<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom" xmlns:content="http://purl.org/rss/1.0/modules/content/"><channel><title>Mechanics with Calculus on Teddy Rook Book</title><link>https://teddyrookbook.com/physics/mechanics/</link><description>Recent content in Mechanics with Calculus on Teddy Rook Book</description><image><title>Teddy Rook Book</title><url>https://teddyrookbook.com/img/share.jpg</url><link>https://teddyrookbook.com/img/share.jpg</link></image><generator>Hugo</generator><language>en</language><atom:link href="https://teddyrookbook.com/physics/mechanics/index.xml" rel="self" type="application/rss+xml"/><item><title>Velocity as a Derivative</title><link>https://teddyrookbook.com/physics/mechanics/velocity-derivative/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/velocity-derivative/</guid><description>v = dx/dt gives the velocity at any instant from the position function. Mechanics with Calculus · Physics Ladder</description></item><item><title>Acceleration as a Derivative</title><link>https://teddyrookbook.com/physics/mechanics/acceleration-derivative/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/acceleration-derivative/</guid><description>a = dv/dt = d²x/dt², and zero velocity at an instant says nothing about the acceleration. Mechanics with Calculus · Physics Ladder</description></item><item><title>Velocity and Position from Acceleration</title><link>https://teddyrookbook.com/physics/mechanics/motion-from-acceleration/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/motion-from-acceleration/</guid><description>Integrate a(t) once for v(t) and again for x(t), using the starting values to fix the constants. Mechanics with Calculus · Physics Ladder</description></item><item><title>Deriving the Constant-Acceleration Equations</title><link>https://teddyrookbook.com/physics/mechanics/derive-kinematics/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/derive-kinematics/</guid><description>Integrating a constant acceleration twice gives the familiar equations and shows exactly when they apply. Mechanics with Calculus · Physics Ladder</description></item><item><title>Acceleration That Depends on Position</title><link>https://teddyrookbook.com/physics/mechanics/acceleration-of-position/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/acceleration-of-position/</guid><description>When a depends on x, write a = v dv/dx and integrate over x. Mechanics with Calculus · Physics Ladder</description></item><item><title>Position, Velocity and Acceleration Vectors</title><link>https://teddyrookbook.com/physics/mechanics/motion-vectors/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/motion-vectors/</guid><description>r(t), v = dr/dt and a = dv/dt describe motion in two and three dimensions, one component at a time. Mechanics with Calculus · Physics Ladder</description></item><item><title>Projectiles with Calculus</title><link>https://teddyrookbook.com/physics/mechanics/projectile-optimization/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/projectile-optimization/</guid><description>Use derivatives to find the highest point, the range and the launch angle that goes farthest. Mechanics with Calculus · Physics Ladder</description></item><item><title>Relative Motion and Galilean Frames</title><link>https://teddyrookbook.com/physics/mechanics/galilean-frames/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/galilean-frames/</guid><description>Frames moving at constant velocity disagree about velocities but agree about accelerations and forces. Mechanics with Calculus · Physics Ladder</description></item><item><title>Tangential and Centripetal Acceleration</title><link>https://teddyrookbook.com/physics/mechanics/tangential-normal-acceleration/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/tangential-normal-acceleration/</guid><description>On a curve, acceleration splits into dv/dt along the path and v²/r toward the center. Mechanics with Calculus · Physics Ladder</description></item><item><title>Motion Under a Time-Varying Force</title><link>https://teddyrookbook.com/physics/mechanics/time-varying-force/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/time-varying-force/</guid><description>Integrate F(t)/m to find the velocity when the force changes with time. Mechanics with Calculus · Physics Ladder</description></item><item><title>Linear Drag and Terminal Velocity</title><link>https://teddyrookbook.com/physics/mechanics/linear-drag/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/linear-drag/</guid><description>With drag F = −bv, the speed approaches v_T = mg/b as v(t) = v_T(1 − e^(−t/τ)), with τ = m/b. Mechanics with Calculus · Physics