Calculate the probability that the electron in the hydrogen atom, in its ground state, will be found between spherical shells whose radii are a and 2a , where a is the Bohr radius?

Short Answer

Expert verified

The required probability is P=0.439.

Step by step solution

01

Identification of the given data:

The given data is listed below.

  • Radii of the spherical shells are given as a and 2a .
02

Formula for finding the probability of electron:

The ground state wave function of hydrogen atom is given by,

ψ100(r,θ,ϕ)=1π(1a)32e-ra

Here, the Bohr radius is a=5.292×10-11m.

03

Determine the probability of the electron in the hydrogen atom in its ground state:

The probability of finding the electron found between spherical shells is,

P=a2a0π02πψ100r,θ,ϕ2r2drsinθdθdϕ=a2a1π1a32e-ra2r2dr0π=1π1a3a2ae-ra2r2dr×-cosθ0πθ02π=1π1a3-14ae-2raa2+2ar+2r2a2a×-cosπ+cos02π-0

P=1π1a3-a4e-22aaa2+2a2a+22a2-e-2aaa2+2a2+2a2×--1+12π=1π1a3-a4e-413a2-e-25a2×4π=41a3-a40.018313a2-0.13535a2P=4-140.018313-0.13535=-4140.2379-0.6765=0.439

Hence, the probability of the electron in the hydrogen atom in its ground state is 0.439.

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Most popular questions from this chapter

The wave functions for the three states with the dot plots shown in Fig. 39-23, which have n = 2 , l = 1 , and 0, and ml=0,+1,-1, are

Ψ210(r,θ)=(1/42π)(a-3/2)(r/a)r-r/2acosθΨ21+1(r,θ)=(1/8π)(a-3/2)(r/a)r-r/2a(sinθ)e+Ψ21-1(r,θ)=(1/8π)(a-3/2)(r/a)r-r/2a(sinθ)e-

in which the subscripts on Ψ(r,θ) give the values of the quantum numbers n , l , and ml the angles θand ϕ are defined in Fig. 39-22. Note that the first wave function is real but the others, which involve the imaginary number i, are complex. Find the radial probability density P(r) for (a)Ψ210 and (b)Ψ21+1 (same as for Ψ21-1 ). (c) Show that each P(r) is consistent with the corresponding dot plot in Fig. 39-23. (d) Add the radial probability densities for Ψ210 , Ψ21+1 , andΨ21-1 and then show that the sum is spherically symmetric, depending only on r.

An electron is trapped in a one-dimensional infinite potential well. For what (a) higher quantum number and (b) lower quantum number is the corresponding energy difference equal to the energy difference E43 between the levels n = 4 and n = 3 ? (c) Show that no pair of adjacent levels has an energy difference equal to 2E43 .

In atoms, there is a finite, though very small, probability that, at some instant, an orbital electron will actually be found inside the nucleus. In fact, some unstable nuclei use this occasional appearance of the electron to decay by electron capture. Assuming that the proton itself is a sphere of radius 1.1×10-15mand that the wave function of the hydrogen atom’s electron holds all the way to the proton’s center, use the ground-state wave function to calculate the probability that the hydrogen atom’s electron is inside its nucleus.

An electron is trapped in a one-dimensional infinite potential well that is 100 pm wide; the electron is in its ground state. What is the probability that you can detect the electron in an interval of width centered at x = (a) 25 pm, (b) 50 pm, and (c) 90 pm? (Hint: The interval x is so narrow that you can take the probability density to be constant within it.)

You want to modify the finite potential well of Fig. 39-7 to allow its trapped electron to exist in more than four quantum states. Could you do so by making the well (a) wider or narrower, (b) deeper or shallower?

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