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Spectra of Gas Discharges
(http://astro.u-strasbg.fr/%7Ekoppen/discharge/index.htm)
Note by J.K.: the intensities of the lines in these
spectra appear to be different from what is seen in ordinary street
lamps. Whether this is because the excitation is different in the
street lamp from the laboratory setup with which these data were
obtained, and what is the exact reason, I do not know at the present
time.
I plan to overhaul these pages ...
Colour spectra of elements undergoing electrical discharge
excitation.
Note by J.K.: the colours on your screen may not
closely correspond to the colours which you would observe with your
eyes. Also, the relative intensities of the lines shown here may be
quite different in the lamp you observe, as they depend on the
excitation conditions in the discharge. The region shown is the
wavelength interval from 400 nm (left edge) to 700 nm (right edge),
with wavelength going linearly with position on the screen.
This is how my eyes perceive the colours of the
solar continuum
and this is how my eyes perceive the solar spectrum
Hydrogen
Helium
Oxygen
Carbon
Nitrogen
Neon
Magnesium
Silicon
Sulfur
Iron
Aluminum
Calcium
Argon
Sodium
Krypton
Xenon
Mercury
JPEG screen grabs of an applet
which computes and plots the spectra in a web browser window.
The above images aren't dithered.
They may appear so if your display doesn't have enough colors to
represent the entire color range.
Displays limited to 256 colors or less don't produce acceptable
spectra.
Try increasing your color resolution to 16 or 24 bits (16 million
colors).
This Java program reads a file containing a list
of emission line wavelengths and their corresponding strengths
then simulates the appearance of the spectrum in a good visual
spectroscope.
Note: This program generates deep 24 bit color plots,
therefore you may need to increase the color depth of your system
to view subtle details in these spectra.
Warning:
There may be a small delay as the Applet loads it's element emission
line file and computes the spectra...
- Click on an element name in the first column of the table below
to launch
the spectra viewer
- If you prefer not to run the Applet click corresponding JPG
in the next to last column to obtain an image.
Note by J.K. Some of the line intensities do not agree with
what one would expect from discharge lamps we encounter in everyday
life. I have not traced under what excitation conditions the
intensities in the data files were obtained. Since one was primarily
interested in determining the wavelengths of the lines of each element,
the excitation may have been much different from say a street lamp! As
Paolo Sirtoli told me, the NIST Atomic
Spectra Database also provides data with line intensities.
Atomic Number |
The number of protons in the nucleus of the element. |
Element |
Click on the name in this column to launch the Applet
which displays an emission line spectrum of the corresponding element |
Symbol |
Symbol from the table of the elements |
Data File |
Click on the name to download a text file containing an a
list of emission lines
in Ångstroms and their associated strengths for the corresponding
element |
Emission Lines
4000-7000 Å |
Number of tabulated emission lines in the visible wavelength
range |
Jpeg Image |
JPEG screen grab (784 X 8). The narrow
height is to reduce transmission time, it expands to 64 pixels
using HEIGHT=64 option in IMG tag of HTML file.
To use images outside the context of a web browser,
you should expand them vertically with image processor.
|
Original Data |
Spectra of neutral and singly ionized elements from the
Astronomical Data Center
(ADC)
catalog
A6016,
by Reader J., Corliss Ch.H. :1981, 'Line Spectra of the Elements',
CRC Handbook of Chemistry and Physics; NSRDS-NBS 68 |
The element, wavelength range and line width are all
controlled by applet parameter (PARAM) tags in the HTML source for this
page.
There are other options such as width and height of spectra in pixels
and
contrast which can also be controlled. There are also
options to overlay a continuous blackbody spectrum
of varying strength and to limit the wavelength range.
For example here are the parameters for Neon :
<APPLET CODE=discharge.class WIDTH=784 HEIGHT=64>
<PARAM NAME=element VALUE=neon.txt>
<PARAM NAME=startWavelength VALUE=4000>
<PARAM NAME=endWavelength VALUE=7000>
<PARAM NAME=lineWidth VALUE=2.5>
<PARAM NAME=contrast VALUE=10>
<PARAM NAME=continuum VALUE=0.3>
</APPLET>
The simulated gas discharge spectrum is synthesized by assigning
each emission line to a gaussian and each point in the spectra
is computed as a mathematical sum of all the emission lines.
