148
CHAPTER 4. HYDRODYNAMIC MODELS
where
xp
■
Xm -
zp
Zm
Nx -
Nz -
prototype horizontal dimension
- model horizontal dimension
prototype vertical dimension
model vertical dimension
horizontal length scale
vertical length scale
and the factor “A” is now defined in terms of the horizontal lengths as
X
D
±L. = K^- or NX = KND
(4.119)
Xm
Dm
where D is the stone size.
The solid lines in Figure 4.6 are lines of constant values of the factor, A,
and the abscissa is a dimensional factor that combines several parameters
of the rubble-mound structure. This factor (similar to Eqn. 4.35) is
L>p3Pp5
(4.120)
where
Hi
NL
height of the incident wave.
- average width of the core material section,
(therefore, AHi/NL is the gradient of head
loss through the voids in the core material).
DP
effective quarrystone diameter (in centimeters)
of the prototype core material, and it is taken as 10%
smaller than quarrystone from the core material
gradation curve.
P
porosity of the core material (0 < P < 1).
It is important to note that Dp must be a prototype stone diameter in
centimeters. Also, the parameters Hi and AL must be prototype values
because they form a ratio that will not be preserved in a geometrically
distorted long-wave model.
Hudson, et al. (1979) stated that Keulegan’s (1973) method, as represented by Eqns. 4.36 - 4.40, can also be used to size model stone structures
for correct wave transmission provided Eqn. 4.119 is used to determine the
relationship between Dp and Dm.
CHAPTER 4. HYDRODYNAMIC MODELS
where
xp
■
Xm -
zp
Zm
Nx -
Nz -
prototype horizontal dimension
- model horizontal dimension
prototype vertical dimension
model vertical dimension
horizontal length scale
vertical length scale
and the factor “A” is now defined in terms of the horizontal lengths as
X
D
±L. = K^- or NX = KND
(4.119)
Xm
Dm
where D is the stone size.
The solid lines in Figure 4.6 are lines of constant values of the factor, A,
and the abscissa is a dimensional factor that combines several parameters
of the rubble-mound structure. This factor (similar to Eqn. 4.35) is
L>p3Pp5
(4.120)
where
Hi
NL
height of the incident wave.
- average width of the core material section,
(therefore, AHi/NL is the gradient of head
loss through the voids in the core material).
DP
effective quarrystone diameter (in centimeters)
of the prototype core material, and it is taken as 10%
smaller than quarrystone from the core material
gradation curve.
P
porosity of the core material (0 < P < 1).
It is important to note that Dp must be a prototype stone diameter in
centimeters. Also, the parameters Hi and AL must be prototype values
because they form a ratio that will not be preserved in a geometrically
distorted long-wave model.
Hudson, et al. (1979) stated that Keulegan’s (1973) method, as represented by Eqns. 4.36 - 4.40, can also be used to size model stone structures
for correct wave transmission provided Eqn. 4.119 is used to determine the
relationship between Dp and Dm.
