The following two pictures taken from the classical NACA's “Summary of airfoil data” by Abbott, Von Doenhoff and Stivers depict the trend of $C_l$ and $C_d$ in respect of $Re$:


Reynolds number is defined as the ratio of the inertial force possesses by the airflow in relation to the viscous (shear) forces within it:
$Re=\frac{\rho Vc}{\mu}$
This can be better seen multiplying both numerator and denominator by $V$ and rewriting the definition of $Re$ as:
$Re=\frac{\rho V^2}{\mu(V/c)}$
Now the numerator resembles the classical expression for kinetic energy while the denominator represent the shear force given by the viscosity $\mu$ due to a speed variation $V/c$.
So, big Reynolds numbers imply bigger inertial forces than viscous ones. Small Reynolds numbers imply bigger viscous forces than inertial ones.
Intuitively that means that at small Reynolds numbers, viscous characteristics are predominant: thicker boundary layer, bigger viscous drag and earlier stall i.e. lower $C_{l_{max}}$.