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In the Situation Shown in Figure T2 0.021U0.021 U If We Multiply

Question 104

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In the situation shown in figure T2.5c, the width of the bell curve at half its peak value is 0.021U0.021 U . If we multiply NAN_{A} , NBN_{B} , and UU by a factor of 100 , then the peak's width (as you can check) is about 0.0021U0.0021 U . Suppose that we increase each solid's NN and the system's total energy by another factor of 101810^{18} to create solids containing 1/61 / 6 of a mole of atoms (still pretty small objects by everyday standards) . Assuming that the trend continues, what will be the approximate width of the combined system's probability bell curve as a fraction of UU ?
 In the situation shown in figure T2.5c, the width of the bell curve at half its peak value is  0.021 U . If we multiply  N_{A} ,  N_{B} , and  U  by a factor of 100 , then the peak's width (as you can check)  is about  0.0021 U . Suppose that we increase each solid's  N  and the system's total energy by another factor of  10^{18}  to create solids containing  1 / 6  of a mole of atoms (still pretty small objects by everyday standards) . Assuming that the trend continues, what will be the approximate width of the combined system's probability bell curve as a fraction of  U  ?   A)   2 \times 10^{-20}  (c)  0.0 B)   2 \times 10^{-22}  Figure T2.5 C)   2 \times 10^{-10}  D)   \mathbf{2} \times \mathbf{1 0}^{-12}  E)   2 \times 10^{-40}  F)   2 \times 10^{-42}   \mathrm{T} . Some other factor (specify) .


A) 2×10202 \times 10^{-20}
(c) 0.0
B) 2×10222 \times 10^{-22}
Figure T2.5
C) 2×10102 \times 10^{-10}
D) 2×1012\mathbf{2} \times \mathbf{1 0}^{-12}
E) 2×10402 \times 10^{-40}
F) 2×10422 \times 10^{-42}
T\mathrm{T} . Some other factor (specify) .

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