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Use the method of cylindrical shells to calculate the volume enclosed when the curve y = x 2 , 0 x 3, is rotated about the x-axis (Figure 8.20).
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For comparison purposes, we have chosen the three most probable distributions and four of the least likely distributions. Looking at the four least likely distributions in Fig. 5-5, the total number of ways to arrive at any of these four distributions is the sum of their permutations, or 355. If we compare this to the total number of permutations of all 22 distributions (i.e., 355 compared to 24,310), we see that these four distributions combined amount to less than 1.5% of the total number of ways to partition the energy. That is, there is less than a 1.5% chance of finding our system in any of these four distributions combined. This suggests that we could simply ignore these four distributions, and we would introduce an error of no more than 1.5% to our calculations. Such a small amount of error is insignificant for many situations. We can therefore say that in such situations these distributions are negligible; that is, they can safely be ignored.
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