Mechanics of Materials — formula sheet

Strength of materials · vessels · joints & the shop floor · 69 formulas · metric edition 1

Normal (Axial) Stress
σ=PA\sigma = \frac{P}{A}
Normal Strain (ε = δ/L)
ε=δL\varepsilon = \frac{\delta}{L}
Young's Modulus (E = σ/ε)
E=σεE = \frac{\sigma}{\varepsilon}
Axial Deformation (δ = PL/AE)
δ=PLAE\delta = \frac{P L}{A E}
Average Shear Stress (τ = V/A)
τ=VA\tau = \frac{V}{A}
Shear Modulus (G = τ/γ)
G=τγG = \frac{\tau}{\gamma}
Poisson's Ratio
ν=εlatεax\nu = \frac{\varepsilon_{lat}}{\varepsilon_{ax}}
Relation Between E, G and ν
E=2G(1+ν)E = 2G(1 + \nu)
Factor of Safety
FS=σuσallowFS = \frac{\sigma_{u}}{\sigma_{allow}}
Thermal Stress in a Restrained Member
σ=EαΔT\sigma = E \alpha \Delta T
Polar Moment of Inertia — Solid Shaft
J=πd432J = \frac{\pi d^{4}}{32}
Torsional Shear Stress (τ = Tr/J)
τ=TrJ\tau = \frac{T r}{J}
Angle of Twist (φ = TL/JG)
φ=TLJG\varphi = \frac{T L}{J G}
Shaft Torque from Power and Angular Speed
T=PωT = \frac{P}{\omega}
Rotational Power (P = τω)
P=τωP = \tau \omega
Shaft Diameter from Allowable Torsional Shear
d=16Tπτ3d = \sqrt[3]{\frac{16 T}{\pi \tau}}
Shear Stress in a Parallel Key
τ=2TdwL\tau = \frac{2T}{d \, w \, L}
Area Moment of Inertia — Rectangle
I=bh312I = \frac{b h^{3}}{12}
Area Moment of Inertia — Solid Round Bar
I=πd464I = \frac{\pi d^{4}}{64}
Parallel Axis Theorem (I = I_c + Ad²)
I=Ic+Ad2I = I_c + A d^{2}
Moment of Inertia — I-Beam or Built-Up Section
I=BH3(Btw)(H2tf)312I = \frac{B H^{3} - (B - t_w)(H - 2t_f)^{3}}{12}
Elastic Section Modulus (S = I/c)
S=IcS = \frac{I}{c}
Max Bending Moment — Centre Point Load
M=PL4M = \frac{P L}{4}
Max Bending Moment — Uniform Load
M=wL28M = \frac{w L^{2}}{8}
Bending Stress (σ = Mc/I)
σ=McI\sigma = \frac{M c}{I}
Bending Stress from Section Modulus (σ = M/S)
σ=MS\sigma = \frac{M}{S}
Transverse Shear Stress (τ = VQ/Ib)
τ=VQIb\tau = \frac{V Q}{I b}
Shear Flow (q = VQ/I)
q=VQIq = \frac{V Q}{I}
Beam Deflection — Simply Supported, Centre Load
δ=PL348EI\delta = \frac{P L^{3}}{48 E I}
Beam Deflection — Simply Supported, Uniform Load
δ=5wL4384EI\delta = \frac{5 w L^{4}}{384 E I}
Cantilever Deflection — End Load
δ=PL33EI\delta = \frac{P L^{3}}{3 E I}
Cantilever Deflection — Uniform Load
δ=wL48EI\delta = \frac{w L^{4}}{8 E I}
Radius of Gyration (r = √(I/A))
r=IAr = \sqrt{\frac{I}{A}}
Slenderness Ratio (KL/r)
λ=KLr\lambda = \frac{K L}{r}
Euler Critical Buckling Load
Pcr=π2EI(KL)2P_{cr} = \frac{\pi^{2} E I}{(K L)^{2}}
Hoop Stress in a Thin-Walled Cylinder
σh=pd2t\sigma_{h} = \frac{p d}{2 t}
Longitudinal Stress in a Thin-Walled Cylinder
σl=pd4t\sigma_{l} = \frac{p d}{4 t}
Combined Axial and Bending Stress
