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A hydrogen atom starts out in the following linear combination of the stationary states n=2, l=1, m=1 and n=2, l=1, m=-1.

ψ(r,0)=12(ψ211+ψ21-1)

(a) Constructψ(r,t)Simplify it as much as you can.

(b) Find the expectation value of the potential energy,<V>. (Does it depend on t?) Give both the formula and the actual number, in electron volts.

Short Answer

Expert verified

(a) The value of ψr,tis -12πa4a2re-r/2αsinθsinϕe-iE2t/h.

(b) The expectation value of the potential energy is -6.8eV.

Step by step solution

01

Definition of potential energy

The output of the movement of the electrons in a molecule defines the potential energy. The energy that holds the atom in the covalent bond is known as potential energy.

02

(a) Construction of ψ(r,t)

Consider a hydrogen atom which starts out at t=0 in the following linear combination of the stationary states n=2.l=1,m=1 and n=2,l=1,m=-1 that is expressed as follows,

ψr,0=12ψ211+ψ21-1 …(i)

Write the required expressions from problem 4.11.

ψ211=-18πra5/2e-r/2asinθeψ21-1=-18πra5/2e-r/2asinθe-

Constructψr,t that is wavefunction at t, multiply equation (i) by e-iE2t/h.

ψr,t=12ψ211+ψ21-1eiE2t/h

Write the expression for the energy of both data-custom-editor="chemistry" ψ211and data-custom-editor="chemistry" ψ21-1which is same.

E2=E1n2=E14=-h28ma2

Adddata-custom-editor="chemistry" ψ211 and data-custom-editor="chemistry" ψ21-1.

data-custom-editor="chemistry" ψ211+ψ21-1=1πa18a2re-r/2asinθe-e-

Usedata-custom-editor="chemistry" e-e-=2isinϕ in the above expression.

ψ211+ψ21-1=-iπa4a2re-r/2asinθsin(ϕ)

Thus, the value of data-custom-editor="chemistry" ψr,tis -i2πa4a2re-r/2αsinθsinϕe-iE2t/h.

03

(b) Determination of the expectation value of potential energy (V)

Write the expression for the expected value of the potential energy.

V=ψ2Vd3r

Write the value of the potential energy of the electron in the hydrogen atom.

V=-e4πε01r

Substitute the above value in the expression of expected value of the potential energy.

data-custom-editor="chemistry" V=ψ2-e4πε01rd3r

From part (a) determine the modulus square of the wave function.

ψ2=12πa16a4r2e-r/asin2θsin2ϕ

Substitute the above value in the expression of expected value of the potential energy.

ψ2=12πa16a4-e24πε0r2e-r/asin2θsin2ϕ1rr2sinθdrdθdϕ=132πa5-h2ma20r2e-r/adr0πsin3θdθ02πsin2ϕdϕ=h232πma63!a443π=h24ma2

Simplify the above expression.

V=12E1=12-13.6eV=-6.8eV

Thus, the expectation value of the potential energy is -6.8eV.

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Most popular questions from this chapter

Suppose two spin -1/2particles are known to be in the singlet configuration (Equation Let Sa(1)be the component of the spin angular momentum of particle number 1 in the direction defined by the unit vectora^ Similarly, letSb(2) be the component of 2’s angular momentum in the directionb^ Show that

Sa(1)Sb(2)=-24cosθ

where θ is the angle between a^ andb^

Quarks carry spin 1/2. Three quarks bind together to make a baryon (such as the proton or neutron); two quarks (or more precisely a quark and an antiquark) bind together to make a meson (such as the pion or the kaon). Assume the quarks are in the ground state (so the orbital angular momentum is zero).

(a) What spins are possible for baryons?

(b) What spins are possible for mesons?

Find the matrix representingSxfor a particle of spin3/2 (using, as

always, the basis of eigenstates ofSz). Solve the characteristic equation to

determine the eigenvalues ofSx.

Use equations 4.27 4.28 and 4.32 to constructy00,y21Check that they are normalized and orthogonal

An electron is at rest in an oscillating magnetic field

B=B0cos(ωt)k^

whereB0 andω are constants.

(a) Construct the Hamiltonian matrix for this system.

(b) The electron starts out (at t=0 ) in the spin-up state with respect to the x-axis (that is:χ(0)=χ+(x)). Determine X(t)at any subsequent time. Beware: This is a time-dependent Hamiltonian, so you cannot get in the usual way from stationary states. Fortunately, in this case you can solve the timedependent Schrödinger equation (Equation 4.162) directly.

(c) Find the probability of getting-h/2 , if you measure Sx. Answer:

sin2(γB02ωsin(ωt))

(d) What is the minimum field(B0) required to force a complete flip inSx ?

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