1937
DOI: 10.1021/j150384a006
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The Identification of Opaque Solids by Selective Iridescent Filming. I. Optics.

Abstract: On the contrary, if the thickness of the film is such that reflections of the zero and first orders differ by a full wave, bz will lag behind bl by PA, bo -(bl + bz + b3 + . . . . + bp). n, FIG. 2.Multiple reflections a t a filmed surface since its retardation involves not only that due to the thickness of the film, but also one moreretardation due to reflection into a rare medium at n dense medium boundary; likewise b, will lag behind bl by 2.3X or 3 X ; br by 3 .$A or PA, etc. X 2 The amplitude of the net re… Show more

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Cited by 7 publications
(6 citation statements)
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“…The vibrational partition can be written as 3n--6 qvib : II (1 --exp--hcv/kT) -1 [16] Providing ~(in cm -I) is large, which is the usual case for real vibrations, qvJb is essentially unity.…”
Section: Appendixmentioning
confidence: 99%
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“…The vibrational partition can be written as 3n--6 qvib : II (1 --exp--hcv/kT) -1 [16] Providing ~(in cm -I) is large, which is the usual case for real vibrations, qvJb is essentially unity.…”
Section: Appendixmentioning
confidence: 99%
“…For the rotational partition function, an equation similar to [16] was used because species in solution are subject to strong interactions by neighboring molecules or ions (e.g., as in hydrogen bonding) and the molecule will not be free to rotate but will exhibit librational motion. Using the harmonic oscillator approximation [c.f.…”
Section: Appendixmentioning
confidence: 99%
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