Visually: Forces are shown using free-body diagrams (FBDs), where each force acting on an object is represented by an arrow. Arrows indicate magnitude (length) and direction, helping visualize net force and interactions.
Algebraically: Forces are expressed as vectors with components. We apply Newton’s Second Law to each axis to set up equations
Newton’s First Law (Inertia): If ∑F = 0, then a=0: constant velocity or rest.
Newton’s Second Law: ∑F=ma Describes how net force causes acceleration, allowing us to calculate motion from forces or vice versa.
Newton’s Third Law: For every force F_{AB}, there is an equal and opposite force F_{BA}, such that F_{AB} = -F_{BA}. Useful in analyzing interactions, especially in systems of multiple objects.
Newton's three laws of motion
forces as interactions between bodies
that forces acting on a body can be represented in a free-body diagram
that free-body diagrams can be analysed to find the resultant force on a system
the nature and use of the following contact forces
normal force FN is the component of the contact force acting perpendicular to the surface that counteracts the body
surface frictional force Ff acting in a direction parallel to the plane of contact between a body and a surface, on a stationary body as given by Ff ≤ μsFN or a body in motion as given by Ff= μdFN where s and d are the coefficients of static and dynamic friction respectively
tension
elastic restoring force FH following Hooke's law as given by FH=-kx where k is the spring constant
viscous drag force Fd acting on a small sphere opposing its motion through a fluid as given by Fd= 6πηrv where η is the fluid viscosity, r is the radius of the sphere and v is the velocity of the sphere through the fluid
buoyancy Fb acting on a body due to the displacement of the fluid as given by Fb= ρVg where V is the volume of fluid displaced
the nature and use of the following field forces
gravitational force Fg is the weight of the body and calculated is given by Fg= mg
electric force Fe
magnetic force Fm