Physics (10th Edition)

Published by Wiley
ISBN 10: 1118486897
ISBN 13: 978-1-11848-689-4

Chapter 14 - The Ideal Gas Law and Kinetic Theory - Problems - Page 386: 47

Answer

(a) $2.08\space s$ (b) $1.6\times10^{-5}s$ (c) The answer is given below

Work Step by Step

(a) Time (t) required for the first solute to = $\frac{L^{2}}{2D}$ traverse a channel of length 0.01 m $$t=\frac{(0.01\space m)^{2}}{2(2.4\times10^{-5}m^{2}/s)}=2.08\space s$$ (b) Here we use equation 14.6 $KE_{Avg}=\frac{1}{2}mv_{rms}^{2}$ to find the time. $KE_{Avg}=\frac{1}{2}mv_{rms}^{2}=>v_{rms}=\sqrt {\frac{2(KE_{Avg})}{m}}-(1)$ We can write, mass of a single = $\frac{[2(1.00794)+15.9994]\times10^{-3}kg/mol}{6.022\times10^{23}mol^{-1}}=2.99\times10^{-26}kg-(2)$ molecule (m) $KE_{Avg}=\frac{3}{2}kT=\frac{3(1.38\times10^{-23}J/K)(293\space K)}{2}=6.07\times10^{-21}J-(3)$ (2),(3)=>(1), $v_{rms}=\sqrt {\frac{2(6.07\times10^{-21}J)}{2.99\times10^{-26}kg}}=637\space m/s$ So, the time required for a water molecule to travel the distance 0.01 m is, $t=\frac{0.01\space m}{637\space m/s}=1.6\times10^{-5}s$ (c) When a water molecule diffuses through air, it makes a very large amount of collisions with air molecules. So, speed and direction change abruptly as a result of each collision. Due to this case, the water molecules move slowly in a zigzag path from one end of the channel to the other. But in part (b) there are no obstacles and will have a larger displacement over a much shorter time. Therefore, the answer to part (a) is much larger than the answer to part (b)
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