pods for primates: a catalogue of surfboards in australia since 1900
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  surfboard dynamics
   fundamentals of surfboard dynamics


INTRODUCTION
It is not necessary to scientifically understand the dynamics of surfboard motion  to succesfully ride a surfboard.
This appears to be the case for ancient Hawaiian surf-riders (note however,  there may be communication or translation difficulties in this report) ...
... the natives could not explain why they were propelled shoreward with such astonishing speed, nor
could  I (Mr. Caton) explain it myself (himself), nor could my (his) friends.
He hoped that someday, someone would study the question and find an answer to it. (6)
John Dean Caton  : Surf-riding at Hilo, 1880. (in Blake).

Attempts to analayse surfboard dynamics in the early 20th century have not always greatly advanced our understanding.
For example, continuing  the above narrative Blake goes on to suggest a, not altogether satisfactory, solution ...

The answer is relatively simple. Gravity does the trick.
The front slope of the wave on which one slides presents a down-hill path, while the friction of the
slippery board against the water is very small. (7)
It's the same as skiing on a snow-covered hill, and there is no doubt as to what makes one slide down
a hill on skis.
However, in skiing, one can start down hill from a stationary position, while in surfriding some
momentum must first be attained , to catch up with the incoming swell.
This is accomplished by paddling the board with the hands and arms. (8)  - Blake(1935) page 43.

7. "the friction of the slippery board against the water is very small"
My physics is a bit rusty, but I think that the friction on the board is significant - overwise the board would sink.
More work/thought required.

8. "to catch up with the incoming swell ... by paddling the board with the hands and arms."
One of the most common misunderstandings by surfriders - technically the wave "catches" the rider.


1. As a wave approaches the shore and enters shallow water...
1.1 The wave speed decreases.
Ws > 0
1.2 The angle of the wave face increases.
Wf > 90 degrees
White Water
Wave of Translation
Breaking Wave 
Peak at Max Height
Shoulder in Deep Water

2. The minimum planing speed of a surfboard is a function of its planning area (volume? displacement?) and the rider's mass, less drag.
Mps = f (Pa / Rm - d)
3.
A surfboard and rider are propelled by a wave when the minimun planning speed equals the wave speed.
Mps = Ws
4.
A surfboard planes on a wave face when its gravitational potential energy is released as the angle of the wave face increases.
As Wf > 90 degrees, PE increases 
5.
A given surfboard will plane independently at a given angle of the wave face.
The lower the minimum planning speed of a board,  the required wave face angle is smaller.
As Mps > 0, then Wf < 90 degrees
See Minimum Planning Speed and Wave Face Angle Notes

6. The Take - Off - "Catching the Wave"
The surfer does not catch the wave, if anything the wave catches the surfer.
A surfer can not paddle any craft at wave speed.
The surfer paddles the board to a position where the angle of the wave face is steep enough for the board to achieve minimum planning speed.

7. The Architecture of Planning Hulls
Excepts from
Lord, Lindsay : Naval Architecture of Planing Hulls
Cornell Maritime Press  241West 23rd Street New York 11, N.Y.Lord, Lindsay 1946

Although surfboard design is not studied in this book, they are planing hulls and severval principles expounded by Lindsay Lord appear applicable...

7.1. "hydrostatic naval architecture is not applicable  to the planning hull...The fundamental hydraulic laws upon which standard naval architecture proceedures are based simply do not apply to a hull skimmimg the surface."
Preface, Page vii

7.2. "the submerged body, moving with sufficient rapidity, increases turbulence and the resulting suction drag, soon reaching a speed at which the viscosity of the liquid prevents further increase in speed regardless of practical increases in power.
With the plate (surfboard) moving in its own plane, this type of suction drag due to the viscosity of the liquid is not a factor in the performance.
Rather, the resistance, aside from skin friction, is largely due to the simple transfer of kinetic energy at the leading edge.
Thus it becomes apparent that the leading edge of the plane at once accounts for a major portion of both drag and lift.
But since lift rises as the square of the speed, and drag increases at less than the square of the speed, every proportionate increase in leading edge increment becomes successively more and more worthwhile.
In other words, while incresasing speeds require the displacement hull to become progressively narrower, the planning hull moving at high speed requires the widest possible beam.
To simplify still further, the displacement hull can improve its speed only with added length; the planning hull requires added beam."
Pages 12 - 13.

