Everything seems fine, except right at the end. You are equating the average power delivered by the inductor L, with the average power delivered by the power supply (\$V_{in}\$). As you found out, this is only true if \$D=1\$ (duty cycle of 100%).
Simply put, during \$T_{off}\$ the power supply adds its voltage to the voltage that L develops, and share the same current, so the energy delivered to the load HAS to be more than what the inductor delivers (which can't be more than what it accumulated during Ton).
In the general case, during the on-time (\$T_{on}\$) the power supply delivers an energy of \$V_{in}I_{avg}T_{on}\$ exclusively to the inductor L. All of this energy has to be delivered to the load during the off-time (\$T_{off}\$), because this is supposed to be perfectly cyclical. But during \$T_{off}\$, \$V_{in}\$ is still delivering current, with the same average as in \$T_{on}\$ (we're calling it \$I_{avg}\$), and that energy \$V_{in}I_{avg}T_{off}\$ is going to the load as well.
So in the end the load gets, per cycle, an energy of \$V_{in}I_{avg}(T_{on}+T_{off})\$, which means the average power \$P = V_{in}I_{avg}\$. But this is not the same as the average power delivered by the inductor, which is only \$V_{in}I_{avg}(\frac{T_{on}}{T_{on}+T_{off}})\$.
A way to look at it is that, per cycle:
- [Total Energy received by the load] = [Total Energy delivered by power supply] = [Energy delivered by the power supply during Ton] + [Energy delivered by the power supply during Toff].
- [Energy delivered by the power supply during Ton] = [Energy delivered to the inductor during Ton] = [Energy delivered to the load by the inductor during Toff] < [Total energy delivered to the load].
So your last equation is correct:
\$ P_L=ft_{on}V_{in}\hat{I}_{in} \$
But it just talks about the average power delivered by the inductor, and is not all the average power delivered by the power supply:
\$ P_{PS} = V_{in}\hat{I}_{in} \$
Well, only if \$ ft_{on}=1\$ (100% duty cycle), or Iavg=0 (0% duty cycle). But we wouldn't even be in the correct operating mode in those cases.
The basic trade off between a linear (step down only, and buck and/or boost switching regulators, aside from efficiency, is lower part count, easier layout, & heat vs higher part count, layout concerns, & noise.
Going with a module makes the first two moot, but the third is still an issue for audio or rf or high speed data. Switching supplies can cause interference in some cases based on their switching nature. Linear regulators on the other hand, can smooth out noise. In exchange, switching regulators are relatively cool, while linear regs heat up more as the current increases.
Best Answer
The efficiency of the boost converter is \$P_{out}/P_{in}. P_{in} \$ is a sum of the average power drawn out of the input source during steady-state operation of the converter and the power used by the gate driver. \$P_{out}/P_{in} = 80.49 W/(84.7 W + 0.205 W) = 0.948 W/W \$ to be exact.