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Work

Reference data and engineering information about work for dynamics applications.

work

Overview

Engineering reference data for Work in dynamics.

Key Formulas

Newton's Second Law

F=maF = ma

Force = mass × acceleration.

Kinetic Energy

Ek=12mv2E_k = \frac{1}{2}mv^2

Energy of motion.

Momentum

p=mvp = mv

Mass × velocity.

Work

W=FdcosθW = Fd\cos\theta

Force × displacement × cos(angle).

Variables

Symbol Description Unit
FF Force N
mm Mass kg
aa Acceleration m/s²
vv Velocity m/s
EkE_k Kinetic energy J

Work Done by a Constant Force

Work is the product of a constant force acting on an object and the distance the object moves in the direction of that force. The work-energy theorem states that the net work done on an object equals its change in kinetic energy. WF=FsW_F = F s where WFW_F is work (J, ft·lbf), FF is constant force (N, lbf), and ss is displacement in the direction of force (m, ft).

Example: A constant force of 20 N moves an object 30 m.
WF=(20N)(30m)=600JW_F = (20\,\text{N})(30\,\text{m}) = 600\,\text{J}

Work Done by a Spring Force

Springs exert a variable force described by Hooke's Law. The work done is proportional to the square of the displacement and equals the average force multiplied by the distance. Wspring=12ks2=12Fspring_maxsW_{\text{spring}} = \frac{1}{2} k s^2 = \frac{1}{2} F_{\text{spring\_max}} s where kk is the spring constant (N/m), ss is displacement from equilibrium (m), and Fspring_max=ksF_{\text{spring\_max}} = k s is the maximum spring force.

Example: A spring with constant k=1k = 1 N/m is stretched 1 m.
Wspring=12(1N/m)(1m)2=0.5JW_{\text{spring}} = \frac{1}{2} (1\,\text{N/m})(1\,\text{m})^2 = 0.5\,\text{J}

Rotational Work

Work can also be done by a torque (moment) acting through an angular displacement. WM=TθW_M = T \theta where WMW_M is rotational work (J, ft·lbf), TT is torque (N·m, ft·lbf), and θ\theta is angular displacement (radians).

Example: A shaft applies a torque of 300 N·m over one revolution (θ=2π\theta = 2\pi rad).
WM=(300N⋅m)(2πrad)1884JW_M = (300\,\text{N·m})(2\pi\,\text{rad}) \approx 1884\,\text{J}

General Representations of Work

Work can be expressed as a path integral, accounting for force due to gravity or pressure. W=Fds=mgdh=pdVW = \int \mathbf{F} \cdot d\mathbf{s} = \int m g \, dh = \int p \, dV where mm is mass (kg), gg is gravitational acceleration (m/s²), hh is height (m), pp is pressure (Pa), and dVdV is the change in volume (m³).

References