Engineering Mechanics: formula sheet

Statics & dynamics · first-year engineering · 56 formulas · metric edition 1

Module 1 · Statics: Forces and Moments
Engineering Mechanics-1 Newton's Second Law
F=maF = m a
Force equals mass times acceleration.
Engineering Mechanics-2 Weight (W = mg)
W=mgW = m g
Weight of a mass at Earth's surface, using standard gravity g = 9.80665 m/s² (exact by definition).
Engineering Mechanics-3 Pressure (P = F/A)
P=FAP = \frac{F}{A}
Pressure as perpendicular force spread over an area.
Engineering Mechanics-4 Torque
τ=rFsin⁡θ\tau = r F \sin\theta
Turning effect of a force applied at distance r from a pivot, at angle θ to the lever arm.
Engineering Mechanics-5 Weight Component Along an Incline (mg sin θ)
F∥=mgsin⁡θF_{\parallel} = m g \sin\theta
Component of an object's weight acting down the slope of an incline: the force that drives it…
Engineering Mechanics-6 Normal Force on an Incline (N = mg cos θ)
N=mgcos⁡θN = m g \cos\theta
Normal force pressing a resting mass into an incline, equal to the component of its weight…
Engineering Mechanics-7 Maximum Static Friction (f = μₛN)
fs,max⁡=μsNf_{s,\max} = \mu_s N
Largest static friction force available before an object breaks loose and slides, from the static…
Engineering Mechanics-8 Kinetic Friction Force (f = μₖN)
fk=μkNf_k = \mu_k N
Friction force resisting a sliding surface, equal to the coefficient of kinetic friction times the…
Engineering Mechanics-9 Angle of Repose (μ = tan θ)
μs=tan⁡θ\mu_s = \tan\theta
Steepest angle a surface can be tilted before an object slides, where the coefficient of static…
Engineering Mechanics-10 Torque with a Lever Arm (τ = rF sin θ)
τ=rFsin⁡θ\tau = r F \sin\theta
Torque produced by a force applied at distance r from the pivot, at angle θ to the lever.
Engineering Mechanics-11 Mechanical Advantage of a Lever
MA=dedlMA = \frac{d_e}{d_l}
Mechanical advantage of a lever as the ratio of effort arm to load arm, showing how much the lever…
Engineering Mechanics-12 Pulley System Effort Force
F=WnF = \frac{W}{n}
Effort force needed to lift a load with a pulley system, divided down by the number of rope…
Engineering Mechanics-13 Machine Efficiency
η=WoutWin\eta = \frac{W_{out}}{W_{in}}
Efficiency of a machine as useful work out divided by work in, with the shortfall lost to friction,…
Engineering Mechanics-14 Support Reaction: Simple Beam, Off-Centre Point Load
RA=P(L−a)LR_A = \frac{P (L - a)}{L}
Reaction at the near support of a simply supported beam with one point load at distance a from it.
Engineering Mechanics-15 Max Moment: Simple Beam, Off-Centre Point Load
M=Pa(L−a)LM = \frac{P a (L - a)}{L}
Maximum bending moment in a simply supported beam with a single point load at distance a from one…
Engineering Mechanics-16 Support Reaction: Simple Beam, Uniform Load (R = wL/2)
R=wL2R = \frac{w L}{2}
Reaction at each support of a simply supported beam under a uniformly distributed load: half the…
Engineering Mechanics-17 Beam Reaction by Moment Equilibrium: Two Point Loads
RA=P1(L−a1)+P2(L−a2)LR_A = \frac{P_1 (L - a_1) + P_2 (L - a_2)}{L}
Reaction at support A of a simply supported beam carrying two point loads, from ΣM = 0 taken about…
Module 2 · Dynamics of a Particle
Engineering Mechanics-18 Final Velocity (Uniform Acceleration)
v=v0+atv = v_0 + a t
Final velocity after accelerating uniformly from an initial velocity for a given time.
