The coil needs to dissipate approximately all of the transmitted power so it sounds a bit lightweight. It's not so much the copper wire thickness itself, but the rest of the mechanical details.
Final performance will depend on
- the former that the coil is wound on
- what temperature the former can cope with
- the duty cycle of the transmitter (eg. 600 W SSB PEP is only ~150 W average while talking)
- the mechanical stability of the coil as it heats up - any change in dimensions will de-tune the coil.
The wire thickness isn't all that important, within reason, as much of the heat dissipation will be through whatever it's wound on. I'd start by looking at the overall surface area of the coil as it's wound and estimate the temperature rise.
In house wiring, the figures for allowable current in a certain diameter copper cable, are really taking into account the heat that can be dissipated by a typical cable containing two of these wires, and its overall dimensions and materials.
Some calculations about the power loss:
(edit: typed in formulas, redone calculation in metres, all the numbers change slightly)
110 uH at 80 m (3.5 - 3.8 MHz) has a reactance of ~2500 ohms.
I look up two useful formulas at antenna-theory. Note:
- We are definitely in Short Dipole territory here, length << wavelength, so the current distribution is triangular (if you like, the very end of a sinusoid, the part where sin(x) ≈ x )
- Remember all these are for dipole antennas so the length and impedance is double that of the monopole case.
First, the reactance, to match that of the coil:
$$ X_{dipole} = {{-120\lambda}\over{\pi L}}\left( \text{ln}\left( \frac{L}{2a}\right)-1\right) $$
Experimenting a bit (I can't solve it) I find a 4 m long dipole of diameter 4 mm has about -5000 ohm reactance, i.e. -2500 ohms on a 2 metre monopole, which will resonate with that coil, and is a reasonable whip length for a vehicle. So you're probably making a base loading coil for a whip antenna (this is just me reverse-engineering the intended application).
Knowing the antenna type and length we can estimate the radiation resistance (on a perfect ground plane):
$$ R_{rad} = 20 \pi^2\left(\frac{L}{\lambda}\right)^2$$
The radiation resistance of a 4 metre dipole on 80 m is 0.5 ohms, so the monopole antenna will be about 0.25 ohms and there will be a few ohms of ground loss.
The coil Q might be as much as 100, to be generous, meaning it will have a resistance of 25 ohms.
Now I can draw a circuit model of the whole antenna:

simulate this circuit – Schematic created using CircuitLab
The series circuit of coil loss resistance, radiation resistance and ground loss, shows you that over 90% of the power is lost in the coil, depending on the size of the vehicle and the type of ground, more likely 99%. (you can estimate the coil Q just by looking at the bandwidth of the antenna when it's tuned).
So you need to plan for the coil to dissipate 100-200 watts without catching fire or getting out of shape. This also means that less than 1% of the power is radiated. This is the unfortunate reality of mobile HF antennas, especially for 80 m.
There are ways to raise the Q of the coil to several hundred - making it a larger diameter, thicker wire, keeping metal away from the ends, and using a ferrite core. It's also more efficient to put the coil halfway up, as Hustler does. These can dramatically improve the transmitted power, but you can see they won't make a big difference to the power dissipated in the coil.
Here's an example of a commercially available resonator for 80 m, capable of "1000 W" (right):

From memory, the Hustler RM-80S is about the size of a 0.5 to 1 litre water bottle.
So for 600 W, you probably want your coil to be about half this size.