-unstable molecular cloud in the Galaxy collapsed on its free-fall timescale and converted essentially all of its gas into stars, the Milky Way’s star-formation rate would be roughly one to two orders of magnitude higher than the observed rate (a discrepancy quantified across many studies, e.g. Zuckerman & Evans 1974; Krumholz & Tan 2007, ApJ 654, 304) -- clear observational evidence that something beyond simple free-fall collapse is regulating star formation.
Boundary and common confusion. Treating the free-fall time as a prediction of how long real star formation actually takes. It is explicitly a lower bound (the fastest possible collapse, absent any opposing physics); presenting t_ff itself as "the star-formation timescale" without the efficiency correction epsilon_ff is exactly the kind of overclaiming this course’s review standard requires catching and correcting. The term should therefore be applied only after identifying the measured quantity, the model assumption that links it to the desired physical quantity, and the regime in which that link remains valid.
gravitational collapse
Contraction driven by self-gravity when support and boundary forces cannot maintain equilibrium. In this lecture, the term is not an isolated label: This concept is needed to reason about gravitational collapse: free-fall time and the star-formation efficiency problem. This is a strict lower bound on the true collapse time for any cloud with additional support (thermal pressure, turbulence, magnetic fields, or rotation), since those all act to slow collapse relative to the pure free-fall rate; comparing a cloud’s actual observed lifetime or star-formation timescale to t_ff quantifies how much slower real collapse is than the idealized free-fall rate.
It is tied to the lecture’s observables or evidence in this way: If every Jeans-unstable molecular cloud in the Galaxy collapsed on its free-fall timescale and converted essentially all of its gas into stars, the Milky Way’s star-formation rate would be roughly one to two orders of magnitude higher than the observed rate (a discrepancy quantified across many studies, e.g. Zuckerman & Evans 1974; Krumholz & Tan 2007, ApJ 654, 304) -- clear observational evidence that something beyond simple free-fall collapse is regulating star formation. A second connection is important for using the term in physical reasoning: The empirically low star-formation efficiency per free-fall time (epsilon_ff~1-2%) is now understood, at least qualitatively, as resulting from turbulence continually creating and dissolving locally Jeans-unstable overdensities faster than they can fully collapse, combined with magnetic support (Lecture 14) and stellar feedback (radiation pressure, winds, and eventually supernovae) that removes gas or injects additional turbulent energy before an entire cloud can collapse at once. The observational interpretation is constrained by The empirically inferred star-formation efficiency per free-fall time, epsilon_ff (the fraction of a cloud’s mass converted to stars in one free-fall time), is measured to be only about 1-2% across a wide range of Galactic molecular clouds (Krumholz & Tan 2007; Evans et al. 2009, ApJS 181, 321) -- turbulence and magnetic fields (Lectures 08 and 14) are the leading physical explanations for why collapse is so inefficient rather than proceeding at the free-fall rate everywhere at once.
Boundary and common confusion. Treating the free-fall time as a prediction of how long real star formation actually takes. It is explicitly a lower bound (the fastest possible collapse, absent any opposing physics); presenting t_ff itself as "the star-formation timescale" without the efficiency correction epsilon_ff is exactly the kind of overclaiming this course’s review standard requires catching and correcting. The term should therefore be applied only after identifying the measured quantity, the model assumption that links it to the desired physical quantity, and the regime in which that link remains valid.
star-formation efficiency
The fraction of an available gas mass converted into stars over a specified region and time interval. In this lecture, the term is not an isolated label: This concept is needed to reason about gravitational collapse: free-fall time and the star-formation efficiency problem. The empirically low star-formation efficiency per free-fall time (epsilon_ff~1-2%) is now understood, at least qualitatively, as resulting from turbulence continually creating and dissolving locally Jeans-unstable overdensities faster than they can fully collapse, combined with magnetic support (Lecture 14) and stellar feedback (radiation pressure, winds, and eventually supernovae) that removes gas or injects additional turbulent energy before an entire cloud can collapse at once.
