Newton’s Law of Cooling and the Ornstein-Uhlenbeck Process
The Law of Cooling says the temperature difference between an object (say a hot cup of coffee) and the ambient temperature (the temperature in the room) declines exponentially:
If T(t) is the temperature of the object at time t, we have the ODE:
d/dt(T(t) – Troom) = b (T(t) – Troom) b < 0, Troom is a constant.
Equivalently, dT/dt = b (T – Troom)
T(0) is the starting temperature of the object (T(0) > Troom); b is the rate.
[1] Solve this ODE to obtain T as a function of t.
If we make this process stochastic in the simplest way possible – by adding a Brownian motion to the increment – we obtain the Ornstein-Uhlenbeck process:
dS = b (S - S) dt + s dW
S(0) = S0 b, s, and S are constants
b < 0
The condition b < 0 means that when S(t) is larger than S the drift will pull S(t) down (closer to S). When S(t) is smaller than S the drift will pull S(t) up (closer to S).
[2] Solve the SDE.
Hint: Consider the function A(S,t) = exp(-bt) S. Compute the increment dA using Ito’s Formula. You should end up with:
dA = f(t) dt + g(t) dW for functions f(t) and g(t).
Is the increment dA normally distributed?
It should be easy to integrate this type of SDE.
[3] Explain why the random variable S(T) is normally distributed.
[4] How does the standard deviation of S(T) grow with T? Does it grow without bound?
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