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Classical Mechanics
Foundations & Vectors
01SI Units and the Constants That Define Them02Defining the Second and the Meter03Redefining the Kilogram via Planck's Constant04Defining SI Units from Fixed Constants05Radians, Steradians & Small Angles06Dimensional Analysis: M, L, and T07Deriving Laws from Dimensions08Fermi EstimationProblem set0/10Problem set 20/10
01Vector Addition and Scalar Multiplication02Cartesian and Cylindrical Coordinates03Vector Components in Cartesian Coordinates04Solving Vector Problems with Components05Vector Components Under Coordinate Rotation06The Cross Product07The Cross Product FormulaProblem set0/10Problem set 20/10
Kinematics
01Position, Time Intervals, and Displacement02Instantaneous Velocity and the Derivative03Acceleration as the Second Derivative04Kinematic Equations from Graph Areas05Integration and the Fundamental Theorem06Polynomial and Piecewise AccelerationProblem set0/10Problem set 20/10MIT problem set0/4
01Independent Motion Along x and y Axes02Setting Up a Projectile Motion Problem03Time of Flight and Maximum Height04Eliminating Time to Find the Parabola05Aim Straight at the Falling BucketProblem set0/10Problem set 20/10MIT problem set0/1
01Centripetal Acceleration and Central Motion02Polar Unit Vectors and the Velocity of Circular Motion03Deriving v = rω from Chord Length and Small Angles04Radial and Tangential Acceleration in Polar Coordinates05Uniform Circular Motion: Period, Frequency, and v²/R06Angular Velocity and Acceleration as Vectors07Variable Radius: Radial Velocity and the Coriolis TermProblem set0/10Problem set 20/10
Newton's Laws & Forces
01Defining Force: Mass, Acceleration, and Force as a Vector02Newton's First Law: Inertia and Inertial Reference Frames03Newton's Second and Third Laws: Force as the Rate of Change of MomentumProblem set0/10Problem set 20/10
01Force Laws and Hooke's Law: Measuring the Spring Force02Universal Gravitation and the Principle of Equivalence03Electric Charge, Coulomb's Law, and Newton's Third LawProblem set0/10Problem set 20/10MIT problem set0/1
01The Normal Force: Why It Isn't Your Weight02Static and Kinetic Friction and the f = μN Laws03Free-Body Diagrams and Building a Physical Model04Tension in a Rope: Massless vs. Massive05Tension in a Hanging Rope: Two MethodsProblem set0/10Problem set 20/10MIT problem set0/4
Applying Newton's Laws
01The Staircase Problem: Friction, Launch, and Landing02Cart, Pulley, and Hanging Block: Finding the Tension03Inextensible Strings: Constraints in a Pulley System04A Block on an Accelerating Frictionless Wedge05The Capstan Equation: Rope Friction Around a Post06Terminal Velocity and the Hyperbolic-Tangent LawProblem set0/10Problem set 20/10MIT problem set0/4
01The Drag Force: Two Regimes of Fluid Resistance02Stokes' Law: Terminal Velocity of a Falling Sphere03Quadratic Drag: The Reciprocal Velocity DecayProblem set0/10Problem set 20/10MIT problem set0/2
01Newton's Second Law for Circular Motion02Universal Gravitation: Deriving the Moon's Period03Geostationary Satellites and Binary Star Orbits04Tension in Circular Motion: From Masses to a Rope05Circular Motion on a Cone and a Turntable06The Shell Theorem: Gravity Acts From the CenterProblem set0/10Problem set 20/10MIT problem set0/6
Momentum
01Impulse and Momentum: Newton's Second Law as an Integral02Drawing the System Boundary: Why Only External Forces Count03Center of Mass: From Two Particles to a Continuous Rod04Center-of-Mass Motion and Conservation of Momentum05Setting Up Any Momentum Problem: System, Axes, Diagrams06The Exploding Projectile: Where the Larger Fragment Lands07Inelastic Collision Then Friction: The Plane and the SandbagProblem set0/10Problem set 20/10MIT problem set0/5
01Reference Frames and the Galilean Transformation02Relative Velocity Worked Examples: Circle and Cart03Feynman, Challenger, and the Limits of a Curve Fit04Momentum with Flowing Mass: The Four Categories05Leaking Sand vs. Blown-In Grain: Two Freight Cars06The Boat and the Fire Hose: Mass In, Momentum In07Deriving the Rocket Equation: Where Thrust Comes From08Rocket Speed, Mass Ratio, and Why Rockets StageProblem set0/10Problem set 20/10MIT problem set0/5
Work & Kinetic Energy
01Conservation of Energy: System, Boundary, and Surroundings02Kinetic Energy: From Speed Squared to Force Times Distance03Work Done by a Constant Force: Positive, Negative, or Zero04Work as Area Under the Curve and the Work-Energy Theorem05Power: Average, Instantaneous, and Force Times VelocityProblem set0/10Problem set 20/10MIT problem set0/2
01The Scalar Product: Work as Force Dot Displacement02Work as a Line Integral Along Any Curved Path03Inverse-Square Forces, 3D Work-Energy, and Power04Reduced Mass and the Work Inside a Two-Body SystemProblem set0/10Problem set 20/10MIT problem set0/1
Energy Conservation & Collisions
01Conservative Forces: Why Gravity's Work Ignores the Path02The Closed-Loop Theorem: Why Conservative Forces Give Energy Back03Defining Potential Energy from Newton's Third Law04Three Potential Energies from One Recipe, and Where the Zero GoesProblem set0/10Problem set 20/10MIT problem set0/1
01Conservation of Mechanical Energy: Closed Systems, Conservative Forces02The Spring Energy Diagram: Turning Points and Forbidden Regions03Stable vs Unstable Equilibrium on a Cubic Energy Diagram04Non-Conservative Forces: When Mechanical Energy Is Not Conserved05Dissipation and the System Boundary: Where Friction's Energy GoesProblem set0/10Problem set 20/10MIT problem set0/2
01Escape Velocity: Zero Total Energy on Asteroid Toro02Loop-the-Loop: Pairing Energy with Newton's Second Law03Friction That Grows With Distance: The Energy Integral04Maximum Spring Compression on a Frictional Incline05Sliding Off a Sphere: The Angle Where Contact BreaksProblem set0/10Problem set 20/10MIT problem set0/2
01Relative Velocity, Reduced Mass, and the Center-of-Mass Frame02Coefficient of Restitution and the One-Dimensional Elastic Collision03Elastic Collisions Reverse in the Center-of-Mass Frame04Stacked Superballs: Why the Small Ball Rises Nine Times Higher05Two-Dimensional Elastic Collisions in the Laboratory Frame06The Right-Angle Rule for Equal Masses, via the Dot Product07From Center-of-Mass Angle to Laboratory Angle in ScatteringProblem set0/10Problem set 20/10MIT problem set0/6
Rotation & Torque
01Rigid Bodies and Fixed-Axis Rotation02Angular Signs: Speeding Up or Slowing Down03Rotational Kinetic Energy and Moment of Inertia04The Uniform Disc and the Parallel Axis Theorem05Energy Conservation with a Massive Pulley06The Rod-and-Disc Pendulum: Speed at the Bottom07Proving the Parallel Axis TheoremProblem set0/10Problem set 20/10MIT problem set0/3
01Torque About a Point: Moment Arm and Sign Conventions02Torque by Components: A Tilted Lever and the Ankle on Tiptoe03Deriving τ = Iα: Newton's Second Law for Rotation04Center of Gravity and Unequal Tensions on a Massive Pulley05Measuring a Rotor's Moment of Inertia from Two RunsProblem set0/10Problem set 20/10MIT problem set0/1
01Torque Through an Angle: Rotational Work and Power02Static Equilibrium and the Lever Law03The Generalized Lever Law: Forces at an Angle04The Hinged Rod and the Person on a Hill05The Knee Joint and Torque About Any PointProblem set0/10Problem set 20/10MIT problem set0/2
Angular Momentum & Rolling
01Angular Momentum of a Particle: r Cross p02Circular Orbit About Two Points: Angular Momentum Cone03Torque Changes Angular Momentum: The Grazing Meteor04Systems of Particles: Only External Torque Counts05Fixed-Axis Rotation: Why L-z Equals I Omega06Conservation About a Pivot: The Struck Rod07Angular Impulse: The Dropped WasherProblem set0/10Problem set 20/10MIT problem set0/5
01Rolling Without Slipping: Why the Contact Point Is at Rest02Bead on a Rolling Wheel: Circle Plus Line Gives a Cycloid03Rolling Constraints: Incline, Yo-Yo and Two Unwinding Drums04Orbital and Spin Angular Momentum: The Earth Around the Sun05Rolling Kinetic Energy and Chasles's TheoremProblem set0/10Problem set 20/10MIT problem set0/3
01Torque About the Center of Mass: Orbital and Spin Equations02One Push, Two Motions: Rigid-Body Work-Energy and Angular Impulse03Normal Forces on a Turning Train: Why the Outer Foot Pushes Harder04The Falling Yo-Yo: Tension, Acceleration and Final Spin05Rolling Down an Incline Three Ways: Forces, Energy, Torque06Sliding to Rolling: Why a Bowling Ball Ends at Five Sevenths Its Speed07Puck Strikes a Stick on Ice: Same Spin About Any PointProblem set0/10Problem set 20/10MIT problem set0/2

