Ram pressure stripping of galaxies: The long- and short-pulse limits
Joachim Köppen Kiel September 2017
Some brief explanations
This utility allows the user to estimate the consequences of ram pressure stripping on
the gas disk of a galaxy:
Is the ram pressure pulse longer than the period for vertical oscillations in
the galactic disk (typically 100 Myr), one may treat the problem by a quasi-static
argument (Gunn & Gott, 1972): gas is removed from the disk, if the ram pressure
exceeds the maximum of the vertical restoring force. This may also be called
the long-pulse limit, and the result depends on the maximum ram pressure.
If, on the other hand, the pulse is much shorter, it depends the amount of momentum
deposited in the gas element whether the gas can escape. This is called
the short-pulse limit, and the outcome depends on the time-integrated ram pressure
How much gas is removed from a given galaxy as the result of
a certain ram pressure history, is uniquely characterized on these two parameters if
the ram pressure is a pulse with e.g. a Lorentzian time profile.
The solution is best shown in the plane spanned by time-integrated ram pressurevΣ
and maximum ram pressurepmax. This utility allows the user
to explore this diagram.
For a given galaxy and a specified deficiency (i.e. stripped mass fraction)
the vΣ-pmax diagram marks the long-pulse limit with a black
line, the short-pulse limit with a blue line, and
the red curve as the interpolating curve
between the two limits. The red dot marks the intersection of the two limits. The green
line indicates the relation between vΣ and pmax
for a Lorentzian pulse with the specified pulse duration.
For the long-pulse limit the relations between the maximum ram pressure value
and the parameters for the outcome: stripping radius, lost mass fraction, deficiency
are shown.
Likewise, for the short-pulse limit the dependence of the outcome parameters on
the time-integrated ram pressure are displayed.
The model for the galaxy consists of a stellar bulge, a disk of stars and gas, and a dark
matter halo. Each component is specified by its parameters: total mass inside a truncation
radius and a radial scale length, with a scale height for the disk's components.
For comparison purposes, a point mass in the galactic centre may be added.
The maximum restoring force in the criterion of Gunn & Gott is computed from the
gravitational potential of the entire galaxy
Likewise, this potential is used to compute circular and escape speeds for the short-pulse
limit.
The display is controlled by:
X, Y: chose the abscissa and the ordinate among:
maximum ram pressure
time integrated ram pressure AKA (vΣ)ICM
gas mass fraction: the fraction of the inital mass that remains.
deficiency = log10(initial mass/remaining mass).
stripping radius = the outer radius of the remaining gas disk.
wipe&plot: clear the plot area and draws the last curve in red. Changing any
parameter value (and hitting the Enter key) will overplot the new curve in red.
overplot: after changing any parameter value, these button will overplot
the new curve in the corresponding colour.
Central point mass
Mass [MSUN] Bulge ( = Plummer sphere)
Mass [MSUN]
Radial scale [kpc]
Truncation radius [kpc] Stellar disk ( = Miyamoto-Nagai)
Mass [MSUN]
Radial scale [kpc]
Truncation radius [kpc]
Thickness [kpc] Gas disk ( = Miyamoto-Nagai)
Mass [MSUN]
Radial scale [kpc]
Truncation radius [kpc]
Thickness [kpc] Dark matter halo ( = Plummer sphere)
Mass [MSUN]
Radial scale [kpc]
Truncation radius [kpc]
stripped mass fraction
deficiency
pulse duration [Myr]