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Coincident spectral lines. 43According to the Rydberg formula (Equation 4.93) the wavelength of a line in the hydrogen spectrum is determined by the principal quantum numbers of the initial and final states. Find two distinct pairs{ni,nf} that yield the same λ. For example,role="math" localid="1656311200820" {6851,6409} and{15283,11687}will do it, but you're not allowed to use those!

Short Answer

Expert verified

The two distinct pairs ni,nfthat yield the same λis 35,25175,35

Step by step solution

01

Determine the Rydberg formula

The Rydberg formula is a mathematical method for calculating light wavelength. The energy of an electron varies when it moves from one atomic orbit to another.

1λ=R1nf21ni2

02

Determine the two distinct pairs

Out mission in this problem is to find the four numbers such that they produce the same spectral lines.

According to the Rydberg formula:

1λ=R1nf21ni2

It is very difficult to just guess some values.

The given numbers to find new numbers, the given pair of numbers are 6851,6409and 15283,11687.

For these two pairs, find their prime factors:

6851=13×17×316409=13×17×2915283=17×29×3111687=13×29×31

The first pair of numbers have two common factors and also the second pair have two common factors, where each member of the first pair uses one of the prime factors of the second pair, and vice versa.

The numbers can be written as:

164092-168512=1116872-1152832113×17×292-113×17×312=113×29×312-117×29×312Leta=31,b=29,c=17andd=13,thenwecanwrite:1bcd2-1acd2=1abd2-1abc2a2-b2abcd2=c2-d2abcd2a2-b2=c2-d2a+ba-b=c+dc-d

The method is to choose two prime numbers a and b, then we find the difference a2-b2after that we find the factors of the difference, from these factors we take two number and such thatc+dc-d=a2-b2

Let a=7and b=5then a2-b2=24which has factors of 1,2,3, 6,8 and 12 note that we have already used 2 and 12

Therefore a+b=12and a-b=2we pick another two numbers, say, 4 and 6 , that is:

c=5c+d=65+d=6d=6-5d=1

Substitute d=1in the above equation

c-d=4c-1=4c=4+1c=5

But :

1bcd2-1acd2=1abd2-1abc2

where the pairs are bcd,acdand abd,abc,so:

1252-1352=1352-11752

So the pairs are:

35,25175,35

Follow this method to find another pairs but you have to be careful, since not all the numbers work using this method, so you have to check your pairs.

Therefore, the two distinct pairs ni,nfthat yield the same λis35,25175,35

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Most popular questions from this chapter

An electron is at rest in an oscillating magnetic field

B=B0cos(ωt)k^

whereB0 andω are constants.

(a) Construct the Hamiltonian matrix for this system.

(b) The electron starts out (at t=0 ) in the spin-up state with respect to the x-axis (that is:χ(0)=χ+(x)). Determine X(t)at any subsequent time. Beware: This is a time-dependent Hamiltonian, so you cannot get in the usual way from stationary states. Fortunately, in this case you can solve the timedependent Schrödinger equation (Equation 4.162) directly.

(c) Find the probability of getting-h/2 , if you measure Sx. Answer:

sin2(γB02ωsin(ωt))

(d) What is the minimum field(B0) required to force a complete flip inSx ?

For the most general normalized spinor (Equation 4.139),

compute{Sx},{Sy},{Sz},{Sx2},{Sy2},and{Sx2}.checkthat{Sx2}+{Sy2}+{Sz2}={S2}.

X=(ab)=aX++bX(4.139).

[Refer to. Problem 4.59for background.] Suppose A=B02(X^-yI^) andφ=Kz2, where B0 and Kare constants.

(a) Find the fields E and B.

(b) Find the allowed energies, for a particle of mass m and charge q , in these fields, Answer: E(n1,n2)=(n1+12)ħω1+(n2+12)ħω2,(n1,n2=0,1,2,...)whereω1qB0/mandω22qK/m. Comment: If K=0this is the quantum analog to cyclotron motion;ω1 is the classical cyclotron frequency, and it's a free particle in the z direction. The allowed energies,(n1+12)ħω1, are called Landau Levels.

If the electron were a classical solid sphere, with radius

rc=e24πO0˙mc2

(the so-called classical electron radius, obtained by assuming the electron's mass is attributable to energy stored in its electric field, via the Einstein formula E=mc2), and its angular momentum is (1/2)h then how fast (in m/sm/s) would a point on the "equator" be moving? Does this model make sense? (Actually, the radius of the electron is known experimentally to be much less than5.156×1010m/src, but this only makes matters worse).

a) Check that the spin matrices (Equations 4.145 and 4.147) obey the fundamental commutation relations for angular momentum, Equation 4.134.

Sz=h2(100-1)(4.145).Sx=h2(0110),sy=h2(0-ii0)(4.147).[Sx,Sy]=ihSz,[Sy,Sz]=ihSx,[Sz,Sx]=ihSy(4.134).(b)ShowthatthePaulispinmatrices(Equation4.148)satisfytheproductruleσx(0110),σy(0-ii0),σz(100-1)(4.148).σjσk=δjk+io'IjklσI,(4.153).

Wheretheindicesstandforx,y,orz,ando'jklistheLevi-Civitasymbol:+1ifjkl=123,231,or2=312;-1ifjkl=132,213,or321;otherwise.

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