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How many different 3d states are there? What physical property (as opposed to quantum number) distinguishes them, and what different values may this property assume?

Short Answer

Expert verified

There are five states in the case of 3d states.

The angular momentum could be 0 or±h or±2h .

Step by step solution

01

Given data

The principal quantum number, n = 3, and the subshell is d.

02

To find different 3d states and angular momentum

The state 3d means principal quantum number n = 3 , the azimuthal quantum number l=n-1=2 so that magnetic quantum number ml, can take values from -l to +l as -2, -1, 0, 1 2.

So, there are five states.

The states that have differentrole="math" localid="1659781123812" ml have different orbits and electron probability densities. They have different angular momentum in the z-direction, that isLz=mih .

The angular momentum could be 0 or±h or±2h .

03

Conclusion

There are five states in the case of 3d states.

The angular momentum could be 0 or±h or±2h

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Most popular questions from this chapter

Consider a cubic 3D infinite well.

(a) How many different wave functions have the same energy as the one for which (nx,ny,nz)=(5,1,1)?

(b) Into how many different energy levels would this level split if the length of one side were increased by 5% ?

(c) Make a scale diagram, similar to Figure 3, illustrating the energy splitting of the previously degenerate wave functions.

(d) Is there any degeneracy left? If so, how might it be “destroyed”?

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

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

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.)

(a) What is the expectation value of the distance from the proton of an electron in a 3p state? (b) How does this compare with the expectation value in the 3 d state, calculated in Example 7.7? Discuss any differences.

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