astro-ph/9511019 03 Nov 95 University of Arizona CHEMICAL Based on Received I I UCOLick Astronomy Department University of observations Steward Observatory University of EFFECTS ABUNDANCES Astronomy Department University of University of California and Observatory and the Smithsonian Church St S E Minneap olis obtained OF shieldsastroasutexasedu skillmanzonspaumnedu Rob ert dennislickucscedu robkasarizonaedu Gregory A Shields at CLUSTER Evan Dennis the Multiple Board C Kennicutt Jr D Skillman Institution and IN Zaritsky Santa of Astronomy and accepted VIRGO Arizona Tucson Mirror Texas Austin TX ENVIRONMENT Cruz CA MN Minnesota SPIRAL Astrophysics AZ a joint facility of the

ABSTRACT

We present new measurements of chemical abundances in H II regions in

spiral galaxies of the and a comparison of Virgo galaxies and eld

spirals With these new data there now exist nine Virgo spirals with abundance

measurements for at least four H II regions Our sample of Virgo galaxies ranges

from H I decient ob jects near the core of the cluster to galaxies with normal H I

prop erties far from the cluster core We investigate the relationship b etween H I

disk characteristics and chemical abundances to determine whether dynamical

pro cesses that remove gas from the disk such as stripping by the

also aect the chemical abundances

We divide the nine Virgo spirals into three groups of three galaxies each

those with strong H I deciencies intermediate cases and those with no H I

deciencies The three most H I decient Virgo spirals have larger mean

abundances to dex in OH than the spirals on the p eriphery of the

cluster This suggests that dynamical pro cesses asso ciated with the cluster

environment are more imp ortant than cluster membership in determining the

current chemical prop erties of spiral galaxies There is also weak evidence of

shallower abundance gradients in the H I decient Virgo spirals

We also compare the abundance prop erties of our Virgo sample to a

large sample of eld spirals studied by Zaritsky Kennicutt Huchra

Those authors found that the mean abundance of the disk gas increases with

increasing maximum circular velocity increasing luminosity and decreasing

earlier Hubble type but with a large disp ersion in the mean abundances

and abundance gradients The disp ersion in the prop erties of eld galaxies

and the small size of the Virgo sample make it dicult to draw denitive

conclusions ab out any systematic dierence b etween the eld and Virgo spirals

Nevertheless the H I decient Virgo galaxies have larger mean abundances than

eld galaxies of comparable luminosity or Hubble type while the spirals at the

p eriphery of the cluster are indistinguisha ble from the eld galaxies

Simple illustrative chemical evolution mo dels with infall of metalp o or gas

are constructed and compared to mo dels in which the infall is terminated The

mo dels are constrained by comparison with observed gas mass fractions current

formation rates and gas consumption times The mo del results indicate

that the curtailment of infall of metalp o or gas onto cluster core spirals may

explain part of the enhanced abundance However additional work is needed

particularly mo deling of the eects of truncating the outer gaseous disk within

the context of mo dels with radial gas transp ort

The increased abundances in cluster core latetype spirals relative to eld

galaxies may b e imp ortant in the interpretation of observations of these

galaxies Sp ecically we p oint to p ossible eects on the TullyFisher and

Cepheid variable distance determinations and the interpretation of colors in the

ButcherOemler eect

Subject headings galaxies abundances galaxies clustering galaxies

evolution galaxies galaxies intergalactic medium

galaxies structure galaxies distances nebulae H II regions

INTRODUCTION

Spiral galaxies are mo died by the environment within a rich cluster of galaxies see

reviews by Haynes and Whitmore and the introduction to Henry et al

Such eects as tidal stripping ram pressure stripping and ablation by the intracluster

medium must aect evolution The cluster environment clearly inuences galaxy

morphology Dressler Postman Geller and so a natural question is whether it

also aects the history and chemical evolution of galaxies Do es the cluster

environment predetermine galaxy morphology by solely inuencing initial conditions or

do es it continually inuence the evolution of a member galaxy Comparing the chemical

abundances of eld and cluster members may provide clues to these fundamental questions

Moreover a systematic abundance dierential b etween cluster and eld galaxies would have

implications for the stellar p opulations and could impact a number of currently p opular

distance indicators

The Virgo cluster due to its proximity provides the logical starting p oint for the study

of environmental eects on abundances in cluster spirals The Virgo cluster is irregular

and in some resp ects this compromises the study of environmental eects However the

extensive catalog of the p ositions morphologies and radial velocities of galaxies by

Binggeli Sandage Tammann allows a denition of the clusters structure In

addition the structure of the hot gas comp onent which has b een revealed through sensitive

mapping of the Xray emission made p ossible by ROSAT Boringer et al is very

similar to the galaxy distribution

Substantial evidence p oints to dierences b etween the spiral galaxies in the core of the

Virgo cluster and eld spiral galaxies Davies Lewis rst p ointed to a deciency in

H I gas in Virgo spirals when compared to eld spirals Giovanelli Haynes showed

that galaxies in the outer parts of the Virgo cluster and eight other clusters were less

decient in H I than the galaxies in the core of the cluster From H I synthesis observations

of Virgo cluster spirals Warmels concluded the H I deciencies could b e attributed

to a depletion of the H I at large galacto centric radii This was supp orted by Cayatte et al

CKBG

Because the star formation history of a galaxy is related to its gas content it is logical

to ask if the chemical abundances in the cluster spirals are dierent from those of eld

galaxies Shields Skillman Kennicutt SSK presented sp ectrophotometry of H II

regions in ve Virgo spirals The Virgo spirals app eared to b e considerably more metal

rich  dex than the typical galaxy in their eld sample SSK suggested that such a

dierence could result from dierences in infall or radial inow rates Henry et al

HPLC and Henry Pagel Chincarini HPC conducted intensive studies of two

Virgo spirals and found the evidence of a Virgoeld dierential less convincing

Hence the issue of chemical abundance anomalies in the Virgo cluster is unresolved

The existing data sets have b een to o small to address the most fundamental physical

question whether the chemical prop erties of the H I decient galaxies in the core of the

Virgo cluster are dierent from those of undisturb ed galaxies in Virgo or elsewhere We

have undertaken a larger investigation which is aimed at addressing these problems in four

ways by enlarging the Virgo sample choosing galaxies within Virgo that span the

range of observed H I prop erties using published data on the H I distributions within

galaxies to examine the relationship b etween the H I distribution and chemical abundance

and by comparing the prop erties of the Virgo galaxies to a much larger sample of eld

spirals than was previously available

This study includes measurements of more H II regions in the strongly H I decient

galaxies NGC and NGC for which SSK had only one H II region each and in

several spirals with mo derate or no H I deciency Our work increases the number of Virgo

spirals with abundance measurements of four or more H II regions to nine For a comparison

eld sample we use the data for eld spirals recently published by Zaritsky Kennicutt

