What is the relationship between hourglass flowrate and local gravity?
As in the excellent answer to a related question (hourglass flowrate vs. sand grain size) and this published paper, the mass flowrate $Q$ through an hourglass is dependent on local gravity as
$Q\ \propto\ \sqrt{g}$
This is derived through dimensional analysis, as follows. (Quoting from the answer by Georg Sievelson linked above.)
Let us consider a cylinder of diameter $D$, with a circular hole punched on the bottom side with radius $a$. We fill the cylinder with a height $H$ of sand. If we look at the speed of sand grains going out the bucket, we observe (experimentally) that it does not depend of the height of sand $H$, if $H$ is big enough (compared to the diameter $D$ - because the constraint saturates). We are left with two parameters : the diameter of the hole $a$ and the gravity field $g$ that makes it fall, so the output speed $v$ has to be proportional to $\sqrt{g a}$. The flow rate is the speed times the section, thus it is $Q \propto v \, a^2$, so it is of order $Q \propto g^{1/2} a^{5/2}$ (this is the Beverloo law).
Assuming you have the same hourglass on the Earth and the Moon, then the hourglass has the same mass of sand to move $m$ but different mass flowrates $Q$ so it will take a different time $t$. Since $Q=\frac{m}{t}$ and $Q\ \propto\ \sqrt{g}$, simple algebra shows:
$\frac{t_{Moon}}{t_{Earth}} = \sqrt{\frac{g_{Earth}}{g_{Moon}}}$
Since $\frac{g_{Earth}}{g_{Moon}}=6$ then:
$t_{Moon} = t_{Earth} \sqrt{6}$
So your $2$ minute egg timer here on Earth becomes a $\approx 5$ minute egg timer on the Moon. Thankfully we have more reliable methods of timekeeping in space!