Engineering Mechanics-19 Displacement (Uniform Acceleration)
d=v0t+12at2d = v_0 t + \tfrac{1}{2} a t^2
Distance travelled under constant acceleration, starting from an initial velocity, over a time t.
Engineering Mechanics-20 Velocity-Displacement Relation (v² = v₀² + 2ad)
v2=v02+2adv^2 = v_0^2 + 2 a d
Links initial and final speeds to acceleration and displacement without involving time.
Engineering Mechanics-21 Acceleration Down a Frictionless Incline
a=gsin⁡θa = g \sin\theta
Acceleration of an object sliding freely down a frictionless incline, set only by gravity and the…
Engineering Mechanics-22 Acceleration Down an Incline with Friction
a=g(sin⁡θ−μkcos⁡θ)a = g\left(\sin\theta - \mu_k \cos\theta\right)
Acceleration of an object sliding down an incline once kinetic friction opposes the motion, from…
Engineering Mechanics-23 Rope Tension When Lifting a Mass
T=m(g+a)T = m\left(g + a\right)
Tension in a rope lifting a mass with an upward acceleration, exceeding the static weight by the…
Engineering Mechanics-24 Atwood Machine Acceleration
a=(m1−m2)gm1+m2a = \frac{\left(m_1 - m_2\right) g}{m_1 + m_2}
Acceleration of an Atwood machine: two masses joined by a rope over a frictionless pulley, driven…
Engineering Mechanics-25 Drag Force (F = ½CdρAv²)
FD=12CdρAv2F_D = \tfrac{1}{2} C_d \rho A v^{2}
Aerodynamic drag on a body moving through a fluid, growing with the square of speed and with…
Engineering Mechanics-26 Terminal Velocity
vt=2mgρACdv_t = \sqrt{\frac{2 m g}{\rho A C_d}}
Steady falling speed at which drag balances weight, from mass, air density, frontal area, and the…
Module 3 · Work, Energy, Momentum
Engineering Mechanics-27 Work (W = Fd cos θ)
W=Fdcos⁡θW = F d \cos\theta
Work done by a constant force acting at an angle to the displacement.
Engineering Mechanics-28 Kinetic Energy
Ek=12mv2E_k = \tfrac{1}{2} m v^{2}
Energy of a mass in motion.
Engineering Mechanics-29 Gravitational Potential Energy (U = mgh)
U=mghU = m g h
Energy stored by raising a mass to height h near Earth's surface, with g = 9.80665 m/s².
Engineering Mechanics-30 Work–Energy Theorem
W=12m(v2−v02)W = \tfrac{1}{2} m \left(v^{2} - v_0^{2}\right)
Net work done on an object equals its change in kinetic energy, linking force and distance to a…
Engineering Mechanics-31 Hooke's Law
F=kxF = k x
Restoring force of an ideal spring, proportional to its displacement from rest.
Engineering Mechanics-32 Elastic Potential Energy
U=12kx2U = \tfrac{1}{2} k x^{2}
Energy stored in an ideal spring displaced x from its rest length.
Engineering Mechanics-33 Power (P = W/t)
P=WtP = \frac{W}{t}
Average power as work or energy delivered per unit time.
Engineering Mechanics-34 Power from Force and Velocity (P = Fv)
P=FvP = F v
Instantaneous power delivered by a force parallel to the velocity.
Engineering Mechanics-35 Linear Momentum (p = mv)
p=mvp = m v
Momentum as the product of an object's mass and velocity.
Engineering Mechanics-36 Impulse (J = FΔt)
J=F ΔtJ = F \, \Delta t
Impulse delivered by an average force acting over a contact time, equal to the change in momentum.