Huchra ZKH

In this pap er we describ e the observations and discuss the implications for the questions

raised ab ove In Section we discuss the sample selection new observations data reduction

pro cedures and OH abundance determinations In Section we discuss the abundance

prop erties of the Virgo spirals test for any dep endence of abundance prop erties on cluster

lo cation or H I deciency and use the ZKH results to determine whether there are any

systematic dierences b etween the eld and cluster galaxies In Section we characterize

and quantify the abundance dierential seen for the H I decient spiral galaxies In Section

we assess these results in the context of a simple mo del for environmental eects on

chemical evolution and in Section we outline future observational pro jects and discuss

the implications of elevated abundances for other studies of cluster spirals

OBSERVATIONS

Galaxy Selection

The primary ob jective of this program is to measure H II region abundances for a large

number of Virgo cluster spirals that span a larger range of H I deciency Following SSK

we chose to restrict our sample to latetype spirals those classied as type Sb c or later in

the Revised ShapleyAmes Catalog RSA Sandage Tammann This was done to

limit the variation in abundances due to variations in galaxy type Oey Kennicutt

OK ZKH and to take advantage of the brighter H II regions in latetype galaxies

We compiled a list of spirals in this type range that were mapp ed in H I by Warmels

or Cayatte et al We then selected a subset of galaxies exhibiting the full

range of H I prop erties from galaxies clearly decient in H I NGC NGC NGC

to intermediate ob jects NGC NGC NGC and nally to those

lo cated in the outskirts of the cluster and exhibiting apparently normal H I distributions

NGC NGC NGC By limiting our interest to Sb c and Sc galaxies our

sample excludes the most H I decient spirals closest to the Virgo core These ob jects

are earlytype spirals SaSb which generally contain much fainter H II regions than the

latetype spirals Kennicutt Edgar Ho dge OK Their H II regions are to o faint for

this program future observations of these ob jects will provide an imp ortant additional test

for environmentally induced changes in the chemical evolution of spirals Figure shows a

map of the p ositions of the Virgo cluster spirals relative to the main structural features

identied and discussed by Binggeli Tammann Sandage see their Figure

Table summarizes the prop erties of the Virgo sample Listed are the pro jected

separation from M radial velocity RSA and RC types de Vaucouleurs et al

luminosity rotation velocity as determined from the H I rotation curve optical diameter as

dened in the RC and H I to optical diameter ratio where the H I diameter is dened as

the diameter at which the H I surface density falls b elow M p c following Warmels

Warmels has argued that the latter ratio is a go o d indicator of the degree to which

H I has b een removed from the disk Following ZKH we have adopted a distance of

Mp c for the Virgo cluster galaxies Tully which is in go o d agreement with the

recently measured Cepheid distance of Mp c for M Freedman et al Figure

shows the variation of D D for a sample of eld spirals compiled by Warmels

H O

plotted as a function of RC Ttype the error bars indicate the disp ersion among eld

spirals of the same type The corresp onding values for the Virgo spirals in our sample are

plotted as p oints and lab eled This plot demonstrates the large range in D D for a given

H O

Ttype in the eld sample the general tendency for smaller H I diameters among Virgo

spirals as a whole and the variation in D D within the Virgo sample

H O

The radial H I surface proles of the Virgo spirals are shown in Figure The p oints

represent the azimuthally averaged H I surface densities from Warmels and CKBG

and for NGC from van der Hulst et al while the solid lines represent the

mean distributions for eld spirals of the same morphological type from CKBG CKBG

demonstrate that the radial H I surface density distribution of a eld is

determined by its morphological type if it is normalized to the optical size of the galaxy

We have normalized the observed proles of the Virgo spirals in the same manner using

the D diameters from the RC Figure conrms the variation in H I deciency within

O

the Virgo sample esp ecially at the extremes eg compare NGC and NGC

with NGC We have ordered the panels in Figure in increasing D D relative

H O

to the mean for the appropriate Ttype with the result that the galaxies group into the

deciency groups discussed ab ove This sub division into three groups is in general

agreement with an indep endent classication by CKBG

Sp ectrophotometry

Sp ectrophotometry for H II regions in the Virgo spirals was obtained in April

and May using the Blue Channel Sp ectrograph on the Multiple Mirror Telescope

MMT The H II regions were identied from H images obtained by RCK using a fo cal

reducer CCD imager on the Steward Observatory m telescop e The images also provided

precise co ordinates and nuclear osets for the sp ectrophotometric observations Preference

in selection was given to bright H II regions that sample the greatest p ossible radial extent

within each galaxy

The observing setup at the MMT was identical to that describ ed in SSK The

sp ectrograph was used with the channel element intensied Reticon photon

counting detector When used with a gpm grating A longpass blo cking lter and

00 00

 ap erture it provided a wavelength coverage of A at approximately A

FWHM resolution Ob ject and sky ap ertures were b eamswitched every sec and total

integration times ranged from to sec dep ending on the brightness of the ob ject

and sky conditions Ob jects were observed at high zenith angles to avoid problems with

dierential refraction Observing conditions ranged from clear to thin clouds and b ecause

of the variable conditions and small ap erture sizes only relative line uxes are rep orted here

The sp ectra were calibrated using observations of standard from Filipp enko

Greenstein and Massey et al as well as the usual internal wavelength and

ateld lamp calibrations Fluxes and equivalent widths for the principal sp ectral lines

were then measured using the SPLOT package in IRAF We conrmed that the SPLOT

measurements agreed with the automated measuring techniques of ZKH Line strength

uncertainties were determined from the rms deviations in the adjacent continuum In

some cases the sky ap erture fell within the galaxy so the the ob ject sp ectrum constructed

by subtracting o the sky sp ectrum is contaminated This can articially increase the

emission line equivalent widths and the uncertainties in the line strengths and this eect

has not b een accounted for in our error estimates The Balmer lines were corrected for

underlying stellar absorption with an assumed constant equivalent width of A McCall

Rybski Shields MRS and then the reddening was determined from the relative

Balmer line strengths assuming the values for an electron temp erature of K and an

electron density of cm Bro cklehurst All line strengths were then corrected for

reddening using the Galactic reddening law compiled by Seaton as parameterized

by Howarth The resultant line strengths and asso ciated uncertainties are listed in

IRAF is distributed by the National Optical Astronomy Observatories which is op erated

by the Asso ciation of Universities for Research in Astronomy Inc AURA under co op erative

agreement with the National Science Foundation

Table

Abundance Determinations

The new sp ectra of H II regions rep orted here when combined with previously

measured sp ectra from SSK MRS HPLC and HPC provide data for a total of H II

regions in the Virgo galaxies listed in Table Because accurate measurements of the

electron temp erature are not available for the regions we have used the oxygen excitation

index R  O II O III H  I H to estimate the

nebular abundances Edmunds Pagel

To ensure consistency among the abundances measured for the various eld galaxies

and the ZKH eld galaxy sample we have applied the same empirical R abundance

calibration as used by ZKH for all of the Virgo cluster H II regions The ZKH calibration

is an average of three calibrations by Edmunds Pagel MRS and Dopita

Evans Since we are mainly interested in dierential comparisons of the abundance

prop erties of dierent ob jects the precise choice of the R calibration is not critical and

as argued by ZKH the use of three separate calibrations provides an explicit although

incomplete estimate of the error in the derived oxygen abundances Typically these

calibrations are based on directly measured electron temp eratures in the low abundance

regime and photoionizatio n mo del ts for high abundances low excitation Presumably

the uncertainties are greatest at the high abundance end see discussions in OK Henry

and Shields Kennicutt which applies to most of the Virgo cluster H II regions

In any case the derived abundance is monotonic in R over the excitation range of interest

here and it should b e meaningful at the very least as a relative abundance sequencing

parameter

Table lists the abundances derived in this way for the entire Virgo H II region sample

