The purpose of this experiment is to obtain the experimental equation concerning the projective area of a twine portion on the knotless twisted netting, as the basic research for the study of the fluid dynamical coefficient at a certain attack arlgle θ, when the netting is set into a flow.
The netting samples used are seven kinds of knotless netting composed of varying twine dimeter
d and leg length
l. And the respective netting is fixed on the ?? -shaped netting frame at hanging angle of 45°, by thin stainless steel wire, while among sevwn, one netting is fixed at the six stages of hanging angleØ.
Th ?? projective area of the twine portion is obtained from the enlarged photograph, concerning the area measured by a planimeter of one mesh which is made up of two knots and four legsforming two netting elements.
Results obtained are as follows:
(1) The projective area of a twine portion on the (
i×
j) mesh sample, at the range of attack angle Θ<θ ?? 90° is calculated easily, using the following experimental equation.
S
θ'=4.4
ijdlsinδ+(
i+
j-2.2
ij)
d2/sin2ε+0.44
d2(2.2
ij-
i+
j/2)sin2∅sinθ
(2) The projective area, of a twine portion on the (
i×
j) mesh netting, at the range of attack angle 0° ?? θ ?? Θ is derived in the following experimental equation.
S
θ'=0.84[
j{(2
i-1)
l2sin2∅sinθ+2
dlsinδ}+π
d2/4cos∅{1+(
i-1)θ/Θ}]
Where,
δ: Angle between the leg and the horizontal plane on the ABC plane
ε: Apparent hanging angle on a projected plane
θ: Attack angle
Θ: Attack angle when the adjacent legs were touched on a projected plane
Sθ': Projective area of the twine portion of the knotless netting at attack angle Θ<θ ?? 90°.
SΘ': Upper described area of the knotless netting at attack angle 0° ?? θ ?? Θ.
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