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What is the probability that an electron in the ground state of the hydrogen atom will be found between two spherical shells whose radii are r and r + ∆r, (a) if r = 0.500a and ∆r=0.010aand (b) if r = 1.00a and ∆r=0.01a, where a is the Bohr radius? (Hint: r is small enough to permit the radial probability density to be taken to be constant between r and r+∆r.)

Short Answer

Expert verified
  1. The required probability is 0.0037 .
  2. The required probability is 0.0054 .

Step by step solution

01

Describe the radial probability density for the ground state of hydrogen:

The radial probability density for the hydrogen ground state is obtained by multiplying the square of the wave function by the spherical element of the shell volume.

The radial probability density for the ground state of hydrogen is given by,

P(r)=(4r2a3)e-2r/a

Find the probability of finding the electron between two spherical shells whose radii are r and ∆r. If ∆r is small enough then write the probability as follows:

P(r)=P(r)∆rP(r)=(4r2∆ra3)e-2r/ae-2r/a

….. (1)

Here, the Bohr radius is a=52.292×10-12m.

02

(a) Define the probability if r = 0.500a and ∆r=0.010a :

Substitute 0.500a for r, 0.010a for ∆r, and 52.292×10-12m for a in equation (1).

p0.500a=40.500a20.010aa3e-2(0.500a)a=40.500a20.010e-1=0.010×0.3678=0.0037

Therefore, the required probability is 0.0037.

03

(b) Determine the probability if r = 1.00a and ∆r=0.010a :

Substitute 1.00a for r, and 0.010a for ∆rin equation (1).

p0.500a=41.00a2(0.010a)a3e-2(1.00a)a=41.00a2(0.010a)e-21.00=0.04×0.1353=0.0054

Therefore, the required probability is 0.0054.

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Most popular questions from this chapter

The wave function for the hydrogen-atom quantum state represented by the dot plot shown in Fig. 39-21, which has n = 2 and l=ml=0, is

Ψ200(r)=142πa-3/2(2-ra)e-r/2a

in which a is the Bohr radius and the subscript onΨ(r)gives the values of the quantum numbers n,l,ml. (a) PlotΨ(2002r)and show that your plot is consistent with the dot plot of Fig. 39-21. (b) Show analytically thatΨ(2002r)has a maximum at r=4a. (c) Find the radial probability densityP200(r)for this state. (d) Show that

∫0∞P200(r)dr=1

and thus that the expression above for the wave function Ψ200(r)has been properly normalized.

Schrodinger’s equation for states of the hydrogen atom for which the orbital quantum number l is zero is

1r2ddr(r2dψdr)+8ττ2mr2[E-Ur]ψ=0

Verify that Eq. 39-39, which describes the ground state of the hydrogen atom, is a solution of this equation?

In a simple model of a hydrogen atom, the single electron orbits the single proton (the nucleus) in a circular path. Calculate

  1. The electric potential set up by the proton at the orbital radius of52.0 pm
  2. The electric potential energy of the atom,
  3. The kinetic energy of the electron.
  4. How much energy is required to ionize the atom (that is, to remove the electron to an infinite distance with no kinetic energy)? Give the energies in electron-volts.

Calculate the radial probability density P(r) for the hydrogen atom in its ground state at (a) r = 0 , (b) r = a , and (c) r = 2a, where a is the Bohr radius.

For what value of the principal quantum number n would the effective radius, as shown in a probability density dot plot for the hydrogen atom, be 1.00 mm? Assume that has its maximum value of n-1. (Hint:See Fig.39-24.)

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