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  1. V. R. Stull and G. N. Plass, “Spectral emissivity of hydrogen chloride from 1000–3400 cm−1,” Publ. No. U-461. (Aeronutronic, Newport Beach, California, May15, 1959).
  2. B. Kivel, H. Mayer, and H. A. Bethe, Ann. phys. (N. Y.) 2, 57 (1957).
    [Crossref]
  3. J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
    [Crossref]
  4. A more complete account of the theoretical treatment will be published elsewhere by S. S. Penner, K. G. P. Sulzmann, and C. B. Ludwig.
  5. S. S. Penner, Quantitative Molecular Spectroscopy and Gas Emissivities (Addison-Wesley Publishing Company, Inc., Reading, Massachusetts, 1959), p. 398.
  6. Reference 4, Eqs. (14–7) and (2–19).
  7. Equation (3a) is identical with Eq. (11–141) of reference 4.
  8. In our calculations we used a numerical estimate for f1,0 equivalent to that employed by Plass for the sum of the isotopic species HCl35 and HCl37. This value is probably somewhat low (cf. reference 4).

1959 (1)

J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
[Crossref]

1957 (1)

B. Kivel, H. Mayer, and H. A. Bethe, Ann. phys. (N. Y.) 2, 57 (1957).
[Crossref]

Bethe, H. A.

B. Kivel, H. Mayer, and H. A. Bethe, Ann. phys. (N. Y.) 2, 57 (1957).
[Crossref]

Camm, J. C.

J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
[Crossref]

Keck, J. C.

J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
[Crossref]

Kivel, B.

J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
[Crossref]

B. Kivel, H. Mayer, and H. A. Bethe, Ann. phys. (N. Y.) 2, 57 (1957).
[Crossref]

Ludwig, C. B.

A more complete account of the theoretical treatment will be published elsewhere by S. S. Penner, K. G. P. Sulzmann, and C. B. Ludwig.

Mayer, H.

B. Kivel, H. Mayer, and H. A. Bethe, Ann. phys. (N. Y.) 2, 57 (1957).
[Crossref]

Penner, S. S.

S. S. Penner, Quantitative Molecular Spectroscopy and Gas Emissivities (Addison-Wesley Publishing Company, Inc., Reading, Massachusetts, 1959), p. 398.

A more complete account of the theoretical treatment will be published elsewhere by S. S. Penner, K. G. P. Sulzmann, and C. B. Ludwig.

Plass, G. N.

V. R. Stull and G. N. Plass, “Spectral emissivity of hydrogen chloride from 1000–3400 cm−1,” Publ. No. U-461. (Aeronutronic, Newport Beach, California, May15, 1959).

Stull, V. R.

V. R. Stull and G. N. Plass, “Spectral emissivity of hydrogen chloride from 1000–3400 cm−1,” Publ. No. U-461. (Aeronutronic, Newport Beach, California, May15, 1959).

Sulzmann, K. G. P.

A more complete account of the theoretical treatment will be published elsewhere by S. S. Penner, K. G. P. Sulzmann, and C. B. Ludwig.

Wentink, T.

J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
[Crossref]

Ann. phys. (N. Y) (1)

J. C. Keck, J. C. Camm, B. Kivel, and T. Wentink, Ann. phys. (N. Y) 7, 1 (1959).
[Crossref]

Ann. phys. (N. Y.) (1)

B. Kivel, H. Mayer, and H. A. Bethe, Ann. phys. (N. Y.) 2, 57 (1957).
[Crossref]

Other (6)

V. R. Stull and G. N. Plass, “Spectral emissivity of hydrogen chloride from 1000–3400 cm−1,” Publ. No. U-461. (Aeronutronic, Newport Beach, California, May15, 1959).

A more complete account of the theoretical treatment will be published elsewhere by S. S. Penner, K. G. P. Sulzmann, and C. B. Ludwig.

S. S. Penner, Quantitative Molecular Spectroscopy and Gas Emissivities (Addison-Wesley Publishing Company, Inc., Reading, Massachusetts, 1959), p. 398.

Reference 4, Eqs. (14–7) and (2–19).

Equation (3a) is identical with Eq. (11–141) of reference 4.

In our calculations we used a numerical estimate for f1,0 equivalent to that employed by Plass for the sum of the isotopic species HCl35 and HCl37. This value is probably somewhat low (cf. reference 4).

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Figures (2)

Fig. 1
Fig. 1

Comparison of spectral emissivities in the weak-line approximation obtained by numerical calculations1 (dotted curves) and spectral emissivities obtained by using Eq. (3a) (solid curves) for various optical depths at 600°K.

Fig. 2
Fig. 2

Comparison of spectral emissivities in the weak-line approximation obtained by numerical calculations1 (dotted curves) and spectral emissivities obtained by using Eq. (3a) (solid curves) for various optical depths at 2400°K.

Equations (8)

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h c ω ( n - n ) ± 2 j h c B e ,
j ( j ) 2 h c B e = [ ω / 2 B e - ( n - n ) / 2 h c B e ] 2 h c B e
d f n , n d ω = 1 2 f n , n h c ω - ( n - n ) 2 B e k T × exp { - [ h c ω - ( n - n ) ] 2 4 h c B e k T } .
f n , n = f n - n , 0 χ 2 n , n ,
P ω n , n π e 2 m c 2 N n p d f n , n d ω ( 1 - e - h c ω / k T ) ,
P ω = n P ω n , n 1 2 π e 2 m c 2 f n - n , 0 N T p Q v h c 2 B e k T [ 1 - exp ( - h c ω / k T ) ] × n χ 2 n , n [ exp ( - n / k T ) ] ω - ω n , n × exp [ - h c ( ω - ω n , n ) 2 4 B e k T ] ,
P ω , h , o . = 1 2 π e 2 m c 2 f 1 , 0 N T p Q v [ 1 - exp ( - h c ω / k T ) ] [ exp ( - h c ω 0 / 2 k T ) ] × [ 1 - exp ( - h c ω 0 / k T ) ] - 2 h c ω - ω 0 2 B e k T [ exp - h c ( ω - ω 0 ) 2 4 B e k T ] ,
ω 1 - exp ( - P ω , h . o . p l ) ,