- Contrast:
- Range: 1 to 10000 (the upper limit comes from intensity of
the weakest line)
- Default: 1 (maximum of strongest line assigned to maximum
intensity, no distortion of line profile)
- Should be adjusted to 'burn out' the strongest lines and
boost the
intensity of the weaker lines. Should not be too high or some line
blending may occur, also the relative difference between the various
emission line strengths is lost. A compromise should be reached.
- Line Width:
- Range: 0 to 100
- Default: 3
- The width of emission lines is user controlled and should be
adjusted so that the line profile covers at least one pixel;
too small a width causes undersampling to occur and some lines
may 'disappear'! However too broad a line will cause blending
of lines that are closer together. Again, a compromise must be reached.
- Continuum:
- Range: 0 to 1
- Default: 0.3
- Physics: In many plasma environments some residual
broadband background light 'pollutes' the spectrum,
either by scattering from an external white source or internal
transitions involving the ion continuum. This causes a smooth
background to appear as weak 'rainbow' below the level of most
of the emission lines. This creates a 'pleasing' colored background
which 'fills' in the empty gap between the emission lines.
This applet was successfully run under the following browsers :
- NetScape Navigator 3.01
- NetScape Communicator 4.01, 4.03, 4.04
- HotJava 1.0
- Microsoft Internet Explorer v3.01
An upcoming version of this Applet will include
a more graphical user interface for controlling these parameters.
This Applet was created by John Talbot.
Source code is available : discharge.java
(Currently limited to 200 emission lines, however this limit can
easily be removed by changing the source code and recompiling.
There are more details on the color encoding
subroutine)
You can also download the source file, class file,
these HTML pages and all the element data as :
discharge.zip
(43 kBytes)
Physics Background
There are two basic line broadening mechanisms; instrumental and
intrinsic :
- Instrumental Broadening
- The first is due to finite spectroscopic resolution and can
be controlled by the researcher. Often higher resolution can be
achieved by larger gratings or coarse gratings operated in higher order
or longer path lengths for fourier transform spectrometers.
- Intrinsic Broadening
- The second is fundamental line broadening which can be caused
by at least three factors:
- Doppler Broadening
- Related to special relativity: Motion components
of a particle along the line of sight causes a shift in
radiation frequency. Since particles generally have a distribution
of velocities, this creates a gaussian blurring in the spectral lines.
- Lifetime Broadening
- Quantum mechanical in origin : Allowed transitions
have a short lifetime and this
translates to some uncertainty in the frequency of atomic
oscillators creating a Lorentzian line profile.
- Density Broadening
- Combination of quantum mechanical and electromagnetic
effects: Ions are bombarded by transient electric and magnetic fields
of high speed electrons zipping nearby, these electric fields
split and shift the energy levels. This constant perturbation within
the plasma environment depends most strongly on density and causes
strong line broadening in higher density plasmas. Temperature,
ionization level and the particular quantum transition involved
also plays a role.
In most thin plasmas one sees a combination of Doppler and
Lorentzian broadening called Voigt profiles. The Lorentzian component
affects mostly the low intensity 'wings' of the emission lines
so line profiles can be approximated as gaussians, especially
considering the dynamic range limitations of computer screens.
Most of the time spectra taken by researchers do not fully
resolve the intrinsic line profile so the lines are broadened
mainly by instrumental imperfection.
The data for these spectra is courtesy of the
Astronomical Data Center, and the National Space Science
Data Center through the World Data Center A for Rockets
and Satellites.
References
- Spectra of neutral and singly ionized elements from the
Astronomical Data Center
(ADC)
catalog
A6016,
by Reader J., Corliss Ch.H. :1981, 'Line Spectra of the Elements',
CRC Handbook of Chemistry and Physics; NSRDS-NBS 68
slightly modified by: J.Köppen, 13 Feb. 2003