1Tangential Stress
$S_t=\frac{PD}{2te_j}
2Longitudinal Stress
$S_L=\frac{PD}{4te_j}
3Thickness Diameter Ratio Thin Walled
$\frac{t}{D_i}\leq 0.05$
$\frac{t}{R_i}\leq 0.1
4Spherical Thin-Walled Stress
$S=\frac{PD}{4te_j}
5Thickness Diameter Ratio Thick Wall
$\frac{t}{D_i}> 0.05$
$\frac{t}{R_i}> 0.1
6Axial Stress Thick Wall
$S_a=\frac{P_ir_i^2-P_or_o^2}{r_o^2-r_i^2}
7Radial Stress Thick Wall
$S=\frac{P_ir_i^2-P_or_o^2}{r_o^2-r_i^2}-\frac{(P_i-P_o)r_o^2r_i^2}{r_o^2-r_i^2}(\frac{1}{r^2})
8Hoop/Tangential/Circumferential Stress
$S=\frac{P_ir_i^2-P_or_o^2}{r_o^2-r_i^2}+\frac{(P_i-P_o)r_o^2r_i^2}{r_o^2-r_i^2}(\frac{1}{r^2})
9Lame's Equation (t)
$t=\frac{D_i}{2}\sqrt{\frac{S_t+P_i}{S_t-P_i}}-1
10Bach's Equation 2 formulas (t)
$t=\frac{D_i}{2}\sqrt{\frac{S_t+0.4P_i}{S_t-1.3P_i}}-1$
$t=\frac{D_i}{2}\sqrt{\frac{S_t+(1-2v)P_i}{S_t-(1+v)P_i}}-1
11Torque Friction Disk Clutchr
$T=fnF_ar_m
12Power
$P=\frac{NT}{factor}
13Uniform Wear Method (old) $r_m
$r_m=\frac{r_o+r_i}{2}$
$r_m=\frac{D_o+D_i}{4}
14Uniform Pressure Method (new) rm
$r_m=\frac{2}{3}\left[\frac{r_o^3-r_i^3}{r_o^2-r_i^2}\right]$
$r_m=\frac{1}{3}\left[\frac{D_o^3-D_i^3}{D_o^2-D_i^2}\right]
15Axial Force Clutch
$F_a=PA
16Uniform Wear Method (old) for Axial Force
$A=πDt
17Uniform Pressure Method (new) for Axial Force
$A=\frac{π}{4}(D_o^2-D_i^2)
18$Brass Tubes=T/D<0.025$
Collapsing Pressure
$P_{cr}=250,150,000\left(\frac{t}{d}\right)^3
19$Brass Tubes=T/D>0.030$
collapsing pressure
$P_{cr}=93,365\left(\frac{t}{d}\right)-2474
20Torque Cone Clutch
$T=\frac{fnF_ar_m}{sin\alpha}
21Torque Cone Engage
$T=\frac{fnF_ar_m}{sin\alpha+fcos\alpha}
22Torque Cone Disengage
$T=\frac{fnF_ar_m}{sin\alpha-fcos\alpha}
23Bearing Stress$
$S_b=\frac{F}{A_b}=\frac{F}{LD}
24Heat Radiating Capacity
$Q=\frac{Q_f}{A}=\frac{Ffv}{LD}=\frac{fF(πDN)}{LD}
25Frictional Torque Bearing
$T_f=Ffr=Ff\frac{D}{2}
26Petroff's Equation (T)
$T_f=\frac{r^3\mu N4π^2L}{C_r}$
radial clearance
$C_r=C_d/2