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Traditional Pacific Island sails – analysis by Graham Sanborn.

I created a program to help me understand the traditional sails of the canoes of Pacific Islands. These sails seem very effective, yet very simple. So I wanted to understand these sails better. My program currently renders only triangular sails with straight edges, similar to the sails of the Marshall Island canoes of Waan Aelõñ in Majel (Canoes of the Marshall Islands).

The example shown in these videos is an equilateral triangle sail that has straight edges. The top spar is inclined at an angle of 10° from vertical. This example is supposed to be a sail that is filled with wind and the main sheet is pulled enough that the sail makes a 90° arc of the cone. The point of attachment of the main sheet is on a line that would be on the centerline of the canoe’s main hull.

The first 3 videos show the relationship between the sail and the cone that the sail is a slice of. The last 3 videos present a simple analysis of the sail’s shape. The first of these shows the maximum camber and the position of the maximum camber as a percent of the chord’s length. The next shows the angles of the airfoil chords (the “twist angle”) relative to the forward direction of the hull. The last shows the angle of the leading edge of the sail in the horizontal plane relative to the forward direction of the hull.

Most of the triangular sails of the Pacific Island canoes appear to be completely lashed to the top and bottom spar. When they are, it appears that these sails form a conical shape when they fill with wind. The shape is probably not exactly conical. But I suspect that the shape is close enough that a cone is a reasonable approximation. It appears that the airfoil of this sail is created by the conical shape. It is known from a field in mathematics called conic sections that horizontal slices in an inclined cone form elliptical, parabolic, or hyperbolic shapes, depending on the amount of inclination of the code and the shape of the cone. In this case, the cone dips below the horizon, so the conic sections are hyperbolas. Therefore, the airfoils are short hyperbolic arcs.

The sails of the Pacific Islands are fascinating. But I cannot find any technical information about these sails on the internet. I cannot find any analyses of their aerodynamic properties or their design principles. There do not appear to be many how-to guides to help people who want to make them or hints to know if we are using them correctly. Therefore, I have decided to investigate them a little myself.


The relationship between the sail and the cone:

At any height, the airfoil shape made by this sail is a hyperbolic arc.この動画にある帆の翼の形は双曲線の円弧です。

Opublikowany przez Grahama Sanborna Czwartek, 15 kwietnia 2021
Animation no. 1 – created by Graham Sanborn

The sail is an equilateral triangle. The sail would be lashed to the top and bottom spar. When the wind fills the sail, it forms a conical shape. この帆は平である時に正三角形です。帆は上と下のスパーに結ばれています。風が吹くと円錐的な形になるようです。その形をプログラムで描きました。

Opublikowany przez Grahama Sanborna Czwartek, 15 kwietnia 2021
Animation no. 2 – created by Graham Sanborn

Horizontal lines drawn on this cone would have a hyperbolic shape. この円錐に水平な線を書けば、双曲線になります。

Opublikowany przez Grahama Sanborna Czwartek, 15 kwietnia 2021
Animation no. 3 – created by Graham Sanborn
The airfoil shapes, twist angle, and leading edge angle:

The red line shows the chord of the airfoils. The text shows the maximum camber and its location. This sail in this configuration has an 11% thickness airfoil with the maximum thickness at 39% of the chord length in the lower portion of the sail. Above the clew, the maximum camber decreases to 0 at the head of the sail. And the maximum camber moves from 39% of the chord to 50% at the head.赤い線は翼弦を表します。文字は最大キャンバーと最大キャンバーの翼弦にある場所を表します。帆のタックからクリューまでの間、この帆の最大キャンバーは11%であり、場所は39%です。クリューからピークまで、最大キャンバーは11%から0%まで減ります。場所は39%から50%まで下がります。

Opublikowany przez Grahama Sanborna Czwartek, 15 kwietnia 2021
Animation no. 4 – created by Graham Sanborn

This video shows the sail’s twist. The text shows the angle between the chord line (the red line) and the forward direction. Below the clew, the there is no twist in the sail. The angle of the chord is about 16° in the lower section. Above the clew, the sail naturally twists the chord to about 53°. So the total change in twist is about 37°.これは帆のねじれを表します。数字は赤い翼弦の線と真っ直ぐの方向の違いです。帆の下の方は翼げんは16°であって、クリューより上は16°から53°ぐらいまで変わります。ねじれは大体37°であるように計算しました。

Opublikowany przez Grahama Sanborna Czwartek, 15 kwietnia 2021
Animation no. 5 – created by Graham Sanborn

I am making many new videos of the Marshallese style triangular sail. But they are not all finished yet. So I will upload upload them one video at a time, or one group of videos at a time.I added the angle of the leading edge of the sail relative to the forward direction to my sail rendering program. 0° means triangle is completely flat, so the leading edge of the triangle points exactly forward. This angle is very important. If the apparent wind angle is less than this value, then the sail will luff. The sail will not fill with wind. For a triangular sail with straight edges, this value is the same everywhere on the top spar. If the canoe is moving, then the apparent wind angle will vary by height. The apparent wind angle must be greater than this value at all heights for the sail to generate thrust. As I showed in a previous post, the angle of the chord relative to the forward direction does change with height on a triangular Pacific Island canoe sail.マーシャル諸島的な三角形帆の映像と動画をたくさん作る途中です。作るのは時間がかかるので、一つの動画や、一つの関係がある動画の部類が出来たら載せます。私が作ってる、三角形の帆の描くソフトには帆の最先端の方向線と真っ直ぐから離れた角度を示す機構を入れました。特には伝統的な、太平洋諸島の船の帆にはこの方向は大事だと思います。見かけの風の角度はこの最先端の角度より小さければ、と言うのは見かけの風がこの角度よりもっと前から来ていたら、帆は機能しない筈です。船が動いているなら高さによって見かけの風の方向が違うと言っても、三角形の帆の最先端の方向はどんな高さでも同じです。ですが、以前載せた動画には伝統的な太平洋諸島の三角形の翼型の翼弦は高さと方向が変わります。

Opublikowany przez Grahama Sanborna Sobota, 24 kwietnia 2021
Animation no. 6 – created by Graham Sanborn

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