A hydrogen atom in its ground state is subjected to an external magnetic field of 1.0 T. What is the energy difference between the spin-up and spin-down states?

Short Answer

Expert verified

The energy difference between the spin-up and spin-down states is1.16×10-4eV

Step by step solution

01

Definition of external magnetic field

External magnetic field(s)" aremagnetic fields that affect an electron microscope from the outside. Measures to prevent an adverse influence of the external magnetic fields on the instrument performance are needed.

02

Aim of the question

This question wants us to calculate the difference in energy between the spin-up and spin-down states when a hydrogen atom in the ground state is subjected to a 1.0 T magnetic field.

03

Determine the orientation energy equation

The energy U due to an applied magnetic field is.-μ.BIf we takeB to be in the z directionBZ, then U=-μzB.

From equations, we get the orientation energy as follows

U=ememshB (1)

Where μz=-ememsh, and msis the spin quantum number.

04

Find a formula to know the energy difference

Knowing that of an electron can only have two values; 12for spin-up and -12for a spindown, then the difference in energy can be calculated as follows using equation (1)

ΔU=e2mehB--e2mehB=e2mehB+e2mehB=emehB.....................(2)

05

Calculate the energy difference

Substituting the known values of the constants and B=1.0 T in equation (2), we get

ΔU=1.6×10-19C9.1×10-31kg1.055×10-34J·s1.0T=1.855×10-23J1eV1.6×10-19J=1.16×10-4eV

Therefore the energy difference between the spin-up and spin-down states is1.16×10-4eV

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Most popular questions from this chapter

Exercise 45 refers to state I and II and put their algebraic sum in a simple form. (a) Determine algebraic difference of state I and state II.

(b) Determine whether after swapping spatial state and spin state separately, the algebraic difference of state I and state II is symmetric, antisymmetric or neither, and to check whether the algebraic difference becomes antisymmetric after swapping spatial and spin states both.

The Kαline in copper is a very common one to use in X-ray crystallography. To produce it, electrons are accelerated through a potential difference and smashed into a copper target. Section 7.8 gives the energies in a hydrogen like atom asZ2(-13.6eV/n2) . Making the reasonable approximation that ann=1 electron in copper orbits the nucleus and half of its fellow n=1electron, being unaffected by the roughly spherical cloud of other electrons around it. Estimate the minimum accelerating potential needed to make a hole in copper'sKshell.

Suppose that the channel’s outgoing end is in the hydrogen l=0Stem-Gerlach apparatus of the figure. You place a second such apparatus whose channel is aligned with the first but rotated 90°about the x-axis, so that its B –field lines point roughly in the y-direction instead of the. What would you see emerging at the end of your added apparatus? Consider the behavior of the spin-up and spin-down beams separately. Assume that when these beams are separated in the first apparatus, we can choose to block one or the other for study, but also assume that neither deviates too far from the center of the channel.

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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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