This document summarizes a student's observational astronomy project analyzing different galaxy types based on Hubble's Tuning Fork classification system. The student observed and analyzed images of 5 galaxies: NGC 4125 (E5 elliptical), M51 (Sbc spiral), M89 (E0 elliptical), M81 (SAab spiral), and M82. Ellipticity calculations classified the elliptical galaxies, while arm tightness classified the spirals. Radial plots also helped identify structure. The student found the galaxies matched their predicted Hubble types based on visual characteristics like color and shape.
Artigo descreve a descoberta dos astrônomos de 4 imagens de uma supernova geradas pelo efeito de lente gravitacional e formando o raro padrão da Cruz de Einstein.
Observed the open star cluster M103, reduced the data, a created an H-R diagram. An H-R diagram relates the brightness and the color of stars and is a useful tool in astronomy.
Artigo descreve a descoberta dos astrônomos de 4 imagens de uma supernova geradas pelo efeito de lente gravitacional e formando o raro padrão da Cruz de Einstein.
Observed the open star cluster M103, reduced the data, a created an H-R diagram. An H-R diagram relates the brightness and the color of stars and is a useful tool in astronomy.
Detection of solar_like_oscillations_in_relies_of_the_milk_way_asteroseismolo...Sérgio Sacani
Asteroseismic constraints on K giants make it possible to infer radii, masses and ages of tens
of thousands of field stars. Tests against independent estimates of these properties are however
scarce, especially in the metal-poor regime. Here, we report the detection of solar-like
oscillations in 8 stars belonging to the red-giant branch and red-horizontal branch of the globular
cluster M4. The detections were made in photometric observations from the K2 Mission
during its Campaign 2. Making use of independent constraints on the distance, we estimate
masses of the 8 stars by utilising different combinations of seismic and non-seismic inputs.
When introducing a correction to the Δν scaling relation as suggested by stellar models, for
RGB stars we find excellent agreement with the expected masses from isochrone fitting, and
with a distance modulus derived using independent methods. The offset with respect to independent
masses is lower, or comparable with, the uncertainties on the average RGB mass
(4 − 10%, depending on the combination of constraints used). Our results lend confidence to
asteroseismic masses in the metal poor regime. We note that a larger sample will be needed
to allow more stringent tests to be made of systematic uncertainties in all the observables
(both seismic and non-seismic), and to explore the properties of RHB stars, and of different
populations in the cluster.
A 50000 solar_mass_black_hole_in_the_nucleous_of_rgg_118Sérgio Sacani
Astrônomos usando o Observatório de Raios-X Chandra da NASA e o Telescópio Clay de 6.5 metros no Chile, identificaram o menor buraco negro supermassivo já detectado no centro de uma galáxia. Esse objeto paradoxal poderia fornecer pistas sobre qual o tamanho de buracos negros formados juntos com suas galáxias hospedeiras a 13 bilhões de anos atrás, ou mais.
Os astrônomos estimam que esse buraco negro supermassivo tem cerca de 50000 vezes a massa do Sol. Isso é menos da metade do buraco negro anterior de menor massa encontrado no centro de uma galáxia.
O buraco negro está localizado no centro do disco da galáxia anã, chamada de RGG 118, localizada a cerca de 340 milhões de anos-luz de distância da Terra. A imagem principal desse post, foi feita pelo Sloan Digital Sky Survey e o detalhe mostra uma imagem feita pelo Chandra do centro da galáxia. A fonte pontual de raios-X, é produzida pelo gás quente que faz um movimento de redemoinho ao redor do buraco negro.
Os pesquisadores estimaram a massa do buraco negro estudando o movimento do gás frio perto do centro da galáxia, usando dados na luz visível obtidos pelo Telescópio Clay. Eles usaram os dados do Chandra para descobrir o brilho em raios-X do gás quente espiralando na direção do buraco negro. Eles encontraram que a força de empurrão da pressão da radiação desse gás quente é equivalente a cerca de 1% da força de puxão da gravidade interna, o que se ajusta bem com as propriedades de outros buracos negros supermassivos.
Anteriormente, uma relação tinha sido notada entre a massa dos buracos negros supermassivos e o intervalo de velocidades das estrelas no centro da galáxia hospedeira. Essa relação também é mantida para a RGG 118 e seu buraco negro.
O buraco negro na RGG 118 é cerca de 100 vezes menos massivo do que o buraco negro supermassivo encontrado no centro da Via Láctea. Ele é também cerca de 200000 vezes menos massivo do que o buraco negro mais massivo já encontrado no centro de outras galáxias.
