All is Well

Iowa County, Wisconsin needs a secular, four-part (soprano, alto, tenor, bass) choir for adult singers that meets regularly. When was the last time this area had something like that? I really miss singing in the tenor section of the Sul Ross State University Concert Choir under the outstanding leadership of Dr. Donald Freed.  Dr. Freed is quite a good choral composer, too.  What a privilege it was to sing a number of his choral works during my years in Alpine, Texas.

Fortunately, each year I have the opportunity to sing with the Lands’ End Choir here in Dodgeville each holiday season, under the capable leadership of Phil DeKok, conductor, and Dawn Lingard, accompanist.  It is an amateur choir, of course, and though we rehearse just once a week over the noon hour from late October through early December, it is always a joy to be singing again.

This year, my favorite piece by far was All is Well by Michael W. Smith and Wayne Kirkpatrick (words & music) in a beautiful arrangement by Lloyd Larson.  Here is Lloyd talking about the piece:

https://www.youtube.com/watch?v=c6wqL6Kt_L4

I get pretty emotional about music, and I had a hard time getting through this particular piece without getting a little choked up and teary eyed.

The son of one of our choir members, Bev Adams-Sugden, recorded our performance of this work in Bldg. 5 over the noon hour on Tuesday, December 20, 2016.  Enjoy!

http://skythisweek.info/Lands End Choir 201612 B5 All is Well.mp4

 

Avoid Blue-Rich LED Lighting

As Dodgeville (and many other towns and cities) are planning to replace their streetlights with LED luminaires, it is imperative that we use LEDs with a CCT (correlated color temperature) of 3000 K or less (Jin et al. 2015).  This is a “warm” white light (similar to incandescent) rather than the “cold” blue-rich light often seen with LEDs.  Outdoor LED luminaires often come in at least three “flavors”: 3000K, 4000K, and 5000K.  For example, American Electric Lighting’s Autobahn Series.  5000K luminaires provide the bluest light, and should be avoided at all costs.  Of these three, 3000K would be best, and if 2700K is offered, use that.

Why does this matter?  On June 14, 2016, the American Medical Association issued guidance on this subject.

High-intensity LED lighting designs emit a large amount of blue light that appears white to the naked eye and create worse nighttime glare than conventional lighting.  Discomfort and disability from intense, blue-rich LED lighting can decrease visual acuity and safety, resulting in concerns and creating a road hazard.

The detrimental effects of high-intensity LED lighting are not limited to humans.  Excessive outdoor lighting disrupts many species that need a dark environment.  For instance, poorly designed LED lighting disorients some bird, insect, turtle and fish species, and U.S. national parks have adopted optimal lighting designs and practices that minimize the effects of light pollution on the environment.

Recognizing the detrimental effects of poorly-designed, high-intensity LED lighting, the AMA encourages communities to minimize and control blue-rich environmental lighting by using the lowest emission of blue light possible to reduce glare.  The AMA recommends an intensity threshold for optimal LED lighting that minimizes blue-rich light.  The AMA also recommends all LED lighting should be properly shielded to minimize glare and detrimental human health and environmental effects, and consideration should be given to utilize the ability of LED lighting to be dimmed for off-peak time periods.

Incidentally, for your residential lighting needs, a good local source for LED bulbs that are not blue-rich is Madison Lighting.  They have many LED bulbs in both 3000 K and 2700 K. I use 2700K bulbs exclusively in my home, and the warm white light they provide is an excellent replacement for incandescent and compact fluorescent bulbs.  Never purchase LED lighting without knowing the color temperature of the lights.

If you’re skeptical that the color temperature of LEDs is an important issue, I suggest you purchase a 2700K bulb and a 4000K or 5000K bulb with the same output lumens and compare them in your home.  I believe that you will much prefer the 2700K lighting.  If 2700K lighting is best for your home, then why should it not be best for outdoor lighting as well?

