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Unit · year 1

PU-101 · Newtonian Mechanics

Threads force · energy · matter · waves · fields · symmetry26 lectures22 derivations

Starting from Newton's three laws and the notion of an inertial frame, the unit builds the full deductive machinery of classical particle and rigid-body dynamics, showing how the conservation laws of energy, momentum, and angular momentum follow from force law and symmetry. It culminates in the central-force solution of the Kepler problem and in d'Alembert's principle, which reformulates the whole edifice as the Euler-Lagrange equations and hands the student off to analytical mechanics.

PREREQUISITES

PU-102, PU-103, PU-104

Lectures

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Derivations homed in this unit

D-021

Galilean Invariance of Newton's Laws

Newton's second law is form-invariant under Galilean boosts, translations, and rotations, which is what singles out the inertial frames.

D-022

The Work-Energy Theorem

Integrating F = ma along a trajectory shows the work done by the net force equals the change in kinetic energy.

D-023

Conservative Forces and Potential Energy

A force field is path-independent iff it is curl-free iff it is the negative gradient of a scalar potential energy.

D-024

Conservation of Mechanical Energy

For systems acted on only by conservative forces the sum of kinetic and potential energy is a constant of the motion.

D-025

Momentum Conservation from Newton's Third Law

Pairwise internal forces cancel, so the total linear momentum of an isolated system of particles is conserved.

D-026

The Center-of-Mass Theorem

The center of mass of a system accelerates as though the total external force acted on the total mass concentrated there.

D-027

Angular Momentum, Torque, and Central Forces

The time derivative of angular momentum equals the net torque, so angular momentum is conserved under central forces.

D-028

The Two-Body Problem and Reduced Mass

Separating center-of-mass and relative coordinates reduces the two-body central problem to one particle of reduced mass in a fixed potential.

D-029

Effective Potential and the Orbit Equation

Angular-momentum conservation collapses a central-force problem to one-dimensional radial motion in an effective potential, yielding the Binet orbit equation.

D-030

Kepler's Three Laws from Gravity

Solving the inverse-square orbit equation gives elliptical orbits, the equal-areas law, and the period-semimajor-axis relation.

D-031

Small Oscillations and Simple Harmonic Motion

Linearizing any smooth potential about a stable equilibrium yields the harmonic-oscillator equation and its characteristic frequency.

D-032

Damped, Driven Oscillators and Resonance

Solving the driven damped oscillator gives the steady-state amplitude, phase lag, and the resonance peak with its quality factor.

D-033

Coupled Oscillators and Normal Modes

Diagonalizing the coupled linearized equations of motion gives normal modes as eigenvectors and normal frequencies as eigenvalues.

D-034

The Tsiolkovsky Rocket Equation

Applying momentum conservation to a variable-mass body gives the logarithmic relation between velocity gain, exhaust speed, and mass ratio.

D-035

The Moment-of-Inertia Tensor

The angular momentum of a rigid body is a linear map of its angular velocity, defining the symmetric inertia tensor and its principal axes.

D-036

Euler's Equations and Torque-Free Precession

Writing angular-momentum balance in the body frame yields Euler's equations and predicts free precession and the stability of rotation axes.

D-037

Rotating Frames: Centrifugal and Coriolis Forces

Transforming Newton's law into a rotating frame produces the centrifugal, Coriolis, and Euler fictitious forces.

D-038

Euler-Lagrange Equations from d'Alembert

d'Alembert's principle in generalized coordinates converts Newton's equations into the Euler-Lagrange equations for the Lagrangian.

D-420

Projectile Motion from Constant-Acceleration Kinematics

Integrating constant acceleration gives the kinematic equations; in uniform gravity they make a parabola with range v0^2 sin 2theta / g.

D-421

Uniform Circular Motion and Centripetal Acceleration

Differentiating a circular path twice gives an inward acceleration v^2/r, so circular motion needs a net inward force m v^2/r.

D-422

Friction: the Coulomb Model and the Inclined Plane

The Amontons-Coulomb laws on an incline: rest while tan theta <= mu_s, slide with a = g(sin theta - mu_k cos theta), friction work lost as heat.

D-423

Gravitational Field, Potential, Circular Orbits and Escape Velocity

From the inverse-square law to the potential -GM/r, circular orbit speed sqrt(GM/r), Kepler's third law and escape speed sqrt(2GM/R).