1000 Solved Problems in Modern Physics

(Grace) #1

1.3 Solutions 81


(b)B(x)=

N!pxqN−x
x!(N−x)!

=

N(N−1)...(N−x−1)px(1−p)N−x
x!

=

N(N−1)...(N−x+1)(Np)x(1−p)N−x
Nxx!

=

mx
x!

(

1 −

1

N

)(

1 −

2

N

)

···

(

1 −

x− 1
N

)

(1−p)N−x

=

mx
x!

(

1 −N^1

)(

1 −N^2

)

···

(

1 −x−N^1

)

(1−p)N
(1−p)x
The poisson distribution can be deduced as a limiting case of the bino-
mial distribution, for those random processes in which the probability of
occurrence is very small,p1, while the number of trialsNbecomes
very large and the mean valuem=pnremains fixed. ThenmNand
xN, so that approximately
(1−p)N−x≈e−p(N−x)≈e−pN=e−m
ThusB(x)→P(x)=e

−mmx
x!

1.97 S=(g−b)±


g
tg

+

b
tb

t=tb+tg=constant
tg=t−tb

σ^2 =σg^2 +σb^2 =

g
t−tb

+

b
tb
must be minimum. Therefore,∂(σ

(^2) )
∂tb =^0
g
(t−tb)^2



b
tb^2

= 0

tb^2
(t−tb)^2

=

b
g


tb
tg

=


b
g

1.98 A=A 0 e−λt

ln

(

A 0

A

)

=λt

y=λt
S=y−λt
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