# NavList:

## A Community Devoted to the Preservation and Practice of Celestial Navigation and Other Methods of Traditional Wayfinding

**Re: Measuring (and**

**From:**Bruce J. Pennino

**Date:**2013 Feb 28, 21:10 -0500

Hi Brad:

I've read these results several times and the
conclusions are unclear to me. What is the best method? Is the NA
table for dip consistently high, low ? Considering all of the
errors involved for real life practice, NA seems good enough for me with my
shaky hand and fluttering eye.

I admit this is very interesting.

Bruce

----- Original Message -----From:Brad MorrisSent:Thursday, February 28, 2013 5:26 PMSubject:[NavList 22545] Re: Re: Re: Re: Re: Re: Re: Measuring (and

Dr. Langley The link you offered offered is a site by Andrew Young, with special notice to the equation >> dip = arccos ( (R/(1-k)) / ( h + R/(1-k)) ) >> where R is the radius of the earth >> k is the refraction factor (?) >> h is the height of eye I have directly addressed Dr. Young with this email, as he might actually enjoy this conversation. For those wishing a scientific paper on this topic, please see http://www.fer3.com/arc/imgx/Dip-of-the-horizon-Freiesleb.pdf Within this paper, you will find a device referenced as the Pulfrich instrument. This measures both horizons simultaneously. My Reflecting Circle is capable of this same measurement. For those wishing to see a self guided tour of the instrument in question, please see http://www.fer3.com/arc/imgx/Prismatic-Circle-of-Reflecti.ppt Today I had occasion to repeat the dip measurement at Orient Point. It was midday, warm and this time I was very sure to avoid any islands that could influence the dip result. I was able to obtain a measurement in 13 minutes of time. The practice from last time is beginning to pay off. Firstly, I preset the Reflecting Circle to a nominal 179 degrees 40 minutes and determined which way to turn the adjusting knob. Why 179 degrees and 40 minutes? I'm holding the instrument upside down to better pull my head out of the optical path, so this is the same as measuring 180 degrees 20 minutes. It is a circle after all! I carefully aligned the horizons and then observed the indices. There are TWO index verniers on my device, such that any eccentricity error in the indices are eliminated. The index error for Index A has been made to be 0. Index B has an index error of 2' 20", on the arc. The reading for Index A was 179 degrees 55 minutes 0 seconds. The reading for Index B was 179 degrees 57 minutes 30 seconds, correcting for index error (its on, take it off) yields 179 degrees 55 minutes 10 seconds. Chauvenet tells us to average the two readings to realize the final measurement, yielding 179 degrees 55 minutes and 5 seconds. Since we measured upside down, will subtract that from 360 degrees, yielding a final 180 degrees 4 minutes 55 seconds. At NDBC Buoy 44017 (Atlantic Ocean) we have air temp 41.9F water temp 42.1F. At NDBC Buoy 44039 (Long Island Sound) we have air temp 37.8F water temp 36.3 The winds were relatively calm Height of eye 10 feet 9 inches = 3.268 meters Using the equation dip=0.02977 sqrt(h), we obtain 0.0538 degrees (3'14"). Since there's two dips, we must double that, yielding 6'28". The error term is 1'33" Using the equation from Andrew Young's site (see above), with k=0.13, R=6,371,000 meters, we obtain 0.05412 degrees (3'14"), for the same error term as above In the paper above, we have Koss (equation I) which is dip = 1.82'sqrt(h) -0.37'*(delta temp between water temp and air temp, degrees C) For the Atlantic we have dip = 1.82'*sqrt(3.268) - 0.37*(.1111) dip =3.2901 minutes ( 3'15") For Long Island Sound, we have dip = 1.82*sqrt(3.268)-0.37*(.8333) dip = 2.9817 (2'59") Summing the two, we obtain 6'14", for an error term of 1'19". In paragraph 7 (page 295) of the paper, dip is shown to be dip = 1.74sqrt(h)-.47*delta Atlantic Dip 3.0932 minutes (3'6") Long Island Sound Dip 2.7538 minutes (2'45") Total Dip = 3'6"+2'45"= 5'45" Error Term 50" Naturally, there may still be bias in my measurement. Marcel has indicated that I should look at Dr. Young's paper Sunset Science II, for his equation. I found the paper to cost me $30, so I respectfully decline. Should others have access to this paper (like Dr. Young himself), perhaps they will attempt this