It is tied to the lecture’s observables or evidence in this way: The empirically inferred star-formation efficiency per free-fall time, epsilon_ff (the fraction of a cloud’s mass converted to stars in one free-fall time), is measured to be only about 1-2% across a wide range of Galactic molecular clouds (Krumholz & Tan 2007; Evans et al. 2009, ApJS 181, 321) -- turbulence and magnetic fields (Lectures 08 and 14) are the leading physical explanations for why collapse is so inefficient rather than proceeding at the free-fall rate everywhere at once. A second connection is important for using the term in physical reasoning: For a uniform sphere of density rho collapsing purely under its own gravity from rest, integrating the equation of motion for a test particle at the sphere’s edge (using the shell theorem to justify treating only the interior mass) gives a closed-form collapse time to the center, the free-fall time t_ff = sqrt(3 pi/(32 G rho)) -- a classical result depending only on the initial density, not on the cloud’s total mass or size individually. The observational interpretation is constrained by If self-gravity is the only force acting (idealized, pressureless collapse), a uniform sphere collapses to a point in a finite time, the free-fall time, that depends only on the initial density -- a classical result of Newtonian gravity applicable to any self-gravitating fluid, from stellar interiors to molecular-cloud cores.
Boundary and common confusion. Treating the free-fall time as a prediction of how long real star formation actually takes. It is explicitly a lower bound (the fastest possible collapse, absent any opposing physics); presenting t_ff itself as "the star-formation timescale" without the efficiency correction epsilon_ff is exactly the kind of overclaiming this course’s review standard requires catching and correcting. The term should therefore be applied only after identifying the measured quantity, the model assumption that links it to the desired physical quantity, and the regime in which that link remains valid.
star-formation rate
The stellar mass formed per unit time, distinct from the dimensionless efficiency of converting a gas reservoir. In this lecture, the term is not an isolated label: This concept is needed to reason about gravitational collapse: free-fall time and the star-formation efficiency problem. For a uniform sphere of density rho collapsing purely under its own gravity from rest, integrating the equation of motion for a test particle at the sphere’s edge (using the shell theorem to justify treating only the interior mass) gives a closed-form collapse time to the center, the free-fall time t_ff = sqrt(3 pi/(32 G rho)) -- a classical result depending only on the initial density, not on the cloud’s total mass or size individually.
It is tied to the lecture’s observables or evidence in this way: If self-gravity is the only force acting (idealized, pressureless collapse), a uniform sphere collapses to a point in a finite time, the free-fall time, that depends only on the initial density -- a classical result of Newtonian gravity applicable to any self-gravitating fluid, from stellar interiors to molecular-cloud cores. A second connection is important for using the term in physical reasoning: This is a strict lower bound on the true collapse time for any cloud with additional support (thermal pressure, turbulence, magnetic fields, or rotation), since those all act to slow collapse relative to the pure free-fall rate; comparing a cloud’s actual observed lifetime or star-formation timescale to t_ff quantifies how much slower real collapse is than the idealized free-fall rate. The observational interpretation is constrained by If every Jeans-unstable molecular cloud in the Galaxy collapsed on its free-fall timescale and converted essentially all of its gas into stars, the Milky Way’s star-formation rate would be roughly one to two orders of magnitude higher than the observed rate (a discrepancy quantified across many studies, e.g. Zuckerman & Evans 1974; Krumholz & Tan 2007, ApJ 654, 304) -- clear observational evidence that something beyond simple free-fall collapse is regulating star formation.
Boundary and common confusion. Treating the free-fall time as a prediction of how long real star formation actually takes. It is explicitly a lower bound (the fastest possible collapse, absent any opposing physics); presenting t_ff itself as "the star-formation timescale" without the efficiency correction epsilon_ff is exactly the kind of overclaiming this course’s review standard requires catching and correcting. The term should therefore be applied only after identifying the measured quantity, the model assumption that links it to the desired physical quantity, and the regime in which that link remains valid.
turbulence/magnetic support
Nonthermal resistance to collapse supplied by gas motions and magnetic stresses, neither of which acts as a simple isotropic thermal pressure in every geometry. In this lecture, the term is not an isolated label: This concept is needed to reason about gravitational collapse: free-fall time and the star-formation efficiency problem. This is a strict lower bound on the true collapse time for any cloud with additional support (thermal pressure, turbulence, magnetic fields, or rotation), since those all act to slow collapse relative to the pure free-fall rate; comparing a cloud’s actual observed lifetime or star-formation timescale to t_ff quantifies how much slower real collapse is than the idealized free-fall rate.
