Odwzorowanie liniowe

H_r>H_r’

$f \geq 2_{\text{rε}}\frac{\sin^{2}\frac{{(H}_{r}{*H}_{r}')}{2}}{\sin H_{r}'}$ $R_{\text{zt}} = f\frac{\sin H_{r}{*H}_{r}'}{sin(H_{r} + H_{r}^{'})}\text{\ \ \ \ }r_{\varepsilon} = 0$

Odwzorowanie łukowe

H_r > H_r′

$$f \leq 2r_{\varepsilon}\text{sinH}_{r}'{\text{\ \ \ \ \ \ \ }\text{\ \ \ \ \ \ \ \ \ }\text{\ \ \ \ \ R}}_{\text{zt}} \approx \frac{f^{2}}{8}_{\text{rε}}$$

Rzt frezowanie walcowe

$$R_{\text{zt}} = \frac{{f_{z}}^{2}}{4D}$$

Rzt frezowanie czołowe

f ≤ 2r_εsinH_r′

$R_{z} + \left( \varphi \right) = \frac{f_{z}\varphi^{2}}{8r_{\varepsilon}}$

f_zφ = f_zsinφ $\text{\ \ \ }\text{\ \ \ }\text{\ \ }f_{z} = \frac{\text{Vf}}{z*n}$

V_f = f_z * z * n $R_{\text{zt\ max}} = \frac{{f_{z}}^{2}}{8_{\text{rε}}}$

Toczenie

Fc=Cc*ap^ec*f^Uc [N]

Ff=Cf*ap^ef*f^Uf [N]

Fp=Cp*ap^ep*f^Up [N]

M=Fc*$\frac{d}{2}$ [Nmm] Pe=$\frac{\text{Fc}*\text{Vc}}{60000}$ [kW]

Wiercenie

Ff=Cf*D^af*f^Uf*K_M

M=C_M*D^aM*f^UM*K_M Pe=$\frac{M*n}{9,55*10^{6}}$

Powiercanie, rozwiercanie, pogłębianie

Ff=Cf*D^af*ap^ef*f^Uf*K_M

M=C_M*D^aM*ap^eM*f^UM*K_M Ѱ_Z=$\frac{360}{z}$

Wzory doświadczalne

Fcφ=Cc*ap*fz^m+1*sin^m+1φ

Fco=Fco*ap*z*D^ac*a_e^ec*fz^Uc

Pe=$\frac{\text{Fco}*\text{Vc}}{60000}$ fz=$\frac{\text{ft}}{z*n}$

Fcmax=Cc*ap*fz^m+1*sin^m+1Ѱ

Ѱ=arccos(1-$\frac{2\text{ae}}{D})$ Zc=$\frac{Ps}{Psz}$ Fz=$\frac{\text{ft}}{z*n}$

FctTotmax=Cc*ap*fz^m+1[sin^m+1(Ѱz)+sin^m+1(Ѱ- Ѱz)]

Wzór Taylora

T=$\frac{C_{T}}{V_{c}^{s}}$ [min] V_CT=$\frac{C_{v}}{T^{m}}$