reduction. Best Regards Brad Morris On Thu, Feb 28, 2013 at 12:05 PM, Richard B. Langleywrote: > ________________________________ > > This link might also be useful: > http://mintaka.sdsu.edu/GF/explain/atmos_refr/dip.html > > -- Richard Langley > > On 2013-02-27, at 8:51 PM, Marcel Tschudin wrote: > >> Brad, >> >> The dip results - in addition to the geometric angle - from the refraction >> of the air between observer and horizon which is governed by the temperature >> gradient above the earth's surface. The problem of estimating the dip >> corresponds therefore to the one of estimating the temperature gradient at >> the location of observation. (If I remember right: The calculator on Andy >> Young's site assumes that you know the temperature gradient or calculates it >> from two temperatures at different heights.) If one would measure the >> temperature distribution of the air layers between eyes and horizon with >> high accuracy one would likely also be able to calculate the dip to similar >> accuracy. For the cases where this is not possible the various authors tried >> to find ways how the temperature gradient and its influence on the dip could >> be estimated. >> >> In Sunset Science II Andy Young and G. Kattawar show that the dip depends >> almost entirely on the difference in temperature between the observer and >> the tops of the waves. Do you have a possibility to obtain copies of this >> publication from a library? You could now measure the dip and compare it >> e.g. with the one resulting from their paper. >> >> Regarding 'k': Calculating the dip does not necessarily require knowing or >> calculating beforehand 'k'. (The simple formula provided in Bowditch (and >> N.A.?) for calculating the dip does not mention it.) This parameter is only >> a different mean for expressing the amount of refraction, or - together with >> the earth's radius of curvature - also a mean for expressing the amount of >> dip. >> >> Marcel >> >> >> >> On Wed, Feb 27, 2013 at 11:15 PM, Brad Morris wrote: >> Hi Marcel >> >> For this location we have several National Data Buoy Center buoys. These >> report air and water temperatures, with a one hour granularity. >> >> Example: Right now Buoy 44039 (Long island Sound) shows air 40.6 deg F; >> water 36.5 deg F. Buoy 44017 (nearby Atlantic Ocean) shows air 45.0 deg F; >> water 41.9 deg F >> >> How do I calculate 'k' from this data, even for a nominal value? >> >> I've been all over Andrew Young's site and nothing jumps off the page at >> me. He does have a calculator for determining the lapse rate, but this >> assumes there is a target (like a light house). My target is the horizon! >> >> Best Regards >> Brad >> >> >> >> >> On Feb 27, 2013 1:40 PM, "Marcel Tschudin" wrote: >> Hi Brad, >> >> Please find below some further comments inserted into your last >> contribution. I do not know how much this special aspect of navigation is of >> general interest for the other members of NavList. If this should turn out >> to be a pure dialog then it might be preferable to continue with it off list >> ... until obtaining useful results which then would likely be again of >> interest here. >> >> Marcel >> >> There is an additional feature of Orient Point (and Montauk Point). >> Horizon A is the Long Island Sound and Horizon B is the Atlantic Ocean. The >> tide plays an important role in the sea surface temperature on the Sound. >> Tide coming in yields the same temp as the Atlantic. Tide going out yields >> warmer surface temps for the Sound, due to the E/W alignment of the Sound >> and the choke of flow at the western end. (Of course, the tide also affects >> the height of eye.) >> >> I would try to find out whether someone measures systematically the water >> temperature at this location. Such data may eventually be collected by and >> available online from some organisations like meteorology, fishery, >> environmental research etc. This water temperature may eventually differ >> from the Sea Surface Temperature (SST) or the temperature of the upper most >> stratum of the waves. The Sea Surface Temperature, generally the temperature >> without diurnal effects, can be obtained on an analysed basis e.g. here >> http://ourocean.jpl.nasa.gov/ by selecting and clicking at the bottom of >> this page on the button "Go To