The OH abundances listed in Table show two asso ciated errors The rst error is

the result of propagating the formal errors of the emission line uxes into the empirical

calibration of R by ZKH The second set of errors in parentheses reect the uncertainty

of the R calibration adopted by ZKH In most cases the latter are signicantly larger

than the former Following ZKH we use these larger errors throughout our analysis unless

noted otherwise The derived abundances are plotted as a function of galacto centric radius

normalized to the eective radius following McCall in Figure The ordering of the

galaxies is identical to that used in Figure

Following ZKH we have tted a linear relation in log OH versus radius to the

abundances of the individual H II regions to determine the mean value of OH at a

ducial radius Like ZKH we use a fraction of the isophotal radius R as the ducial

O

radius ZKH found this preferable b ecause it is less sensitive than other choices to various

selection eects see discussion in ZKH The results from these ts are given in Table

and plotted in Figure Hereafter we will refer to the mean value as that taken at

R The errors in the mean abundances were determined in the standard manner for a

O

weighted linear leastsquares t where the weighting was inversely prop ortional to the

formal errors in R the rst set of errors in Table and normalized to give Chisquared

equal to one This prevents the uncertainties in the R calibration from propagating into

the uncertainty in the the mean abundance ie we are interested in the uncertainty in the

abundance dierences b etween galaxies and not the absolute uncertainty in the abundance

scale For calculating the gradients the second set of errors in Table the larger ones

were used since the uncertainty in the absolute calibration is relevant to the uncertainty in

the magnitude of the gradient

Note that the outermost H II region in NGC lies well ab ove the trend established

by the other H II regions As a result the calculated mean abundance is slightly higher and

the abundance gradient is slightly shallower than would result from a determination based

on the inner H II regions At this time we have no reason to drop this discrepant p oint

from the t or to choose a more complex tting function From a comparison of the results

in SSK HPLC and HPC it is quite p ossible for an error in the abundance of a single H II

region of dex and an error of this size would bring the outermost H II region in NGC

into line with the trend established in the inner galaxy However if the inection in

the abundance distribution in NGC is real then this galaxy deserves a more detailed

abundance study

THE EFFECT OF H I DEPLETION ON THE ABUNDANCES IN VIRGO

SPIRALS

General Trends in the Virgo Spirals

We b egin our analysis with a qualitative discussion of the abundances in the Virgo

galaxies based on a comparison of Figures and We fo cus on the question of whether

the H I decient Virgo galaxies have dierent abundance prop erties than the Virgo galaxies

with normal H I disks Figures and are generally consistent as to which galaxies are

decient in H I although the D D parameter is a limited indicator NGC NGC

H O

and NGC are clearly decient the latter two even at small radii NGC

NGC and NGC are outlying galaxies with normal H I disks The remaining

three galaxies are intermediate cases Comparing the H I data with the abundance patterns

in Figure we note that the p eripheral galaxies have strong radial gradients in OH and

reach rather low values log OH  at the largest radii In contrast the three

most H I decient galaxies show high abundances with little evidence for radial gradients

but note that the radial range of H II regions is very limited in the H I decient spirals

This is further illustrated in Figure which shows the characteristic OH values

and gradients from Table for the Virgo galaxies as a function of D D In the top

H O

panel of Figure a trend of decreasing OH with increasing D D is evident for the

H O

Virgo galaxies The top half of Figure shows that our grouping into three categories is

somewhat arbitrary as all nine Virgo spirals display a continuum of decreasing mean OH

with decreasing H I deciency

The b ottom panel of Figure illustrates the relationship b etween oxygen abundance

gradient and H I deciency Here we tentatively see weak evidence for a trend of stronger

gradient with decreasing H I deciency The most notable exception is NGC but as

noted ab ove a single linear t to the radial abundance trend in NGC is a p o or t

The evidence for a trend in abundance gradient trend is weak in part b ecause we have

conservatively included the uncertainty in the R calibration in the calculation of the

uncertainty in the gradient However the main problem with this comparison is that only

a small number of H II regions sampling a very restricted range of radius were measured in

the H I decient Virgo spirals Note that this comparison is further complicated b ecause

the range of radii prob ed in each galaxy is dierent and b ecause the radial normalization

the isophotal radius may also b e aected by the cluster environment

The number of Virgo galaxies available is obviously less than one would like and the

number of H II regions sampled p er galaxy is less than satisfactory for all but p erhaps two

or three of the galaxies It is p ossible that the trends shown by the Virgo galaxies in Figure

are simply statistical ukes On the other hand one cannot make these trends go away

simply by discarding any one galaxy The three H I decient galaxies have signicantly

higher characteristic abundances and p ossibly smaller gradients than the three galaxies

with normal H I prop erties

Comparison of the Virgo and Field Spirals

Do Virgo galaxies have dierent abundance prop erties than comparable eld galaxies

We have argued ab ove that the H I decient galaxies in the cluster core show higher

abundances than the outlying galaxies Studies of abundance patterns in eld galaxies

demonstrate that the mean abundances of disks are systematically correlated with galaxy

type luminosity and circular velocity eg Pagel Edmunds MRS Garnett

Shields Skillman Kennicutt Ho dge VilaCostas Edmunds VCE

OK ZKH and it is imp ortant to check that the patterns in Figure are not due to

underlying variations in those prop erties For example many of the Virgo spirals are very

luminous galaxies and so they might b e metalrich ob jects solely on that basis indep endent

of cluster environment

To address this issue we have used the ZKH survey to compare the abundances of the

Virgo galaxies to those of the eld galaxies as functions of absolute magnitude maximum

disk circular velocity V and morphological Ttype In Figure we have added the Virgo

C

spirals to the eld spirals from Figure of ZKH We exclude strongly barred spirals RC

B type from the comparison b ecause bars have b een shown to aect the gradient slop e

Pagel et al VCE ZKH Martin Roy Friedli Benz Kennicutt

Note that although none of the Virgo sample spirals are strongly barred four are classied

as transitional X types NGC NGC NGC and NGC In Figure

a we plot the mean OH and gradient as a function of M The H I decient Virgo

B

galaxies have higher oxygen abundances than the eld galaxies as exp ected from the earlier

discussion This is seen again in Figure b where the mean OH value is plotted against V

C

and in Figure c where the galaxies are plotted as a function of Ttype The outstanding

impression rendered by Figure is that the three H I decient Virgo spirals are al l at the top

of the abundance distributions of galaxies with similar properties

This is supp orted by a simple statistical test Each of the three H I decient Virgo

galaxies has the largest characteristic abundance for galaxies of its corresp onding Ttype

cf Figure c The N probability of this happ ening for each galaxy if the abundances

are distributed randomly within galaxies of the same Ttype are and

for NGC NGC and NGC resp ectively Because each of these presumably

represents an indep endent event the probability that all three would have the largest

abundances within galaxies of their Ttype by chance is We discuss other p ossible

factors in greater detail b elow but we conclude here that there is strong evidence that the

H I decient galaxies have elevated characteristic abundances

In making this comparison b etween Virgo spirals and eld spirals we need to b e careful

that we have not introduced a bias in the comp osition of the sample For example our

simple statistical test could b e biased by other factors that aect abundance ie we know

that luminosity and abundance are correlated This is related not only to the question of

the reality of any Virgo abundance dierential but also to the broader issue of how Hubble

types are inuenced by cluster membership In Figure we plot M and V versus Ttype

B C

There is no evidence that the H I decient group suers a bias in comparison to the eld

sample Among the H I decient Virgo spirals NGC is near the top of the distribution

in M and V but NGC and NGC are near to the middle of the distributions

B C

in V and nearer the b ottom in M Thus their higher mean abundances do not app ear

C B

to b e due to their intrinsic prop erties of luminosity or mass However the subsample of

intermediate galaxies may b e skewed All three intermediate galaxies are near the top of

the distributions in M and V for their Ttypes

B C

Finally we checked our result from the preceding section showing a dep endence of

