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1
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77950004720
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Weak interactions must exist in order for the gas to achieve thermodynamic equilibrium. It is assumed that these interactions have negligible effects on the equations of state
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Weak interactions must exist in order for the gas to achieve thermodynamic equilibrium. It is assumed that these interactions have negligible effects on the equations of state.
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2
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77949969411
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The term photon was coined by Gilbert N. Lewis, The conservation of photons, Nature (London) 118, 874-875 (1926).
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The term "photon" was coined by Gilbert N. Lewis, "The conservation of photons," Nature (London) 118, 874-875 (1926).
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3
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0032354789
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The introductory university physics project 1987-1995: What has it accomplished,?
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and references therein. See
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See Lawrence A. Coleman, Donald F. Holcomb, and John S. Rigden, "The introductory university physics project 1987-1995: What has it accomplished,?" Am. J. Phys. 66, 124-137 (1998), and references therein.
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(1998)
Am. J. Phys
, vol.66
, pp. 124-137
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Coleman, L.A.1
Holcomb, D.F.2
Rigden, J.S.3
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4
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77949996131
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2nd ed, Saunders College Publishing, New York
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Stephen T. Thornton and Andrew F. Rex, Modern Physics, 2nd ed. (Saunders College Publishing, New York, 2000), pp. 91-96, 296-298.
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(2000)
Modern Physics
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Thornton, S.T.1
Rex, A.F.2
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6
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0038758336
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Addison-Wesley Longman, Reading, MA
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Eugene Hecht, Optics (Addison-Wesley Longman, Reading, MA, 1998), pp. 50-57, 575-583.
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(1998)
Optics
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Hecht, E.1
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8
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0003915234
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Cambridge University Press, Cambridge
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Ralph Baierlein, Thermal Physics (Cambridge University Press, Cambridge, 1999), pp. 116-130.
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(1999)
Thermal Physics
, pp. 116-130
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Baierlein, R.1
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12
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77949972221
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Raj K. Pathria, Statistical Mechanics, 2nd ed. (Butterworth-Heineman, Oxford, 1996), Appendixes B, D, E.
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Raj K. Pathria, Statistical Mechanics, 2nd ed. (Butterworth-Heineman, Oxford, 1996), Appendixes B, D, E.
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13
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33744606715
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World Scientific, Singapore, Relevant kinetic theory is discussed in Part I, Chap. 1, and the photon gas is discussed in Part IV, Chap. 4
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Daniel J. Amit and Yosef Verbin, Statistical Physics: An Introductory Course (World Scientific, Singapore, 1995). Relevant kinetic theory is discussed in Part I, Chap. 1, and the photon gas is discussed in Part IV, Chap. 4.
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(1995)
Statistical Physics: An Introductory Course
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Amit, D.J.1
Verbin, Y.2
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14
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77949938735
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in preparation
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Harvey S. Leff (in preparation).
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Leff, H.S.1
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15
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77949964777
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Students of introductory physics do not typically encounter enthalpy in their courses, and the discussion in the text can be skipped. On the other hand, students are introduced to enthalpy in their chemistry courses, and the discussion in the text might help them appreciate, if not fully understand, enthalpy in a wider context.
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Students of introductory physics do not typically encounter enthalpy in their courses, and the discussion in the text can be skipped. On the other hand, students are introduced to enthalpy in their chemistry courses, and the discussion in the text might help them appreciate, if not fully understand, enthalpy in a wider context.
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16
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77949989057
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See Ref. 10, p. 33
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See Ref. 10, p. 33.
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17
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77949959498
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In Eq. (11), the prefactor 60.4 in r arises from an integral, which gives 8π(3)Γ(3)=60.4. Here ̄(3) and Γ(3) are zeta and gamma functions, respectively.
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In Eq. (11), the prefactor 60.4 in r arises from an integral, which gives 8π(3)Γ(3)=60.4. Here ̄(3) and Γ(3) are zeta and gamma functions, respectively.
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20
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77949995026
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The assumption of elastic collisions does not hold for walls that can absorb and emit photons. In that case, however, isotropy guarantees that Eq, Al still holds because the average number of photons coming from a wall section in any time interval must equal the number approaching the wall, and the average momentum approaching must equal the average momentum leaving. The mathematical treatment used for elastic collisions thus holds in an average sense when inelastic collisions occur, and isouropy holds
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The assumption of elastic collisions does not hold for walls that can absorb and emit photons. In that case, however, isotropy guarantees that Eq. (Al) still holds because the average number of photons coming from a wall section in any time interval must equal the number approaching the wall, and the average momentum approaching must equal the average momentum leaving. The mathematical treatment used for elastic collisions thus holds in an average sense when inelastic collisions occur, and isouropy holds.
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