Jimmy Cornell - World Cruising Routes World Cruising Routes by Jimmy Cornell

      

Other books by Jimmy Cornell
| Home | Mailing Lists | Bookstore | Weather | Tide Predictions | Bowditch |

Latitude and Longitude by "Noon Sun"

From: Frank Reed (no email)
Date: Sat Jun 04 2005 - 19:54:15 EDT

  • Next message: Frank Reed: "Re: suggestion for a satisfactory celnav narrative"

    First things first: I've put the phrase "Noon Sun" in quotes here because
    the set of sights required for this system goes a little beyond the standard
    procedure for shooting the Noon Sun for latitude only.

    This short method of celestial navigation will get you latitude and
    longitude to about +/-2 miles and +/-5 miles respectively --more than adequate for
    any conceivable modern practical purpose. You can cross oceans safely and
    reliably for years on end using this technique if it suits you to do so. Its
    enormous advantage is simplicity. It's easy to teach, easy to demonstrate, easy to
    learn, and also easy to re-learn if necessary. I mention this because most
    people who are learning celestial navigation today will quickly forget it.
    What's the point of learning something if you can't reconstruct your knowledge
    of it quickly when and if the need actually arises to use it? It's tough to
    resurrect an understanding of the tools of standard celestial navigation on
    short notice, but easy with this lat/lon at noon method. Additionally, this
    method does not require learning all the details of using a Nautical Almanac (you
    don't need one at all --only a short table of declination and equation of
    time, possibly graphed as an "analemma") and it needs no cumbersome sight
    reduction tables.

    Here's how it's done:

    Start 20 or 30 minutes before estimated local noon. Shoot the Sun's altitude
    with your sextant every five or ten minutes (or more often if you're so
    inclined) and record the altitudes and times by your watch (true GMT). Continue
    shooting until 20 or 30 minutes after local noon. [note the difference from a
    noon latitude sight --we're recording sights leading up to and following
    noon-- usually these are thrown away]

    Next you need to correct for your speed towards or away from the Sun. For
    example, if we're sailing south and the Sun is to the south of us, then each
    altitude that we have measured will be a little higher as we get closer to the
    latitude where the Sun is straight up. We need to 'back out' this effect so
    that the data can be used to get a fix at a specific point and time. This isn't
    hard. First, we need the fraction of our speed that is in the north-south
    direction. If I'm sailing SW at 10 knots, then the portion southbound (in the
    Sun's direction) is about 7.1 knots. You can get this fraction by simple
    plotting or an easy calculation. Next we need the Sun's speed. The position where
    the Sun is straight overhead is moving north in spring, stops around June
    21, then heads south in fall, bottoming out around December 21 (season names
    are northern hemisphere biased here). It is sufficient for the purposes of this
     method to say that the Sun's speed is 1 knot northbound in late winter
    through mid spring, 1 knot southbound from late summer through mid autumn, and 0
    for a month or two around both solstices (it's easy to prepare a monthly table
     if you want a little more accuracy). Add these speeds up to find out how
    much you're moving towards or away from the Sun. If you're moving towards the
    Sun, then for every six minutes away from noon, add 0.1 minutes of arc for
    every knot of speed to the altitudes before noon and subtract 0.1 minutes of arc
    for every knot of speed to the altitudes after noon. Reverse the rules if
    you're moving away from the Sun. Spelled out verbally like this, this speed
    correction can sound tedious but the concept is really very simple and it's very
    easy to do. [Incidentally, George Huxtable deserves credit for emphasizing
    the importance of dealing with this issue (although I don't think he ever
    spelled out how to do it)]