Besides, most streetlighting is currently high pressure sodium (HPS), which is inherently non-blue-rich.  You will find that 2700K LED lights offers better color rendering than HPS without the need to go to even bluer lights.

If you have ever been irritated at night by an oncoming vehicle with those awful “blue” headlights, you’ve experienced firsthand why blue-rich light in our nighttime environment must be minimized.

Why are 4000K and 5000K LED lights so prevalent?  They are easier and cheaper to manufacture, but with increased demand of 2700K and 3000K LED lights, economies of scale will reduce their cost, which today are generally slightly higher than blue-rich LEDs.

Now, a bit more about why blue light at night can be detrimental to human health, and the primary reason why the AMA issued a guidance on this subject.

In addition to image-forming rods and cones, there exist non-image-forming retinal cells in the human eye called intrinsically photosensitive retinal ganglion cells (ipRGCs) that help regulate our circadian rhythms.  Studies have shown that blue light is far more disruptive to our circadian rhythms than redder light (Lockley et al. 2003).

Now, on to the environment.  Using a clever technique that compared sky brightness at several locations on several nights both with and without snow cover, Fabio Falchi (Falchi 2011) determined that at least 60% of light going up into the night sky is direct waste lighting, and 40% or less is reflected light.  This is as good an argument as any that we still have a long way to go towards using only full-cutoff luminaires that do not produce any direct uplight.  Blue light scatters much more in the night sky than red light, and this is due to Rayleigh scattering which tells us that the amount of scattering is proportional to the inverse of the wavelength of light to the fourth power, σs ∝ 1 / λ4.  This also explains why the daytime sky is blue.

Bluer wavelengths of light thus increase artificial sky glow to a much greater extent than redder wavelengths do.  Not only is an increase in blue light bad for astronomy, but its impact on the natural world is likely to be adverse as well.

Falchi recommends a total ban of wavelengths shorter than 540 nm for nighttime lighting, both outdoor and indoor.  He goes on to say that, at the very least, no more light shortward of 540 nm should be allowed than that currently emitted by high pressure sodium lamps, lumen for lumen.

References
Falchi, F. 2011, MNRAS, 412, 33
Falchi, F. 2016, The World Atlas of Light Pollution, p. 44
Jin, H., Jin, S., Chen, L., et al. 2015, IEEE Photonics Journal. 7(6), 1-9
Lockley, S. W., et al. 2003, J Clin Endocrinol Metab. 88(9), 45025

Polarization of Starlight

The space between stars is not a perfect vacuum. It contains gas molecules and dust grains, although they are few and far between by any terrestrial standard. In the presence of a magnetic field, many types of interstellar dust grains line up in a way that is reminiscent of iron filings near a bar magnet. When light from a star passes through a region of space with magnetically-aligned dust grains (though in this case the short axis of the dust grains aligns with the local magnetic field), light with the electric field vector perpendicular to the long axis of the grains is less likely to be absorbed by the grains than light whose electric field vector is parallel to the long axis of the grains. This causes the light passing through such regions of space to become slightly polarized, and the polarization of starlight is something we can measure easily here on Earth. In this way, the strength and orientation of invisible interstellar or circumstellar magnetic fields can be determined at a distance.

Various astrophysical processes result in polarized electromagnetic radiation.  The differential absorption already mentioned polarizes the light from all stars to one degree or another.  Only the Sun—which is vastly nearer—offers us almost completely unpolarized light. Scattering of light off of interstellar clouds and planetary surfaces also results in polarization.  Finally, both synchrotron and cyclotron emission produce a characteristic polarization.

The polarization of starlight can be measured by the use of a polarimeter attached to the telescope.  Unlike standard photometry, polarization is simpler to measure with ground-based telescopes because the measurements are relative rather than absolute and, under normal circumstances, the Earth’s atmosphere does not affect the polarization state of incoming light.  Care must be taken, however, to ensure that the telescope itself does not create instrumental polarization due to oblique reflections.  Placing the polarimeter at the unfolded Cassegrain focus is one desirable configuration (Hough 2006).