OH on D D in the Virgo spirals ie we needed to check for such a trend in eld

H O

spirals Constructing a comparison for the eld galaxies is not straightforward Only ab out

twothirds of the galaxies in the ZKH sample have published H I synthesis observations and

unlike the uniform H I observations of the Virgo cluster sample the H I observations of the

eld galaxies were obtained with a large range in linear resolution Despite such diculties

a comparison was constructed and we found no evidence of a trend in OH with D D in

H O

the eld spirals This suggests that the trend is due to the eects of the cluster environment

and not a characteristic of galaxies in general

Are the H I Decient Virgo Spirals Chemically Dierent

From a comparison of ve Virgo spirals and nine eld spirals SSK found the Virgo

spirals to b e considerably more metal rich  dex than comparable eld spirals

HPLC added observations of NGC and HPC added observations of NGC These

observations were found to b e in general agreement with those of SSK From a comparison

of the three Virgo spirals with more than observed H II regions with ve eld spirals

HPC concluded that the Virgo spirals might b e more metal rich than the eld spirals by

ab out dex SSK HPLC and HPC all suggested that a uniform eld sample and

an understanding of eects due to galaxy mass and structure were needed b efore rm

conclusions ab out environmental inuences could b e drawn

We have addressed these concerns by increasing the number of observed Virgo galaxies

to nine increasing the number of observed H II regions in these galaxies and making the

comparison to the large uniform sample of ZKH By concentrating on the comparison

b etween the H I decient Virgo spirals and the eld and p eripheral cluster galaxies we have

claried the evidence of an abundance dierential In retrosp ect the need to separate the

Virgo galaxies into H I decient and H I normal classes is an obvious one The intended

exp eriment is to test for the eects of cluster environment on the ISM abundances of cluster

spirals so it makes sense to search for the eects in those galaxies which show evidence of

altering by the cluster environment

We conclude that H I decient spirals in the cluster core have larger abundances

than comparable eld spirals or outlying Virgo spirals It is noteworthy that the outlying

Virgo spirals are indistinguis habl e from eld galaxies of comparable type and luminosity

Quantifying the size of the abundance dierential is problematic due to the small sample

size the disp ersion in the eld comparison sample the change in b oth mean abundance and

gradient and the variation in dierential with the degree of H I deciency We will return

to this in the next section

QUANTIFYING THE ABUNDANCE DIFFERENTIAL

To mo del the eect of cluster environment on spiral abundance patterns it is necessary

to quantify the size of the abundance dierential that we claim to see For this we

concentrate on the three most H I decient galaxies in the Virgo sample Taking the

characteristic abundances group ed by morphological type and averaging the logarithmic

values we nd an average characteristic abundance of  for the T galaxies

from the ZKH sample This is dex or lower than the characteristic value for

NGC The T galaxies yield an average of  which is dex or

lower than NGC The T galaxies have an average of  which

is dex or lower than NGC although with only comparison galaxies a

statistical comparison for NGC do es not seem justiable

The ab ove analysis fo cuses on characteristic abundances but it is useful to compare

entire chemical abundance distributions to ensure that the choice of a ducial radius is

not biasing our result For example by restricting our comparison to the characteristic

abundances it is p ossible that we could underestimate the chemical comp osition dierence

in the H I decient Virgo spirals since the observed shallower gradients means that the

eect is largest at the last measured p oint To investigate this p ossibili ty we have

constructed Figure where the radial abundance patterns of the three most H I decient

Virgo spirals are compared to the abundance patterns of the nonbarred eld spiral galaxies

of comparable morphological type from the ZKH compilation The most striking case is

NGC shown in the top panel of Figure NGC has measured H II regions out

to R  and for which the data are consistent with no gradient Comparing the OH

E

at the last measured p oint for NGC with the median value for the comparison eld

galaxies the abundance dierential is again roughly dex The comparison for NGC

is less dramatic A similar comparison of the OH at the last measured p oint to the

median for the comparison sample yields a dierential of roughly dex Note however

that NGC has a lower luminosity than all but one of the comparison eld galaxies

and should therefore b e exp ected to have lower abundances than the comparison galaxies

NGC has a small comparison sample but shows a dierential similar to that seen in

NGC Thus using characteristic abundances and outermost measured p oints give

similar answers

Finally in Figure we construct a comparison of OH versus RR disk Vband

E

surface brightness and gas mass fraction similar to Figure of SSK We plot all of

the individual H II regions in the Virgo sample using dierent symbols for the H II regions

in H I decient intermediate and H I normal galaxies This comparison is relatively free of

distance uncertainties The disk Vband surface brightnesses were taken from the radial

averages of Ko daira et al The gas mass fractions were calculated by taking the

radial average molecular gas masses from Kenney Young the radial average H I

gas masses of Warmels and assuming a Vband masstolight ratio of for the disks

The gas mass fractions must b e considered very uncertain in an absolute sense particularly

due to the uncertainty of converting CO observations to a molecular mass surface density

and the assumption of a constant masstolight ratio for the stellar disk but there should

b e at least some sense in the relative ranking of radial gas mass fraction As p ointed out

by SSK the value of plotting OH versus gas mass fraction is that it shows that the elevated

abundances in the H I decient galaxies are not a result of otherwise normal galaxies simply

converting most of their gas into stars

In Figure we nd that the H II regions from the H I decient galaxies form a relatively

distinct group at the highest abundances in all three comparisons The oset b etween the

H I decient galaxies and the H I normal galaxies app ears to b e of  to dex in the

top two panels The middle panel the comparison with disk Vband surface brightness

app ears to show the greatest order in the separation b etween the H I decient intermediate

and H I normal groups VCE have shown that lo cal metallicity correlates well with radially

averaged disk surface brightness and have argued that the correlation is improved when

total surface brightness disk plus bulge light is used Ryder has conrmed the

metallicity surface brightness relationship using Iband surface photometry for southern

spirals and Fband surface photometry for of the spirals in the ZKH sample Our results

show that the abundance dierential app ears prominently in the comparison with surface

brightness In the comparison with there is less order in the distributions This could b e

interpreted as indicating that the dierent galaxies have exp erienced dierent evolutionary

histories or may just reect the uncertainty of the calculation of

It is imp ortant to recall that the most H I decient galaxies in the Virgo cluster are all

early type spirals which we excluded from our sample due to the diculty of measuring the

abundances of their very faint H II regions and additionall y due to the less extensive eld

galaxy comparison sample Conservatively we conclude from these data that abundance

dierentials at least as large as and plausibly as large as dex are pro duced by the

cluster environment When plotted in the metallicity surface brightness plane all three

H I decient galaxies stand apart from the H I normal spirals

INTERPRETATION OF THE VIRGO ABUNDANCE DIFFERENTIAL

Having empirically established the abundance dierential and provisionally quantied

the magnitude of the eect it is reasonable to ask if the observed eect is consistent with the

physical pro cesses known to b e op erating in the Virgo cluster environment Our framework

is that spiral galaxies are falling into the Virgo cluster Tully Shaya and that

removal of gas from the infalling spirals by the cluster environment is primarily resp onsible

for the H I deciencies observed Warmels We review the evidence supp orting these

mechanisms and then turn to the question of whether the observed abundance dierential

is consistent with this scenario

Overview of Cluster Pro cesses

Tully Shaya studied the phase space distribution of the galaxies in and near

the Virgo cluster and developed a mass distribution mo del in which galaxies within ab out

