Example #1
0
def B_term(r, z, *p):
    n1, a1, b1 = p

    br, bz = rt1.bvec(r, z, separatrix)
    bb = np.sqrt(br**2 + bz**2)

    if rt1.check_coilcase(r, z):
        return 0.0
    else:
        return (bb / rt1.b0(r, z, separatrix))**(-b1)
Example #2
0
def ne_single_gaussian(r, z, *p):
	n1, a1, b1, rm = p

	br, bz = rt1.bvec(r, z, separatrix)
	bb = np.sqrt(br**2 + bz**2)

	if r == 0.0:
		return n1 * np.exp(-a1 * abs((rt1.psi(r, 0.0, separatrix)-psix)/psi0)**2)

	if rt1.check_coilcase(r, z):
		return 0.0
	else:
		return n1 * np.exp(-a1*abs((rt1.psi(r, z, separatrix) - psix)/psi0)**2) * (bb/rt1.b0(r, z, separatrix))**(-b1)
Example #3
0
    psi_z620 = np.zeros(len(z620))
    psi_z700 = np.zeros(len(z700))
    bb620 = np.zeros(len(z620))
    bb700 = np.zeros(len(z700))
    b0620 = np.zeros(len(z620))
    b0700 = np.zeros(len(z700))

    for i, x in enumerate(x450):
        rx = np.sqrt(x**2 + r450_para**2)
        psi_x450[i] = rt1.psi(rx, 0.0, separatrix)

    for j, z in enumerate(z620):
        psi_z620[j] = rt1.psi(r620_perp, z, separatrix)
        br, bz = rt1.bvec(r620_perp, z, separatrix)
        bb620[j] = np.sqrt(br**2 + bz**2)
        b0620[j] = rt1.b0(r620_perp, z, separatrix)

    for j, z in enumerate(z700):
        psi_z700[j] = rt1.psi(r700_perp, z, separatrix)
        br, bz = rt1.bvec(r700_perp, z, separatrix)
        bb700[j] = np.sqrt(br**2 + bz**2)
        b0700[j] = rt1.b0(r700_perp, z, separatrix)

    print('                                      ')
    print('      start 1st optimization....      ')
    print('                                      ')
    err_max = 1e10

    if not (view_mode is True):
        if gaussian == 'single':