References
Hough, J. 2006, A&G, 47, 3.31

Eridanus Delights

The sixth largest constellation in the sky stretches from near Rigel on the west side of Orion down to 1st-magnitude lucida Achernar (declination -57°), a star that rotates so rapidly that its polar diameter is not even ¾ its equatorial diameter (Domiciano de Souza et al. 2014).  Achernar (α Eri) is appropriately named.  It means “The End of the River” in Arabic.

Eridanus, the River, contains two very special, easily seen, stars. 40 Eridani (also known as Keid and Omicron2 Eridani), a visual triple star system (magnitudes 4.4, 9.5, and 11.2) just 16.3 light years away, presents the most easily observed white dwarf star, 9.5-magnitude 40 Eri B, visible in any telescope.

A little further west we can find 3.7-magnitude Epsilon Eridani, the nearest star beyond the Alpha Centauri system thought to harbor one or more planets. Compared to our Sun, ε Eri is cooler (K2V), much younger (200-800 Myr), and somewhat metal-deficient (74% solar), and it is just 10.5 light years away. This youthful star still sports a dusty disk between radii 35 and 75 AU (Greaves et al. 1998), inside of which its putative planet, Epsilon Eridani b—at least 0.6 to 0.9 Jupiter masses—travels around the star in a highly elliptical orbit, completing one revolution every 6.85 to 7.26 years. At periastron, Epsilon Eridani b lies between 1.0 and 2.1 AU from its parent star, and at apastron, its distance is 4.9 to 5.8 AU (Mizuki et al. 2016). However, the existence of this or any other planets in the system is still far from certain, primarily due to the high level of photospheric activity that is difficult to disentangle from the radial velocity signals of any possible orbiting planets (Giguere et al. 2016).

References
Domiciano de Souza, A., Kervella, P., et al. 2014, A&A, 569, A10
Giguere, M. J., Fischer, D. A., et al. 2016, ApJ, 824, 150
Greaves, J. S., Holland, W. S., et al. 1998, ApJL, 506, L133
Mizuki, T., Yamada, T., et al. 2016, A&A, 595, A79

A Space Shuttle Remembrance

On Tuesday, December 19, 2006, I witnessed a delightful event: the Space Shuttle Discovery and the International Space Station traveling together through the western sky, only about 1° apart.

Around 6:34 p.m., I spotted a -1 magnitude International Space Station (ISS) traveling NE above the western horizon. It quickly became apparent that there was a +1 magnitude point of light moving right along with the ISS, leading it by about one degree. It was the Space Shuttle Discovery, which had undocked from the ISS just 2h25m earlier (4:09 p.m.)!

I quickly surmised that Discovery must have fired retrorockets to put some distance between it and the ISS by lowering Discovery‘s altitude. Since Discovery was at a lower altitude, it had been orbiting faster, which is why it was leading the ISS by about a degree. As the pair approached the constellation Lyra, further evidence of Discovery‘s lower altitude occurred when it disappeared into the shadow of the Earth several degrees further west of where the ISS disappeared a few seconds later.

Intergalactic Stars

Did you know that a few percent of all stars are traveling alone through intergalactic space, no longer a part of any galaxy?  Gravitational interactions between stars or between stars and black holes can occasionally accelerate a star to galactic escape velocity so that it is thrown (eventually) into intergalactic space.  When the star first enters intergalactic space, the view of your home galaxy would be pretty remarkable, but eventually (eons later, of course) there would be very few naked eye objects in your night sky. Just moons and planets, meteors, aurora, comets, the zodiacal light, and maybe a galaxy or two. Anything else would require a telescope.  And an observer, of course.

The first evidence for intergalactic stars came from the detection of diffuse light between galaxies (Zwicky 1952).  Much later, intergalactic planetary nebulae were detected in the Fornax galaxy cluster (Theuns & Warren 1997).  More recently, intergalactic red giant stars have been detected in the Virgo galaxy cluster using the Hubble Space Telescope (Ferguson et al. 1998).

