Oh, I didn't intend to pick nits.
I take it that when that sentence was written, other origins might have been unknown.
This might be debatable re the "Strait" --though there, one could think "of course,
that is essential of any
such mid-line eye knot". Re "Benson", egads, THIS
one is Ashley's #1421 --that should be at least suspected and then confirmed (by
(m)any party(s))! And re Anglers Loop, no, not a nit : look in most any angling
shop and you will find the very knot tied in that modern material Toss claims made
it obsolete. (And re this knot, I might've discovered a version that works as well
and maybe stronger --some simple testing to be done, yes-- and that can serve
in rope.) Beyond these, one should also take issue with the assertion under
an earlier section on "Lashmanship / Pulley, Frap, and Wdge", where a theoretical
3:1 construct is given "close to" that advantage even considering friction
--whereas the practical user should expect less than 2:1. (The issue re such
constructs has been debated in this forum, with my contributing some data
from simple testing with even 'biners (more efficient than cordage!) & weights.
It was quite eye-opening to see the loss of advantage.)
The discourse in this thread has changed my view on the tying method slightly
It occurs to me that one can begin by forming a turn around a bight,
then bringing the bight's tail around appropriately to insert through itself.
For the Carrick Bend, in order to avoid slip of the ends, the pattern, once formed, must be flipped over,
so that the ends hang freely down from the knot. When done like that, there is no slip when it is drawn tight.
I think it's more problematic than this --I'm not fearing gravity's draw
on ends, but imbalanced folding especially in firm slick rope where
movement can occur more for one than the other rope.
BTW, much is sometimes made of Ashley's calling this bend nearly perfect,
and many sources claim it to be very strong. In fact, some test data (old)
shows it to have unexceptional strength, and I don't know of any modern
testing (i.e., using modern cordage). It has been said to serve well the
Alaskan crabbing industry (by one contact, and apparent use shown on
t.v. on one boat). I know of no test of the seized lattice form.
.:. We are wallowing in --too often the case re knots--
a great void of information from the lab & from the field.
In such emptiness, there is room to go off in all directions
unobstructed and only encountering sounds, mostly echoes! - - - - - - - - - - - -
XaraX, you need to look more carefully at the knot, not the keyboard.
1. Whatever of the two ends/tails the standing part pulls, it has exactly the same result in the knot s strength, I think.
There is a noticeable difference of geometry if one orients the knot's tails
in a certain way. In the simple and commonly presented geometry, they
align adjacent on the axis of tension, SParts making a 1-diameter turn around
them; but in the version I intend, the Sparts turn more broadly, and that is
what leads me to conjecture "greater strength". Getting this orientation takes
some careful placing of the ends and then careful setting --dressing AND setting
are mindful acts.
But all of this plays on fine details of form, material, and load (and where is
strength --or i.p. what actual difference might be in the balance here-- much
of any importance except when doing breaking-strength tests? (But where is
XaraX much at all concerned about knots --in his latter-day feeling-- than in
such tests of knotting
theory ?!!
)
- - - - - - -
In the disposition of the knots' tails, I see a trio of orientations for the
Carrick bend and at least as many for
Rosendahl's bend .
In the former, Inkanyezi shows one in the OP, tails making a sort of
2-diameter object perpendicular to the axis of tension; then there is
the case where the tail is brought in the direction SPart draw is pulling
it, where it is pressed into the knot's collar; and then one can push
the tails around in the opposite direction (and these two latter versions
give more of a 1diameter SPart u-turn). For
Rosendahl's Z. bendone can get that first
Carrick form, too, each SPart pulling a tail
into such orientation; one can also form the knot as I argue above and
as is commonly shown, where tails go in opposite directions from the
first-described form. There can be variance per loading, but with careful
dressing I think that these forms can be dependably given.
--dl*
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