Os astrônomos estão tentando entender a formação de buracos negros com bilhões de vezes a massa solar que têm sido detectados a menos de um bilhão de anos depois do Big Bang. O buraco negro na RGG 118 dá aos astrônomos uma oportunidade de estudar um buraco negro supermassivo, pequeno e próximo, pertencente à primeira geração de buracos negros que não são detectáveis pela nossa tecnologia atual.
Os astrônomos acreditam que buracos negros supermassivos podem se formar quando grandes nuvens de gás, com uma massa entre 10000 e 100000 vezes a massa do Sol, colapsa num buraco negro. Muitos desses buracos negros semeiam então fusões para formar buracos negros supermassivos ainda maiores. De maneira alternativa, um buraco negro supermassivo poderia surgir de uma estrela gigante, com cerca de 100 vezes a massa do Sol, que no final da sua vida, depois de consumir todo o seu combustível, colapsa e forma um buraco negro.
Os pesquisadore
Discovery two embedded_clusters_with_wise_in_the_galactic_latitude_cloud_hrk8...Sérgio Sacani
Artigo descreve descoberta feita por astrônomos brasileiros de dois aglomerados estelares localizados bem distante da região tradicional onde eles normalmente são encontrados. Esses aglomerado formam estrelas e com isso pôde-se mostrar que o processo de formação de estrelas da Via Láctea pode ocorrer em locais inesperados.
A smack model_of_colliding_planetesimals_and_dust_in_the_beta_pictoris_debris...Sérgio Sacani
Uma nova simulação de supercomputador da NASA do planeta e do disco de detritos ao redor da estrela Beta Pictoris revela que o movimento do planeta dirige ondas espirais através do disco, um fenômeno que gera colisões entre os detritos em órbita. Padrões nas colisões e a poeira resultante parece ser responsável por muitas feições observadas que pesquisas anteriores tinham sido incapazes de serem explicadas completamente.
Detection of solar_like_oscillations_in_relies_of_the_milk_way_asteroseismolo...Sérgio Sacani
Asteroseismic constraints on K giants make it possible to infer radii, masses and ages of tens
of thousands of field stars. Tests against independent estimates of these properties are however
scarce, especially in the metal-poor regime. Here, we report the detection of solar-like
oscillations in 8 stars belonging to the red-giant branch and red-horizontal branch of the globular
cluster M4. The detections were made in photometric observations from the K2 Mission
during its Campaign 2. Making use of independent constraints on the distance, we estimate
masses of the 8 stars by utilising different combinations of seismic and non-seismic inputs.
When introducing a correction to the Δν scaling relation as suggested by stellar models, for
RGB stars we find excellent agreement with the expected masses from isochrone fitting, and
with a distance modulus derived using independent methods. The offset with respect to independent
masses is lower, or comparable with, the uncertainties on the average RGB mass
(4 − 10%, depending on the combination of constraints used). Our results lend confidence to
asteroseismic masses in the metal poor regime. We note that a larger sample will be needed
to allow more stringent tests to be made of systematic uncertainties in all the observables
(both seismic and non-seismic), and to explore the properties of RHB stars, and of different
populations in the cluster.
A 50000 solar_mass_black_hole_in_the_nucleous_of_rgg_118Sérgio Sacani
Astrônomos usando o Observatório de Raios-X Chandra da NASA e o Telescópio Clay de 6.5 metros no Chile, identificaram o menor buraco negro supermassivo já detectado no centro de uma galáxia. Esse objeto paradoxal poderia fornecer pistas sobre qual o tamanho de buracos negros formados juntos com suas galáxias hospedeiras a 13 bilhões de anos atrás, ou mais.
Os astrônomos estimam que esse buraco negro supermassivo tem cerca de 50000 vezes a massa do Sol. Isso é menos da metade do buraco negro anterior de menor massa encontrado no centro de uma galáxia.
O buraco negro está localizado no centro do disco da galáxia anã, chamada de RGG 118, localizada a cerca de 340 milhões de anos-luz de distância da Terra. A imagem principal desse post, foi feita pelo Sloan Digital Sky Survey e o detalhe mostra uma imagem feita pelo Chandra do centro da galáxia. A fonte pontual de raios-X, é produzida pelo gás quente que faz um movimento de redemoinho ao redor do buraco negro.
Os pesquisadores estimaram a massa do buraco negro estudando o movimento do gás frio perto do centro da galáxia, usando dados na luz visível obtidos pelo Telescópio Clay. Eles usaram os dados do Chandra para descobrir o brilho em raios-X do gás quente espiralando na direção do buraco negro. Eles encontraram que a força de empurrão da pressão da radiação desse gás quente é equivalente a cerca de 1% da força de puxão da gravidade interna, o que se ajusta bem com as propriedades de outros buracos negros supermassivos.
