add calcParamFast to helicascan
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@@ -710,6 +710,75 @@ class HelicalScan(MotionBase):
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res=(cx,cz,w,fy)
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return res
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def calcParamFast(self,x=((-241.,96.),(-162.,-293.)),
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y=(575.,175.),
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z=((-1401.,-1401.),(-1802.,-1303.)),
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w=(1.2,1.4),
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mode=1):
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'''
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the rotation center of the stage does not change for a new cristal.
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after the function calcParam was called once,
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this faster coordinate transformation can be used.
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FOR SMALL ANGLES USE MODE==0.
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!!! THIS CODE IS NOT YET TESTED !!!
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'''
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#x: ((x_w0y0, x_w1y0),(x_w0y1, x_w1y1)
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#y: lower and upper cristal point
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#z: distance, similar to x
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#w: start and end angle in radians
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#mode 0:use x and z needs to define 1 point at start and 1 point at end
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# 1:use x change with 2 angles needs to define 2 point at start and 2 point at end
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#mode 0 uses:
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#x: ((x_w0y0, None ),(None , x_w1y1)
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#z: ((z_w0y0, None ),(None , z_w1y1)
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#w: (w0,w1)
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#mode 1 uses:
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#x: ((x_w0y0, x_w1y0),(x_w0y1, x_w1y1)
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#z: ((None, None ),(None , None )
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#w: (w0,w1)
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# param[i]=(z_i, y_i, x_i, r_i,phi_i)
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# z_i not changed
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# y_i trivial
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# x_i not changed
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# r_i calculate
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# phi_i calculate
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try:
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param=self.param
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except AttributeError as e:
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raise AttributeError('calcParam must be called first')
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if mode==0:
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for i in range(len(y)):
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# param[i]=(z_i, y_i, x_i, r_i,phi_i)
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r_i =np.sqrt(x[i]**2+z[i]**2)
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phi_i=np.arctan2(z[i],x[i])
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param[i, 1]=y[i]
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param[i, 3:]=(r_i,phi_i)
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else: #mode==1:
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for i in range(len(y)):
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# param[i]=(z_i, y_i, x_i, r_i,phi_i)
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r_i=np.sqrt(x[i]**2+z[i]**2)
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x0=x[i][0]-param[i,2]
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x1=x[i][1]-param[i,2]
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ww=w[i]
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if x0>x1:
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phi_i=np.arctan2(np.cos(ww)-x1/x0,np.sin(ww))
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r_i =x0/np.cos(phi_i)
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else:
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phi_i=np.arctan2(np.cos(ww)-x0/x1,np.sin(ww))
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r_i =x1/np.cos(phi_i)
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param[i, 1]=y[i]
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param[i, 3:]=(r_i,phi_i)
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pass
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def calcParam(self,x=((-241.,96.,-53.),(-162.,-293.,246.)),
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y=(575.,175.),
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z=((-1401.,-1401.,-1802.),(-1802.,-1303.,-1402.))):
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