It is tied to the lecture’s observables or evidence in this way: If every Jeans-unstable molecular cloud in the Galaxy collapsed on its free-fall timescale and converted essentially all of its gas into stars, the Milky Way’s star-formation rate would be roughly one to two orders of magnitude higher than the observed rate (a discrepancy quantified across many studies, e.g. Zuckerman & Evans 1974; Krumholz & Tan 2007, ApJ 654, 304) -- clear observational evidence that something beyond simple free-fall collapse is regulating star formation. A second connection is important for using the term in physical reasoning: The empirically low star-formation efficiency per free-fall time (epsilon_ff~1-2%) is now understood, at least qualitatively, as resulting from turbulence continually creating and dissolving locally Jeans-unstable overdensities faster than they can fully collapse, combined with magnetic support (Lecture 14) and stellar feedback (radiation pressure, winds, and eventually supernovae) that removes gas or injects additional turbulent energy before an entire cloud can collapse at once. The observational interpretation is constrained by The empirically inferred star-formation efficiency per free-fall time, epsilon_ff (the fraction of a cloud’s mass converted to stars in one free-fall time), is measured to be only about 1-2% across a wide range of Galactic molecular clouds (Krumholz & Tan 2007; Evans et al. 2009, ApJS 181, 321) -- turbulence and magnetic fields (Lectures 08 and 14) are the leading physical explanations for why collapse is so inefficient rather than proceeding at the free-fall rate everywhere at once.
Boundary and common confusion. Treating the free-fall time as a prediction of how long real star formation actually takes. It is explicitly a lower bound (the fastest possible collapse, absent any opposing physics); presenting t_ff itself as "the star-formation timescale" without the efficiency correction epsilon_ff is exactly the kind of overclaiming this course’s review standard requires catching and correcting. The term should therefore be applied only after identifying the measured quantity, the model assumption that links it to the desired physical quantity, and the regime in which that link remains valid.
initial mass function (IMF)
The distribution of stellar birth masses, usually expressed as the number of stars formed per mass interval. In this lecture, the term is not an isolated label: This concept is needed to reason about gravitational collapse: free-fall time and the star-formation efficiency problem. The empirically low star-formation efficiency per free-fall time (epsilon_ff~1-2%) is now understood, at least qualitatively, as resulting from turbulence continually creating and dissolving locally Jeans-unstable overdensities faster than they can fully collapse, combined with magnetic support (Lecture 14) and stellar feedback (radiation pressure, winds, and eventually supernovae) that removes gas or injects additional turbulent energy before an entire cloud can collapse at once.
It is tied to the lecture’s observables or evidence in this way: The empirically inferred star-formation efficiency per free-fall time, epsilon_ff (the fraction of a cloud’s mass converted to stars in one free-fall time), is measured to be only about 1-2% across a wide range of Galactic molecular clouds (Krumholz & Tan 2007; Evans et al. 2009, ApJS 181, 321) -- turbulence and magnetic fields (Lectures 08 and 14) are the leading physical explanations for why collapse is so inefficient rather than proceeding at the free-fall rate everywhere at once. A second connection is important for using the term in physical reasoning: For a uniform sphere of density rho collapsing purely under its own gravity from rest, integrating the equation of motion for a test particle at the sphere’s edge (using the shell theorem to justify treating only the interior mass) gives a closed-form collapse time to the center, the free-fall time t_ff = sqrt(3 pi/(32 G rho)) -- a classical result depending only on the initial density, not on the cloud’s total mass or size individually. The observational interpretation is constrained by If self-gravity is the only force acting (idealized, pressureless collapse), a uniform sphere collapses to a point in a finite time, the free-fall time, that depends only on the initial density -- a classical result of Newtonian gravity applicable to any self-gravitating fluid, from stellar interiors to molecular-cloud cores.
Boundary and common confusion. Treating the free-fall time as a prediction of how long real star formation actually takes. It is explicitly a lower bound (the fastest possible collapse, absent any opposing physics); presenting t_ff itself as "the star-formation timescale" without the efficiency correction epsilon_ff is exactly the kind of overclaiming this course’s review standard requires catching and correcting. The term should therefore be applied only after identifying the measured quantity, the model assumption that links it to the desired physical quantity, and the regime in which that link remains valid.