Force Warning: You are not logged in. Your IP address will be publicly visible if you make any edits. If you log in or create an account, your edits will be attributed to your username, along with other benefits.Anti-spam check. Do not fill this in! === Second law === {{main|Newton's second law}} According to the first law, motion at constant speed in a straight line does not need a cause. It is ''change'' in motion that requires a cause, and Newton's second law gives the quantitative relationship between force and change of motion. [[Newton's second law]] states that the net force acting upon an object is equal to the [[time derivative|rate]] at which its [[momentum]] changes with [[time]]. If the mass of the object is constant, this law implies that the [[acceleration]] of an object is directly [[Proportionality (mathematics)|proportional]] to the net force acting on the object, is in the direction of the net force, and is inversely proportional to the [[mass]] of the object.<ref name="openstax-university-physics" />{{rp|pages=204–207}} A modern statement of Newton's second law is a vector equation: <math display="block" qid=Q104212301>\vec{F} = \frac{\mathrm{d}\vec{p}}{\mathrm{d}t},</math> where <math> \vec{p}</math> is the momentum of the system, and <math> \vec{F}</math> is the net ([[Vector (geometric)#Addition and subtraction|vector sum]]) force.<ref name="openstax-university-physics" />{{rp|page=399}} If a body is in equilibrium, there is zero ''net'' force by definition (balanced forces may be present nevertheless). In contrast, the second law states that if there is an ''unbalanced'' force acting on an object it will result in the object's momentum changing over time.<ref name="Principia"/> In common engineering applications the mass in a system remains constant allowing as simple algebraic form for the second law. By the definition of momentum, <math display="block">\vec{F} = \frac{\mathrm{d}\vec{p}}{\mathrm{d}t} = \frac{\mathrm{d}\left(m\vec{v}\right)}{\mathrm{d}t},</math> where ''m'' is the [[mass]] and <math> \vec{v}</math> is the [[velocity]].<ref name=FeynmanVol1/>{{rp|((9-1,9-2))}} If Newton's second law is applied to a system of [[Newton's Laws of Motion#Open systems|constant mass]], ''m'' may be moved outside the derivative operator. The equation then becomes <math display="block">\vec{F} = m\frac{\mathrm{d}\vec{v}}{\mathrm{d}t}.</math> By substituting the definition of [[acceleration]], the algebraic version of [[Newton's second law]] is derived: <math display="block" qid=Q2397319>\vec{F} =m\vec{a}.</math> Summary: Please note that all contributions to Christianpedia may be edited, altered, or removed by other contributors. If you do not want your writing to be edited mercilessly, then do not submit it here. You are also promising us that you wrote this yourself, or copied it from a public domain or similar free resource (see Christianpedia:Copyrights for details). Do not submit copyrighted work without permission! Cancel Editing help (opens in new window) Discuss this page