Put a stick in the ground. Try to make it vertical I think. Watch the length of the shadow for many days and years. You’ll see that every day the shadow is long then short then long. There is a moment when it is shortest. You could just pick some day and the moment when the shadow is shortest and call that noon. If you want a little more significance to your $t_0$ you could wait for the shortest day of the year and call the shadow short time on that day noon.
If you’re using something other than earths rotation as a clock then you’ll find that that first day is the only day when the short shadow time happens at exactly noon. Otherwise you’ll see it drift around a bit and this is due to instability of either the earths rotation or your clock due to various physical effects.
If you trust earths rotation more you should recalibrate your clock occasionally so that noon does occur at the short shadow time. If you trust your clock more you should consider the difference between the short shadow time and noon on your clock to be a measurement of instability in earths rotation.
Note that earths rotation is kind of a funny clock because it’s not only random noise that makes the rotation not perfectly harmonic, but there are other periodic effects, such as revolution around the sun or various precessions, that cause periodic fluctuations in the earths rotation rate. But, there is also regular drift and noise familiar from other types of clocks.
edit: Note the procedure above allows you to set $t_0$ for your accurate/stable clock but it doesn't set the ticking period $T$. To set the ticking period $T$ to match Earth's rotation you would operator your clock for many days/years periodically tuning its oscillation frequency $T$ to match the rotation of the Earth. But again, note that this is kind of a funny process if your clock is actually more stable than the Earth's rotation because you will get different answers for calibrated clock tick rate depending on how long you wait. This is because the duration of a single day (i.e. noon to noon) varies over the course of the year so a more practical approach would be to let 1 day be the start of your calibration, then 365 days be the end. Make sure your clock ticks "noon" on the last day. This means your clocks $T$ will be calibrated to the 365-day average of the length of a single day, at least during that 365 day period (because the average day length might vary from year to year).
So the takeaway is that we can use "astronomical" observations of noontime to set both $t_0$ and $T$ for our clock. But, as I've described above, if your clock is more stable than the rotation of the Earth (which it's not actually that hard to do) then you'll have to arbitrarily designate some noon to be $t_0$ and you'll have to arbitrarily designate some duration of days/years to be your calibration time during which you calibrate $T$. After that you take your clock as the stable reference and you interpret discrepancies between your clock and the Earth's rotation to be due to fluctuations in the Earth's rotation rate.
You can confirm that it is Earth drifting and not your clock by making multiple different clocks all with better stability than the Earth's rotation, and noticing that all of these clocks drift less relative to each other than the Earth does relative to any one of them. And it's the best if the different clocks are based off of different types of mechanisms to ensure there isn't some common mode drift to all your purportedly stable clocks that would trick you into thinking your clocks are more stable than they are (when in fact they drift, just at the same rate as all their peers).