Anteriormente, uma relação tinha sido notada entre a massa dos buracos negros supermassivos e o intervalo de velocidades das estrelas no centro da galáxia hospedeira. Essa relação também é mantida para a RGG 118 e seu buraco negro.
O buraco negro na RGG 118 é cerca de 100 vezes menos massivo do que o buraco negro supermassivo encontrado no centro da Via Láctea. Ele é também cerca de 200000 vezes menos massivo do que o buraco negro mais massivo já encontrado no centro de outras galáxias.
Os astrônomos estão tentando entender a formação de buracos negros com bilhões de vezes a massa solar que têm sido detectados a menos de um bilhão de anos depois do Big Bang. O buraco negro na RGG 118 dá aos astrônomos uma oportunidade de estudar um buraco negro supermassivo, pequeno e próximo, pertencente à primeira geração de buracos negros que não são detectáveis pela nossa tecnologia atual.
Os astrônomos acreditam que buracos negros supermassivos podem se formar quando grandes nuvens de gás, com uma massa entre 10000 e 100000 vezes a massa do Sol, colapsa num buraco negro. Muitos desses buracos negros semeiam então fusões para formar buracos negros supermassivos ainda maiores. De maneira alternativa, um buraco negro supermassivo poderia surgir de uma estrela gigante, com cerca de 100 vezes a massa do Sol, que no final da sua vida, depois de consumir todo o seu combustível, colapsa e forma um buraco negro.
Os pesquisadore
Discovery two embedded_clusters_with_wise_in_the_galactic_latitude_cloud_hrk8...Sérgio Sacani
Artigo descreve descoberta feita por astrônomos brasileiros de dois aglomerados estelares localizados bem distante da região tradicional onde eles normalmente são encontrados. Esses aglomerado formam estrelas e com isso pôde-se mostrar que o processo de formação de estrelas da Via Láctea pode ocorrer em locais inesperados.
A smack model_of_colliding_planetesimals_and_dust_in_the_beta_pictoris_debris...Sérgio Sacani
Uma nova simulação de supercomputador da NASA do planeta e do disco de detritos ao redor da estrela Beta Pictoris revela que o movimento do planeta dirige ondas espirais através do disco, um fenômeno que gera colisões entre os detritos em órbita. Padrões nas colisões e a poeira resultante parece ser responsável por muitas feições observadas que pesquisas anteriores tinham sido incapazes de serem explicadas completamente.
You've no doubt heard about Millennials (also known as Generation Y, born after 1980) for years now. ... Born after 1995, members of the emerging Gen Z are expected to become the dominant business influencers of tomorrow
Materials RequiredComputer and internet accessCalcula.docxwkyra78
Materials Required:
Computer and internet access
Calculator
Ruler
Pencils and pens, eraser
Digital camera and/or scanner
Print out
Galaxy Image
Prints document
Total Time Required:
Approximately 2-3 Hours
Part 1. The Local Group
In Table 1, you will find a list of most of the galaxies in the Local Group. This group is made up of our own galaxy, the Milky Way, and its closest neighbors. (Note: 1 kpc = 1 kiloparsec = 1000 parsec; 1 parsec = 3.26 light years)
Table 1. Galaxies of the Local Group
Name
Distance (kpc)
Diameter (kpc)
Name
Distance (kpc)
Diameter (kpc)
Milky Way
-
40.0
IC 1522
610
1.5
Sculptor
60
0.3
WLM
610
2.1
Large Magellanic Cloud (LMC)
60
6.1
Andromeda I
675
0.6
Carina
90
0.2
Andromeda II
675
0.6
Draco
90
0.2
Andromeda III
675
0.9
Ursa Minor
90
0.3
M32
675
1.5
Sextans I
90
0.9
NGC 185
675
1.8
Small Magellanic Cloud (SMC)
90
4.6
NGC 147
675
3.1
Fornax
150
0.9
NGC 205
675
3.1
Leo II
185
0.2
M31 (Andromeda Galaxy)
675
61
Leo I
185
0.3
IC 1613
765
3.7
NGC 6822
520
2.5
M33 (Triangulum Galaxy)
765
14.0
DDO 210
920
1.2
Below is a visual representation of our Local Group of galaxies. You can access and zoom into this image to see galaxies more clearly using this link
Local Group
.
Figure 1.
Local Group Visualization.
Type and label your answers to the below questions in your lab report.