7.3.''With planning hulls, then, there is no theoretically sound proceedure by which the total resistances of one hull can be directly compared to the total resistances of another hull radically different in size."
Page 25, follows analysis of Froude's Law of Comparison and the Reynolds number.

7.4 ''Unfortunately, airfoil or hydrofoil data is of limited value as an approach to this problem (of bottom loading).
The boat's (surfboard's) bottom operating at the boundary between two mediums, one of which is approximately 800 times as dense as the other, allows but for one working face of the plane.
Furthermore, while this one face should ideally be subjected only to positive pressures, certain configurations of the average bottom lead to varying degrees of transient negative pressures which may detract from the net dynamic lift of the plane."
Page 31.
Note that this does not apply to fins, which are true hydrofoils.


8. The straight line speed (that is, directly towards the beach) of a surfboard of a given beam is increased if the length is decreased. From 7.2, above...
to "improve its speed ...; the planning hull requires added beam."
Important Note - this does not apply to "cutting", which is a unique phenonomem.
9. Cutting

The angle along the wave face is a function of the rate of peel.
It is independent of wave height and wave speed.
10. When the board cuts or angles across the wave face, natural wave dynamics cause the leading edge of the board to extend longitudinally, thereby greatly increasing the board's speed.
11. For a given wave (Height, Wave speed, Angle of the face and Rate of peel),

Board speed is a function of the planning area (volume? displacement?) and the rider's mass, less drag.
Bs = (Wh x Ws x Wf  x Wp)  x  f (Pa / Rm - d)
To simplify :
The smaller the board, the greater maximum planning speed.
The larger the board, the lower the minimun planning speed.
This has been demonstated by Tow-In boards - a large board is needed to take off on a large wave, but once planning a small board is faster.
The problem for surfboard designers has not been to make the boards go faster (the solution is to make them smaller), but to maintain control at speed.
The major developments in this area have been light weight, the soft down rail, the breakaway edge  and sophisicated bottom rocker.
Simon Anderson's Thrustrer - Three fin design provided stability and control in extreme conditions , unimagined by earlier designers.

Notes : Minimum Planning Speed and The Wave Face Angle

Consider the following boards with similar beam and planshape.
Increase in length increases the planning area.
For a given wave and a given rider, each board will have a different minimum planning speed.
Assume...
Board A achieves minimum planning speed at wave face angle f a.
Board B achieves minimum planning speed at wave face angle  f b.
Board C achieves minimum planning speed at wave face angle f g.
Board C
6 ft x 22''
Wf = f g
Board B
8 ft x 22'
Wf = f b
Board A
10 ft x 22''
Wf = f a

Now assume a bottom formation of several sections at decreasing depth levels such that a given wave maintains a given wave face angle over a reasonable distance.
At each change in depth (1, 2 etc), the wave face angle becomes steeper.
Such wave conditions are rare, but not unknown, for example Waikiki, Ohau.
The Hawaiian language has a word "ohu", defined as "a  low wave that rises without breaking but is of sufficient strength to be ridden with a surfboard. " Finney and Houston, page 95.

In these conditions, then...

Board A will plane when the wave reaches Position 1, and will travel at wave speed to Position 2.
Board B will plane when the wave reaches Position 2, and will travel at wave speed to Position 3.
Board C will plane when the wave reaches Position 3, and will travel at wave speed to Position 4.
and
At Point 2, Board A's potential speed is increasing and the wave speed is decreasing.
Similarly for Board B at Point 3, or Board C at Point 4.
There are three possible outcomes -

i. The board accelerates down the face towards the trough.
This will ultimately result in rapid deceleration as the wave face angle approaches 0.

ii. The rider stalls the board (applies drag) and maintains board speed at wave speed.

iii. The board travels at an angle to the wave face, the resultant vector being at wave speed.
In this instance potential board speed is further increased because...
 "When the board cuts or angles across the wave face, natural wave dynamics cause the leading edge of the board to extend longitudinally, thereby greatly increasing the board's speed." (#10. above)





An Analytical Dilemma
Assume...
1. A long walled hollow point break.

