Looking at the governing equations, you can clearly see that if R1 << R2, then the duty cycle is close to 50%.
With that done, I also would have fixed the cap to something that is available. Ignoring R1 for the moment (because I just need to ensure R2 is bigger), I solve for R2 in the frequency equation. It is approximately 72 kOhms.
I notice that a nonzero value of R1 is really there to tune the frequency. As long as R1 is much smaller than R2, then the frequency equation is more sensitive to changes in R1 than the duty cycle equation. So I can play with different small values of R1 to tune my frequency to get closer.
Finally, since I know that I’m likely using imprecise resistor tolerances, I know that I can pass if I just get close, so I might not need to be picky about R1.
In my opinion, this chain of reasoning (effective modeling, function sensitivity wrt parameters, tolerance specs) is what the lab experiment is actually about. Developing circuits that are tolerant to parameter variation is the key to real hardware products. That gives you so much flexibility in price and manufacturer and requires the designer to keep this kind of reasoning frontmost.