本文整理汇总了Python中Physics.normalize方法的典型用法代码示例。如果您正苦于以下问题：Python Physics.normalize方法的具体用法？Python Physics.normalize怎么用？Python Physics.normalize使用的例子？那么恭喜您, 这里精选的方法代码示例或许可以为您提供帮助。您也可以进一步了解该方法所在类Physics的用法示例。
在下文中一共展示了Physics.normalize方法的5个代码示例，这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞，您的评价将有助于系统推荐出更棒的Python代码示例。
示例1: __set_g
# 需要导入模块: import Physics [as 别名]
# 或者: from Physics import normalize [as 别名]
def __set_g(self, g):
self.__g = array(g)
self.gnorm = Physics.norm(g)
self.gnormalized = Physics.normalize(g)
# angular coordinates (azimuth and colatitude) of the g versor
self.gtheta = math.acos(self.gnormalized[2])
self.gphi = Physics.atan2(g[1], g[0])示例2: __set_k
# 需要导入模块: import Physics [as 别名]
# 或者: from Physics import normalize [as 别名]
def __set_k(self, k):
self.__k = array(k)
self.knorm=Physics.norm(k)
self.knormalized = Physics.normalize(k)
# Calculates wavelength and energy of the photon
if self.knorm==0.:
self.__e, self.__lam=0., '+inf'
else:
self.__lam=2.*pi/self.knorm
self.__e=Booklet.hc/self.__lam示例3: __set_g
# 需要导入模块: import Physics [as 别名]
# 或者: from Physics import normalize [as 别名]
def __set_g(self, g):
self.__g = array(g)
self.gnorm = Physics.norm(g)
self.gnormalized = Physics.normalize(g)
# angular coordinates of the reciprocal lattice vector g
# gtheta is the polar angle (the angle between z axis and g vector)
# gphi is the azimuthal angle (in the plane xy, from the x axis)
self.gtheta = math.acos(self.gnormalized[2])
self.gphi = Physics.atan2(g[1], g[0])示例4: local_eranges
# 需要导入模块: import Physics [as 别名]
# 或者: from Physics import normalize [as 别名]
def local_eranges(self, Emin=1., Emax=1000., sphi=0., stheta=pi, deltasource=0):
l = math.sqrt(self.photon.r[0]**2 + self.photon.r[1]**2)
#stheta = stheta - self.divergence_stheta(l, deltasource)
sphi = self.divergence_sphi(self.photon.r)
local_xtal_g = self.change_the_g(self.xtal.g)
lgn=Physics.normalize(local_xtal_g)
local_xtal_gphi = Physics.atan2(local_xtal_g[1], local_xtal_g[0])
local_xtal_gtheta = math.acos(lgn[2])
order, reached_max_order = 0,False
factor = 2.5
Darwin_Width = Physics.darwinwidth(self.xtal.Z, self.xtal.hkl, self.photon.e)
if self.xtal.structure == "mosaic":
Deltatheta = 1.0 * (self.xtal.fwhm/60/180*pi)
else:
Deltatheta = Darwin_Width + (self.xtal.dim[2] * self.xtal.curvature) / factor
Delta_curvature = self.xtal.curvature * self.xtal.dim[0]
thetamin, thetamax = local_xtal_gtheta-Deltatheta/2, local_xtal_gtheta+Deltatheta/2
constant=-Booklet.hc/(2.*self.xtal.d_hkl)
eranges=[]
while not reached_max_order:
order+=1
cosdeltaphi=math.cos(sphi-local_xtal_gphi)
sinstheta=math.sin(stheta)
cosstheta=math.cos(stheta)
sinthetamin=math.sin(thetamin)
costhetamin=math.cos(thetamin)
sinthetamax=math.sin(thetamax)
costhetamax=math.cos(thetamax)
Eminim_= constant*order/(cosdeltaphi*sinstheta*sinthetamin+cosstheta*costhetamin)
Emaxim_= constant*order/(cosdeltaphi*sinstheta*sinthetamax+cosstheta*costhetamax)
if Emaxim_ >= Emax:
if Eminim_>=Emax: return eranges
else:
reached_max_order=True
Emaxim_=Emax
if Eminim_ <= Emin:
if Emaxim_ <= Emin: pass
else:
Eminim_=Emin
eranges.append((Eminim_, Emaxim_))
else: eranges.append((Eminim_, Emaxim_))
return eranges示例5: best_thickness
# 需要导入模块: import Physics [as 别名]
# 或者: from Physics import normalize [as 别名]
def best_thickness(keV):
"""Wrapper for the Physics module function"""
return Physics.best_thickness(keV, Z, hkl, eta)
g=20
theta_0=0
D=2000
dim1=1.5
dim2=1.5
dim3=0.3
g=0
gnormalized = Physics.normalize(g)
gtheta = 0.0
EB = 100.0
def extinction_factor(keVB, theta_0):
return Physics.extinction_factor(keVB, Z, hkl, microthick, theta_0)
def getDelta(self, tB, OFFSET=0.):
return pi/2-gtheta-tB
mat_facs = Booklet.mat_fac(Z, hkl)