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An electron is in anI = 3state of the hydrogen atom, what possible angles might the angular momentum vector make with the z-axis.

Short Answer

Expert verified

The possible angles that the angular momentum vector makes with the z-axis are

=150,125.3,106.8,90,73.2,54.7,30..

Step by step solution

01

Value of Angular momentum:

The azimuthal quantum number defines the orbital angular momentum and the shape of the orbital. While magnetic quantum number determines the orientation of the orbital in space.

Consider the given data as below.

I = 3

As you know, angular momentum = L = L=I(I+I)h

Where, is the Azimuthal Quantum number and Plank鈥檚 constant that is 1.05510-34J.s..

Here, if I = 3 the angular momentum is,

role="math" localid="1659324698388" L=33+1h=12hL=3.46h.........(1)

02

Values of  Lz  (z  – component of angular momentum):

If : I = 3

Thenthe magnetic quantum number is,

ml=0,123

Hence, possible z-components are,

Lz=0,h,2h,3h

03

Conclusion:

You will be finding all the possible angles using the below equation

Lz=L肠辞蝉胃 鈥.. (3)

Where, is the angle of angular momentum vector from z- axis.

Now, by using equations (1) and (2) in equation (3), you get the following.

Substitute 3.46h for L and 0 for Lzinto equation (3), so the angle is,

localid="1659325137879" 0=3.46hcoscos=0=cos-1(0)=90

Substitute 3.46 for L and h for Lzinto equation (3), so the angle is,

localid="1659325202540" h=3.46hcoscos=0.289=cos-1(0.289)=73.2

Substitute 3.46h for L and -h for Lzinto equation (3), so the angle is,

-h=3.46hcoscos=-0.289=cos-1(-0.289)=106.8

Substitute 3.46h for L and 2h for Lzinto equation (3), so the angle is,

2h=3.46hcoscos=0.578=cos-1(0.578)=54.7

Substitute 3.46h for L and -2h for Lzinto equation (3), so the angle is,

2h=3.46hcoscos=0.578=cos-1(0.578)=125.3

Substitute 3.46h for L and 3h for Lzinto equation (3), so the angle is,

3h=3.46hcoscos=-0.867=cos-1(0.867)=30

Substitute 3.46h for L and -3h for Lzinto equation (3), so the angle is,

-3h=3.46hcoscos=-0.867=cos-1(-0.867)=150

Hence, the possible angles that the angular momentum vector makes with the z-axis are =150,125.3,106.8,90,73.2,54.7,30..

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Most popular questions from this chapter

Verify that the solution given in equation (7.6) satisfy differential equations (7.5) as well as the required boundary conditions.

Classically, it was expected that an orbiting electron would emit radiation of the same frequency as its orbit frequency. We have often noted that classical behaviour is observed in the limit of large quantum numbers. Does it work in this case? (a) Show that the photon energy for the smallest possible energy jump at the 鈥渓ow-n-end鈥 of the hydrogen energies is 3|E0|/n3, while that for the smallest jump at the 鈥渉igh-n-end鈥 is 2|E0|/n3, where E0is hydrogen鈥檚 ground-state energy. (b) Use F=ma to show that the angular velocity of a classical point charge held in orbit about a fixed-point charge by the coulomb force is given by =e2/4蟺蔚0mr3. (c) Given that r=n2a0, is this angular frequency equal to the minimum jump photon frequency at either end of hydrogen鈥檚 allowed energies?

Calculate the electric dipole moment p and estimate the transition time for a hydrogen atom electron making an electric dipole transition from the

(n,l,m)=(3,2,0)to the (2,1,0) state.

Roughly, how does the size of a triply ionized beryllium ion compare with hydrogen?

The only visible spectral lines of hydrogen are four Balmer series lines noted at the beginning of Section 7.3. We wish to cause hydrogen gas to glow with its characteristic visible colors.

(a) To how high an energy level must the electrons be exited?

(b) Energy is absorbed in collisions with other particles. Assume that after absorbing energy in one collision, an electron jumps down through lower levels so rapidly that it is in the ground state before another collision occurs. If an electron is to be raised to the level found in part (a), how much energy must be available in a single collision?

(c) If such energetic collisions are to be affected simply by heating the gas until the average kinetic energy equals the desired upward energy jump, what temperature would be required? (This explains why heating is an impractical way to observe the hydrogen spectrum. Instead, the atoms are ionized by strong electric fields, as is the air when a static electric spark passes through.)

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