A force is any interaction that causes a change in the motion of an object or its state of rest. It is a vector quantity and measured in newtons (N).
F = ma
, where m is inertial mass.W = mg
.Ideal pulleys and strings are assumed massless unless stated otherwise. Let's analyze a few scenarios:
If masses m₁ > m₂
:
Acceleration: a = ((m₁ – m₂) / (m₁ + m₂)) * g
Tension: T = (2m₁m₂ / (m₁ + m₂)) * g
Acceleration: a = (m₁g) / (m₁ + m₂)
Tension: T = (m₁m₂g) / (m₁ + m₂)
Acceleration: a = ((m₁ – μm₂) / (m₁ + m₂)) * g
Tension: T = (m₁m₂(1 + μ) / (m₁ + m₂)) * g
a = ((m₁ – m₂) / (m₁ + m₂ + M)) * g
T₁ = ((2m₂ + M) / (m₁ + m₂ + M)) * m₁g
T₂ = ((2m₁ + M) / (m₁ + m₂ + M)) * m₂g
Acceleration: a = ((m₁ – m₂ sinθ) / (m₁ + m₂)) * g
Tension: T = (m₁m₂(1 + sinθ) / (m₁ + m₂)) * g
Acceleration: a = (m₁ sinθ₁ – m₂ sinθ₂) * g / (m₁ + m₂)
Tension: T = (m₁m₂ / (m₁ + m₂)) * (sinθ₁ – sinθ₂) * g
F = ma
and a = 0
where applicable.In accelerating frames, an additional force must be introduced for Newton’s laws to apply. For linear acceleration a, the pseudo force is -ma
. For rotating frames, the centrifugal force mω²r
acts outward.
A conical pendulum consists of a bob revolving in a horizontal circle, with its string tracing a cone. The tension and angle depend on centripetal force requirements.
mg
m(g + a)
m(g – a)
Friction arises from intermolecular forces between contacting surfaces. It opposes motion and can be static or kinetic.
μₛN
fₘₐₓ = μₛN
fₖ = μₖN
Since μₖ < μₛ
, rolling an object requires less force than sliding it.
The smallest angle of incline at which an object starts sliding. Given by: μ = tanα