G1SST". Select in the new window the date >> (with available data) and underneath under "Blended SST" also the option >> "Gap-free". Under the global graph you can narrow done your area of interest >> by setting e.g. North 41.3, South 41.0, West -72.5, East -72.0 and click the >> plot button. The temperature of interest to you would probably be an >> estimated mean value. >> >> The water temperature delta is particularly pronounced in the summer. So >> anomalous refraction effects on dip will indeed be noted. >> >> Spring and autumn are generally the seasons with large temperature >> differences, but may be this is different in your area. >> >> I have noticed, over the years, your expertise on this topic. >> >> >> Not really. So far I only collected a lot of data from which I try now to >> extract some results. >> >> I am just a novice, so please be gentle! I have seen >> dip = arccos ( (R/(1-k)) / ( h + R/(1-k)) ) >> where R is the radius of the earth >> k is the refraction factor (?) >> h is the height of eye >> But in this equation, we are left to guess at k, nominally assigned a >> value of 0.13. In doing so, the equation agrees within seconds to the >> 0.02977 result. >> >> >> Yes, personally I also work with this factor k.. >> >> >> I guess that I should compute each dip separately. Is there some table of >> air temp to water temp yielding 'k'? >> >> >> All the various authors from Andy Young's bibliography tried to improve >> somehow the estimation of the dip, i.e. of the value for k. Try to obtain >> copies of the English publications. >> >> I hesitate to construct such a table for myself just yet, as there is no >> surety in my measurements. I need much more practice at 180 degrees. >> >> >> Well, you could gain surety in your measurements. You probably would first >> have to calibrate your Reflecting Circle and would then have to gain >> practice to measure the dip to noticeably better than one min of arc; may be >> to about a quater of it? You then start collecting your measurements and the >> corresponding meteorological data. A few years later, when you arrived at >> several hundred or thousand observations you analyse them. Your result will >> then tell others how, according to your observations, the value for k is >> best estimated. This is a long term project. But may be you are sufficiently >> interested in it to give it a try. >> >> Regards >> Brad >> >> On Feb 27, 2013 6:39 AM, "Marcel Tschudin" wrote: >> > >> > ________________________________ >> >> >> > Brad, you wrote: >> >> >> >> ________________________________ >> >> >> >> I had to begin somewhere! I will try again soon. >> > >> > >> > Congratulation for having given it a try! And yes, please continue! You >> > might eventually end up with a valuable data set. >> > >> > The value 0.02977 for calculating the dip may give a wrong impression on >> > the attainable accuracy. One can find different values for estimating the >> > dip. My guess is that these simplified estimations agree with those observed >> > under "any condition" to not better than about +/- 1 to 2 min of arc >> > (Std.Dev.). This can possibly be reduced by avoiding recognisable "bad >> > conditions" or/and by considering more relevant parameters in the >> > estimation. >> > >> > The dip can indeed vary considerably. This remains mostly unnoticed >> > because one generally observes the horizon without an object serving as a >> > fixed angle reference. One way to make these variations visible consists in >> > observing the horizon from a place (same eye position) where the horizon is >> > seen close to a nearby construction feature like a roof or a fence. >> > Unfortunately I did not have such a feature for my sunset photos for >> > measuring refraction. However, there are numerous photos where the apparent >> > sea horizon is in front of some skyline protruding from behind the horizon, >> > and at some days the height of the same skyline feature above the sea >> > horizon differs by up to about 5 min of arc. Note that the dip depends on >> > temperature differences near the earth's surface and that the temperature >> > difference between ambient air and sea changes during the day. Ambient air >> > is generally coldest at sun rise and warmest during afternoon whereas the >> > sea (surface) temperature