def mean_surge_force(w, depth, radius, RAOs, N=10, deep_water=False):
"""Mean surge force on a surging and pitching cylinder
From Drake2011.
"""
g = 9.81
k = w**2 / g # XXX deep water
ka = k * radius
kd = k * depth
# This is the part of the force which depends on the incoming waves
hankel_term = lambda n, ka: 1 - ((hankel1d(n, ka) * hankel2d(n - 1, ka)) /
(hankel2d(n, ka) * hankel1d(n - 1, ka)))
terms = np.nansum([hankel_term(n, ka) for n in range(1, N)], axis=0)
if deep_water:
incoming_part = 1 * terms
else:
incoming_part = (1 + (2 * kd / sinh(2 * kd))) * terms
# This is the part which depends on the first-order motion
hankel_term2 = (hankel2d(0, ka) / hankel1d(0, ka) +
hankel2d(2, ka) / hankel1d(2, ka))
if deep_water:
motion_part = 2j * (
(RAOs[:, 0] - (RAOs[:, 4] / k)) * hankel_term2 / hankel2d(1, ka))
else:
motion_part = 2j * ((RAOs[:, 4] *
(1 - cosh(kd)) / k + RAOs[:, 0] * sinh(kd)) /
(cosh(kd) * hankel2d(1, ka)) * hankel_term2)
return 0.5 / ka * np.real(incoming_part + motion_part)
def first_order_excitation(k, draft, radius, water_depth):
"""Returns F/(rho g a^2 A) -- from Drake, but adapted by me to
integrate down to the draft depth only (not to the seabed)"""
ka = k * radius
kd = k * draft
kh = k * water_depth
# XXX check this!
f1 = -1j * (jn(1, ka) - jnd(1, ka) * hankel2(1, ka) / hankel2d(1, ka))
#f1 = -1j * (jn(1, ka) - jnd(1, ka) * hankel1(1, ka) / hankel1d(1, ka))
M = (kd * sinh(kh - kd) + cosh(kh - kd) - cosh(kh)) / (k * cosh(kh))
F = (-sinh(kh - kd) + sinh(kh)) / cosh(kh)
X = np.zeros(M.shape + (6, ), dtype=np.complex)
X[..., 0] = (-2 * pi / ka) * f1 * F
X[..., 4] = (-2 * pi / ka) * f1 * M
return X
def excitation_force(w, draft, radius, water_depth):
"""Excitation force on cylinder using Drake's first_order_excitation"""
k = w**2 / 9.81
ka = k * radius
kd = k * draft
kh = k * water_depth
rho = 1025
g = 9.81
# XXX check this!
f1 = -1j * (jn(1, ka) - jnd(1, ka) * hankel2(1, ka) / hankel2d(1, ka))
#f1 = -1j * (jn(1, ka) - jnd(1, ka) * hankel1(1, ka) / hankel1d(1, ka))
M = (kd * sinh(kh - kd) + cosh(kh - kd) - cosh(kh)) / (k**2 * cosh(kh))
F = (-sinh(kh - kd) + sinh(kh)) / (k * cosh(kh))
zs = zeros_like(F, dtype=np.complex)
X = np.c_[F, zs, zs, zs, M, zs]
X *= (-rho * g * pi * radius) * 2 * f1[:, newaxis]
return X
