Quote of the Day

Patience is also a form of action.

— Auguste Rodin, Sculptor

## Introduction

I love to read stories of the sea and about the voyages made during the age of sail. I personally have never thought that I would have an opportunity for ocean sailing, but I recently began working with an engineer who is an avid sailor and teacher of sailing. He has sailed all over the world and recently trained another engineer in my group to sail. This newly trained sailor just returned from a trip to Bora Bora, which he found to be enjoyable and the sailing uneventful.

My discussions with this sailing instructor have given me some hope that I may yet get to do some sailing. This hope has reawakened my interest in some of the traditional technologies of sailing, like ropework and celestial navigation.

This post is the first in a series on correcting sextant (Figure 1) measurements for impairments. There are a number of measurements impairments: index error, refraction, and dip. This post will look at the impairment known as dip.

## Background

### Definitions

- altitude
- The angular distance of a celestial object above an observer's horizontal plane . There are published tables of the altitudes of various celestial objects. However, it is difficult to obtain a stable horizontal reference on a moving ship. The horizon provides a very stable reference and we can use a sextant to accurately measure the altitudes of celestial objects with respect to the horizon. Figure 2 shows the relationship between the horizontal and the horizon. The are related through the angle called dip.
- dip of the horizon
- Dip of the horizon is the the angular depression of the horizon below the horizontal plane. If we were taking sights on a stable land site, we could measure altitudes using a theodolite with its horizontal established using a bubble level. At sea, however, nothing is stable except the horizon. We use a sextant at sea to measure the altitude of a celestial object with respect to the horizon and then use our dip calculation to change the altitude reference from the horizon to the horizontal.
- dip short of the horizon
- There are times when it may be necessary to measure the altitude of a celestial object even though we do not have a visible horizon because of an obstruction. However, if we the distance to the obstruction we can calculate a dip value that will allow us to correct our sextant measurement. We refer to this dip value as the dip short of the horizon. Typically, we will measure the altitude relative to the water level at the obstruction, which is a relatively stable reference.

### Objective

I will be deriving commonly used formulas for dip to the horizon and dip short of the horizon. I should point out that I have seen many formulas for these dip values and I arbitrarily picked two formulas to investigate more closely here.

## Analysis

### Standard Dip Short of the Horizon Table and Formula

#### Common Presentation

Figure 3 shows the values for the dip short of the horizon using a common table (Norie's) and formula (Bowditch). They give similar, though not identical results. In Figure 3, I show how you can take Norie's tabular data, fit it to a Bowditch-like formula, and you find that Norie's table and Bowditch's formula produce similar results.

I should note that the results for dip short the horizon used in both Norie and Bowditch ignore refraction. This makes sense because most obstructions used for navigation purposes would be relatively near, and the effects of refraction will be minimal.

Figure 3 also shows a snippet of Bowditch's formula dip short of the horizon, which is given by Equation 1.

Eq. 1 |

where

*d*is the distance to the obstruction [nautical miles].*h*is the height above sea level of the observer's eye [feet].*d*is the dip short of the horizon [arcmin]._{short}

#### Derivation

Figure 4 shows the geometry of the dip short of the horizon situation.

Figure 5 shows how you can derive an expression very similar to that of Bowditch's.

While the expression shown in Figure 5 is not identical to that in Bowditch, it is quite close.

### Dip to the Horizon Formula

The dip to the horizon formula is shown in Figure 6 (source).

The derivation of this formula is similar to the dip short of horizon formula, but now we will model refraction. For the dip to the horizon, I have only seen formulas that are functions of the square root of the observer's height *h*.

Equation 2 shows a common expression for dip of the horizon, *d _{horizon}*.

Eq. 2 |

Figure 8 shows how you can derive Equation 2.

My derivation yielded a function similar in form to the that shown in Figure 6, but with a larger coefficient term. The coefficient term is a function of the atmospheric conditions, and I assume that my atmospheric assumptions are different. The results differ by ~10%, which is well within the bounds of atmospheric variation.

## Conclusion

I believe that I understand where the dip tables and formulas come from. I also understand that some dip equations take refraction into account (Figure 7) and some do not (Figure 3). Dip was a good impairment to use to kickoff my learning process – next are index error and refraction.

I'm just starting to pick this up, however I am struggling with Dip, in the high desert

5-6000 ft is there a formula besides heading to the coast, so I can still practice inland.

The article starts with a picture of a sextant. In sextant navigation, the correction is best given in minutes of of elevation (altitude angle), not distance to the horizon. A table is given in the Davis Mk 15 Sextant Manual: (5ft': -2'; 10ft: -3'; 15ft: -4'; 25ft: -5'; 40ft: -6') where the first number is eye height above sea level, and the second is the correction in minutes. Note one minute of latitude = one nautical mile.

I asked this same question, about altitude above sea level, of an experienced navigation instructor recently, and he replied that terrestrial altitude doesn't matter as long as you have a good horizon. Thus a high altitude lake at least three miles across gives as good a horizon as the ocean, and requires only standard dip. If your body of water is less than three miles across use the table for "Dip Short of the Horizon" to adjust dip in minutes of arc on the sextant reading . But the altitude of the lake does not matter.

"But the altitude of the lake does not matter."

This is technically correct when considering only dip. However, for a sight of a celestial body at significant observer altitudes, the subsequent refraction correction should be reduced on account of the reduced atmosphere above the observer. This polynomial gives results that fit the International Standard Atmosphere, where AltM is observer altitude in metres. Multiply refraction correction by (1 - 0.00009519 * AltM + 0.0000000031 * AltM * AltM).

At 1000M the refraction correction should be multiplied by 0.908.

Hi, you mentioned you're measuring in the high desert, i.e. no water surface, right? Make sure the altitudes of where you're standing and your "horizon" match, otherwise you should factor in the total altitude difference between your eye and the horizon "target".

Alternatively you can use an artificial horizon, i.e. a bowl of water with side walls to keep the wind from causing ripples on it.

You can cobble your own or buy one from good ol' celestaire

https://www.celestaire.com/sextant-accessories/davis-artificial-horizon-detail.html

(I am not in any way affiliated with them, but bought my sextant, tables, etc. there).

note that with artificial horizon your corrections are different!

It was nicely explained here. I tried to measure height of a building staying at long distance. But I didn't know the proof. Thanks.