T. Bjork Arbitrage Theory in Continous Time reports the following Lemma at page 57: Let $f(t)$ be a deterministic function of time and define the process $X$ by
$$X(t) = \int_{0}^{t}f(s)dW(s)$$
Then $X(t)$ has a normal distribution with zero mean and variance given by
$$Var[X(t)] = \int_{0}^{t} f^2(s)ds$$
If by "solving" you mean find the distribution, this lemma allows you to do that easily, since $e^{\mu s}$ is clearly a deterministic function.
If you are wondering where does this Lemma come from, here comes a sketchy proof. The mean is obviously zero, because $X(t)$ is an Ito's Integral. Now, let's calculate the expected value of $E[e^{iuX(t)}]$, i.e. the characteristic function. To do so, we first have to find the Ito differential of $Z(t) = e^{iuX(t)}$ for a fixed $t$:
$$dZ(t) = -\frac{1}{2}u^2Z(t)dX^2+iuZ(t)dX = -\frac{1}{2}u^2f^2(t)Z(t)dt+iuf(t)Z(t)dW$$
Integrate both members and take expectations
$$E[Z(t)] = -\frac{1}{2}u^2\int_{0}^{t}f^2(s)E[Z(t)]ds+1$$
We have to add one at the end of it because we've assumed $Z(0)=1$. This looks like an integral equation, by we just need to differentiate both members to end up with a standard differential equation for $m(t) = E[Z(t)]$
$$\dot m(t) = -\frac{u^2}{2}f(t)m(t)$$
$$\Rightarrow m(t) = E[Z(t)] = exp\{-\frac{u^2}{2}\int_{0}^{t}f^2(s)ds\}$$
Once you have the characteristic function, calculate the second momentum, i.e. the variance, and you're done. QED