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References

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  1. P. W. Bridgman, The Physics of High Pressure (Macmillan Co., New York, 1931).
  2. T. C. Poulter, Phys. Rev. 40, 860 (1932).
    [Crossref]
  3. Poulter and Benz, Phys. Rev. 40, 872 (1932).
    [Crossref]
  4. Lyons, “The Behavior of the 4930A Absorption Band of Uranine Solutions under High Pressure,” this issue.

1932 (2)

T. C. Poulter, Phys. Rev. 40, 860 (1932).
[Crossref]

Poulter and Benz, Phys. Rev. 40, 872 (1932).
[Crossref]

Benz,

Poulter and Benz, Phys. Rev. 40, 872 (1932).
[Crossref]

Bridgman, P. W.

P. W. Bridgman, The Physics of High Pressure (Macmillan Co., New York, 1931).

Lyons,

Lyons, “The Behavior of the 4930A Absorption Band of Uranine Solutions under High Pressure,” this issue.

Poulter,

Poulter and Benz, Phys. Rev. 40, 872 (1932).
[Crossref]

Poulter, T. C.

T. C. Poulter, Phys. Rev. 40, 860 (1932).
[Crossref]

Phys. Rev. (2)

T. C. Poulter, Phys. Rev. 40, 860 (1932).
[Crossref]

Poulter and Benz, Phys. Rev. 40, 872 (1932).
[Crossref]

Other (2)

Lyons, “The Behavior of the 4930A Absorption Band of Uranine Solutions under High Pressure,” this issue.

P. W. Bridgman, The Physics of High Pressure (Macmillan Co., New York, 1931).

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Figures (3)

F. 1
F. 1

Top view of prism and lugs.

F. 2
F. 2

Lever system and vertical sections through cylinder.

F. 3
F. 3

Horizontal section through observation slits, with collimator and telescope.

Equations (5)

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P + U = F + W ,
P D = F + W ,
2 P + ( U D ) = 2 W ,
P = W ( U D ) / 2 .
cot A 2 = ( μ cos D 2 ) / sin D 2 .