Ladder</description></item><item><title>Quadratic Drag</title><link>https://teddyrookbook.com/physics/mechanics/quadratic-drag/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/quadratic-drag/</guid><description>Fast objects in air feel drag ½CρAv², which gives a terminal speed √(2mg/(CρA)). Mechanics with Calculus · Physics Ladder</description></item><item><title>Banked Curves With and Without Friction</title><link>https://teddyrookbook.com/physics/mechanics/banked-curves/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/banked-curves/</guid><description>Find the design speed of a banked road and the range of speeds friction allows. Mechanics with Calculus · Physics Ladder</description></item><item><title>Constraints in Pulley Systems</title><link>https://teddyrookbook.com/physics/mechanics/pulley-constraints/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/pulley-constraints/</guid><description>The fixed length of a rope links the accelerations, so a movable pulley gives a₁ = 2a₂. Mechanics with Calculus · Physics Ladder</description></item><item><title>Center of Mass by Integration</title><link>https://teddyrookbook.com/physics/mechanics/center-of-mass-integral/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/center-of-mass-integral/</guid><description>x_cm = (1/M)∫x dm, with dm = λ dx for a rod whose density varies. Mechanics with Calculus · Physics Ladder</description></item><item><title>Work by a Variable Force</title><link>https://teddyrookbook.com/physics/mechanics/work-integral/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/work-integral/</guid><description>W = ∫F dx, the area under the force–position curve. Mechanics with Calculus · Physics Ladder</description></item><item><title>Work Along a Path</title><link>https://teddyrookbook.com/physics/mechanics/work-along-path/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/work-along-path/</guid><description>W = ∫F · dr adds up only the part of the force along each small step of the path. Mechanics with Calculus · Physics Ladder</description></item><item><title>The Work-Energy Theorem from Newton's Second Law</title><link>https://teddyrookbook.com/physics/mechanics/work-energy-derivation/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/work-energy-derivation/</guid><description>Integrating m dv/dt over x turns F = ma into W_net = ΔK. Mechanics with Calculus · Physics Ladder</description></item><item><title>Conservative Forces</title><link>https://teddyrookbook.com/physics/mechanics/conservative-forces/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/conservative-forces/</guid><description>A force is conservative when its work doesn&amp;#39;t depend on the path, so its work around any closed loop is zero. Mechanics with Calculus · Physics Ladder</description></item><item><title>Potential Energy from Force</title><link>https://teddyrookbook.com/physics/mechanics/potential-from-force/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/potential-from-force/</guid><description>U(x) = −∫F dx, which gives ½kx² for a spring and mgy for uniform gravity. Mechanics with Calculus · Physics Ladder</description></item><item><title>Force from Potential Energy</title><link>https://teddyrookbook.com/physics/mechanics/force-from-potential/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/force-from-potential/</guid><description>F = −dU/dx: the force points downhill on the potential energy curve. Mechanics with Calculus · Physics Ladder</description></item><item><title>Potential Energy Diagrams</title><link>https://teddyrookbook.com/physics/mechanics/energy-diagrams/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/energy-diagrams/</guid><description>Read turning points, allowed regions and stable or unstable equilibria from a graph of U(x). Mechanics with Calculus · Physics Ladder</description></item><item><title>Instantaneous Power</title><link>https://teddyrookbook.com/physics/mechanics/instantaneous-power/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/instantaneous-power/</guid><description>P = dW/dt = F · v gives the power at each instant. Mechanics with Calculus · Physics Ladder</description></item><item><title>Gravitational Potential Energy and Escape Speed</title><link>https://teddyrookbook.com/physics/mechanics/escape-speed/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/escape-speed/</guid><description>From U = −GMm/r, the escape speed is √(2GM/r), the same for any mass. Mechanics with Calculus · Physics Ladder</description></item><item><title>Impulse as an Integral</title><link>https://teddyrookbook.com/physics/mechanics/impulse-integral/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/impulse-integral/</guid><description>J = ∫F dt for any force that changes in time. Mechanics with Calculus · Physics Ladder</description></item><item><title>Solving Elastic Collisions</title><link>https://teddyrookbook.com/physics/mechanics/elastic-collisions-1d/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/elastic-collisions-1d/</guid><description>Combine conservation of momentum and of kinetic energy: the relative speed reverses in a one-dimensional elastic collision. Mechanics with Calculus · Physics Ladder</description></item><item><title>Collisions in Two Dimensions</title><link>https://teddyrookbook.com/physics/mechanics/collisions-2d/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/collisions-2d/</guid><description>Conserve the x- and y-components of momentum separately. Mechanics with Calculus · Physics Ladder</description></item><item><title>Newton's Second Law for a System</title><link>https://teddyrookbook.com/physics/mechanics/system-of-particles/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/system-of-particles/</guid><description>ΣF_external = M·a_cm, because the internal forces cancel in pairs. Mechanics with Calculus · Physics Ladder</description></item><item><title>The Rocket Equation</title><link>https://teddyrookbook.com/physics/mechanics/rocket-equation/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/rocket-equation/</guid><description>A rocket gains Δv = v_e ln(m₀/m_f) by throwing mass backward. Mechanics with Calculus · Physics Ladder</description></item><item><title>Angular Velocity and Acceleration with Calculus</title><link>https://teddyrookbook.com/physics/mechanics/angular-calculus/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/angular-calculus/</guid><description>ω = dθ/dt and α = dω/dt; integrate α(t) to find ω and θ. Mechanics with Calculus · Physics Ladder</description></item><item><title>Moment of Inertia by Integration</title><link>https://teddyrookbook.com/physics/mechanics/moment-of-inertia-integral/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/moment-of-inertia-integral/</guid><description>I = ∫r² dm gives the rotational inertia of rods, rings, disks and spheres. Mechanics with Calculus · Physics Ladder</description></item><item><title>The Parallel-Axis Theorem</title><link>https://teddyrookbook.com/physics/mechanics/parallel-axis/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/parallel-axis/</guid><description>I = I_cm + Md² for an axis shifted a distance d from the center of mass. Mechanics with Calculus · Physics Ladder</description></item><item><title>Torque as a Cross Product</title><link>https://teddyrookbook.com/physics/mechanics/torque-cross-product/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/torque-cross-product/</guid><description>τ = r × F, with its direction given by the right-hand rule. Mechanics with Calculus · Physics Ladder</description></item><item><title>Rolling Dynamics</title><link>https://teddyrookbook.com/physics/mechanics/rolling-dynamics/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/rolling-dynamics/</guid><description>Static friction makes rolling work: on a ramp a = g sin θ/(1 + I/(MR²)). Mechanics with Calculus · Physics Ladder</description></item><item><title>From Skidding to Rolling</title><link>https://teddyrookbook.com/physics/mechanics/skidding-to-rolling/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/skidding-to-rolling/</guid><description>A ball that starts out sliding skids until v = Rω, losing energy to kinetic friction on the way. Mechanics with Calculus · Physics Ladder</description></item><item><title>Angular Momentum of a Particle</title><link>https://teddyrookbook.com/physics/mechanics/angular-momentum-particle/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/angular-momentum-particle/</guid><description>L = r × p, so even a particle moving in a straight line has angular momentum about a point. Mechanics with Calculus · Physics Ladder</description></item><item><title>Collisions with Rotation</title><link>https://teddyrookbook.com/physics/mechanics/rotational-collisions/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/rotational-collisions/</guid><description>When a ball sticks to a pivoted rod, angular momentum about the pivot is conserved but linear momentum is not. Mechanics with Calculus · Physics Ladder</description></item><item><title>Work and Power in Rotation</title><link>https://teddyrookbook.com/physics/mechanics/rotational-work-power/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/rotational-work-power/</guid><description>W = ∫τ dθ and P = τω. Mechanics with Calculus · Physics Ladder</description></item><item><title>Gyroscopes and