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

Question: Early on, the lanthanides were found to be quite uncooperative when attempts were made to chemically separate them from one another. One reason can be seen in Figure 8.16. Explain.

What is the angle between Land Sin a (a) 2p3/2and(b) 2p1/2 state of hydrogen?

Question: Concisely, why is the table periodic?

Exercise 44 gives an antisymmetric multiparticle state for two particles in a box with opposite spins. Another antisymmetric state with spins opposite and the same quantum numbers is ψn(x1)n2(x2)ψnn(x1)ψn(x2)

Refer to these states as 1 and 11. We have tended to characterize exchange symmetry as to whether the state's sign changes when we swap particle labels. but we could achieve the same result by instead swapping the particles' stares, specifically theandin equation (8-22). In this exercise. we look at swapping only parts of the state-spatial or spin.

(a) What is the exchange symmetric-symmetric (unchanged). antisymmetric (switching sign). or neither-of multiparticle states 1 and Itwith respect to swapping spatial states alone?

(b) Answer the same question. but with respect to swapping spin states/arrows alone.

(c) Show that the algebraic sum of states I and II may be written(ψn(x1)ψn'(x2)ψn'(x1)ψn(x2))(+)

Where the left arrow in any couple represents the spin of particle 1 and the right arrow that of particle?

(d) Answer the same questions as in parts (a) and (b), but for this algebraic sum.

(e) ls the sum of states I and 11 still antisymmetric if we swap the particles' total-spatial plus spin-states?


(f) if the two particles repel each other, would any of the three multiparticle states-l. II. and the sum-be preferred?

Explain.

The Slater determinant is introduced in Exercise 42. Show that if states n and n'of the infinite well are occupied. with the particle in state n being spin up and the one in being spin down. then the Slater determinant yields the antisymmetric multiparticle state: ψn(x1)ψn'(x2)ψm2(x1)ψn(x2).

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