At first, we know that for a particle in a box:
"\\Psi_{n}(x)=\\sqrt{\\frac{2}{L}}sin(\\frac{n\\pi x}{L}), n=1, 2, 3, ..."
For the problem, we have n=101 (because n=2 is the first excited state), and we will calculate the probability with the integral
"P=\\int_0^{L\/100}[\\Psi_{n}(x)]^2dx \\\\ P=\\int_0^{L\/100}[\\sqrt{\\frac{2}{L}}sin(\\frac{n\\pi x}{L})]^2dx \\\\ P=\\frac{2}{L}\\int_0^{L\/100}sin^2(\\frac{n\\pi x}{L})dx"
Then, to solve the integral we use the formula for the squared sine:
"sin^2(\\frac{n\\pi x}{L})=\\frac{1}{2}[1-cos(\\frac{2n\\pi x}{L})]"
We substitute and find the result of the integral:
"P=\\frac{2}{L}\\int_0^{L\/100}sin^2(\\frac{n\\pi x}{L})dx \\\\ P=\\frac{1}{L}\\int_0^{L\/100}[1-cos(\\frac{2n\\pi x}{L})]dx \n\\\\P= \\frac{1}{L} [x-\\frac{L}{2n\\pi}sin(\\frac{2n\\pi x}{L})]\\lvert_0^{L\/100}"
Then we substitute the limits to find the probability between x=0 and x=L/100
"P= \\frac{1}{L}\\{ [\\frac{L}{100}-\\frac{L}{2(101)\\pi}sin(\\frac{2\\pi(101) \\frac{L}{100}}{L})]-[0-\\frac{L}{2(101)\\pi}sin(0)]\\}\n\\\\P= \\frac{1}{L}\\{\\frac{L}{100}-\\frac{L}{202\\pi}sin(2.02\\pi)\\}"
This last formula after simplification gives "\\\\ P= \\frac{1}{100}-\\frac{sin(2.02\\pi)}{202\\pi}" , which is equal to
"P= \\frac{1}{100}-\\frac{sin(2.02\\pi)}{202\\pi}\\approxeq0.01-\\frac{0.06279}{202\\pi}\\approxeq0.01-0.000098945"
"\\\\ P\\approxeq 0.009901; \\% P\\approxeq 0.9901 \\%"
In conclusion, the probability to find the particle between x= 0 to x=L/100, in an infinite potential
well given that the particle is in the 100th excited state is P=0.009901 or 0.9901%.
Reference:
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