Mp c of the Virgo cluster are now falling back toward the cluster Two of our H I normal

galaxies NGC and NGC are predicted to enter the Virgo cluster environment

within the next Gyr Within their mo del the ma jority of the elliptical galaxies in Virgo

have b een there for a substantial fraction of the age of the universe while most spirals have

entered the cluster in the last onethird to onehalf of the age of the universe This implies

that the Virgo spirals were formed in lower density environments more like eld galaxies

and have only lately entered the high density cluster environment Additionally Dressler

compared the velocity disp ersions of H I decient and normal spirals in nine clusters

including Virgo and found that the H I decient galaxies were more likely on radial orbits

that would carry them into the cluster cores These results corresp ond well with our

observation that the spirals in the p eriphery of the cluster the H I normal galaxies have

abundance patterns similar to those observed in eld spirals and that the interaction with

the cluster environment not simply cluster membership is the determining factor for H I

deciency

Through H I synthesis mapping of Virgo spiral galaxies and a comparison with a

compilation of eld spirals Warmels conrmed the H I deciencies of the central

Virgo cluster galaxies He identied ram pressure stripping of the outer neutral gas by the

intracluster medium as the main cause of H I deciency based on four lines of evidence

First the D D ratios for the spirals in the inner three degrees of the cluster are much

H O

smaller than for b oth the cluster spirals which are at pro jected radii greater than ve

degrees and the eld spirals Second the scale lengths of the declining part of the radial H I

distributions of the inner Virgo spirals are smaller than those of the outer Virgo spirals

Third only the H I surface densities in the outer parts of the H I decient galaxies app ear

to b e aected although this conclusion has b een questioned by later studies Kenney

Young CKBG Fourth the H I distributions of the inner Virgo galaxies show large

asymmetries Warmels compared his observations with the predictions from mo dels of

galaxy collisions tidal stripping thermal evaporation and rampressure stripping and

concluded that the observations were only consistent with rampressure stripping mo dels

Following the simple mo del of Gunn Gott and assuming an intracluster density

of  cm and a galaxy velocity of km s Warmels was able to repro duce the

size of the eects observed Subsequently this simple mo del was shown to work for the

Virgo IC Skillman et al and Sancisi Thonnard Ekers

discovered a cloud of H I which app eared to b e stripp ed completely from a dwarf galaxy in

the vicinity of NGC see also Henning Sancisi McNamara

Kenney Young observed CO emission from Virgo cluster spirals and

compared the radially averaged neutral atomic and molecular gas distributions They

concurred with Warmels conclusion that the outer parts of the inner Virgo spirals were

H I decient but noted that the inner parts of those galaxies were also H I decient by a

factors of  Perhaps surprisingly Kenney Young found that the CO emission

from the H I decient Virgo galaxies was not decient This is esp ecially interesting in light

of the results of Kennicutt who found that star formation rates inferred from H

luminosities are lower in spirals in the Virgo cluster core than in comparable eld galaxies

However Kennicutt has shown that star formation rates do not correlate well with

the amount of molecular hydrogen present in the disk as inferred from CO observations

Because the CO emission is conned to the centers of spiral galaxies the normal CO

emission from H I decient spirals is not in conict with a mo del of ram pressure stripping

of the H I decient cluster spirals Note also that the ab ove discussion assumes a metallicity

indep endent conversion of CO emission to molecular gas content

CKBG have divided the Virgo cluster galaxies into four groups I normal I I

stripp ed by transp ort pro cesses such as turbulent viscosity and thermal conduction

Nulsen I I I rampressure stripp ed and IV completely stripp ed but recovering

The observational distinction b etween groups II and III is that group III galaxies have

smaller pro jected cluster radii larger central H I surface densities and smaller D D

H O

ratios than group II galaxies CKBG conclude that the group II galaxies are to o far from

the cluster core for rampressure stripping to dominate and that transp ort pro cesses which

would b e eective over the entire disk dominate Of our nine galaxies all three galaxies

in our H I decient group and the intermediate case NGC are classied as group I I

while the rest of the sample are classied as group I galaxies Our preference for latetype

spirals has excluded the type I I I and IV galaxies as all are Ttype and If the reasoning

presented by CKBG is true then we should b e trying to interpret the abundance dierential

b etween our group I and group I I galaxies within the framework of a stripping mo del based

on turbulent viscosity and thermal conduction and not rampressure stripping

Simple Mo dels with Termination of Infall

SSK argued that galaxies immersed in the hot gas of the Virgo cluster core would not

accrete primordial gas from their surroundings The lack of accretion might cause these

galaxies to evolve chemically like the simple closed b ox mo del of chemical evolution

whereas eld galaxies would have their abundances depressed by infall of metal p o or

gas The simple mo del predicts the relation Z y ln where Z is the abundance of

heavy elements y is the yield of heavy elements p er unit star formation and is the gas

mass fraction SSKs Figure suggests that the curtailment of infall might elevate the

abundances in the Virgo spirals by as much as  dex Since the H I decient Virgo

spiral H II regions have metallicities from dex to dex higher than the normal Virgo

spiral H II regions it would app ear that curtailment of infall alone is insucient to pro duce

the observed abundance dierential We will not attempt an exhaustive discussion of

alternative explanations for the Virgo abundance dierential but as an illustration we

have constructed some simple mo dels to obtain rough estimates of the dierential eects

on abundance color equivalent width and gas consumption time that might result from

termination of infall of metal p o or gas

Three observational constraints will b e used The rst constraint is the gas mass

fraction While the simple closed b ox mo del predicts Z y ln an infall mo del with

instantaneous recycling and constant M predicts Z y exp Larson

g

The second constraint is the present star formation rate SFR This is parameterized

by the ratio of the present SFR to the average SFR over the history of the disk b

SFR tSFR Scalo The conversion of b values into the observable prop erties

of H equivalent widths EW H and BV colors is very mo del dep endent However

Kennicutt Tamblyn Congdon KTC give relationships b etween b and the BV

colors and EW H for mo dels with steady or decreasing star formation rates similar to

our mo dels and we use them here The third constraint is the gas consumption time or

Rob erts time see discussion in KTC Following KTC we distinguish b etween

R

two values of the gas consumption time the total gas mass divided by the SFR and

R

the corresp onding ratio within the optical disk R alone

Rd O

In Table we list representative values for the Virgo galaxies in this study and for the

nonp eculiar eld galaxies in Table of KTC The rst line presents the average values of

the oxygen abundances for each of the three Virgo sample subgroups The EW H and

BV values for the Virgo galaxies are taken from Kennicutt Kent and the RC

resp ectively The EW H and BV values for the eld Scs are taken from Kennicutt

who also nds that the ratio of hydrogen to blue luminosity M L is ab out

H B

dex smaller in Virgo Scs than those in the eld The three Virgo groups show a progression

in EW from A for the H I decient galaxies to A for the normal galaxies consistent

with the prop osition that the outlying Virgo galaxies are like normal eld galaxies The

progression in colors likewise resembles the dierence b etween Virgo and eld Scs quoted

by Kennicutt From Table of KTC average values of b are for the Virgo core

galaxies and for the eld galaxies

Rob erts time values are also taken from KTC For our sample the values of and

R

esp ecially are smaller for the normal galaxies than for the H I decient galaxies This

