** Parsecs**

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INTRODUCTION

The sweep of the night sky can be awe inspiring. Our ancestors thought the unapproachable stars might be campfires of powerful and mysterious beings or even immortal gods tracing never ending paths impervious to change and thus free of imperfection and decay. Whatever our early musings, the study of the distant heavens has been a difficult one. Only gradually over many centuries have we painstakingly been able to map its motions and chart its depths. Indeed, we might consider that we only knew of the existence of galaxies and the scale of the universe, stretching to just less than about 100 billion light years, within the last century and just within the bounds of living human memory.

Today we have both a direct and indirect method of measuring extraterrestrial distances. In the indirect method, we need to know how intrinsically bright a star is. This is the luminosity or total amount of light emitted and depends on the temperature, or color, and the width of the star. Knowing such fundamental properties solves the problem of whether a particular star is a bright one far away or a dim one much closer. This it is because it is a straightforward task to calculate how much fainter that star would appear as function of distance from earth.

For nearby stars, we have a direct technique called “parallax” which does not depend on luminosity but rather on simple geometry. Fortunately, knowing a few unmistakable distances via this method allows us to develop stellar models based on spectra and to group these closer stars into different categories. Each category has roughly the same intrinsic brightness creating what astronomers call “standard candles”. Assuming stars much further away have the same properties as those nearby, this gives us a yardstick for the cosmos.

PARALLAX

Parallax is our most important and trustworthy technique. It relies on the fact that as we move, nearby objects appear to shift their positions more than objects which are further away. The standard demonstration is to ask you to stretch out your arm and hold up your thumb. Then close one eye only and then the other. Your thumb will appear to move slightly with respect to the distant background.

The same thing happens for stars as the earth swings around the sun. Most stars are so far away that despite heroic efforts, we can see no shift whatever against the distant background. These fixed stars form a dense matrix of well known constellations. But a relatively few do shift their position ever so slightly and by amounts we can just barely measure. Basically the target star appears to move in an ellipse against the distant background [1]. The trick is to measure the angle, θ, between that star and the center of the ellipse. This is sometimes made more difficult if the star is not visible in the night sky during part of the year. Motions of fainter stars are also more difficult to accurately determine. But in any event, the greater the angular extent of the ellipse, the closer the star as diagrammed below [2].

In the above drawing, “A” is an astronomical unit (AU) or the distance from the Earth to the Sun. In modern times this has been measured to great precision and is on average 92,955,807 miles or 149,597,871 km. But since the orbit of the earth is slightly elliptical, the earth-sun distance varies from a farthest point or 1.017 AU at aphelion in July to a nearest point of 0.983 AU at perihelion in January. The difference amounts to about 3.16 million miles. And yes, for those of us in the Northern Hemisphere, we are closer to the sun in winter but then the seasons are caused by the tilt of the earth and not the distance to the sun. And for those emotionally challenged by this absurdity, the Southern Hemisphere has the opposite and expected relationship.

In any event the equation for the distance is

Where we have made the two assumptions that

PARSEC

A “parsec” is that distance from the earth to star when the angle, θ, is one arc-second and is a distance of 3.26 light years. Note that the parallax angle is inversely proportional to distance.

For reference, one arc-second is

[ (2π) radians / (360) degrees] * (1/60) degree/arc-minutes
* (1/60) arc-minutes/arc-seconds =
4.848 * 10^{-6} radians

so that the distance d_{2} for that angle is

Switching units, we note one light year is

(365.25) days/year * (24) hours/day * (3600) seconds/hour *
(186,280) miles/second = 5.878 * 10^{12}
miles

so that

In the Star Wars movie franchise, the loveable smuggler Hans Solo brags that his ship, the Millennium Falcon, made the infamous “Kessel” run in less than 12 parsecs breaking a long standing record. Attempting to sound both hip and scientific, the writers confused units of distance for those of speed. Bewildered fans, whose lives revolve around movies and movie characters, were only slightly placated when director Stephen Spielberg spun the mistake as referring to the quality of the ship’s navigational computer plotting shorter routes rather than any ability to outrun revenue agents.

ASSUMPTIONS

We have first made the assumption that because d_{1 }>>
d_{2} then we can set the angle, φ, to zero. We would have preferred
to measure the angle the star makes with respect to the sun (90 – α) instead of
approximating it with (θ + φ). But we cannot generally observe both during
daylight hours. Also the measurement would be difficult since we would have to
locate the exact center of the sun to great precision.

We can straightforwardly calculate the error in the
estimation of d_{2} is because of this assumption. To accomplish this we
define a few specific lengths as follows

where we have defined the lengths

Where an assumption has been made that φ = 0. We can write

The first step is to use the Pythagorean theorem to calculate several lengths

which can be refined even more using

So that finally

We can apply this to the error estimate giving

And the absolute value of the relative error is

And if we parameterize the distances using

So for reasonable values of the parameters, this assumption
is more than reasonable. For instance the nearest star, Proxima Centauri is
4.243 light years or 268,300 AU and the distant background stars thousands of
times farther away than that. So for k_{2} = 268,300 and k_{1}
> 1000, we have

which is well below our best instrumental measurement errors.

We also note that the angle
θ is never more than one arc-second which is 4.848 * 10^{-6 }radians. And so a simple expansion of the tangent( θ
) function is as follows

For one arc-second the error associated with this
approximation is on the order of one part in 10^{12 }and even less for
smaller angles.

PROGRESS

From the surface of the earth the blurring of the atmosphere limits the maximum angle we can measure to slightly less than about 0.01 arcseconds for the brightest stars. This corresponds to stellar distances of 100 parsecs or about 320 light years. This proved so difficult that the first measurement was only made in 1838 by Friedrich Bessel of Germany for the star 61 Cygni which has a parallax angle of about 0.287 arc seconds. The closest star Proxima Centauri, has the largest parallax observed of 0.772 arc seconds. Indeed, the total number of stellar parallaxes ever observed from the surface of the Earth is barely one hundred.

This changed in 1989 with the launch of the Hipparcos mission which returned data until 1993 when it consumables were exhausted. From Earth orbit, the distances to about 120,000 of the brighter stars were measured with an accuracy of roughly 1000-2000 micro arc seconds or 1600-3200 light years. An additional one million stars were measured to an accuracy of 10,000 micro arc seconds. There are about 80 million stars within 2000 light years so this is a small fraction of the total.

In July of 2014, the Gaia satellite was launched and expects to measure the parallaxes of one billion stars. The best accuracy will be 6.7 micro arc seconds and a few tens of micro arc seconds for fainter objects. This is roughly one percent of the entire Milky Way Galaxy.

NOTES

1. The actual motion of the star against the background is a projection of the earth’s orbit onto a plane which is perpendicular to a line drawn from the sun to the star. And the projection of an ellipse is also an ellipse.

2. For simplicity, the target star diagrammed is along a line at right angles to the plane of the earth’s orbit. But without loss of generality, the geometry have the same considerations for any star. Note that if the star were on a line that was entirely along the plane of the earth’s orbit, its apparent path would collapse from an ellipse to a back and forth motion along a line.