The Fornax cluster lies about 62 million light years distant, and the Virgo cluster 54 million light years distant.  Have any intergalactic stars been detected near our Milky Way galaxy?  Brown et al. (2005) discovered the first hypervelocity star, SDSS J090745.0+024507, a 20th-magnitude star in the constellation Hydra.  Though it is just 160,000 light years from the center of our galaxy, it is moving away from the Galactic center at an astonishing radial velocity of 709 km/s.  Even though this one-dimensional radial velocity1 is only a lower limit to the star’s true 3D space motion, it is far and away fast enough to escape our Milky Way galaxy altogether.  Gaia will probably be able to measure this runaway star’s proper motion in right ascension and declination, thus allowing a determination of the true space velocity of SDSS J090745.0+024507 relative to the Galactic center.

Several more hypervelocity stars have been discovered since 2005.  One of them, US 708, a 19th-magnitude white dwarf in Ursa Major, is exiting our galaxy at a velocity of at least 1200 km/s!  This makes it the fastest on record (Geier et al. 2015).

1The observed one-dimensional radial velocity as seen from Earth is corrected for the Earth’s rotation and motion around the Sun, and the Sun’s motion around the center of the Milky Way galaxy to determine the galactocentric radial velocity.

References
Brown, W. R., Geller, M. J., Kenyon, S. J., Kurtz, M. J. 2005, ApJ, 622, L33
Ferguson, H. C., Tanvir, N. R., & von Hippel, T. 1998, Nature, 391, 461
Geier, S., Fürst, F., Ziegerer, E., et al. 2015a, Science, 347, 1126
Theuns T., Warren S. J., 1997, MNRAS, 284, 11
Zwicky F., 1952, PASP, 64, 242

We Miss You, Carl Sagan

It is hard to believe that Carl Sagan has been gone now for 20 years.  In fact, he died on this day in 1996 of myelodysplastic syndrome at the age of 62.  He was one of the 20th century’s truly great science popularizers.  In addition to writing or co-writing fifteen books, his 1980 PBS television series Cosmos remains the gold standard against which all other astronomy documentaries will be judged.

Here is a listing of Carl Sagan’s books published during his lifetime:

  • Intelligent Life in the Universe (1966; revised and expanded edition of Iosif Shklovsky’s 1962 book of the same name)
  • Planets (1966; one of the LIFE Science Library series)
  • The Cosmic Connection (1973)
  • Communication with Extraterrestrial Intelligence: CETI (1973; Carl Sagan, editor)
  • Other Worlds (1975)
  • The Dragons of Eden: Speculations on the Evolution of Human Intelligence (1977)
  • Murmurs of Earth: The Voyager Interstellar Record (1978; with others)
  • Broca’s Brain: Reflections on the Romance of Science (1979)
  • Cosmos (1980)
  • Contact (1985)
  • Comet (1985; with Ann Druyan)
  • Shadows of Forgotten Ancestors: A Search for Who We Are (1993; with Ann Druyan)
  • Pale Blue Dot: A Vision of the Human Future in Space (1994)
  • The Demon-Haunted World: Science as a Candle in the Dark (1995)
  • Billions and Billions: Thoughts on Life and Death at the Brink of the Millennium (written 1996, published posthumously in 1997)

Carl Sagan’s final interview was with Charlie Rose on May 27, 1996, less than seven months before his death.  You can see it here.

Carl’s daughter, Sasha Sagan, wrote a loving and thoughtful essay in 2014, the 80th anniversary year of his birth.

Here, now, are just a few of Carl Sagan’s most memorable quotes.

Extraordinary claims require extraordinary evidence.

Somewhere, something incredible is waiting to be known.

The size and age of the Cosmos are beyond ordinary human understanding.  Lost somewhere between immensity and eternity is our tiny planetary home.

We make our world significant by the courage of our questions and by the depth of our answers.

