Chapter 8: Q50E (page 342)
Determine the expected valence of the element with atomic number 117.
Short Answer
The expected valence of the element with atomic numberis or .
Chapter 8: Q50E (page 342)
Determine the expected valence of the element with atomic number 117.
The expected valence of the element with atomic numberis or .
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Get started for freeQuestion: As the 2p levels fill from Z = 5 to 10 the element's first ionization energies tend to increase. But as the figure below clearly indicates it is slightly easier to remove an electron from Z = 8 oxygen than from Z = 7 nitrogen. What might explain this?
Question: In classical electromagnetism, the simplest magnetic dipole is a circular current loop, which behaves in a magnetic field just as an electric dipole does in an electric field. Both experience torques and thus have orientation energies -p.Eand(a) The designation "orientation energy" can be misleading. Of the four cases shown in Figure 8.4 in which would work have to be done to move the dipole horizontally without reorienting it? Briefly explain. (b) In the magnetic case, using B and u for the magnitudes of the field and the dipole moment, respectively, how much work would be required to move the dipole a distance dx to the left? (c) Having shown that a rate of change of the "orientation energy'' can give a force, now consider equation (8-4). Assuming that B and are general, writein component form. Then, noting thatis not a function of position, take the negative gradient. (d) Now referring to the specific magnetic field pictured in Figure 8.3 which term of your part (c) result can be discarded immediately? (e) Assuming thatandvary periodically at a high rate due to precession about the z-axis what else may be discarded as averaging to 0? (f) Finally, argue that what you have left reduces to equation (8-5).
Figureshows the Stern-Gerlach apparatus. It reveals that spin-particles have just two possible spin states. Assume that when these two beams are separated inside the channel (though still near its centreline). we can choose to block one or the other for study. Now a second such apparatus is added after the first. Their channels are aligned. But the second one is rotated about the-axis by an angle \(\phi\) from the first. Suppose we block the spin-down beam in the first apparatus, allowing only the spin-up beam into the second. There is no wave function for spin. but we can still talk of a probability amplitude, which we square to give a probability. After the first apparatus' spin-up beam passes through the second apparatus, the probability amplitude iswhere the arrows indicate the two possible findings for spin in the second apparatus.
(a) What is the probability of finding the particle spin up in the second apparatus? Of finding it spin down? Argue that these probabilities make sense individually for representative values ofand their sum is also sensible.
(b) By contrasting this spin probability amplitude with a spatial probability amplitude. Such as. Argue that although the arbitrariness ofgives the spin cases an infinite number of solves. it is still justified to refer to it as a "two-state system," while the spatial case is an infinite-state system.
To investigate the claim that lowerimplies lower f energy. consider a simple case: lithium. which has twoelectrons and alonevalence electron.
(a)First find the approximate orbit radius, in terms of. of anelectron orbiting three protons. (Refer to Section 7.8.)
(b) Assuming theelectrons shield/cancel out two of the protons in lithium's nucleus, the orbit radius of anelectron orbiting a net charge of just.
(c) Argue that lithium's valence electron should certainly have lower energy in a 25 state than in astale. (Refer Figure 7.15.)
Assume that the spin-orbit interaction is not overwhelmed by an external magnetic field what isthe minimum angle the total angular momentum vector may make with the z -axis in a3state of hydrogen?
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