Rd

means that the SFR in the optical disk is depressed by more than the gas mass and one

might sp eculate that the SFR drops precipitously as the gas surface density falls toward a

threshold value Quirk Kennicutt We adopt a lo cal gas consumption time of

Gyr as the baseline eld spiral the same as in the KTC mo del and roughly consistent

with the value of Gyr for the whole KTC sample

Rd

We construct mo dels that represent a typical eld Sc galaxy and then examine the

changes in chemical abundance and other observables when the infall is terminated Our

mo dels follow the evolution of the abundance of a primary element that is pro duced by

shortlived stars and ejected eectively instantaneously into the interstellar medium The

abundance is calculated in terms of the gross yield y the mass of the heavy elements

g

pro duced p er unit mass of gross star formation undiminished by return of gas by evolving

stars Note that the ab ove expressions for the simple and Larson mo dels involve the net

yield for instantaneous recycling this is y y R where R is the fraction of the stellar

g

mass returned to the interstellar medium Throughout we take y ie Z Z y

g g

Only a single zone is considered with an initial gas mass taken to b e unity There is no

escap e of gas or radial ow The infall rate is parametrized as f t f exp t where

f

mass is measured in the same arbitrary dimensionless units as M and t is in units of

g

Gyr The star formation rate SFR t is given by one of two alternative prescriptions

a linear Schmidt law SFR t M or SFR t f t r t where r

g s

is the rate at which gas is returned by dying stars The latter gives a constant gas mass

M t Larson which is motivated by the idea of a surface density threshold for

g

star formation Mass return from stars of various ages and corresp onding metallicities were

computed using the return rates given in Figure of KTC for the K IMF All mo dels

have nal ages of Gyr and infall ceases at Gyr in the truncation mo dels

Table lists the parameters and results of some illustrative mo dels The mo dels are

lab eled according to S or T for Schmidt Law or Threshold H or L for high or low infall

rate and N or C for no cuto or cuto of infall The rst four mo dels employ a SFR

prop ortional to gas density with Gyr To limit the number of free parameters

R s

we have taken a constant infall rate f t f The value of b is then tuned by adjusting

f Mo del SHN has f so that infall brings in p ercent of the initial gas mass

in Gyr This mo del has b after Gyr However the adopted IMF returns

p ercent of the mass of stars formed in an instantaneous burst by an age of Gyr and

most of this amount within Gyr Thus we have R  and the eective timescale of

conversion of gas to long lived stars is  R  Gyr Hence infall roughly

snet s

balances the net star formation keeping M and the SFR roughly constant This mo del

g

reaches an abundance Z and a gas fraction For comparison the simple

mo del predicts Z and a Larson infall mo del would predict Z in b etter

agreement with our mo del for the simple and Larson mo dels we have taken the net yield

to b e y y M M evaluated at the present ie t Gyr

g sg r oss snet

Mo del SHC shows the result of abruptly cutting o infall Gyr ago in a mo del

otherwise identical to Mo del SHN The result is an increase in Z of dex which is a

substantial fraction of the Virgo abundance dierential indicated by our observations The

star formation parameter drops from b to and decreases from to From

the KTC mo dels this increase in b corresp onds to an increase in BV of ab out dex in

rough agreement with the Virgoeld dierential but the drop in EW H by ab out

dex is ab out half that observed

Mo dels SLN and SLC give a similar comparison for an infall rate decreased by a factor

of four Mo del SLN with no cuto of infall results in lower values of b and and a higher

value of Z than in SHN Cutting o infall again decreases b and increases Z The drop

in b again implies roughly the observed increase in BV but somewhat to o little change in

EW H As exp ected when infall is less imp ortant the increase in Z is less dex

A larger increase in Z would require a larger t t ratio so that ln would decrease

c s

more We conclude from this set of mo dels that a cuto of infall several billion years ago is

roughly consistent with the colors of the Virgo spirals versus the eld but can account for

only part of the observed abundance dierential

The next four mo dels in Table are analogous pairs of mo dels for the case of a constant

gas mass M Note that in contrast to the previous mo dels when infall is cut o

g

the SFR drops precipitously b ecause only recycled gas is available for new star formation

As a result the infall cuto mo dels result in higher values of For the rst pair TLN

and TLC the mo del with infall cuto shows no increase in Z to o large a value of and

R

to o small a value of b Increasing the infall rate mo dels THN and THC results in a Z

increase comparable to the Schmidt Law mo dels but the problems with and b p ersist

R

Increasing the infall rate further in the cuto mo dels results in higher Z and lower but

R

b remains low

We conclude from this discussion that if late type eld spirals exp erience continuing

infall then curtailment of this infall when a galaxy enters the cluster environment may

elevate its chemical abundances by an amount of order to dex There will b e a

corresp onding reduction in the SFR roughly consistent with colors and H equivalent

widths This conclusion applies to mo dels in which star formation continues after infall

cuto in rough prop ortion to the gas mass However mo dels with a constant gas mass

fail to pro duce signicant abundance dierentials when constrained by colors and star

formation rates

FUTURE WORK AND IMPLICATIONS FOR OTHER STUDIES

The simple mo dels describ ed in the last section are not able to directly address the

eects of the cluster environment on the radial abundance gradients All of the mo dels with

continuing infall of signicant magnitude have abundances close to those predicted by the

analytic expression for the Larson infall mo del essentially Z  y for small Such mo dels

should result in very weak radial abundance gradients for radii at which remains small

In contrast strong radial gradients in OH and other ratios are typically observed eg

Figure This is one reason to consider mo dels in which strong radial gas ows o ccur A

number of authors have considered the role of radial gas ows in the chemical evolution of

disk galaxies Mayor Vigroux argue that infall will induce radial ows and derive

a radial abundance gradient similar to that observed in the Milky Way Radial gradients

caused by radial inow are discussed by Tinsley Larson and Gotz Koppen

Lacey Fall Clarke SommerLarson Yoshii and

Edmunds Greenhow have explored mo dels in which gas can ow b oth inward and

outward

SSK noted that the removal of the outer H I disk would prevent radial inow of metal

p o or gas The lack of inow might lead to at abundance gradients and elevated overall

abundance values Our conclusion that curtailment of infall contributes at most a fraction

of the observed Virgo abundance dierential emphasizes that other pro cesses including

radial inow should b e considered We hop e that the simple mo deling in the previous

section will help to illustrate how the Virgo abundance dierential together with other

data such as colors star formation rates and gas masses can b e used to gain insight into

the chemical evolution of galaxies

Determining the mechanism that gives rise to the abundance dierential is b eyond the

scop e of this investigation and clearly there remain some p otentially fruitful observational

pro jects First it would b e desirable to extend this type of study to the earlier type spirals

in the Virgo cluster core including the group I I I and IV galaxies of CKBG The intriguing

prop osition that the inner disks of the group III galaxies are unaected suggests that one

might not see an abundance dierential there The hypothesis that group IV galaxies have

an ISM which consists purely of recent stellar mass loss may aord the opp ortunity for

direct measurement of stellar yields Additional observations of H II regions in the galaxies

studied here would not only improve the statistical arguments but might provide additional

information b eyond the characteristic numbers discovered here see Zaritsky It

would also b e of great interest to carry out a similar investigation for other clusters In

rich clusters like A A and Coma rampressure stripping will b e imp ortant out to

a greater radius and large samples of severely truncated group I I I galaxies are present