A central lesson of science is that to understand complex issues (or even simple ones), we must try to free our minds of dogma and to guarantee the freedom to publish, to contradict, and to experiment.  Arguments from authority are unacceptable.

Science is a way of thinking much more than it is a body of knowledge.

For small creatures such as we the vastness is bearable only through love.

One of the criteria for national leadership should be a talent for understanding, encouraging, and making constructive use of vigorous criticism.

We’ve arranged a global civilization in which the most crucial elements — transportation, communications, and all other industries; agriculture, medicine, education, entertainment, protecting the environment; and even the key democratic institution of voting, profoundly depend on science and technology.  We have also arranged things so that almost no one understands science and technology.  This is a prescription for disaster.  We might get away with it for a while, but sooner or later this combustible mixture of ignorance and power is going to blow up in our faces.

Humans may crave absolute certainty; they may aspire to it; they may pretend, as partisans of certain religions do, to have attained it.  But the history of science — by far the most successful claim to knowledge accessible to humans — teaches that the most we can hope for is successive improvement in our understanding, learning from our mistakes, an asymptotic approach to the Universe, but with the proviso that absolute certainty will always elude us.

The Cosmos is all that is or ever was or ever will be. Our feeblest contemplations of the Cosmos stir us—there is a tingling in the spine, a catch in the voice, a faint sensation, as if a distant memory, of falling from a height. We know we are approaching the greatest of mysteries.

Our Vanishing Sidewalks

I’ll wager that most of you over 50 years of age grew up on a street with sidewalks on both sides of the street and all the way around the block.  You probably made use of them often.  Sidewalks used to be essential in residential neighborhoods.  Today, not so much.  More often then not, newer residential subdivisions do not have sidewalks, nor do they have off-road walking trails meandering through them.  If you walk at all, you have to walk in the street.  Having motorized vehicles and pedestrians sharing the same space is inherently risky, especially at night.

It is interesting to note that the Ancient Romans built sidewalks everywhere, but by the Middle Ages, people were again walking in the streets.  Progress is not inevitable.

Today, developers generally consider sidewalks to be an unnecessary expense, and homeowners are not clamoring for them because they are usually saddled with the expense of keeping them up.

Therein lies the problem.  It is my view that sidewalks should be treated as public infrastructure no different than city streets.  Just as the developer pays most or all of the cost of building the streets in a new residential subdivision, they, too, should be required to build sidewalks or, in a more rural subdivision, walking trails.  Sidewalks should be maintained (and that includes snow removal) by local government supported by tax revenues, not directly by the homeowner.

Perhaps the typical homeowner might be more supportive of sidewalks if they didn’t have to shovel the sidewalk in front of their house each time it snows, or replace sidewalk slabs when they’re broken or cracked.  Sure, they’d still be paying taxes to support those activities, but it would be a win-win situation for the entire community.  And shouldn’t that be our goal—the common good?

Voyager 4.5 by Carina Software

My all-time favorite planetarium software program is Voyager 4.5 from Carina Software.  Hardly a day goes by when I am not using it, and my use of Voyager goes all the way back to 1993.  The current version for Mac OS X (and Windows) is 4.5.7.  Sadly, the last update was in 2010.  I wish there was something we could do to ensure that Voyager will be maintained and enhanced in the future.

Speaking of maintenance, in 2015 Voyager ceased being able to import comet and asteroid orbital elements through its automatic Updates process.  This happened because the URL changed for both.  Seems like a pretty easy fix to me.  If Carina won’t fix it, then maybe someone can edit the executable and change the two URLs?

Fortunately, you can still manually import these orbital elements by following these instructions.

