Classical Mechanics
70 terms · page 3 of 3
Period
Classical Mechanics
s
The time duration required to complete one full cycle of a recurring motion or oscillation.
T = 1 / f = 2π / ω = 2π √(m/k)
Perpendicular Axis Theorem
Classical Mechanics
kg·m²
A theorem stating that for a thin planar lamina, the moment of inertia about an axis perpendicular to the plane equals the sum of moments of inertia about two perpendicular axes in the plane.
Iz = Ix + Iy
Potential Energy
Classical Mechanics
J
The stored energy an object possesses due to its relative position in a conservative force field or its structural deformation.
PE_grav = m g h, PE_elastic = ½ k x²
Power
Classical Mechanics
W (J/s)
The rate at which work is performed or energy is transferred per unit time.
P = dW/dt = F · v
Projectile Motion
Classical Mechanics
m, m/s
The 2D motion of an object launched into a gravitational field under the sole influence of gravity (ignoring air resistance).
x(t) = v0 cos θ t, y(t) = v0 sin θ t - ½ g t²
Radius of Gyration
Classical Mechanics
m
The radial distance from a rotation axis at which total mass could be concentrated without altering the moment of inertia.
k = √(I / m)
Range
Classical Mechanics
m
The total horizontal distance traveled by a projectile from launch to landing at the same vertical height.
R = (v0² sin 2θ) / g
Restoring Force
Classical Mechanics
N
A force that acts to bring a body back toward its stable equilibrium position whenever it is displaced.
F = -k x
Reynolds Number
Classical Mechanics
Dimensionless
A dimensionless quantity in fluid mechanics predicting flow patterns, equal to ratio of inertial forces to viscous forces.
Re = (ρ v L) / η
Rotational Kinetic Energy
Classical Mechanics
J
The kinetic energy possessed by a body due to its rotation about an axis.
KE_rot = ½ I ω²
Simple Harmonic Motion
Classical Mechanics
m, rad/s
Repetitive periodic motion where restoring force is directly proportional to displacement and acts toward the equilibrium position.
x(t) = A cos(ω t + φ), ω = √(k/m)
Simple Machine
Classical Mechanics
Dimensionless
A basic mechanical device that changes the direction or magnitude of an applied force.
MA = F_out / F_in
Static Equilibrium
Classical Mechanics
N, N·m
The state of a rigid body where both net external force and net external torque are zero, keeping the body completely at rest.
∑ F = 0, ∑ τ = 0
Stokes' Law
Classical Mechanics
N
A mathematical law expressing viscous drag force experienced by small spherical particles moving at low speeds through a viscous fluid.
Fd = 6 π η r v
Tension
Classical Mechanics
N
The pulling force transmitted axially through a string, rope, cable, or structural member.
T = m g + m a
Terminal Velocity
Classical Mechanics
m/s
The constant maximum speed attained by a falling body when upward aerodynamic drag equals downward gravitational force.
v_t = √(2 m g / (ρ A Cd))
Time of Flight
Classical Mechanics
s
The total duration a projectile spends in the air from launch until returning to its landing elevation.
T = (2 v0 sin θ) / g
Torque
Classical Mechanics
N·m
The rotational equivalent of linear force, measuring the effectiveness of a force in causing angular acceleration about an axis.
τ = r × F = r F sin θ
Velocity
Classical Mechanics
m/s
A vector quantity expressing the time rate of change of position, possessing both speed and direction.
v = dr/dt
Viscosity
Classical Mechanics
Pa·s (kg/(m·s))
A measure of a fluid's internal resistance to gradual deformation by shear or tensile stress.
τ = η (dv/dy)
Work
Classical Mechanics
J (N·m)
The scalar energy transferred to or from an object by a force acting through a displacement.
W = F · d = |F| |d| cos θ
Work-Energy Theorem
Classical Mechanics
J
The principle stating that net work done by all forces acting on an object equals the net change in its kinetic energy.
W_net = ΔKE = ½ m vf² - ½ m vi²