Conservation About a Pivot: The Struck Rod

Why is angular momentum about the pivot conserved when a rod is struck, even though linear momentum and energy are not?


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Your summary note

    1. 1

      Principle of conservation of angular momentum

      State that zero external torque gives (L⃗S sys)f=(L⃗S sys)i(\vec{L}_S^{\,\text{sys}})_f = (\vec{L}_S^{\,\text{sys}})_i(LSsys​)f​=(LSsys​)i​, and record the experimental status of the assumption that internal torques cancel in pairs.

    2. 2

      Choosing the pivot as the reference point

      Draw the torque diagram about SSS, show the pivot force, the paired contact forces and gravity give zero net torque in an instantaneous collision, and note momentum and mechanical energy are not assured constant.

    3. 3

      Collision stage: the rod's angular speed after impact

      Equate lm1vilm_1v_ilm1​vi​ to lm1vi/2+ISωalm_1v_i/2 + I_S\omega_alm1​vi​/2+IS​ωa​, use the parallel-axis theorem for IS=13m2l2I_S = \frac{1}{3}m_2l^2IS​=31​m2​l2, and derive ωa=3m1vi/(2m2l)\omega_a = 3m_1v_i/(2m_2l)ωa​=3m1​vi​/(2m2​l).

    4. 4

      Swing stage and the elastic condition

      Apply mechanical energy from just after impact to the ceiling to derive vi=(m2/m1)4gl/3v_i = (m_2/m_1)\sqrt{4gl/3}vi​=(m2​/m1​)4gl/3​ with units checked, then impose Ei=EaE_i = E_aEi​=Ea​ to find m2/m1=1m_2/m_1 = 1m2​/m1​=1.

    Attempt 1 of 2