The pound of force or pound-force (symbol: lbf, sometimes lbf,) is a unit of force used in some systems of measurement, including English Engineering units and the foot–pound–second system. Pound-force should not be confused with pound-mass (lb), often simply called "pound", which is a unit of mass; nor should these be confused with foot-pound (ft⋅lbf), a unit of energy, or pound-foot (lbf⋅ft), a unit of torque.
Definitions The pound-force is equal to the gravitational force exerted on a mass of one avoirdupois pound on the surface of Earth. Since the 18th century, the unit has been used in low-precision measurements, for which small changes in Earth's gravity (which varies from equator to pole by up to half a percent) can safely be neglected. The 20th century, however, brought the need for a more precise definition, requiring a standardized value for acceleration due to gravity.
Product of avoirdupois pound and standard gravity The pound-force is the product of one avoirdupois pound (exactly 0.45359237 kg) and the standard acceleration due to gravity, approximately 32.174049 ft/s2 (9.80665 m/s2). The standard values of acceleration of the standard gravitational field (gn) and the international avoirdupois pound (lb) result in a pound-force equal to 32.174049 lb⋅ft/s2 (4.4482216152605 N).
1 lbf = 1 lb × g n = 1 lb × 9.806 65 m s 2 / 0.3048 m ft ≈ 1 lb × 32.174 049 f t s 2 ≈ 32.174 049 l b ⋅ f t s 2 1 lbf = 1 lb × 0.453 592 37 kg lb × g n = 0.453 592 37 kg × 9.806 65 m s 2 = 4.448 221 615 2605 N . {\displaystyle {\begin{aligned}1\,{\text{lbf}}&=1\,{\text{lb}}\times g_{\text{n}}\\&=1\,{\text{lb}}\times 9.806\,65\,{\tfrac {\text{m}}{{\text{s}}^{2}}}/0.3048\,{\tfrac {\text{m}}{\text{ft}}}\\&\approx 1\,{\text{lb}}\times 32.174\,049\,\mathrm {\tfrac {ft}{s^{2}}} \\&\approx 32.174\,049\,\mathrm {\tfrac {lb{\cdot }ft}{s^{2}}} \\1\,{\text{lbf}}&=1\,{\text{lb}}\times 0.453\,592\,37\,{\tfrac {\text{kg}}{\text{lb}}}\times g_{\text{n}}\\&=0.453\,592\,37\,{\text{kg}}\times 9.806\,65\,{\tfrac {\text{m}}{{\text{s}}^{2}}}\\&=4.448\,221\,615\,2605\,{\text{N}}.\end{aligned}}}
… excerpt ends here. Continue reading the full article.
