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That force is the net force. [1] When forces act upon an object, they change its acceleration. The net force is the combined effect of all the forces on the object's acceleration, as described by Newton's second law of motion. When the net force is applied at a specific point on an object, the associated torque can be calculated.
A modern statement of Newton's second law is a vector equation: =, where is the momentum of the system, and is the net force. [ 17 ] : 399 If a body is in equilibrium, there is zero net force by definition (balanced forces may be present nevertheless).
is the position vector (a vector from the point about which the torque is being measured to the point where the force is applied), and r is the magnitude of the position vector, F {\displaystyle \mathbf {F} } is the force vector, F is the magnitude of the force vector and F ⊥ is the amount of force directed perpendicularly to the position of ...
The relation between the net force and the acceleration is given by the equation F = ma (Newton's second law), and the particle displacement s can be expressed by the equation = which follows from = + (see Equations of motion). The work of the net force is calculated as the product of its magnitude and the particle displacement.
[12] [13]: 150 The physics concept of force makes quantitative the everyday idea of a push or a pull. Forces in Newtonian mechanics are often due to strings and ropes, friction, muscle effort, gravity, and so forth. Like displacement, velocity, and acceleration, force is a vector quantity.
with F the net force (a vector), m the mass of a particle and a the acceleration of the particle (also a vector) which would be measured by an observer at rest in the frame. The force F is the vector sum of all "real" forces on the particle, such as contact forces, electromagnetic, gravitational, and nuclear forces.
It is the straight line through the point at which the force is applied, and is in the same direction as the vector F →. [1] [2] The lever arm is the perpendicular distance from the axis of rotation to the line of action. [3] The concept is essential, for instance, for understanding the net effect of multiple forces applied to a body.
This net force is a restoring force, and the motion of the string can include transverse waves that solve the equation central to Sturm–Liouville theory: [() ()] + () = () where () is the force constant per unit length [units force per area] and are the eigenvalues for resonances of transverse displacement () on the string, [2] with solutions ...