Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 39 - Wave Functions and Uncertainty - Exercises and Problems - Page 1177: 41

Answer

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Work Step by Step

$$\color{blue}{\bf [a]}$$ We are told that the wave function must be continuous at $ x = 0 $. This means that the probability density function $ P(x)=|\psi(x)|^2 $ must also be continuous at $ x = 0 $. For $ x = 0 $, the value of $ P(x) $ from the left side (where $ -1 \leq x < 0 $) must equal the value from the right side (where $ 0 \leq x \leq 1 $). For $ -1 \leq x < 0 $, the probability density is given by: $$ P(x) = \frac{a}{1 - x} $$ For $ 0 \leq x \leq 1 $, the probability density is given by: $$ P(x) = b(1 - x) $$ At $ x = 0 $, we must have: $$ \frac{a}{1 - 0} = b(1 - 0) $$ Thus, $$ \boxed{a = b} $$ Therefore, $ a $ and $ b $ must be equal for the wave function to be continuous at $ x = 0 $. $$\color{blue}{\bf [b]}$$ To determine the values of $ a $ and $ b $, we use the fact that the total probability of finding the particle must be 1. $$ \int_{-1}^{1} P(x) \; dx = 1 $$ Thus, from the given formula, $$ \int_{-1}^{0} \frac{a}{1 - x} \; dx + \int_{0}^{1} b(1 - x) \; dx = 1 $$ And since $ a = b $, we can simplify by setting both constants equal to $ a $. $$ a \int_{-1}^{0} \frac{1}{1 - x} \; dx + a \int_{0}^{1} (1 - x) \; dx = 1 \tag 1$$ The first integral: $$ \int_{-1}^{0} \frac{1}{1 - x} \; dx =\ln(1 - (-1)) - \ln(1 - 0) \\ = \ln(2) - \ln(1) = \ln(2) $$ The second integral: $$ \int_{0}^{1} (1 - x) \; dx= \left[ x - \frac{x^2}{2} \right]_{0}^{1} \\ = 1 - \frac{1}{2} = \frac{1}{2} $$ Substituting the results into (1) $$ a \ln(2) + a \cdot \frac{1}{2} = 1 $$ Therefore, $$ a=b = \frac{1}{\ln(2) + \frac{1}{2}} \approx \color{red}{\bf 0.838} $$ $$\color{blue}{\bf [c]}$$ The probability density $ P(x) $ is given by: $$ P(x) = \begin{cases} \dfrac{0.838}{1 - x} & \text{for} \; -1 \leq x < 0 \\\\ 0.838 (1 - x) & \text{for} \; 0 \leq x \leq 1 \end{cases} $$ $$\color{blue}{\bf [d]}$$ The probability of finding the particle to the left of the origin is the integral of $ P(x) $ from $ -1 \; \text{mm} $ to $ 0 \; \text{mm} $: $$ P(-1\lt x < 0) = \int_{-1}^{0} \frac{a}{1 - x} \; dx $$ $$ P(-1\lt x < 0) =a\ln(1 - (-1)) - \ln(1 - 0) =a \ln(2) - a\ln(1) \\ =a\ln(2)= 0.838 \ln(2) $$ $$ P(-1\lt x < 0) =\bf{0.581}=\color{red}{\bf 58\% }$$
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