The units for working with mass and force tend to be confusing for many students. The key to keeping them straight is to remember Newton's Law (the 2nd law of motion):
Historically, there have been two main approaches to systematizing the relationship between mass and force:
Think about the dimensions on Newton's law:
There are at least three different ways of handling things in English units. In most Ch.E. classes, the derived unit is the "pound-force" (lbf), defined as the product of the mass unit and the acceleration of gravity at sea level and 45 degrees latitude.
Others have tried to set up the English system so that "pound" was used for only one unit -- either mass or force, but not both. You should be aware that these exist, although we won't use them (Physics and CE/ME texts may).
Gravitational formulations of this type set the unit of mass as the "slug" and the unit of force as the "pound". Absolute formulations use "pound" as the mass unit, but "poundal" as the force unit.
The conversion between the defined unit of force (N, dyne, lbf) and natural units is so commonly used that we give it a special name and symbol, gc.
Tip: If you're working a problem and have mass units, but want force, divide by gc (or vice versa).
Although common usage allows the word "weight" to be used as a synonym for "mass", in engineering and science you must be aware that weight is defined to be the force exerted on an object by gravity, so an object of mass m subjected to the gravitational acceleration g, will have weight
The acceleration of gravity is not a constant. It varies with the mass of the attracting body (earth, moon, etc.), with the distance between objects, and with position. A "typical" value is used for calculations when the exact value is uncertain. This value (standard gravity) is:
What is the difference in the weight in newtons of a 100 kg rocket at 10 km above the earth (g=9.76 m/s2) as opposed to its weight on the surface (g=9.80 m/s2)?

References:
R.M. Price
Original: 6/1/94
Modified: 9/25/95, 6/19/96; 5/18/2004
Copyright 2004 by R.M. Price -- All Rights Reserved