Giovanelli Haynes Finally observations of the abundances in the spiral galaxies

in the Hydra I cluster would provide a valuable control sample as these cluster spirals show

no evidence of a correlation of H I deciency with cluster radius McMahon

This work has implications b eyond a b etter understanding of the chemical evolution

of eld and cluster spiral galaxies Foremost are implications for distance determination

studies The elevated abundances of H I decient cluster spirals may impact b oth

TullyFisher and distance determinations For example if the dust

content of spiral galaxies scales with abundance van den Bergh Pierce and the

opacity corrections for galaxy luminosity are imp ortant see Giovanelli et al for a

recent discussion then there will b e a systematic oset b etween cluster and eld spiral

galaxy TullyFisher relationships It is also p ossible that chemical abundance studies will

provide insight into the pro cesses by which gas is removed from spiral galaxies as they

enter the cluster environment This may in turn lead to a more secure interpretation of

current studies of the evolution of cluster galaxies eg Dressler et al A b etter

understanding of the chemical abundance patterns in b oth eld and cluster spirals would

put these studies on rmer ground

Throughout this work we have b eneted from discussions with M Edmunds D

Garnett R Henry B Pagel J van Gorkom We gratefully acknowledge supp ort from

NASALTSARP grant NAGW EDS NSF grants AST and AST

RCK and STScI grant GOA GAS RCK would like to thank the Department

of Astronomy at the University of Texas for their generous hospitality and the supp ort of

the Beatrice M Tinsley Centennial Professorship GAS would like to acknowledge supp ort

from the William F Marlar Memorial Foundation and the hospitality and supp ort of the

Department of Space Physics and Astronomy Rice University during Spring We all

acknowledge the capable MMT op erators Carol Heller John McAfee and Janet Miller We

thank an anonymous referee for very helpful comments

TABLE

Virgo Cluster Spiral Galaxy Properties

a b c d e f g h i

Name R Velocity Type TType L V D D D R

c

M B O H O E

 0 0

NGC Scs

 0 0

NGC Scs

 0 0

NGC Scs

 0 0

NGC Sb cs

 0 0

NGC Scs

 0 0

NGC SBcs

 0 0

NGC SBcrs

 0 0

NGC Scs

 0 0

NGC Scs

a

Pro jected distance from M

b

Radial velocity with resp ect to the Galactic center of rest from the RC

c

Morphological type from the RSA

d

Morphological type from the RC

e o

from the Blue Lumminosity in units of L assuming all galaxies at the distance of Mp c and using B

T

RC

f

Maximum rotation curve velocity in km s from Warmels

g

Corrected optical diameter D from the RC

O

h

HI to optical diameter ratio as dened by Warmels

i Disk eective radius derived from the photometry of Ko daira et al

TABLE a

Dereddened Spectra

 Identication NGC NGC NGC NGC NGC NGC NGC NGC

O I I        

H                

H        

H        

O I I I                        

O I I I        

H        

N I I        

S I I              

S I I              

cH        

EWH

TABLE b

Dereddened Spectra

 Identication NGC NGC NGC NGC NGC NGC NGC

O I I       

H           

H       

H       

O I I I         

O I I I       

H       

N I I       

S I I       

S I I       

cH       

EWH

TABLE c

Dereddened Spectra

 Identication NGC NGC NGC NGC NGC NGC NGC

O I I       

H             

H           

H       

O I I I             

O I I I       

H       

N I I       

S I I           

S I I           

cH       

EWH

TABLE d

Dereddened Spectra

 Identication NGC NGC NGC NGC NGC NGC NGC NGC

O I I        

H        

H        

H        

O I I I                

O I I I        

H        

N I I        

S I I          

S I I                

cH        

EWH

TABLE

Virgo Sample H I I Region Abundances

HI I Region RR logR logOH Reference

E

NGC

  MRS

  HPC

  HPC

  HPC

  MRS

  HPC

  HPC

  MRS

  SSK

  HPC

  MRS

  MRS

  HPC

  MRS

  HPC

  SSK

  SSK

  HPC

  HPC

NGC

  SSK

  HPLC

  SSK

  HPLC

  SSK

  HPLC

  HPLC

  HPLC

  SSK

  SSK

  SSK

  HPLC

  HPLC

  HPLC

  SSK

  SSK

  HPLC

  HPLC

  SSK

  SSK

  HPLC

  HPLC

TABLE Continued

HI I Region RR logR logOH Reference

E

NGC

  MRS

  MRS

  SSK

  MRS

  SSK

  MRS

  SSK

  SSK

  SSK

  MRS

NGC

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

NGC

  SKSZ

  SSK

  SKSZ

  SKSZ

NGC

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

NGC

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

  SKSZ

NGC

  SKSZ

  SKSZ

  SKSZ

  SSK

  SKSZ

NGC

  SKSZ

  SKSZ

  SKSZ

  SKSZ

TABLE

Characteristic Abundances and Abundance Gradients

Name log OH Gradient

at R dexR

O O

NGC  

NGC  

NGC  

NGC  

NGC  

NGC  

NGC  

NGC  

NGC  

TABLE

Comparison of Average Characteristic Properties

Prop erty Virgo HI Decient Virgo Intermediate Virgo HI Normal Field

log OH   

EW H A

BV

 yrs

R

 yrs

R;d

TABLE

Results of Model Calculations

Mo del SHN SHC SLN SLC TLN TLC THN THC

infall rate

           

s

           

