$\newcommand{\br}{\\}$ $\newcommand{\R}{\mathbb{R}}$ $\newcommand{\Q}{\mathbb{Q}}$ $\newcommand{\Z}{\mathbb{Z}}$ $\newcommand{\N}{\mathbb{N}}$ $\newcommand{\C}{\mathbb{C}}$ $\newcommand{\P}{\mathbb{P}}$ $\newcommand{\F}{\mathbb{F}}$ $\newcommand{\L}{\mathcal{L}}$ $\newcommand{\spa}[1]{\text{span}(#1)}$ $\newcommand{\dist}[1]{\text{dist}(#1)}$ $\newcommand{\max}[1]{\text{max}(#1)}$ $\newcommand{\min}[1]{\text{min}(#1)}$ $\newcommand{\supr}[1]{\text{sup}(#1)}$ $\newcommand{\infi}[1]{\text{inf}(#1)}$ $\newcommand{\ite}[1]{\text{int}(#1)}$ $\newcommand{\ext}[1]{\text{ext}(#1)}$ $\newcommand{\bdry}[1]{\partial #1}$ $\newcommand{\argmax}[1]{\underset{#1}{\text{argmax }}}$ $\newcommand{\argmin}[1]{\underset{#1}{\text{argmin }}}$ $\newcommand{\set}[1]{\left\{#1\right\}}$ $\newcommand{\emptyset}{\varnothing}$ $\newcommand{\tilde}{\text{~}}$ $\newcommand{\otherwise}{\text{ otherwise }}$ $\newcommand{\if}{\text{ if }}$ $\newcommand{\proj}{\text{proj}}$ $\newcommand{\union}{\cup}$ $\newcommand{\intercept}{\cap}$ $\newcommand{\abs}[1]{\left| #1 \right|}$ $\newcommand{\norm}[1]{\left\lVert#1\right\rVert}$ $\newcommand{\pare}[1]{\left(#1\right)}$ $\newcommand{\brac}[1]{\left[#1\right]}$ $\newcommand{\t}[1]{\text{ #1 }}$ $\newcommand{\head}{\text H}$ $\newcommand{\tail}{\text T}$ $\newcommand{\d}{\text d}$ $\newcommand{\limu}[2]{\underset{#1 \to #2}\lim}$ $\newcommand{\der}[2]{\frac{\d #1}{\d #2}}$ $\newcommand{\derw}[2]{\frac{\d #1^2}{\d^2 #2}}$ $\newcommand{\pder}[2]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\pderw}[2]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\pderws}[3]{\frac{\partial^2 #1}{\partial #2 \partial #3}}$ $\newcommand{\inv}[1]{{#1}^{-1}}$ $\newcommand{\inner}[2]{\langle #1, #2 \rangle}$ $\newcommand{\nullity}[1]{\text{nullity}(#1)}$ $\newcommand{\rank}[1]{\text{rank }#1}$ $\newcommand{\nullspace}[1]{\mathcal{N}\pare{#1}}$ $\newcommand{\range}[1]{\mathcal{R}\pare{#1}}$ $\newcommand{\var}[1]{\text{var}\pare{#1}}$ $\newcommand{\cov}[2]{\text{cov}(#1, #2)}$ $\newcommand{\tr}[1]{\text{tr}(#1)}$ $\newcommand{\oto}{\text{ one-to-one }}$ $\newcommand{\ot}{\text{ onto }}$ $\newcommand{\ceil}[1]{\lceil#1\rceil}$ $\newcommand{\floor}[1]{\lfloor#1\rfloor}$ $\newcommand{\Re}[1]{\text{Re}(#1)}$ $\newcommand{\Im}[1]{\text{Im}(#1)}$ $\newcommand{\dom}[1]{\text{dom}(#1)}$ $\newcommand{\fnext}[1]{\overset{\sim}{#1}}$ $\newcommand{\transpose}[1]{{#1}^{\text{T}}}$ $\newcommand{\b}[1]{\boldsymbol{#1}}$ $\newcommand{\None}[1]{}$ $\newcommand{\Vcw}[2]{\begin{bmatrix} #1 \br #2 \end{bmatrix}}$ $\newcommand{\Vce}[3]{\begin{bmatrix} #1 \br #2 \br #3 \end{bmatrix}}$ $\newcommand{\Vcr}[4]{\begin{bmatrix} #1 \br #2 \br #3 \br #4 \end{bmatrix}}$ $\newcommand{\Vct}[5]{\begin{bmatrix} #1 \br #2 \br #3 \br #4 \br #5 \end{bmatrix}}$ $\newcommand{\Vcy}[6]{\begin{bmatrix} #1 \br #2 \br #3 \br #4 \br #5 \br #6 \end{bmatrix}}$ $\newcommand{\Vcu}[7]{\begin{bmatrix} #1 \br #2 \br #3 \br #4 \br #5 \br #6 \br #7 \end{bmatrix}}$ $\newcommand{\vcw}[2]{\begin{matrix} #1 \br #2 \end{matrix}}$ $\newcommand{\vce}[3]{\begin{matrix} #1 \br #2 \br #3 \end{matrix}}$ $\newcommand{\vcr}[4]{\begin{matrix} #1 \br #2 \br #3 \br #4 \end{matrix}}$ $\newcommand{\vct}[5]{\begin{matrix} #1 \br #2 \br #3 \br #4 \br #5 \end{matrix}}$ $\newcommand{\vcy}[6]{\begin{matrix} #1 \br #2 \br #3 \br #4 \br #5 \br #6 \end{matrix}}$ $\newcommand{\vcu}[7]{\begin{matrix} #1 \br #2 \br #3 \br #4 \br #5 \br #6 \br #7 \end{matrix}}$ $\newcommand{\Mqw}[2]{\begin{bmatrix} #1 & #2 \end{bmatrix}}$ $\newcommand{\Mqe}[3]{\begin{bmatrix} #1 & #2 & #3 \end{bmatrix}}$ $\newcommand{\Mqr}[4]{\begin{bmatrix} #1 & #2 & #3 & #4 \end{bmatrix}}$ $\newcommand{\Mqt}[5]{\begin{bmatrix} #1 & #2 & #3 & #4 & #5 \end{bmatrix}}$ $\newcommand{\Mwq}[2]{\begin{bmatrix} #1 \br #2 \end{bmatrix}}$ $\newcommand{\Meq}[3]{\begin{bmatrix} #1 \br #2 \br #3 \end{bmatrix}}$ $\newcommand{\Mrq}[4]{\begin{bmatrix} #1 \br #2 \br #3 \br #4 \end{bmatrix}}$ $\newcommand{\Mtq}[5]{\begin{bmatrix} #1 \br #2 \br #3 \br #4 \br #5 \end{bmatrix}}$ $\newcommand{\Mqw}[2]{\begin{bmatrix} #1 & #2 \end{bmatrix}}$ $\newcommand{\Mwq}[2]{\begin{bmatrix} #1 \br #2 \end{bmatrix}}$ $\newcommand{\Mww}[4]{\begin{bmatrix} #1 & #2 \br #3 & #4 \end{bmatrix}}$ $\newcommand{\Mqe}[3]{\begin{bmatrix} #1 & #2 & #3 \end{bmatrix}}$ $\newcommand{\Meq}[3]{\begin{bmatrix} #1 \br #2 \br #3 \end{bmatrix}}$ $\newcommand{\Mwe}[6]{\begin{bmatrix} #1 & #2 & #3\br #4 & #5 & #6 \end{bmatrix}}$ $\newcommand{\Mew}[6]{\begin{bmatrix} #1 & #2 \br #3 & #4 \br #5 & #6 \end{bmatrix}}$ $\newcommand{\Mee}[9]{\begin{bmatrix} #1 & #2 & #3 \br #4 & #5 & #6 \br #7 & #8 & #9 \end{bmatrix}}$
Theorem : Expectation and Variance of the Sum of a Random Number of Independent Random Variables

