Before swapping over to the vented hole side plates I wanted to get a better understanding of the effect of the motor RPM on R1, the heat conductivity between the stator and the shell. This will be important for comparing the effectiveness of both internal blades with no holes, and oil filled strategies, as both of these will increase the heat flow from the stator to the shell but don't have any real effect on the ability to dissipate from the shell to ambient.
Here is the raw data at 100, 200, 300, and 400 RPM:
What is interesting is that the temperature rise of the motor core was nearly identical at all speeds, hitting the CA's thermal rollback after 19 minutes. So at first it looks like the RPM has little effect. But, even though the I^2R copper heating is identical in all of them during the first 19 minutes, the faster RPM tests have more eddy/hysteresis losses, and so total heat being dissipated by the hub is greater in those runs, which you can see from the watts in curves
Using the steady state values, it is easy to compute the equivalent R1 term. At 300 RPM for instance, the steady state power is about 205 watts, the stator is 119 degrees, the shell is 63 degrees, so:
1/R1 = 205/(119-63) = 3.66 Watts/degree
Here is the conductivity for R1 from stator to shell, plotted as function of RPM, in the case of a sealed motor with no internal fan blades and no oil:
It would appear from this data that at higher RPMs the motor can sustain more phase current and torque because the abililty to dissipate heat from the stator is improved. After the CA's thermal rollback kicked in and reached steady state, the thermal power input that could be sustained for a 120 degree core in the 400 RPM run was ~222 watts, versus around 175 watts at 100 RPM.
However, that difference (~50 watts) is only slightly more than the additional cogging/hysteresis losses that are also present from the higher RPM, which means that the increase in sustainable phase current at 400 RPM versus 100 RPM is still pretty marginal. Which implies in a nutshell that the steady state torque output capability of the hub motor doesn't improve much at the higher RPMs. What gains there in better internal air turbulance to move the heat around is mostly offset by the additional heat that is generated by the greater motor core losses.
I'm in the process of getting the R1 data at 0, 500, and 600 rpm, but there are complications doing that by the same technique heating them up under load with the dyno so instead I'll heat the motor first and then study the cooling profile while the hub is spinning at those RPM's to get the resistances.