4.16.2 Problem 1
Solution:
We start with the solution we already
obtained for \(E(Y_{i})\) which is
\[ E\left ( Y_{i}\right ) =1+{\displaystyle \sum \limits _{k=1}^{i-1}} E\left ( Y_{k}\right ) P_{ik}\]
Let \(E\left ( Y_{i}\right ) =x_{i}\) hence the above can be written as
\[ x_{i}=1+{\displaystyle \sum \limits _{k=1}^{i-1}} x_{k}P_{ik}\]
But \(P_{ik}=\frac {1}{i}\) then the above
becomes
\[ x_{i}=1+\frac {1}{i}{\displaystyle \sum \limits _{k=1}^{i-1}} x_{k}\]
Multiply by \(i\) the above becomes
\[ i\ x_{i}=i+{\displaystyle \sum \limits _{k=1}^{i-1}} x_{k}\]
Therefore, we obtain the following equations for
\(i=1\cdots r\)
For \(i=1\)
\begin{equation} x_{1}=1 \tag {1}\end{equation}
For \(i=2\)
\begin{equation} 2x_{2}=2+x_{1} \tag {2}\end{equation}
For \(i=3\)
\begin{equation} 3x_{3}=3+x_{1}+x_{2} \tag {3}\end{equation}
For \(i=4\)
\begin{equation} 4x_{4}=4+x_{1}+x_{2}+x_{3} \tag {4}\end{equation}
etc...
Now evaluate (2)-(1) and (3)-(2) and (4)-(3), etc... we obtain the following equations
(2)-(1) gives
\begin{align} 2x_{2}-x_{1} & =2+x_{1}-1\nonumber \\ x_{2} & =\frac {1+2x_{1}}{2} \tag {5}\end{align}
(3)-(2) gives
\begin{align*} 3x_{3}-2x_{2} & =3+x_{1}+x_{2}-2-x_{1}\\ 3x_{3}-2x_{2} & =1+x_{2}\\ x_{3} & =\frac {1+3x_{2}}{3}\end{align*}
etc... Hence we see that for the \(r^{th}\) term we obtain
\begin{equation} x_{r}=\frac {1+r\ x_{r-1}}{r}\nonumber \end{equation}
Hence
\begin{equation} x_{r}=\frac {1}{r}+x_{r-1} \tag {6}\end{equation}
Now replace \(r\) by \(r-1\) in the above we obtain
\[ x_{r-1}=\frac {1}{r-1}+x_{r-2}\]
replace the above in (6) we obtain
\begin{equation} x_{r}=\frac {1}{r}+\left ( \frac {1}{r-1}+x_{r-2}\right ) \tag {7}\end{equation}
And again, in the above, \(x_{r-2}=\frac {1}{r-2}+x_{r-3\text { }}\)hence (7) becomes
\begin{equation} x_{r}=\frac {1}{r}+\left ( \frac {1}{r-1}+\left ( \frac {1}{r-2}+x_{r-3\text { }}\right ) \right ) \tag {8}\end{equation}
and so on, until
we get to \(x_{1}=1\), hence we obtain
\[ \fbox {$x_{r}=\frac {1}{r}+\frac {1}{r-1}+\frac {1}{r-2}+\cdots +1$}\]
Hence
\[ x_{r}={\displaystyle \sum \limits _{k=1}^{r}} \frac {1}{k}\]
Which is the harmonic series. Now, it is known
that
Please see http://en.wikipedia.org/wiki/Harmonic_number
\[ \lim _{r\rightarrow \infty }x_{r}=\log \left ( r\right ) -\gamma \]
Where \(\gamma \) is Euler Gamma constant
given by
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