Given the numbers you quoted, you can easily calculate(*) the semimajor axis $a$ and the semiminor axis $b$. From these, you should know that the total area of the ellipse that the comet follows is $A = \pi\, a\, b$. Now, Kepler's second law says that the rate at which area is swept out by the line between the Sun and the comet is constant. We can calculate the rate over an entire period $P$ of the comet:
\begin{equation}
\frac{dA}{dt} = \frac{\pi\, a\, b} {P}.
\end{equation}
Again, this quantity is constant, no matter whether it's over some infinitesimal amount of time, or the whole orbit. Now, at perihelion (or aphelion), there's no radial motion — it's all angular. So if the comet moves some angle $d\theta$ while it's at radius $r$, the area it sweeps out is $dA = \frac{1}{2} r^2\, d\theta$. But we also know that the velocity is just $r\, d\theta/dt$, so we have
\begin{equation}
\frac{dA}{dt} = \frac{1}{2} r^2 \frac{d\theta}{dt} = \frac{1}{2}r\, v.
\end{equation}
You know what $r$ is, so just solve for $v$, and you've got your answer.
The Wikipedia link I gave has some more details about these steps, if you're wondering.
(*) The semimajor axis is the (arithmetic) mean of the distance at perihelion $r_\mathrm{per}$ and the distance at aphelion $r_\mathrm{ap}$:
\begin{equation}
a = \frac{r_\mathrm{per} + r_\mathrm{ap}} {2}.
\end{equation}
Meanwhile, the semiminor axis is the geometric mean of those distances:
\begin{equation}
b = \sqrt{r_\mathrm{per}\, r_\mathrm{ap}}.
\end{equation}