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In other words, the fraction of particles in this range is 1/3 or 0.3.42. (a) The work is zero in this process since volume is kept fixed.(b) Since CV = R for an ideal monatomic gas, then Eq.
19-39 gives Q = 374 J.(c) ∆Eint = Q – W = 374 J.(d) Two moles are equivalent to N = 12 x 1023 particles.
To the best of our knowledge the Virginia Scoring System predates the Boone & Crockett Scoring System used by many other states. Primary differences is the tip to tip measurement, use of outside beam measured and the way non-symmetry is calculated.
6 9 v v v v v(d) The number of particles with speeds between 1.5v0 and 2v0 is given by 2 1.5 v NPvdv∫.
Consequently, CHAPTER 19 with the subscript 1 referring to the situation (of small volume, high pressure, and high temperature) the system is in at the end of part (a), we obtain5.
(a) Let pi, Vi, and Ti represent the pressure, volume, and temperature of the initial state of the gas.
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The fact that they rotate but do not oscillate means that the value of f given in Table19-3 is relevant.