172 CHAPTER 5. BROWNIAN MOTION
be a sequence of independent, identically distributed Bernoulli random vari-
ables. Note that Var [Yi] = 1, which we will need to use in a moment. Let
Y 0 = 0 for convenience and set
Tn=
∑n
i=0
Yi
be the sequence of sums, which represent the successive net fortunes of our
notorious gambler. As usual, we will sketch the graph ofTnversus time using
linear interpolation between the points (n− 1 ,Tn− 1 ) and (n,Tn) to obtain
a continuous, piecewise linear function. Since this interpolation defines a
function for all time, we could writeWˆ(t), and then for instance,Wˆ(n) =Tn.
NowWˆ(t) is a function defined on [0,∞). This function is piecewise linear
with segments of length
√
- The notationWˆ(t) reminds us of the piecewise
linear nature of the function.
Now we will compress time, and rescale the space in a special way. Let
Nbe a large integer, and consider the rescaled function
WˆN(t) =
(
1
√
N
)
Wˆ(Nt).
This has the effect of taking a step of size± 1 /
√
N in 1/Ntime unit. That
is,
WˆN(1/N) =
(
1
√
N
)
Wˆ(N· 1 /N) =√T^1
N
=
Y 1
√
N
.
Now consider
WˆN(1) =
Wˆ(N)
√
N
=
TN
√
N
.
According to the Central Limit Theorem, this quantity is approximately
normally distributed, with mean zero, and variance 1. More generally,
WˆN(t) =
Wˆ(Nt)
√
N
=
√
t
Wˆ(Nt)
√
Nt
IfNtis an integer, this will be normally distributed with mean 0 and vari-
ancet. Furthermore,WˆN(0) = 0 andWˆN(t) is a continuous function, and
so is continuous at 0. Altogether, this should be a strong suggestion that
WˆN(t) is an approximation to Standard Brownian Motion. We will define
the very jagged piecewise linear functionWˆN(t) asapproximate Brownian
Motion.