Precession</title><link>https://teddyrookbook.com/physics/mechanics/precession/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/precession/</guid><description>A torque at right angles to the spin turns the direction of L, so a top precesses at Ω = τ/L. Mechanics with Calculus · Physics Ladder</description></item><item><title>Static Equilibrium Problems</title><link>https://teddyrookbook.com/physics/mechanics/statics-problems/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/statics-problems/</guid><description>For ladders, hinged beams and hanging signs, choose a pivot that removes the unknowns you don&amp;#39;t need. Mechanics with Calculus · Physics Ladder</description></item><item><title>Gravity of a Spherical Body</title><link>https://teddyrookbook.com/physics/mechanics/shell-theorem/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/shell-theorem/</guid><description>Outside a uniform sphere, gravity acts as if all the mass sat at the center; inside, g grows in proportion to r. Mechanics with Calculus · Physics Ladder</description></item><item><title>Orbital Energy</title><link>https://teddyrookbook.com/physics/mechanics/orbital-energy/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/orbital-energy/</guid><description>A circular orbit has E = −GMm/(2r), so climbing to a higher orbit takes energy yet leaves you moving more slowly. Mechanics with Calculus · Physics Ladder</description></item><item><title>Kepler's Second Law from Angular Momentum</title><link>https://teddyrookbook.com/physics/mechanics/kepler-second-from-newton/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/kepler-second-from-newton/</guid><description>Gravity exerts no torque about the Sun, so L is constant and equal areas are swept in equal times. Mechanics with Calculus · Physics Ladder</description></item><item><title>Kepler's Third Law from Newton</title><link>https://teddyrookbook.com/physics/mechanics/kepler-third-from-newton/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/kepler-third-from-newton/</guid><description>For a circular orbit T² = 4π²r³/(GM), which weighs a planet or star from its satellites. Mechanics with Calculus · Physics Ladder</description></item><item><title>Speed on an Elliptical Orbit</title><link>https://teddyrookbook.com/physics/mechanics/vis-viva/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/vis-viva/</guid><description>v² = GM(2/r − 1/a) gives the speed anywhere on an ellipse, which plans transfer orbits. Mechanics with Calculus · Physics Ladder</description></item><item><title>The Equation of Simple Harmonic Motion</title><link>https://teddyrookbook.com/physics/mechanics/shm-equation/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/shm-equation/</guid><description>x″ = −ω²x is solved by x = A cos(ωt + φ) with ω = √(k/m). Mechanics with Calculus · Physics Ladder</description></item><item><title>Amplitude and Phase from Starting Conditions</title><link>https://teddyrookbook.com/physics/mechanics/shm-initial-conditions/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/shm-initial-conditions/</guid><description>Use x(0) and v(0) to find the amplitude A and the phase φ. Mechanics with Calculus · Physics Ladder</description></item><item><title>Springs Hanging Vertically</title><link>https://teddyrookbook.com/physics/mechanics/vertical-spring/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/vertical-spring/</guid><description>Gravity only moves the equilibrium point; the period stays 2π√(m/k). Mechanics with Calculus · Physics Ladder</description></item><item><title>Simple and Physical Pendulums</title><link>https://teddyrookbook.com/physics/mechanics/physical-pendulum/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/physical-pendulum/</guid><description>A swinging rigid body has T = 2π√(I/(mgd)), and small angles make any pendulum simple harmonic. Mechanics with Calculus · Physics Ladder</description></item><item><title>Damped Oscillations</title><link>https://teddyrookbook.com/physics/mechanics/damped-oscillations/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/damped-oscillations/</guid><description>Drag makes the amplitude shrink as e^(−bt/2m), and too much damping stops the swinging altogether. Mechanics with Calculus · Physics Ladder</description></item><item><title>Driven Oscillations and Resonance</title><link>https://teddyrookbook.com/physics/mechanics/driven-resonance/</link><pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate><guid>https://teddyrookbook.com/physics/mechanics/driven-resonance/</guid><description>Pushing near the natural frequency builds a large amplitude, limited only by damping. Mechanics with Calculus · Physics Ladder</description></item></channel></rss>