Engineering Mechanics-37 Conservation of Momentum (Two Bodies)
m1u1+m2u2=m1v1+m2v2m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2
Conservation of linear momentum in a two-body collision, solving any one mass or velocity from the…
Engineering Mechanics-38 Perfectly Inelastic Collision
v=m1u1+m2u2m1+m2v = \frac{m_1 u_1 + m_2 u_2}{m_1 + m_2}
Common velocity of two bodies that stick together after a perfectly inelastic collision, from…
Engineering Mechanics-39 Coefficient of Restitution
e=v2−v1u1−u2e = \frac{v_2 - v_1}{u_1 - u_2}
Ratio of separation speed to approach speed in a collision, measuring how much of the relative…
Module 4 · Rotation and Vibration
Engineering Mechanics-40 Angular Velocity (ω = θ/t)
ω=θt\omega = \frac{\theta}{t}
Average angular velocity: the angle swept divided by the time taken.
Engineering Mechanics-41 Angular Acceleration
α=ω−ω0t\alpha = \frac{\omega - \omega_0}{t}
Average angular acceleration: the change in angular velocity divided by the time taken.
Engineering Mechanics-42 Linear Speed from Rotation (v = ωr)
v=ωrv = \omega r
A point at radius r on a rotating body moves with linear speed ωr.
Engineering Mechanics-43 Angular Velocity from Period
ω=2πT\omega = \frac{2\pi}{T}
One full revolution is 2π radians, so angular velocity is 2π divided by the period.
Engineering Mechanics-44 Speed in Circular Motion (v = 2πr/T)
v=2πrTv = \frac{2\pi r}{T}
Speed of an object in uniform circular motion: one circumference (2πr, with π ≈ 3.14159265) per…
Engineering Mechanics-45 Newton's Second Law for Rotation (τ = Iα)
τ=Iα\tau = I \alpha
Net torque equals moment of inertia times angular acceleration: F = ma for spinning things.
Engineering Mechanics-46 Moment of Inertia: Solid Disk
I=12mr2I = \tfrac{1}{2} m r^{2}
Rotational inertia of a uniform solid disk or cylinder about its central axis.
Engineering Mechanics-47 Moment of Inertia: Point Mass
I=mr2I = m r^{2}
Rotational inertia of a compact mass circling at radius r from the axis.
Engineering Mechanics-48 Centripetal Acceleration (a = v²/r)
ac=v2ra_c = \frac{v^2}{r}
Inward acceleration of an object moving in a circle at constant speed.
Engineering Mechanics-49 Centripetal Force (F = mv²/r)
Fc=mv2rF_c = \frac{m v^2}{r}
Net inward force required to keep a mass moving in a circle at constant speed.
Engineering Mechanics-50 Centripetal Acceleration (a = ω²r)
ac=ω2ra_c = \omega^{2} r
Centripetal acceleration written in terms of angular velocity rather than linear speed.
Engineering Mechanics-51 Rotational Kinetic Energy
KErot=12Iω2KE_{rot} = \tfrac{1}{2} I \omega^{2}
Kinetic energy stored in rotation: half the moment of inertia times angular velocity squared.
Engineering Mechanics-52 Angular Momentum (L = Iω)
L=IωL = I \omega
Angular momentum of a rotating body: moment of inertia times angular velocity.
Engineering Mechanics-53 Rotational Power (P = τω)
P=τωP = \tau \omega
Mechanical power delivered by a torque turning at angular velocity ω.
Engineering Mechanics-54 Shaft Torque from Power and Angular Speed
T=PωT = \frac{P}{\omega}
The torque in a rotating shaft: transmitted power divided by angular speed, with ω in radians per…
Engineering Mechanics-55 Undamped Natural Frequency
fn=12πkmf_n = \frac{1}{2\pi} \sqrt{\frac{k}{m}}
The frequency a mass on a spring returns to when nothing is driving it: stiffness over mass,…
Engineering Mechanics-56 Natural Frequency from Static Deflection
fn=12πgδstf_n = \frac{1}{2\pi} \sqrt{\frac{g}{\delta_{st}}}
The natural frequency read off the amount the mount sinks under the weight it carries: no spring…