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- import unittest
- from scattnlay import mie, mie_mp
- from scattnlay import mesomie
- # A list of tests for a bulk sphere from
- # Hong Du, "Mie-scattering calculation," Appl. Opt. 43, 1951-1956 (2004)
- # table 1: sphere size and refractive index
- # followed by resulting extinction and scattering efficiencies
- test_cases = [
- # x, m, Qext, Qsca #, test_name
- [0.099, 0.75+0j, 7.417859e-06, 7.417859e-06], # ,'a'],
- [0.101, 0.75+0j, 8.033538e-06, 8.033538e-06], # ,'b'],
- [10, 0.75+0j, 2.232265, 2.232265], # ,'c'],
- [0.055, 1.5+1j, 0.10149104, 1.131687e-05], # ,'g'],
- [0.056, 1.5+1j, 0.1033467, 1.216311e-05], # ,'h'],
- [1, 10+10j, 2.532993, 2.049405], # ,'k'],
- [100, 1.33+1e-5j, 2.101321, 2.096594], # ,'e'],
- [100, 1.5+1j, 2.097502, 1.283697], # ,'i'],
- [1000, 0.75+0j, 1.997908, 1.997908], # ,'d'],
- [100, 10+10j, 2.071124, 1.836785], # ,'l'],
- [10000, 1.33+1e-5j, 2.004089, 1.723857], # ,'f'],
- [10000, 1.5+1j, 2.004368, 1.236574], # ,'j'],
- [10000, 10+10j, 2.005914, 1.795393], # ,'m'],
- # [1.8263846985116234, 0.02867488311561525+1.2957040351341687j, 3, 3]
- ]
- class TestStringMethods(unittest.TestCase):
- def test_bulk_mesomie(self):
- tol = 3e-7
- for solver in [mesomie]:
- print('Using solver: ', solver)
- for case in test_cases:
- x = case[0]
- m = case[1]
- solver.calc_ab(x, # R
- x, # xd
- x * m, # xm
- 1, # eps_d
- m * m, # eps_m
- 0, # d_parallel
- 0) # d_perp
- solver.calc_Q()
- Qext = solver.GetQext()
- Qsca = solver.GetQsca()
- # print(x, m, Qext)
- self.assertTrue((case[2]-Qext)/Qext < tol)
- self.assertTrue((case[3]-Qsca)/Qsca < tol)
- def test_bulk_multilayer(self):
- tol = 3e-7
- for solver in [mie, mie_mp]:
- if solver is None:
- continue
- print('Using solver: ', solver)
- for case in test_cases:
- solver.SetLayersSize(case[0])
- solver.SetLayersIndex(case[1])
- solver.RunMieCalculation()
- Qext = solver.GetQext()
- Qsca = solver.GetQsca()
- self.assertTrue((case[2]-Qext)/Qext < tol)
- self.assertTrue((case[3]-Qsca)/Qsca < tol)
- if __name__ == '__main__':
- unittest.main()
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