# NavList:

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

**Re: Measuring (and Calculating) Dip**

**From:**Greg Rudzinski

**Date:**2013 Mar 3, 07:47 -0800

Brad,

I agree with your following statement:

"Here's an un-verified theory: To further understand the thermal model, I

believe we will have to take into account the wind speed over the water. For a

calm day, the lowest band of air will be approximately the water temperature,

as the air and water are in contact without motion. For higher wind speeds, I

believe the lowest band of air will not take on the water temp, rather it will

maintain itself closer to the air temp at 4 meters! For calm days, we have a

ramping range of temperatures, from air to water. For windy days, we will have

more of a step function."

I call this mixing which will vary with height since wind velocity is slower at the surface do to friction between mediums. Humidity and pressure may also play a roll.

Greg Rudzinski

Hello Marcel

Thank you for the clarification.

This makes the dip formula

dip = 1.74*sqrt(h) - 0.47*(AirTemp - WaterTemp)

where dip is in arcminutes

h is the height of eye in meters

AirTemp is the temperature of air at eye level, degrees C

For this I use the buoy air temperature

WaterTemp is the water surface temperature, degrees C

For this I use the buoy water temperature

Next, we must consider the effect of waves. When observing for dip (or using the horizon as a reference for an altitude) you are actually using the crests of the waves at the horizon, not the mean sea level at the horizon. The above equation for dip is for the mean sea level.

The angular height of waves at your horizon is

wvhtCorr'n = atan((wvht/2)/(3860*sqrt(h)))*60

where wvhtCorr'n is the waveheight correction, in minutes

wvht is the measure of the larger of wind waves or swell at the buoy

which is a peak to trough measurement, we want mean sea level

to peak. Meters

h height of eye, meters

You may recognize the term 3860*sqrt(h) as this is the distance to the visible horizon. So we are taking the arc tangent of Y over X, which is 1/2 the peak to trough wave height divided by the distance to that wave height! Simple Trig!

Let Height of Eye h=3.268 meters. I was standing on land, and I measured the vertical distance to the water.

From 44039 (Long Island Sound) we have wvht=0.1 meters, air=3.5 deg C and water=2.8 deg C.

Dip = 1.74*sqrt(3.268)-0.47*(3.5-2.8)

= 2.82 arc minutes

wvhtCorr'n = atan((0.1/2) / (3860 *sqrt (3.268))) * 60

= 0.02 minutes (0'1")

From 44017 (Atlantic Ocean, near Montauk Point) we have wvht=2.3, air 5.4 deg C and water 5.6 deg C

Dip = 1.74*sqrt(3.268)-.47*(5.4-5.6)

= 3.24 arc minutes

wvhtCorr'n = atan((2.3/2) / (3860* sqrt(3.268))) * 60

= 0.57 arc minutes (0'34")

So my total dip (calculated) is 2.82 - 0.02 + 3.24 - 0.57 = 5.48 minutes (5'29")

My measured dip was 4 minutes 55 seconds (4'55").

Therefore, the total error in calculation was (5'29" - 4'55"=)+34", but since this is two dips, we must divide by two for an average dip error of +17". Just as a side note, the winds were calm at the time of measurement. This is evidenced by the 0.1 meter wave height on the Long Island Sound (3.9 inches peak to trough!).

CONCLUSIONS:

1) The wave height correction proved to be decisive for this measurement. I agree with Hasse in this regard. Nowhere in the standard dip equation do I see an accomodation for wave height (sea state).

2) The precision wave data afforded by the NDBC Buoys is far better than Friedenleben's attempts at this data. We have precise wave measurements, not Beaufort sea state estimates as a function of wind speed.

3) The Buoy air temp is measured at 4 meters above sea level. Consider this in comparison to the height of my eye at 3.268 meters. It is acceptable to use this as the temp of the air at height of eye, for my measurements.

4) The Buoy water temp is 0.6 meters below the surface. This is to be compared to Friesenleben's boats churning about in the water, dipping buckets into the surface and then measuring the water with a thermometer. What could go wrong with that ;-)

Here's an un-verified theory: To further understand the thermal model, I believe we will have to take into account the wind speed over the water. For a calm day, the lowest band of air will be approximately the water temperature, as the air and water are in contact without motion. For higher wind speeds, I believe the lowest band of air will not take on the water temp, rather it will maintain itself closer to the air temp at 4 meters! For calm days, we have a ramping range of temperatures, from air to water. For windy days, we will have more of a step function.

Here's a plain statement of fact: Friesenleben suffered from poor data, quite uncontrolled in quality. This could clearly have affected his results and conclusions.

Best Regards

Brad

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