Using Table 1 above and noting the diameters of the galaxies, which
five
galaxies in the Local Group are the largest? In a few sentences, compare the sizes of the other galaxies in the Local Group to the two largest ones.
Which
three
galaxies have the largest angular size (not including the Milky Way)? These galaxies are the ones that look the largest in the sky. Explain how you get your answer.
By hand and with pencil, create a
scale drawing
of the Milky Way and the Large Magellanic Cloud, showing their
relative sizes
and the
distance
between them in kiloparsecs (the galaxies can be represented by circles).
Write down the scale you use ,
and your calculations to find the scaled-down sizes and distance. (An example of a good scale to use would like something like: 5 mm = 10 kpc, also see this site
Basic-Mathematics.com
for more information on scaling.) You will photo your drawing and insert it into your lab report.
Figure 2.
Local Supercluster Print
Image courtesy of Palomar Sky Survey Photographs
As you have already seen, galaxies can vary a lot in size. Now, we will look at how their shapes are different. Two basic types of galaxies are the spiral galaxies and the elliptical galaxies. Spiral galaxies have a disk-like structure,and a central bulge. Our own Milky Way is a spiral galaxy. Elliptical galaxies appear round, looking a lot like a football .
LIT 2001 FINAL EXAMPlease respond with a complete, thoughtful an.docxSHIVA101531
LIT 2001 FINAL EXAM
Please respond with a complete, thoughtful answer. Be sure to provide detail by referring to specific examples. DO NOT USE OUTSIDE RESEARCH SOURCES.
PART ONE: Answer ONE of the following questions:
1. Describe Langston Hughes’ view of America by tracing at least three of his poems. Also, describe the controversy around the manner in which Hughes portrayed African Americans in his poems.
2. William Carlos Williams uses an “open” style and format and Robert Frost uses a more “constructed”? What are the characteristics of each style – i.e., rhyme, etc. Use examples from their poems.
PART TWO: POEM ANALYSIS
DO NOT USE OUTSIDE RESEARCH SOURCES.
Critically analyze this poem by discussing three major components of analysis: Please read all 7 stanzas of the poem.
1. What are some of the structural elements of the poem? Metaphor, rhyme, symbols, sounds, etc.
2. What does the poem mean? Explain the content of the poem.
3. What is the theme of the poem?
To An Athlete Dying Young by A.E.Housman
The time you won our town the race
We chaired you through the market place;
Man and boy stood cheering by,
And home we brought you shoulder-high.
Today, the road all runners come,
Shoulder-high we bring you home,
And set you at your threshold down,
Townsman of a stiller town.
Smart lad, to slip betimes away
From fields where glory does not stay,
And early though the laurel grows
It withers quicker than the rose.
Eyes the shady night has shut
Cannot see the record cut,
And silence sounds no worse than cheers
After earth has stopped the ears:
Now you will not swell the rout
Of lads that wore their honors out,
Runners whom renown outran
And the name died before the man.
So set, before its echoes fade,
The fleet foot on the sill of shade,
And hold to the low lintel up
The still-defended challenge cup.
And round that early-laureled head
Will flock to gaze the strengthless dead
And find unwithered on its curls
The garland briefer than a girl’s.
Hubble's Law and the Expansion Rate of the Universe
This lab is based on the University of Washington’s “Hubble’s Law and the Expansion of
the Universe” lab. The website where the images and spectra are located is maintained
by the University of Washington Astronomy Department.
Learning Objectives
Using analyses of images and spectra of selected galaxies, you will
1. measure angular sizes of galaxies and find their distances,
2. measure the redshifts of galaxy spectral lines and find the recessional velocities
of the galaxies,
3. create a Hubble Plot to determine a value for Hubble's constant,
4. estimate the age of the Universe from this constant and compare that to the age
of the Sun and the Milky Way,
5. and summarize how our view of the Universe has changed as the value of the
Hubble constant has improved.
Background and Theory
In the 1920's, Edwin P. Hubble discovered a relationship, now known as Hubble' ...
Deja vu all_over_again_the_reapperance_of_supernova_refsdalSérgio Sacani
O Telescópio Espacial Hubble das agências NASA e ESA registrou a imagem pela primeira vez da explosão prevista de uma supernova. O reaparecimento da supernova Refsdal foi calculado a partir de diferentes modelos de aglomerados de galáxias, cuja imensa gravidade está entortando a luz da supernova.
Muitas estrelas terminam a sua vida com uma explosão, mas somente poucas dessas explosões estelares têm sido registradas no ato que acontecem. Quando isso acontece, é pura sorte, pelo menos até agora. No dia 11 de Dezembro de 2015, os astrônomos não somente fizeram a imagem de uma supernova em ação, como também observaram quando e onde ela estava prevista para acontecer.
