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A hydrogen atom in a state having a binding energy (the energy required to remove an electron) of 0.85 eV makes a transition to a state with an excitation energy (the difference between the energy of the state and that of the ground state) of 10.2eV. (a) What is the energy of the photon emitted as a result of the transition? What are the (b) higher quantum number and (c) lower quantum number of the transition producing this emission?

Short Answer

Expert verified

a) The energy of the photon emitted is .

b) The higher quantum number is .

c) The lower quantum number is .

Step by step solution

01

Describe the expression for the energy of the hydrogen atom for the nth state.

The expression for energy of the hydrogen atom for the nthstate is given by,

En=(-13.6eV)1n2

The expression for the energy of the hydrogen atom for the lower excited state is given by,

E1=(-13.6eV)1n12 ….. (1)

The expression for the energy of the hydrogen atom for the higher excited state is given by,

E2=(-13.6eV)1n22 ….. (2)

02

(a) Define the energy of the photon emitted as a result of the transition:

Given that, the excitation energy is 10.2 eV and the ground state energy of the hydrogen atom is -13.6 eV. The initial energy of the hydrogen atom is equal to the sum of the energy of the ground state energy and the excitation energy.

E1=-13.6eV+10.2eV=-3.4eV

The difference between the final energy of the atom and the initial energy of the atom energy is equal to the energy of the emitted photon.

Ephoton=E2-E1=-0.85eV--3.4eV=2.55eV

Therefore, the energy of the photon emitted is 2.55.

03

(b) Define the higher quantum number:

Rearrange the equation (1) as below.

n1=-13.6eVE1

Substitute -0.85 eV for E1in the above equation.

n1=-13.6eV-0.85eV=4

Therefore, the higher quantum number is 4.

04

(c) Calculate the higher quantum number:

Rearrange the equation (1).

n1=-13.6eVE1

Substitute -3.4 eV for E1in the above equation.

n2=-13.6eV-3.4eV=2

Hence, the lower quantum number is 2 .

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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.

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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.)

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.

What is the probability that in the ground state of hydrogen atom , the electron will be found at a radius greater than the Bohr radius?

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