Ludium
EN/日本語
Sign In
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

One Push, Two Motions: Rigid-Body Work-Energy and Angular Impulse

How can one brief push both launch a body's center of mass and set it spinning, and where does its kinetic energy go?


Loading…

←Previous Torque About the Center of Mass: Orbital and Spin EquationsNext Normal Forces on a Turning Train: Why the Outer Foot Pushes Harder →

Your summary note

    1. 1

      Rotational equation τcm,z=Icmαcm,z\tau_{\text{cm},z} = I_{\text{cm}}\alpha_{\text{cm},z}τcm,z​=Icm​αcm,z​ for a rigid body

      Take the zzz-component of the spin relation, substitute Lcm,z=Icmωcm,zL_{\text{cm},z} = I_{\text{cm}}\omega_{\text{cm},z}Lcm,z​=Icm​ωcm,z​, and record the result beside F⃗ext=mA⃗cm\vec{F}^{\text{ext}} = m\vec{A}_{\text{cm}}Fext=mAcm​ as the pair governing translation and rotation separately.

    2. 2

      Work-energy theorem split into translation and rotation

      Derive ∫F⃗ext⋅dR⃗cm=Δ(12mVcm2)\int \vec{F}^{\text{ext}} \cdot d\vec{R}_{\text{cm}} = \Delta(\frac{1}{2}mV_{\text{cm}}^2)∫Fext⋅dRcm​=Δ(21​mVcm2​) and ∫τcm,z dθ=Δ(12Icmω2)\int \tau_{\text{cm},z}\,d\theta = \Delta(\frac{1}{2}I_{\text{cm}}\omega^2)∫τcm,z​dθ=Δ(21​Icm​ω2), then add them to get W=ΔKtrans+ΔKrotW = \Delta K_{\text{trans}} + \Delta K_{\text{rot}}W=ΔKtrans​+ΔKrot​.

    3. 3

      Worked example: an impulse on a two-mass rod

      For masses 2M2M2M and MMM on a rod of length DDD pushed at the lighter mass, find Vcm=FΔt/3MV_{\text{cm}} = F\Delta t/3MVcm​=FΔt/3M, then use zero angular momentum about B to reach ω=FΔt/MD\omega = F\Delta t/MDω=FΔt/MD.

    Attempt 1 of 2