2. Three riders on similar boards take off on a wave at a fixed point (T/O).

3. No board's wake effects the other riders.

4. Rider #1 takes off (T/O) behind the peak and turns into the tube at a second fixed point (T1).
With minor adjustments the surfer stays inside the tube in a straight line till a third fixed point (T2).

5. Rider #2 takes off (T/O) on the shoulder and sets up a bottom turn at the second fixed point (T1).
With major adjustments the surfer climbs and drops on the wave face till a third fixed point (T2).

6. Rider #3 takes off (T/O) on the wall and walks to the board's nose at the second fixed point (T1).
With minor adjustments the surfer noserides in a straight line on the till a third fixed point (T2).

This is represented graphically...

Observations...
1. Rider #2 rode the longest distance.
2. Riders 1# and #3 rode a shorter and equal distance.

Therefore...
Rider #2 has the highest velocity (v = d/t).
Riders #2 and #3 have the same velocity !!! - the Analytical Dilemma.

Weirdo...
Tube riding surfers report that inside the tube "time slows down".
Possibly related to ...
1. Extreme board speed, see above.
2. Visual "tunneling" as predicted by Al Einstein when approaching the speed of light.



REFERENCES
Lord, Linsay :
Naval Architecture of Planing Hulls
Cornell Maritime Press 
241West 23rd Street New York 11, N.Y.1946
Hard cover, 305 pages, 21 black and white photographs, 118 black and white diagrams and graphs, Index
Review
Although surfboard design is not studied in this book, they are planing hulls and severval principles expounded by Lindsay Lord appear applicable.
The book was treasured by seminal Californian board builder, Bob Simmons. 
Many of the models and diagrams appear similar to Simmons' famous wide tailed Spoons of the early 1950's, Lord emphasizing the increase in lift by incorprating parallel running lines, page 71. 
Figure 29, page 72 illustrates one of Lord's models (M2) that features nose scoop, concave bottom and twin keels (fins). See image below.
The chapter on rudders, illustrates a thick foil that resembles some examples of Bob Simmons' fins, page 221.
The chapter on Hull Structure promotes the use of resin laminates, particually plywood, as an emerging and superior constuction technique.
Contemporary reports indicate that others surfers were aware of the book, but (not suprisingly) none could understand it
- see Legendary Surfers : Bob Simmons Vol 1 Chapter 15 1946.


Kinstle, James :
Surfboard Design and Construction
Natural High Express Co.
Long Beach, California.1975
Soft cover, 139 pages, extensive black and white illustrations and diagrams.
Image 
This is not an original, but a photocopied version contributed  by A.
-thanks to A.
Review
1. Probably the most technically detailed work on surfboard design ever published, many sections are unique.
It would be unfair to attempt a critical review at this point since I don't feel that I fully understand much of the work, in particular Chapter 2 Surfboard Dynamics.
2. October 2004
Further analysis of the book appears to indicate that much of the work on surfboard dynamics is in error.
Almost all the diagrams indicate a considerable portion of the board immersed in the wave.
This is generally not the case - as hydronamic planning hulls, surfbards plane on top of the water surface. This is illustrated in many photographs, see Bob Simmons in trim  below.

Kit Horn, Bob Simmons and Buzzy Trent.
Solid Laminates, Malibu, circa 1941 - 1944.
Surfer Magazine
March 1981 Volume 22, Number 3, page 36
The photograph is uncredited.

Supplementary Images

Standing Rider on Paipo/Belly board, 
Kuhio Pier, Waikiki, circa 1962
Photograph by Val Valentine
Kelly, facing page 192.



Plywood surfing, Barbados, circa 1988.
No quite a barn door, but close.
Photograph by Dave DiGirolamo
SURFER magazine
Volume 29 Number 12 page 113

.Click for catalogue, starting with # 100- Duke Kahanamoku's 1914 Alia
home catalogue history references appendix