    Now graph the altitudes (use proper graph paper here if at all possible):
    Sun's altitude on the y-axis versus GMT on the x-axis. The size of the graph
    should be roughly square, maybe 6 inches by 6 inches so that you can clearly see
     the rise and fall of altitude. For longitude, you will need to determine the
     axis of symmetry of the parabolic arch of points that you've plotted. There
    is a simple way to do this: make an eyeball estimate of the center and
    lightly fold the graph paper in half along this vertical (don't "hard crease" the
    fold yet). Now hold it up to the light. You can see the data points preceding
    noon superimposed over the data points following noon which are visible
    through the paper. Slide the paper back and forth until all of the points, before
    and after, make the best possible smooth arch (half a parabola). Now crease
    the paper. Unfold and the crease line will mark the center of symmetry of the
    measured points with considerable accuracy. Reading down along this crease to
     the x-axis, you can now read off the GMT of Local Apparent Noon. Reading
    back up the crease to the data, you can pick off the Sun's maximum noon altitude
    (which is probably already recorded but if you missed the exact moment of
    LAN you can get it this way).

    Next we need two pieces of almanac data: the Sun's declination for this
    approximate GMT on this date and the Equation of Time for the same date and time.
    You do NOT need a current Nautical Almanac for this. The exact value of
    declination and Equation of Time varies in a four-year cycle depending on whether
    this year is a leap year or the first, second, or third year after. So we
    don't need an almanac for this. A simple table will do (where to get one?
    Today, they're very easy to generate on-the-fly... or you could use an old
    Nautical Almanac... or you could also use an analemma drawn on a sufficiently large
    scale).

    Apply the Equation of Time to the GMT of Local Apparent Noon that you found
    above. You now have the Local Mean Time at LAN, and you already know the
    Greenwich Mean Time. The difference between those two times is your longitude.
    Convert this to degrees at the rate of 1 degree of longitude for every four
    minutes of time difference. Done. We've got our longitude.

    Now for latitude. Notice that we didn't correct any of our altitudes for
    index correction or dip or refraction or the Sun's semi-diameter. These
    corrections are totally unnecessary for the longitude determination. But we need them
    for latitude. Take the Sun's altitude at the time of LAN (read off the
    "crease" or actually observed by watching the Sun "hang" at the moment of LAN).
    Correct it for index correction, dip, refraction and semi-diameter as usual.
    This gives you the Sun's corrected observed altitude. Subtract from 90 degrees.
    This "noon zenith distance" tells us how many degrees and minutes we are
    away from the latitude where the Sun is straight up. The latitude where the Sun
    is straight is, by definition, the "declination" that we have looked up
    previously from our tables. So if the Sun is north of us at noon, then we are
    south of the Sun's declination (latitude) by exactly the number of degrees and
    minutes in the noon zenith distance. If the Sun is south of us at noon, then we
    are north of the Sun's declination by the same amount. A simple addition or
    subtraction yields the required latitude. Done.

    We've spent about ten minutes making and recording observations of the Sun's
    altitude over the course of 45 minutes to an hour, and reduced those
    observations to get our latitude and longitude at noon with about five minutes of
    paperwork. Not bad!

    Again, the overwhelming advantage of this "short celestial" is that it can
    be taught easily, learned quickly, and RE-learned quickly on the spot if
    necessary. An additional advantage is that it requires an absolute minimum of
    materials. You need a sextant (metal if at all possible, but plastic will do), a
    decent, cheap watch or small clock, tables of refraction and dip (one sheet
    of paper), a four-year revolving almanac of the Sun's declination and equation
    of time (another sheet or two of paper), and some graph paper and a pencil.
    You could even print out these (or equivalent) instructions and throw
    everything in the case with your sextant.

    As for disadvantages, they really depend on the student and his or her
    expectations. What is it that we want to do with celestial navigation? Why study
    any method? And for a thousand students, you will get a thousand answers. The
    days are gone when celestial navigation was essential and fixed curricula
    could be dictated for students to either take in their entirety or leave. This
    field has moved on to the stage of "a la carte" learning. It can be a pain in
    the neck for instructors accustomed to doing things the same way year after
    year but it's a real liberation for students and possibly also for more
    creative teachers and "information publishers".

    -FER
    42.0N 87.7W, or 41.4N 72.1W.
    www.HistoricalAtlas.com/lunars


  • Next message: Frank Reed: "Re: suggestion for a satisfactory celnav narrative"



    | Home | Mailing Lists | Bookstore | Weather | Tide Predictions | Bowditch | Trawlerworld |