Consider the sum, where $N$ is a random variable that takes nonnegative integer values, and $X_1, X_2, …, X_n$ are identically distributed random variables. Assume that $N, X_1, X_2, …, X_n$ are independent.

$$Y = X_1, X_2, …, X_N$$

Then

$$E[Y] = E[N] E[X] $$

$$\var{Y} = E[N] \var{X} + (E[X])^2 \var{N} $$

Proof
  </span>
</span>
<span class="proof__expand"><a>[expand]</a></span>

Fix a $n > 0$. The random variable $X_1 + … + X_n$ is independent of $N$ and, therefore, independent of $\set{ N = n } $. Hence,

$$\begin{align*} E [ Y | N = n ] &= E [ X_1 + … + X_N | N = n] \br &= E [ X_1 + … + X_n | N = n ] \br &= E [ X_1 + … + X_n ] \br &= n E [ X ] \end{align*}$$

This is true for all $n > 0$, so

$$E [ Y | N ] = N E [ X ] $$

Using the law of iterated expectations, we obtain

$$E[Y] = E[E[Y|N]] = E[NE[X]] = E[N]E[X]$$

Proof
  </span>
</span>
<span class="proof__expand"><a>[expand]</a></span>

Similarly,

$$\begin{align*} \var{ Y | N = n } &= \var{ X_1 + … + X_N | N = n } \br &= \var{ X_1 + … + X_n } \br &= n \var{ X } \end{align*}$$

This is true for all $n > 0$, so

$$\begin{align*} \var{ Y } &= E [ \var{ Y | N } ] + \var{ E [ Y | N ] } \br &= E [ N \var{ X } ] + \var{ N E[X] } \br &= E [ N ] \var{ X } + \pare{E [ X ]}^2 \var{ N } \end{align*}$$

Properties: The Sum of a Random Number of Independent Random Variables

Let $X_1, X_2, …, X_n$

Example: Sum of a geometric number of independent geometric random variables

We let $N$ be geometrically distributed with parameter $p$. We also let each random variable $X_i$ be geometrically distributed with parameter $q$. We assume that all of these random variables are independent. Let $Y = X_1, X_2, …, X_n$. We have

$$M_N(s) = \frac{ p e^s }{ 1 - (1 - p) e^s }, M_X(s) = \frac{ q e^s }{ 1 - (1 - q) e^s }$$

To determine $M_Y(s)$, we start with the formula for $M_N(s)$ and replace each occurrence of $e^s$ with $M_X(s)$. This yields

$$M_Y(s) = \frac{ p M_X(s)}{ 1 - (1 - p) M_X(s)} $$

and, after some algebra,

$$M_Y(s) = \frac{ pq e^s }{ 1 - (1 - pq) e^s } $$

We conclude that $Y $ is geometrically distributed, with parameter $pq$.