σ=PA+McI\sigma = \frac{P}{A} + \frac{M c}{I}
Maximum Principal Stress (Mohr's Circle)
σ1=σx+σy2+(σxσy2)2+τxy2\sigma_1 = \frac{\sigma_x + \sigma_y}{2} + \sqrt{\left(\frac{\sigma_x - \sigma_y}{2}\right)^{2} + \tau_{xy}^{2}}
Minimum Principal Stress (Mohr's Circle)
σ2=σx+σy2(σxσy2)2+τxy2\sigma_2 = \frac{\sigma_x + \sigma_y}{2} - \sqrt{\left(\frac{\sigma_x - \sigma_y}{2}\right)^{2} + \tau_{xy}^{2}}
Maximum In-Plane Shear Stress
τmax=(σxσy2)2+τxy2\tau_{max} = \sqrt{\left(\frac{\sigma_x - \sigma_y}{2}\right)^{2} + \tau_{xy}^{2}}
Stress Concentration (σmax = Kt σnom)
σmax=Ktσnom\sigma_{max} = K_t \, \sigma_{nom}
Thread Tensile Stress Area
At=π4(dktp)2A_{t} = \frac{\pi}{4} \left( d - k_{t} p \right)^{2}
Bolt Preload from Torque (T = KDF)
T=KDFT = K D F
Joint Stiffness Ratio of a Bolted Joint
C=kbkb+kmC = \frac{k_{b}}{k_{b} + k_{m}}
External Load That Separates a Preloaded Joint
P0=Fi1CP_{0} = \frac{F_{i}}{1 - C}
Fillet Weld Effective Throat
a=0.707za = 0.707 \, z
Fillet Weld Capacity from Throat Area
F=τAtF = \tau \, A_t
Fillet Weld Size for a Load per Unit Length
w=f0.707τaw = \frac{f}{0.707 \, \tau_{a}}
Shear Stress on a Fillet Weld Throat
τ=F0.707wL\tau = \frac{F}{0.707 \, w L}
Welding Heat Input
H=ηVISH = \frac{\eta \, V \, I}{S}
Carbon Equivalent (IIW)
CE=C+Mn6+Cr+Mo+V5+Ni+Cu15CE = C + \frac{Mn}{6} + \frac{Cr + Mo + V}{5} + \frac{Ni + Cu}{15}
Cutting Speed and Spindle Speed
V=πDNV = \pi \, D \, N
Milling Table Feed Rate
vf=Nzfzv_f = N \, z \, f_z
Material Removal Rate — Turning
Q=VfapQ = V \, f \, a_p
Machining Time — Turning Pass
tm=LfNt_m = \frac{L}{f \, N}
Taylor Tool Life Equation
VTn=CV \, T^{\,n} = C
Vickers Hardness
HV=2Fsin(136/2)d2=1.8544Fd2HV = \dfrac{2F \sin(136^\circ/2)}{d^{2}} = \dfrac{1.8544\,F}{d^{2}}
Hall–Petch Relation
σy=σ0+kyd1/2\sigma_y = \sigma_0 + k_y \, d^{-1/2}
True Stress from Engineering Stress
σt=σe(1+e),εt=ln(1+e)\sigma_t = \sigma_e \, (1 + e), \qquad \varepsilon_t = \ln(1 + e)
Goodman Fatigue Criterion
σaSe+σmSu=1n\frac{\sigma_a}{S_e} + \frac{\sigma_m}{S_u} = \frac{1}{n}
Basquin S-N Relation
σa=σf(2Nf)b\sigma_a = \sigma_f' \, (2N_f)^{b}
Miner's Cumulative Damage Rule (Three Blocks)
D=n1N1+n2N2+n3N3D = \frac{n_1}{N_1} + \frac{n_2}{N_2} + \frac{n_3}{N_3}
Stress Intensity Factor
K=YσπaK = Y \, \sigma \, \sqrt{\pi a}
Paris Law Crack Growth Rate
dadN=C(ΔK)m\dfrac{da}{dN} = C \left( \Delta K \right)^{m}
Plastic Section Modulus — Rectangle
Z=bh24Z = \frac{b h^{2}}{4}
Plastic Moment Capacity (Mp = Z fy)
Mp=ZfyM_p = Z f_y
LRFD Load Combination (1.2D + 1.6L)
U=1.2D+1.6LU = 1.2 D + 1.6 L
Elastic Modulus from Compressive Strength
Ec=kfcE_c = k \sqrt{f'_c}