Exercise 2: Detecting Interstellar Reddening
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In this exercise, you will learn how
interstellar
reddening affects the spectrum of a planetary nebula. Comparing
the spectra of several nebulae, you will be able to determine which
are more or less affected by interstellar reddening. Combining these
results with the galactic latitudes of these planetary nebulae, you
will be able to conclude something about the distribution of
interstellar dust in our Milky Way Galaxy.
The Balmer Decrement
In the Bohr
model of the hydrogen atom there are many distinct energy levels,
between which electrons can transfer if they emit or absorb the proper
amount of energy. Upward moves require absorption of energy, while
downward ones release energy. Downward electron transitions that end
on the second energy level are called the Balmer
series, and are important in optical astronomy, since these are
the only transitions that involve visible light. The first three of
these are called H
, H
, and H
, for the transitions from 3-2,
4-2, and 5-2, respectively. When many ionized hydrogen atoms are
recombining, as in a planetary nebula where atoms are being ionized
and recombining all the time, the captured electrons cascade down
through the energy levels, emitting photons of the appropriate
wavelengths as they fall. The likelihood of any particular downward
jump is dictated by atomic constants, and thus the ratios of all
possible transitions can be calculated. This leads to the "Balmer
decrement," the well known ratios among the intensities of the Balmer
lines, where H
is the
strongest line, H
is
weaker, H
is weaker still,
and so on. Under typical conditions in planetary nebulae these ratios
are (from Osterbrock, Astrophysics of Planetary Nebulae and Active
Galactic Nuclei, University Science Books, 1989):
H
/H
= 2.86 and
H
/H
= 0.47
The Phenomenon of Interstellar Reddening
Thus, the Balmer decrement, the intensity ratios of Balmer lines in
all planetary nebulae, should be roughly the same. However, this is
not what is observed. Interstellar
reddening produced by micron-sized dust particles selectively dims
shorter-wavelength, bluer light more than it does longer-wavelength,
redder light, leading to Balmer line ratios that differ systematically
from the theoretical predictions. A planetary nebula lying behind a
cloud of interstellar dust will be observed to have the intensity
ratios H
/H
more than 2.86, and
H
/H
less than 0.47. The
more dust, the greater the disparity between the observed and
theoretical Balmer decrements. Turning this concept around, from the
size of the discrepancy between observed and theoretical Balmer
decrements, astronomers can infer the amount of interstellar
reddening, and therefore, dust, between us and a given planetary
nebula.
The Milky Way Galaxy and Galactic Coordinates
Our solar system and all of the planetary nebulae in this database
reside in the Milky
Way Galaxy. The Milky Way is a flattened spiral of stars, gas, and
dust, surrounded by a more spheroidal, extended, and much more diffuse
region, called the galactic halo. Locations in the Milky Way are
conveniently specified by galactic
coordinates, similar to latitude and longitude as seen by someone
viewing from the center of the Earth. The origin of the galactic
coordinate system, though, is not at the center of the Milky Way, but
rather, is located at the sun's position, because that's where we are
as we view the heavens.
The Browse
page of this website lists galactic coordinates for each planetary
nebula as "lll.l (sign)bb.b," where lll.l is the
galactic longitude in degrees, and bb.b is the galactic latitude in
degrees. The plus or minus sign before the galactic latitude indicates
whether the object is above or below the galactic plane, respectively.
The Exercise
Listed below are eight planetary nebulae. For each of
them, you will estimate the relative intensities of the H
and H
lines and compare them with the
theoretical prediction of 2.86 and with each other. Finally, you will
be able to come to some conclusions about the distribution of dust in
the Milky Way.
H4-1
IC 2448
J900
NGC 2022
NGC 6578
NGC 7026
NGC 7662
Pe1-18
Data Collection
- Print out a copy of the data table
for this exercise. You may also find it helpful to print out this page
as well.
- The wavelength of H
is
6563 Angstroms, and for H
it
is 4861 Angstroms. Take a moment to look at the relevant
templates for
wavelength identifications to familiarize yourself with the appearance
of the spectrum in the vicinity of these Balmer lines. You will find
it helpful to print out a copy of the templates containing them.
- Review the Help page
to make sure you know how to view and expand a spectrum.
- Click on one of the nebulae listed above. This will get you to the
"View Spectrum" page where you will see the full spectrum of the
nebula.
- Locate the H
line and
expand the spectrum to zoom in on this wavelength region. Repeat if
necessary to give a good view of the line. (It is usually bracketed on
either side by two lines that come from nitrogen.) Now zoom in on the
upper part of the line so that you can get a good estimate of the
maximum intensity (height) at the center. Write this maximum height
down in the data table, remembering to include the scale exponent,
given at the top left of the graph window (e.g., x10
).
- Zoom back out to the full spectrum by pressing on the "zoom out"
button under the spectrum display. Now zoom in on the bottom of the
H
line. Read the level of
the continuum, or base level of the spectrum near the H
line, and record it on the data
sheet.
- Subtract the continuum level from the maximum height and record
the H
net height in the data
table. Zoom back out to the full spectrum.
- Repeat steps 5-7 for the H
line.
- Now calculate the observed ratio of H
/H
using the net
heights and write the result in the last column of the data
table.
- Repeat steps 5-9 for all remaining nebulae.
Data Analysis
- Fill in Table 2 of the data table, listing the nebulae in order
from highest H
/H
to lowest.
- Fill in the last column with each nebula's galactic latitude,
without the plus or minus sign (i.e., use the absolute value of the
galactic latitude).
- What trend do you notice between the galactic latitude and the
value of the H
/H
ratio?
- Remember that the amount of reddening depends how much dust you
are looking through along the line of sight to any nebula. This in
turn depends on the thickness of the dust and the distance to the
nebula. If all of these nebulae were at the same distance from us
(which they are not, although most of the objects in this
sample are at similar distances), what does your conclusion from step
3 imply about the distribution of dust in the Milky Way? Can you find
images or other material from your textbooks or reliable websites to
support your conclusion?
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