remains almost constant. >> > >> > In the context of the analysis of my photos which provide a measurement >> > of dip AND refraction (I try to separate the two contributions) I received >> > recently from Andrew T. Young from SDSU (known for his Web-pages on >> > refraction and in particular on green-flashs) the following extensive >> > bibliography on dip (in German: Kimmtiefe) which I think is appropriate to >> > mention here: >> > >> > quote >> > >> > Regarding dip: remember that George Kattawar and I found that the dip >> > depends almost entirely on the difference in temperature between the >> > observer and the tops of the waves: >> > >> > A. T. Young, G. W. Kattawar, Sunset Science. II. A Useful Diagram, >> > Appl. Opt. 37, 3785-3792 (1998) >> > >> > -- so the details of the temperature profile in between are not >> > significant. But the problem is to determine the effective wave height, >> > which sets the level at which the "surface" that forms the apparent horizon >> > actually occurs. See the very useful discussions of these matters by H. C. >> > Freiesleben: >> > >> > H. C. Freiesleben, “Die Berechnung der Kimmtiefe,” Deutsche >> > Hydrographische Zeitschrift 1, 26–29 (1948). >> > >> > H. C. Freiesleben, “Geophysikalische Folgerungen aus >> > Kimmtiefenbeobachtungen,” Deutsche Hydrographische Zeitschrift 2, 78–82 >> > (1949). >> > >> > H. C. Freiesleben, “Investigations into the dip of the horizon,” J.. >> > Inst. Navigation (London) 3, 270–279 (1950). >> >> > >> > H. C. Freiesleben, “Die Strahlenbrechung in geringer Höhe über >> > Wasseroberflächen,” Deutsche Hydrographische Zeitschrift 4, 29–44 (1951). >> > >> > with a correction by Brocks: >> > >> > K. Brocks “Bemerkungen zu H. C. Freiesleben, Die Strahlenbrechung in >> > geringer Höhe über Wasseroberflächen,” Deutsche Hydrographische Zeitschrift >> > 4, 121–122 (1951). >> > >> > and finally >> > >> > H. C. Freiesleben “The dip of the horizon,” J. Inst. Navigation 4, 8–9 >> > (March, 1954). >> > >> > and the closely related work by Lutz Hasse: >> > >> > L. Hasse, “Über den Zusammenhang der Kimmtiefe mit meteorologischen >> > Größen,” Deutsche Hydrographische Zeitschrift 13, 181–197 (1960). >> > >> > summarized in English in >> > >> > L. Hasse “Temperature-difference corrections for the dip of the >> > horizon,” J. Inst. Nav. (London) 17, 50–56 (1964) >> > >> > These are the essential papers for understanding the dip, I think. They >> > are all in my on-line bibliography, where I have some comments about their >> > content. You might also be interested in the historical discussion: >> > >> > C. Prüfer “Das Kimmtiefenproblem,” Ann. Hydrog. Maritim. Met. 71, >> > 171–174 (1943). >> > >> > unquote >> > >> > >> > I do not yet have most of these references, but hope to obtain them in >> > the near future. >> > >> > The noticeable correlation I observe in my data with the temperature >> > difference between Sea Surface and ambient air are consistent with his >> > findings that the dip depends on the difference in temperature between the >> > observer and the tops of the waves. >> > >> > So, Brad, how about trying to improve the understanding and estimation >> > of the dip by performing your own measurements? >> > >> > Marcel >> > >> > >> > >> > >> > >> > >> > View and reply to this message: http://fer3.com/arc/m2.aspx?i=122498 >> >> View and reply to this message: http://fer3.com/arc/m2.aspx?i=122499 >> >> >> View and reply to this message: http://fer3.com/arc/m2.aspx?i=122501 >> >> View and reply to this message: http://fer3.com/arc/m2.aspx?i=122505 >> >> >> View and reply to this message: http://fer3.com/arc/m2.aspx?i=122516 >> > > ----------------------------------------------------------------------------- > | Richard B. Langley E-mail: lang---ca | > | Geodetic Research Laboratory Web: http://www.unb.ca/GGE/ > | > | Dept. of Geodesy and Geomatics Engineering Phone: +1 506 453-5142 > | > | University of New Brunswick Fax: +1 506 453-4943 > | > | Fredericton, N.B., Canada E3B 5A3 > | > | Fredericton? Where's that? See: http://www.fredericton.ca/ > | > ----------------------------------------------------------------------------- > > > > > View and reply to this message: http://fer3.com/arc/m2.aspx?i=122528 View and reply to this message: http://fer3.com/arc/m2.aspx?i=122545