Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 19 - The Kinetic Theory of Gases - Problems - Page 579: 32a

Answer

$\frac{5}{3}$

Work Step by Step

$T=20^{\circ}C = 293.15K$ $p=1 torr = 133.322 Pa$ $λ_{Ar} = 9.9\times10^{-6}cm=9.9\times10^{-8}m$ $λ_{N2} = 27.5\times10^{-6}cm=2.75\times10^{-7}m$ Boltzmann constant $k=1.38\times10^{−23}$ Using the mean free path equation $ λ=\frac{kT}{π\times\sqrt 2\times d^{2}\times p}$, we can calculate the diameter of these gases $d=\sqrt {\frac{kT}{λ\times π\times \sqrt 2 \times p}}$ Diameter of an Ar atom $d_{Ar}=\sqrt {\frac{1.38\times10^{−23}\times293.15}{9.9\times10^{-8}\timesπ\times\sqrt 2 \times133.322}}$ $d_{Ar}=8.3\times10^{-9}$ Diameter of an $N_2$ molecule $d_{{N_{2}}}=\sqrt {\frac{1.38\times10^{−23}\times293.15}{2.75\times10^{-7}\timesπ\times\sqrt 2 \times133.322}}$ $d_{{N_{2}}}=4.98\times10^{-9}$ Ratio of the diameter of an Ar atom to that of an $N_2$ molecule = $\frac{d_{Ar}}{d_{N_2}}$ =$ \frac{8.3\times10^{-9}}{4.98\times10^{-9}}$ = $\frac{5}{3}$
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