Well, let's see. A Bessel function of the first kind is defined as:
J_v(x)=\sum\frac{(-1)^m}{m!Γ(m+v+1)}(\frac{x}{2})^{2m+v}
The Kelvin functions would be the real and imaginary parts of the vth order of J(xe^{3πi/4}), therefore:
J_v(x)=\sum_{m=0}^{m=\infty} \frac{(-1)^m}{m!Γ(m+v+1)}(\frac{xe^{3πi/4}}{2})^{2m+v}
which ultimately wields the formulas for Ber(x) and Bei(x) that you can see here (although you have probably seen it already):
http://en.wikipedia.org/wiki/Kelvin_functions#Ker.28x.29
Now, since bessel functions are solutions to the bessel differential equation, it means that kelvin functions (that are derived from these solutions) would be applicable to the same problems.
Again, I'd never heard of Kelvin functions until you asked, so I'm just thinking logically. The theory suggests though that special cases of a differential equation are still solutions to that equation, which means that they describe a specific set of problems that this equation describes. For instance, we could state that Laplace's equation is a special case of Poisson's equation. The special case would still have similar applications, albeit more limited.