A supernova, apelidada de Refsdal, foi registrada no aglomerado de galáxias, conhecido como MACS J1149.5+2223. Enquanto que a luz do aglomerado gasta cerca de cinco bilhões de anos para chegar até nós, a supernova explodiu muito tempo antes, a aproximadamente 10 bilhões de anos atrás.
A história da Refsdal começou em Novembro de 2014, quando os cientistas registraram quatro imagens separadas da supernova num raro arranjo conhecido como Cruz de Einstein, ao redor de uma galáxia dentro do MACS J1149.5+2223. A ilusão de óptica cósmica ocorreu devido ao fato da massa de uma única galáxia dentro do aglomerado estar entortando e ampliando a luz da distante explosão estelar, num processo conhecido como lente gravitacional.
A three-dimensional map of the Milky Way using 66,000 Mira variable starsSérgio Sacani
We study the three-dimensional structure of the Milky Way using 65,981 Mira variable stars discovered
by the Optical Gravitational Lensing Experiment (OGLE) survey. The spatial distribution of the Mira
stars is analyzed with a model containing three barred components that include the X-shaped boxy
component in the Galactic center (GC), and an axisymmetric disk. We take into account the distance
uncertainties by implementing the Bayesian hierarchical inference method. The distance to the GC is
R0 = 7.66 ± 0.01(stat.) ± 0.39(sys.) kpc, while the inclination of the major axis of the bulge to the
Sun-GC line-of-sight is θ = 20.2
◦ ± 0.6
◦
(stat.) ± 0.7
◦
(sys.). We present, for the first time, a detailed
three-dimensional map of the Milky Way composed of young and intermediate-age stellar populations.
Our analysis provides independent evidence for both the X-shaped bulge component and the flaring
disk (being plausibly warped). We provide the complete dataset of properties of Miras that were used
for calculations in this work. The table includes: mean brightness and amplitudes in nine photometric
bands (covering a range of wavelength from 0.5 to 12 µm), photometric chemical type, estimated
extinction, and calculated distance with its uncertainty for each Mira variable. The median distance
accuracy to a Mira star is at the level of 6.6%.
Exercise 1Using the data above in Table 1, make a plot of right .docxrhetttrevannion
Exercise 1
Using the data above in Table 1, make a plot of right ascension versus declination on your printed out Milky Way Globular Clusters Distribution Graph (Diagram 1-the top plot). RA is along the x-axis and goes from 0 to 24 hours, Dec is on the y-axis and goes from +90 to 0 to –90 degrees.) Insert the plot into your lab report with your signature and date.
You will type your answers to the below questions in your lab report and then scan/photo your graph(s) and insert them into your lab document. Again, it would be helpful to review the Exploration from Module 1: “Math Primer for Astronomy” (note this contains link for a free online scientific calculator). There are also good math examples in the Appendix of our eText.
Would you describe the distribution of clusters on the plot as random, or is there a pattern (explain your answer)?
Now look at your plot and point in the direction in which you see most of the globular clusters. This is the general direction of the Galactic Center. Estimate the center of the distribution of the globular clusters. Also estimate (no calculation required — just an educated estimate) the accuracy of determining this center. You have now determined the rough center of our Galaxy!
RA = ____________________ ± ________________
Dec = ____________________ ± ________________
Shapely was correct in thinking that the distribution of globular clusters could reveal something about the Galaxy as a whole. He went one step further. He used the locations of the globular clusters to determine the distance to the Galactic Center. His result was surprisingly accurate and differed from the modern value by less than 10%. So, let’s follow in his footsteps.
The next step is to determine the distance to the clusters. Shapely did this by using RR Lyrae stars. These are variable stars, which have a relatively narrow range of luminosities. From the difference between the apparent magnitudes (measured from his photographic plates) and the absolute magnitudes (calculated from the luminosities), he calculated the distances in parsecs to the star (via: m - M = 5log10(d) + 5). So now we have the distances and the directions of the globular clusters and we can determine the 3-dimensional distributions of the globular clusters relative to us.
However, we will use a different coordinate system that is based on galactic latitude and longitude rather than RA and Dec. The plane of the Galaxy is designated as “0 latitude”. Why would we want to do this? RA and Dec is a messy coordinate system that depends on our orientation in space and the earth’s rotation around its axis. The system based on galactic latitude and longitude is therefore simpler. However, it means that we have to transform the measured RA and DEC positions of the globular clusters and galactic latitude and longitude. To simplify things even further, let’s express the galactic latitude and longitude in terms of x, y, and z coordinates. The advantage of this is that x,.
