Some good ideas so far. Let’s look at how the calculations square with the hands-on approaches.
If we take the example from PI and apply it to a well-known entity (Melges 24) we can calculate the following:
0.5*1.2*62*20^2*2.5*0.5 = 18,600 newtons, or 4,180 pounds force load on the tack line.
The block the Melges 24 uses for the Spinnaker Tack is a Harken Carbo 40, with a Safe Working Load of 485 pounds and a breaking strength of 1620. Considering the tack block is changing the sheet direction roughly 90 degrees that increases the block’s required load rating by 1.41, so the block should break in the neighborhood of 1150 pounds on the tack line. The block should actually not see more than 485/1.41, or 344 pounds force to remain in the SWL.
OK, so let’s re-consider factors. I know the boats will never see 20 m/s apparent wind speed. Maybe 8 m/s is a better factor. Any more than this and it is likely the boat is going to round up with the big ASO kite up.
0.5*1.2*62*8^2*2.5*0.5 = 2976 newtons, or 668 pounds force load on the tack line.
Multiply that by 1.41 and we’re looking at 942 pounds for the block. We’re under the Breaking strength of the Carbo 40 now, but still well beyond the SWL.
Next, let’s look at the assumption of ½ load on the tack. Le’ts assume 33% each to the tack, head, and clew.
0.5*1.2*62*8^2*2.5*0.33 = 1964 newtons, or 441 pounds force at the tack line. Hey, we’re under the SWL.
However, if we’re changing the direction of the sheet more than 60 degrees we could still have a problem. At our assumed 90 degrees the load on the tack block is 441 x 1.41 = 622 pounds. Beyond the SWL still.
If we changed the SWL to a safety factor of 2:1 instead of 3.3:1 we could use 810 as the SWL and now we’re in the ballpark.
Other considerations:
Now if we look at the ASO as a big genoa (it isn’t, but let’s say it is for the argument) then the Melges kite at 62 sq m in 15 knots of wind would have a sheet load of 650 pounds. Maybe we should be assuming the sheet is carrying more load than the tack and head, not equal?
I agree with Steve B, the pole is definitely in compression as well as in bending. If you let the “pole out” line off while the kite is loaded it will retract with a lot of force.
On most poles the tack line is running above the pole, so it is acting somewhat as a bowstring as well.
So far there is some good thinking, but we seem to be making a lot of assumptions. I think there are a lot of the boats out there that have had their poles sorted by "practical engineering". I’m offering a local spar supplier the use of my boat if they have access to a portable load cell, to get some actual loads to compare the theoretical calculations.
Finally, does anyone have a good number for yield stress MPa for a generic carbon/epoxy tube?