Adding Comets
  1. Navigate your web browser to https://www.minorplanetcenter.net/iau/Ephemerides/Comets/Soft00Cmt.txt and save this page to a file, which will automatically be called Soft00cmt.txt.  You can save it anywhere, but I’d suggest you save it in the Import Files folder in the Voyager 4.5 main directory within your Applications folder.
  2. In Voyager, go to File : Import : Comet Orbit File…
  3. Navigate to Applications : Voyager 4.5 : Import Files : Soft00Cmt.txt and click Open.  You will get a message box asking “Before importing new data, do you want to delete all current asteroid/comet/satellite data?”  Click Yes.  Next you will see an Import results box showing you the number of comets added to Voyager’s database.  Click OK.
Adding Asteroids
  1. Navigate your web browser to https://www.minorplanetcenter.net/iau/MPCORB.html and under Available Files right click on MPCORB.DAT (uncompressed) and Save Link As… to your Voyager 4.5 Import Files folder.  Do not open this file in your web browser as it is over 147 Mb in size!  The file saved is called MPCORB.DAT.
  2. Navigate to Applications : Voyager 4.5 : Import Files : MPCORB.DAT and edit the MPCORB.DAT file with the editor of your choice.  Remove the header lines at the top of the file right down through the line of dashes, and save the file.
  3. In Voyager, go to File : Import : Asteroid Orbit File…
  4. Navigate to Applications : Voyager 4.5 : Import Files : MPCORB.DAT and click Open.  You will get a message box asking “Before importing new data, do you want to delete all current asteroid/comet/satellite data?”  Click Yes.  It will take a while to import all the asteroids, and then you will see an Import results box showing you the number of asteroids (and transNeptunian objects, by the way) added to Voyager’s database.  Click OK.

Polar Aligning a Telescope

Whether you have a portable or observatory-mounted equatorial telescope, accurate polar alignment is a must if you plan to do any long-exposure photography.  Here’s one basic procedure you can use.

If you have a fork-mounted Schmidt-Cassegrain telescope, you can begin your polar alignment process during the day.  First, using a bubble level, make sure your telescope base is completely level.  Next, adjust the equatorial wedge so that it is set to the latitude of your observing location.  Then, point the telescope at the zenith and adjust both the right ascension and declination motions until a bubble level atop the telescope end cap reads completely level.  Then set your declination setting circle so that the declination reads the same number as the latitude of your observing location.

As soon as it is dark enough to see a star, align your finderscope and main scope so that the star is at the center of both fields.  When it is dark enough to see Polaris, set your telescope’s declination to 90° and adjust the azimuth of the equatorial wedge until Polaris is as near as possible to the center of the finderscope’s field of view.

With your unaided eyes, note the location of the 2nd brightest star in the Little Dipper, Kochab, relative to Polaris.  Kochab is the bowl star at the opposite end from Polaris that is closest to the bowl of the Big Dipper.  Presently, the North Celestial Pole is located 40 arcminutes (⅔ degree = about one-and-a-quarter moon-widths) away from Polaris in the direction of Kochab.  Adjust the altitude and azimuth of the equatorial wedge so that the center of the finder field is located ⅔° from Polaris in the direction of Kochab.  This may be quite difficult, so just do the best you can.

Now, pick a star on or very near the celestial meridian and the celestial equator (declination 0°).  Center the star in the main scope and make sure the clock drive is on.  If the star drifts south, make a slight adjustment to the equatorial wedge towards the west (counterclockwise).  If the star drifts north, make a slight adjustment to the equatorial wedge towards the east (clockwise).  Ignore any east-west drift.  Keep making adjustments until you have eliminated all drift.

Next, center a star in the main scope that is about 20° above the eastern horizon, and again very near the celestial equator.  If the star drifts south, adjust the altitude of the equatorial wedge so it points slightly higher in the sky.  If the star drifts north, adjust the altitude of the equatorial wedge so it points slightly lower in the sky.  Ignore any east-west drift.  Keep making adjustments until you have eliminated all drift.  (You can also use an equatorial star about 20° above the western horizon, but if the star drifts south you’ll need to lower the equatorial wedge, and if the star drifts north, you’ll need to raise the equatorial wedge.)

Now, pick another equatorial star on the meridian and repeat the procedure outlined in the two paragraphs above until no more adjustments are needed.

Your telescope is now precisely polar aligned.