The stellar orbit distribution in present-day galaxies inferred from the CALI...Sérgio Sacani
Galaxy formation entails the hierarchical assembly of mass,
along with the condensation of baryons and the ensuing, selfregulating
star formation1,2
. The stars form a collisionless system
whose orbit distribution retains dynamical memory that
can constrain a galaxy’s formation history3
. The orbits dominated
by ordered rotation, with near-maximum circularity
λz≈ 1, are called kinematically cold, and the orbits dominated
by random motion, with low circularity λz≈ 0, are kinematically
hot. The fraction of stars on ‘cold’ orbits, compared with
the fraction on ‘hot’ orbits, speaks directly to the quiescence
or violence of the galaxies’ formation histories4,5
. Here we
present such orbit distributions, derived from stellar kinematic
maps through orbit-based modelling for a well-defined,
large sample of 300 nearby galaxies. The sample, drawn from
the CALIFA survey6, includes the main morphological galaxy
types and spans a total stellar mass range from 108.7 to 1011.9
solar masses. Our analysis derives the orbit-circularity distribution
as a function of galaxy mass and its volume-averaged
total distribution. We find that across most of the considered
mass range and across morphological types, there are more
stars on ‘warm’ orbits defined as 0.25 ≤λz≤ 0.8 than on either
‘cold’ or ‘hot’ orbits. This orbit-based ‘Hubble diagram’ provides
a benchmark for galaxy formation simulations in a cosmological
context.
Students determined the age of the universe using an 11 inch telescope and they discover the necessary physical laws experimentally.
As a second step they developed a progressive series of mathematical models for the dynamics of the universe and calculated that the usual matter amounts only 5 % of all matter and energy in the universe.
Easy to use learning material is included for schools as well as for the interested public. More detailed learning material may be requested. The material has been tested successively for three age groups: With the conceptual material, students of classes 4 or higher can comprehend the topic. With more advanced material, students of class 7 or higher can evaluate the measurements mathematically. With fully advanced material, students of class 9 or higher can develop mathematical models for the dynamics of the universe and calculate the statistical significance of the measurements.
1. PHYS 245
Observational Astronomy
Observational Project
5/29/16
Naomi Morishita
EXPLORING DIFFERENT TYPES OF GALAXIES
Abstract
This paper is going to address the theme “Exploring Different Galaxy Types”. In this
paper, the “exploration” is particularly based on Hubble Tuning Fork, the classification of
galaxies that an American astronomer, Edwin Hubble established in 1926. This theme is
interesting because Hubble Tuning Fork presents a method for statistically classifying galaxies,
from which quantitative assessments can be made. Also, it can be used to make statements such
as “The percent of galaxies in this area is x” or “This type of galaxy is more commonly observed
2. 1
than that type”. Hubble stated that “The classification was devised primarily for statistical
studies” in his paper, but still, a number of physical characteristics can be derived from
determining the Hubble Type. My group analyzed five galaxies in the aspects of their sizes, color
and shape by looking at the image, calculating the ellipticity and also the grey value plots (radial
plots). The data analysis and its process of the each galaxy and their significance will be
discussed in the following sections.
Introduction
3. 2
Hubble Tuning Fork was established by American astronomer Edwin Hubble 1926. It
classifies the galaxies mainly by on their visual appearance or morphologies. The biggest two
categories of the galaxies are elliptical and spiral. The types of elliptical galaxies are classified
with subgroups from E0 to E7, with E0 group being most round and E7 being most elliptical.
The specific group a galaxy belongs are determined by the mathematical equation based on its
major and minor axis, which going to be introduced in the following sections. The spiral galaxies
are first classified as either spiral galaxy or barred spiral galaxy. In both groups, the galaxies are
classified into subgroups depending on how tight their wounds are. “S” represents the spiral
galaxy group and “SB” represents the barred spiral galaxy group. In those two groups, there are
galaxies belonging to subgroups ranging from S(B)a to S(B)c, as shown in Figure 1 below.
Galaxies on the left are termed “early”, ones on the right are “late” and galaxies in the middle are
“intermediate” . Opposing to our intuition, this terminology does not refer to the age of the
galaxies, as Hubble Stated in his paper, “The nomenclature, it is emphasized, refers to position in
the sequence and temporal connotations are made at one's peril.”
