Пример #1
0
    def __init__(self,n,m,A,B):
        self.n=n
        self.m=m
        self.A=A
        self.B=B
        self.Bz=SphereHarmonic(n,m,A,B,mode="COS_SIN",harmtype='_{n,m}')




        fact=-(1+delta(m,0))/(2.0*(n+m+1))        
        self.Bxa=SphereHarmonic(n,m+1,A*fact,B*fact,mode="COS_SIN",harmtype='_{n,m}')
        self.Bya=SphereHarmonic(n,m+1,-B*fact,A*fact,mode="COS_SIN",harmtype='_{n,m}')
        fact=((1-delta(m,0))*(n+m)*(n+m+1))
        if fact != 0.0:
            fact=fact/(2.0*(n+m+1))
        self.Bxb=SphereHarmonic(n,m-1,fact*A,fact*B,mode="COS_SIN",harmtype='_{n,m}')
        self.Byb=SphereHarmonic(n,m-1,fact*B,-fact*A,mode="COS_SIN",harmtype='_{n,m}')
Пример #2
0
class FieldHarmonic:
    """
    A Field harmonic described according to Bz=A T_{n,m}+B T_{n,m}^{\prime}
    """
    def __init__(self,n,m,A,B):
        self.n=n
        self.m=m
        self.A=A
        self.B=B
        self.Bz=SphereHarmonic(n,m,A,B,mode="COS_SIN",harmtype='_{n,m}')




        fact=-(1+delta(m,0))/(2.0*(n+m+1))        
        self.Bxa=SphereHarmonic(n,m+1,A*fact,B*fact,mode="COS_SIN",harmtype='_{n,m}')
        self.Bya=SphereHarmonic(n,m+1,-B*fact,A*fact,mode="COS_SIN",harmtype='_{n,m}')
        fact=((1-delta(m,0))*(n+m)*(n+m+1))
        if fact != 0.0:
            fact=fact/(2.0*(n+m+1))
        self.Bxb=SphereHarmonic(n,m-1,fact*A,fact*B,mode="COS_SIN",harmtype='_{n,m}')
        self.Byb=SphereHarmonic(n,m-1,fact*B,-fact*A,mode="COS_SIN",harmtype='_{n,m}')
        
        
    def A_val_point(self,point):
        # The vector potential at the point
        pass

    def S_val_point(self,point):
        # The scalar potential at the point
        pass

    def B_val_point(self,point):
        Bx=self.Bxa.val_point(point)+self.Bxb.val_point(point)
        By=self.Bya.val_point(point)+self.Byb.val_point(point)
        Bz=self.Bz.val_point(point)
        result=Vector((Bx,By,Bz))
        return result