The following picture illustrates the situation of rolling without slipping. I noticed that this is achieved as the direction of $v_{cm}$ is the opposite of $\omega R$, at where the wheel is in contact with the ground.
However, I am confused why can't we, for example, rotate the wheel in picture b) in the counterclockwise direction? Then, if we take the superposition of picture a and picture b as we did in picture c, wouldn't the velocity of each part of the wheel look like the following instead?
Is the above option viable in real life? If not, why not?