4. 3
Figure 1. Hubble Tuning Fork
Hubble Tuning Fork is still used by many researchers today. As its current status, NASA
had a project in 2013 that they made a comparison between the galaxy images that Hubble had
taken and the current images of those galaxies. They found out that even though the size of the
galaxies are growing, the basic pattern of the galaxy structures had not changed since 11 billion
years ago. In this paper, specifically the images of NGC 4125 (E5) , M51 “Whirlpool Galaxy”
(Sbc), M89(E0), M81 (Sab), and M82(E8/E9) will be discussed. These images, except M82
have been taken with R, V, and B filters by us. Then they were reduced and stacked using
Dawn, and three color images were produced by using Gimp for those that we were able to.
Since classifications were originally based on their visual appearance or morphologies, this paper
is analyzing the five galaxies by their groups they belong in Hubble Tuning Fork, and their
“roundness”,wounds, and other apparel aspects. Then we see how well the the images of galaxies
we took and analyzed are fitting the group they actually belong to. Also, for the elliptical
galaxies, major and minor axes have been majored to determine the Hubble Type from the image
we have taken. In addition to that, using Astroimage J, Gray values (counts) vs. Pixels plots
(radial plots) are created for the galaxies NGC 4125, M51, M89, and M81. The grey values
(counts) represents how bright the particular spot in the image is. The lower the grey value, the
dimmer the spot is and vise versa. By looking at the plots, we are able to determine the galaxy
shapes: if there is a curve from the background sky to the galaxy on the plot, we analyze it as a
spiral galaxy, since it indicates the disk (See figure 2 below). If there is no curve from the
background sky to going up to the peak (center of the galaxy), we analyze it as an elliptical
galaxy (See figure 3 below). The detailed procedure and their analysis will be discussed in the
following section.
5. 4
Figure 2. Expected plot type of radial plot of spiral galaxies
Figure 3. Expected plot type of radial plot of elliptical galaxies
Data Acquisition:
During the observation process, me and my group spend few nights to take the images of
relatively luminous and “face-on” galaxies with different characteristics. We used the cycle
exposure function and took plenty of images that are exposed for 30 seconds, 60 seconds, and 90
seconds. Due to the weather and sky conditions, we were not able to get as many images as we
wanted at the quality we had expected, by at least we got enough to analyze, and we also used
the images that were not taken by us.
6. 5
Since Hubble Types are mainly about the appearance of the galaxies, we were
able to learn a lot from the images, though the further quantitative analysis gave us much more
information as we kept on analyzing. Followings are the quantitative methods that were used to
analyze the galaxies.
For the elliptical galaxies, we used the equation ϵ = 1 - β/α , to classify the subgroups that
a galaxy would belong, where α is the major axis and β is the minor axis. For example, the major
axis of NGC 4125 were majored as 77 using Gimp with the image we took and. The semi-major
axis were major to be 40. By substituting those values to the given equation; ϵ = 1 - 40/77≈0.5,
thus NGC 4125 is classified as E5. For M89 has been calculated the
same way. For the spiral galaxies, the comparison with the group
previous and following the group a galaxy belongs are done and also
the plots of grey values (counts) vs. pixels, are presented. We also
analyzed some of them by focusing on their color (B-V value) and the
radial function.
Results/Discussion:
NGC 4125:
Elliptical galaxy in Draco
7. 6
Figure 4: NGC 4125
ϵ = 1 - β/α , where α is the major axis and β is the minor axis. The major axis of NGC
4125 were majored as 77 using the image took and Gimp. The semi-major axis were major to be
40. By substituting those values to the given equation; ϵ = 1 - 40/77≈0.5, thus NGC 4125
is classified as E5.
It belongs to E5 group in Hubble Tuning Fork, which is an elliptical galaxy that is
relatively close to S0 group (lenticular). As it is an elliptical galaxy, its population of stars will
tend to be redder, and thus older by the B-V value -47495.91029.
8. 7
Figure 5: Radial plot of NGC 4125
Figure 6: Radial plot of NGC 4125
These radial plots are fluctuating a lot, but it indicates that the galaxy is elliptical since it is
following the pattern shown in figure 3.
M51 A
Spiral galaxy in Canes Venatici, also known as the “Whirlpool Galaxy”. The other object is
M51B
9. 8
Figure 7: M51A
While it is clearly of the SA type, the subtypes are, by Hubble’s own admission, largely
arbitrary. By comparing our image to images of typed galaxies, we can determine that it belongs
to Sbc group: a spiral galaxy that has relatively loose wound arms, but not as loose as the typical
Sc galaxy.
Figure 8. Comparison of SAb, SAbc, and SAc
10. 9
Figure 9: Radial plot of M51 A (Along Horizontal)
Figure 10: Radial plot of M51 A (Along Horizontal)
11. 10
Figure 11: Radial plot of M51 A (Along Vertical)
Figure 12: Radial plot of M51 A (Along Vertical)
These plots indicates that the galaxy is spiral, since they follow the patterns in figure 2. It is kind
of slight but the curve going into the peak can be observed.
