The cutter teeth periodically strike the workpiece and the vibration waveform is displayed on the right. When the tooth-passing frequency approaches the natural frequency, chatter amplitude grows rapidly.
$$b_{lim,min} = \frac{-1}{2\,K_s\,\mathrm{Re}(\Lambda_{min})}, \qquad \Omega_{lobe} = \frac{60\,f_c}{N\,(k+1)}$$
K_s: specific cutting force (N/m²), Re(Λ): minimum real part of the FRF, N: tooth count, k: lobe order (0,1,2,...), f_c: chatter frequency (≈ f_n).
$$\mathrm{Re}(\Lambda_{min}) = \frac{-1}{4\,k_m\,\zeta\,(1+\zeta)}$$
Worst-case approximation (chatter frequency = natural frequency). k_m: modal stiffness (N/m), ζ: modal damping ratio. Stiffer and more damped structures yield a larger b_lim.
$$\mathrm{MRR} = b\cdot a_e\cdot f_z\cdot N\cdot n, \qquad f_{tooth} = \frac{n\,N}{60}$$
Material removal rate (MRR) and tooth-passing frequency. a_e: radial depth of cut, f_z: feed per tooth, n: spindle speed (rpm). This tool assumes f_z = 0.05 mm/tooth and a_e = D/2.