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References

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  1. H. C. van de Hulst, Light Scattering by Small Particles (John Wiley & Sons, Inc., New York, 1957).
  2. P. Wyatt, Interdisciplinary Conference on Electromagnetic Scattering, edited by M. Kerker (Pergamon Press, Inc., New York, 1963), pp. 25–35.
  3. S. Levine and M. Kerker, reference 2, pp. 37–46.
  4. W. A. Farone, M. Kerker, and E. Matijevic, reference 2, pp. 55–70.
  5. W. Heller, reference 2, pp. 101–120.

Farone, W. A.

W. A. Farone, M. Kerker, and E. Matijevic, reference 2, pp. 55–70.

Heller, W.

W. Heller, reference 2, pp. 101–120.

Kerker, M.

W. A. Farone, M. Kerker, and E. Matijevic, reference 2, pp. 55–70.

S. Levine and M. Kerker, reference 2, pp. 37–46.

Levine, S.

S. Levine and M. Kerker, reference 2, pp. 37–46.

Matijevic, E.

W. A. Farone, M. Kerker, and E. Matijevic, reference 2, pp. 55–70.

van de Hulst, H. C.

H. C. van de Hulst, Light Scattering by Small Particles (John Wiley & Sons, Inc., New York, 1957).

Wyatt, P.

P. Wyatt, Interdisciplinary Conference on Electromagnetic Scattering, edited by M. Kerker (Pergamon Press, Inc., New York, 1963), pp. 25–35.

Other (5)

H. C. van de Hulst, Light Scattering by Small Particles (John Wiley & Sons, Inc., New York, 1957).

P. Wyatt, Interdisciplinary Conference on Electromagnetic Scattering, edited by M. Kerker (Pergamon Press, Inc., New York, 1963), pp. 25–35.

S. Levine and M. Kerker, reference 2, pp. 37–46.

W. A. Farone, M. Kerker, and E. Matijevic, reference 2, pp. 55–70.

W. Heller, reference 2, pp. 101–120.

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Figures (4)

Fig. 1
Fig. 1

Error contour chart for efficiency factor Q. In Region I, RGT agrees with Mie theory to within at least 10%; in Region II, to within at least 100%; in Region III, the error is greater than 100% except in small islands.

Fig. 2
Fig. 2

Same as Fig. 1 for i1 and θ = 10°.

Fig. 3
Fig. 3

Same as Fig. 1 for i1 and θ = 20°.

Fig. 4
Fig. 4

Same as Fig. 1 for i1 and θ = 45°.

Equations (5)

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α = [ ( m 1 ) / 2 π ] d V ,
Q = | m 1 | 2 4 9 x 4 0 x G 2 ( 2 x sin θ 2 ) ( 1 + cos 2 θ ) sin θ d θ
i 1 = | 1 3 [ i 2 k 3 a 3 ( m 1 ) ] G ( 2 x sin θ / 2 ) | 2 ,
G ( u ) = ( 3 / u 3 ) ( sin u u cos u ) = ( 9 π / 2 u 3 ) 1 / 2 J 3 / 2 ( u ) .
( m 2 1 ) / ( m 2 + 2 ) 2 3 ( m 1 ) ,