Given that this galaxy is of type Sbc, we can determine that it has a mass of 109 - 1012
12. 11
Mo, a diameter of 5-100 kpc, and a Mgas/Mtotal ratio of about 0.12. As it is a spiral galaxy, its
population of stars will tend to be bluer, and thus younger.
M89
Figure 13. M89
Elliptical galaxy in Virgo
ϵ = 1 - β/α , where α is the major axis and β is the minor axis. The major axis of M89 were
majored as 49 using Gimp with the image took and. The semi-major axis were major to be 45.
By substituting those values to the given equation; ϵ = 1 - 45/49≈0, thus M89 is
classified as E0.
13. 12
Figure 14: Radial plot of M89
Figure 15: Radial plot of M89
For this one, the radial plots can be said that they are not very accurate: they show the curve
getting into the peak but, it is actually representing the elliptical galaxy, which is supposed to
follow the pattern shown in figure 3. The possible causes are lack of number of data points,
noises in the image, sky condition when the image was taken, etc.
E0 is an elliptical, so its stars will tend to be redder and older. The galaxy itself is also
14. 13
very spherical.
M81
Similar to M51A, M81 is very clearly an SA Type galaxy. By again visually assessing
the tightness of the arms, we can determine that this galaxy falls somewhere between an “a” and
a “b” subtype (SAab). The arms are definitely more tightly bound but since there appear to be
more than just two distinct spiral arms, we can say that it is not simply an “a”.
Figure 16. M81
Figure 17. Comparison of SAa, SAab, and SAb
15. 14
Figure 18. Radial plot of M81
Figure 19. Radial plot of M81
These radial plots beautifully indicate that the galaxy is spiral, by following the pattern
shown in figure 2.
It is a spiral galaxy as explained, and it tends to have younger stars by looking at the
colors. Blue indicates the younger colors while red indicates the older. The calculated B-V value
16. 15
is -1833571.316.
M82
Impossible to determine the Hubble Type.
Assessing the color of the galaxy shows a reddish color both in the composite image,
suggesting that M82 is elliptical, though that is not necessarily the case. If it was/is an elliptical,
it would be an E8 or E9, more elliptical than any galaxy recorded.
Figure 20. M82
While a color analysis suggests an elliptical galaxy, the shape suggests a spiral. Thus, we
must categorize it as irregular.
17. 16
As this paper has been addressing, the Hubble Tuning Fork is a very useful to classify the
galaxies in many different aspects. However, there are some limitations of it. Hubble Tuning
Fork fails to provide classification for irregular galaxies beyond lumping them into the categories
Irr I and Irr II. Also, it may lead to a misconception that the galaxies evolve from E0 group to
either Sc or SBc group, by calling the ones on the left “early” ones and the ones on the right
“late” ones even though that was just Hubble states on his paper “It is just an arbitrary procedure
and is adopted merely because it is possible to distinguish the middle section from the two ends”.
Summary
Using the images that we have taken, we calculated ϵ values for the elliptical galaxies
and compared to the actual groups that those galaxies belong to. For the spiral galaxies we made
comparisons with the galaxies in nearby subgroups by their tightness in the wounds. Then, for
both of them,we compared the observed color and grey value functions and compared. We then
made comments on each comparisons and the things we were able to learn about the galaxies
other than determining their Hubble Types.
It is significant that we keep exploring different types of galaxies even though Hubble
had made the “standard classification”, because there are many aspects in galaxy
formation/evolution that have not yet been discovered. Exploring the different types of galaxies
over long time periods gives us significant amount of information that we can use to test our
18. 17
predictions.
For the future reference, we would start observing earlier so that we get enough/back up
nights for observation. Also for the further analysis, we would take the uncertainties to account.
References
Longair, M. S. Galaxy Formation. Berlin: Springer, 2008. Print.
Takamori, Keisuke. Uchu Ni Tsuite Shiritai Rokujuhachikomoku: Hoshizora to Uchu Ga Attoteki
Ni Omoshiroku Naru. N.p.: Newton, n.d. Print.
19. 18
Carroll, Bradley W., and Dale A. Ostlie. An Introduction to Modern Astrophysics. San Francisco,
Calif. ; Munich: Pearson/Addison Wesley, 2009. Print.
"1971JHA.....2..109H Page 109." 1971JHA.....2..109H Page 109. N.p., n.d. Web. 31 May 2016.
※All of the image citations on the images.