f

M

g

M gross

s

M net

s

Z

Z simple

Z Larson

SFR

M SFR

g

b

REFERENCES

Binggeli B Sandage A Tammann G A AJ

Binggeli B Tammann G A Sandage A AJ

Bohringer H Briel U G Schwarz R A Voges W Hartner G Trumper J

Nature

Bro cklehurst M MNRAS

Cayatte V van Gorkom J H Balkowski C Kotanyi C AJ

Cayatte V Kotanyi C Balkowski C van Gorkom J H AJ CKBG

Clarke C J MNRAS

Davies R D Lewis B M MNRAS

de Vaucouleurs G de Vaucouleurs A Corwin H G Jr Buta R J Paturel G

Fouque P Third Reference Catalogue of Bright Galaxies New York

SpringerVerlag RC

Dopita M A Evans I N ApJ

Dressler A ApJ

Dressler A ApJ

Dressler A Oemler A Jr Sparks W B Lucas R A ApJ L

Edmunds M G Greenhow R M MNRAS

Edmunds M G Pagel B E J MNRAS

Filipp enko A V Greenstein J L PASP

Freedman W L et al Nature

Friedli D Benz W Kennicutt R C ApJ L

Garnett D R Shields G A ApJ

Giovanelli R Haynes M ApJ

Giovanelli R Haynes M Salzer J J Wegner G Da Costa L N Freudling W

AJ

GotzM Koppen J AA

Gunn J E Gott J R ApJ

Haynes M P in Clusters of Galaxies ed W R Oegerle M J Fitchett L Danly

Cambridge Cambridge University Press

Henning P A Sancisi R McNamara B R AA

Henry R B C MNRAS

Henry R B C Pagel B E J Chincarini G L MNRAS HPC

Henry R B C Pagel B E J Lassiter D F Chincarini G L MNRAS

HPLC

Howarth I D MNRAS

Kenney J D P Young J S ApJ

Kennicutt R C Jr AJ

Kennicutt R C Jr ApJ

Kennicutt R C Jr Edgar B K Ho dge P W ApJ

Kennicutt R C Jr Kent S M AJ

Kennicutt R C Jr Tamblyn P Congdon C W ApJ KTC

Ko daira K Watanabe M Okamura S ApJS

Lacey C G Fall S M ApJ

Larson R B Nature Phys Sci

Martin P Roy JR ApJ

Massey P Strob el K Barnes J V Anderson E ApJ

Mayor M Vigroux L AA

McCall M L PhD thesis University of Texas

McCall M L Rybski P M Shields G A ApJS MRS

McMahon P M PhD Thesis Columbia University

Nulsen P E J MNRAS

Oey M S Kennicutt R C ApJ OK

Pagel B E J Edmunds M G ARAA

Pagel B E J Edmunds M G Blackwell D E Chun M S Smith G

MNRAS

Postman M Geller M J ApJ

Quirk W J ApJ L

Rob erts M S ARAA

Ryder S D ApJ

Sancisi R Thonnard N Ekers R D ApJ L

Sandage A Tammann G A A Revised ShapleyAmes Catalog of Bright Galaxies

Washington DC Carnegie Institution RSA

Scalo J M Fund Cos Phys

Schmidt M ApJ

Seaton M J MNRAS p

Shields G A Skillman E D Kennicutt R C Jr ApJ SSK

Shields J C Kennicutt R C Jr ApJ in press

Skillman E D Bothun G D Murray M A Warmels R H AA

Skillman E D Kennicutt R C Jr Ho dge P ApJ

SommerLarson J Yoshii Y MNRAS

SommerLarson J Yoshii Y MNRAS

Tinsley B M Larson R B ApJ

Tully R B Nearby Galaxies Catalog Cambridge Cambridge Univ Press

Tully R B Shaya E J ApJ

van den Bergh S Pierce M J ApJ

van der Hulst J M Skillman E D Kennicutt R C Bothun G D AA

VilaCostas M B Edmunds M G MNRAS VCE

Warmels R H PhD University of Groningen

Warmels R H AAS

Whitmore B C in Clusters of Galaxies ed W R Oegerle M J Fitchett L

Danly Cambridge Cambridge University Press

Zaritsky D ApJL L

Zaritsky D Kennicutt R C Huchra J P ApJ ZKH

A

This manuscript was prepared with the AAS L T X macros v E

Fig A map of the p ositions of the nine Virgo spiral galaxies studied here and the

structures identied by Binggeli Tammann Sandage The p oints are co ded to

represent the three subgroups into which the sample has b een divided see text The

lled circles represent the H I decient galaxies the lled squares represent the intermediate

galaxies and the lled triangles represent the galaxies with normal H I disks

Fig A comparison of the neutral hydrogen to optical diameter ratios D D for the

H O

eld galaxy sample of Warmels and the Virgo spirals studied here The connected

line represents the average value as a function of Ttype for the eld sample of Warmels

The error bars represent the rms standard deviation for each Ttype sample The solid

symbols represent the nine Virgo galaxies studied here and are shown with Ttypes taken

from the RC The symbol co ding is identical to that in Figure

Fig A comparison of the radial H I proles of the Virgo spiral galaxies in our sample

with the average radial H I prole for the eld galaxies of corresp onding Hubble type as

derived by Cayatte et al The galaxies are ordered in increasing D D as taken

H O

from Figure The individual p oints represent the radially averaged H I column densities

while the solid lines represent the average radial H I prole for the corresp onding Hubble

type The lled circles represent the WSRT observations of Warmels while the lled

triangles represent the VLA observations of Cayatte et al and in the case of NGC

van der Hulst et al There is go o d agreement b etween the WSRT and VLA

observations as noted by Cayatte et al

Fig Oxygen abundances from H II regions are plotted versus galactic radius for nine

Virgo spiral galaxies The order of the galaxies is the same as in Figure The oxygen

abundances are determined from measurements of O I I and O I I I in individual H II regions

and calibrated empirically as describ ed in the text The radial p ositions are normalized to

the eective optical radius as dened in the RC The lled circles are taken from MRS

SSK and the new observations presented here The lled triangles are taken from HPC and

HPLC Note the go o d agreement b etween the abundance measurements from the dierent

studies

Fig a A plot of mean OH as a function of D D for the Virgo spirals b Oxygen

H O

abundance gradient versus D D The symbol co ding is identical to that in Figure

H O

Fig Mean OH as a function of a absolute blue magnitude b maximum rotation

curve velocity and c Hubble type for the Virgo spirals and the nonbarred spirals of the

ZKH sample The op en circles corresp ond to the eld sample of ZKH while the p oints for

the Virgo spirals have b een co ded as in Figure

Fig M and V versus Ttype for the ZKH and Virgo spiral samples Co ding as in

B C

Figure

Fig A comparison of the H II region oxygen abundance trends for the H I decient Virgo

cluster galaxies NGC T NGC T and NGC T with eld

galaxies of comparable Hubble type taken from ZKH The H I decient galaxies are shown

as b old lines

Fig A comparison of the oxygen abundances for the individual H II regions in the Virgo

cluster galaxies Top panel The oxygen abundances are plotted versus the galacto centric

radius normalized by the eective radius of the disk Middle panel The oxygen abundances

are plotted versus the V surface brightness of the disk Lower panel The oxygen abundances

are plotted versus the radially averaged gas mass fraction describ ed in text Filled circles

represent HI decient Virgo galaxies Op en squares represent intermediate cases and lled

triangles represent Virgo galaxies with normal HI contents

20 NGC 4651

18

16 NGC 4321

NGC 4501 NGC 4254 NGC 4571 14 NGC 4689 NGC 4654 M M 87 12

10 Dec. (1950) M 49 8 W'

6 W NGC 4713 NGC 4303 4

H I Deficient Virgo Spirals

2 Intermediate Virgo Spirals

H I Normal Virgo Spirals

0 50 40 30 20 10 RA (1950) (12 HOURS + X m)

N4713 N4571 N4654 N4254 N4651 RC3 T-type N4303 N4321 N4689 N4501 Sa Sab Sb Sbc Sc Scd Sd Sdm Sm 0 2 4 6 8 10 3 2 1 0 .5

2.5 1.5

O H /D D

NGC 4713 NGC 4501 NGC 4654 O R/R 0 .5 1 1.5 2 NGC 4651 NGC 4571 NGC 4321 O R/R 0 .5 1 1.5 2 NGC 4689 NGC 4254 NGC 4303 O R/R 0 .5 1 1.5 2

5 0 5 0 5 0

HI x 10 x HI 10 x HI 10 10 10 x HI 10

20 20 20

NGC 4501 NGC 4654 NGC 4713 E R/R 0 1 2 3 NGC 4571 NGC 4321 NGC 4651 E R/R 0 1 2 3 NGC 4689 NGC 4254 NGC 4303 E R/R 0 1 2 3 9 9 9

9.5 8.5 9.5 8.5 9.5 8.5 12 + log(O/H) + 12 log(O/H) + 12 log(O/H) + 12

9.4 O

9.2

9 12 + Log(O/H) at 0.4 R

8.8

) 0 O

-1 Gradient (dex/R

-2 .5 1 1.5 2 2.5

DH/DO

Hubble Type (c) 10 8 6 4 2 C V 100 200 300 (b) B M (a) -16 -18 -20 -22

9

9.4 9.2 8.8 8.6 8.4 12 + log(O/H) + 12

-22

-20 B M

-18

-16

280

200 C V

120

40

2 4 6 8 10 T-type

9.5 T = 6

9

8.5 12 + log (O/H)

8

9.5 T = 4

9

8.5 12 + log (O/H)

8

9.5 T = 3

9

8.5 12 + log (O/H)

8

0 .2 .4 .6 .8 1 1.2 1.4

R/R0

9.5

9 12 + log(O/H)

8.5

0 .5 1 1.5 2 2.5

R/RE

9.5

9 12 + log(O/H)

8.5

20 21 22 23 24 25 µ (V)D

9.5

9 12 + log(O/H)

8.5

-3.5 -3 -2.5 -2 -1.5 -1 -.5 ln(µ)