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Question: In the Stern-Gerlach experiment how much would a hydrogen atom emanating from a 500 K oven(KE=32kBT)be deflected in traveling 1 m through a magnetic field whose rate of change is 10 T/m?

Short Answer

Expert verified

Answer

The emanating displacement of a hydrogen atom isS=2.2x10-3m

Step by step solution

01

Definition of kinetic energy

The kinetic energy is the measure of the work that an object does by virtue of its motion.

02

Determine the speed of the travel

As we know the kinetic energy (KE) is given by

KE=12mv2=32kBT

Here mass of the proton, kB=1.38×10-23J/K, and T= 500K

Therefore,

12mv2=121.67×10-27kgv232kBT=32×1.38×10-23×500K

Comparing the above two expressions,we get

121.67×10-27kgv2=32×1.38×10-23J/K×500Kv=3×1.38×10-23J/K500K1.67×10-27kgv=3.52×103m/s

Which gives the speed of travel 3.52 x 103m/s

03

Calculate the time taken by the hydrogen atom

Now the time taken by the H-atom to travel 1 m distance at this speed is

t=distancespeed=1m3.52×103m/s=2.84×10-4s

04

Determine the force and acceleration

Now according to the equation, the z-component of force on the H-atom by the field is

Fz=-emeSzBzz

Here,Sz=ms;andms=-s,...,+s

e=1.6×10-19C=h2π=1.05×10-34J·sme=9.1×10-31kgBzz=10T/m

Therefore, by substituting the aboveexpression, we get the force is

Fz=1.6×10-19C9.1×10-31kg×12×1.05×10-34J·s×10=9.23×10-23N

As we know the acceleration is

a=Fzm=9.23×10-23N6.67×10-27kg=5.55×104

05

Find the emerging displacement of the hydrogen atom

Now the displacement is

S=ut+12at2=125.55×1042.84×10-4s2=2.2×10-3m

Here the initial velocity u = 0

Therefore the displacement is 2.2×10-3m

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Most popular questions from this chapter

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.

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Consider row 4 of the periodic table. The trend is that the4xsubshell fills. Then the 3d, then the 4p.

(a) Judging by adherence to and deviation from this trend, whit might be said of the energy difference between the 4sand 3drelative to that between the 3dand 4p?

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