Simple Harmonic Motion: SHM • Linear Restoring Force: Ideal Spring k Fx = ma x = − kx a x (t ) = − x(t ) m k k Spring Constant k amax = xmax = A m m • Energy Conservation: E = KE + U = mv + kx 1 2 2 x 1 2 At xmax = A vx = 0 hence E = 12 kA2 = 12 mvx2 + 12 kx 2 Amplitude A 2 constant (independent of time) m 2 v x (t ) + x 2 (t ) = A2 (true at any time t) k The maximum speed vmax occurs when x = 0. General Solution! R. Field 11/7/2013 University of Florida vmax = k A m x(t ) = A cos(ωt + φ ) v x (t ) = −ωA sin(ωt + φ ) k ω = 2 a x (t ) = −ω A cos(ωt + φ ) spring m PHY 2053 The phase angle φ determines where the mass m is at t = 0, x(t=0) = Acosφ. If x(t=0) = A then φ = 0. Page 1 Uniform Circular Motion & SHM • Uniform Circular Motion: θ (t ) = ωt A θ(t) x(t) x-axis Project uniform circular motion (constant angular velocity ω) of a vector with length A onto the x-axis and you get SHM! x(t ) = A cos[θ (t )] = A cos(ωt ) x(t) • Amplitude Simple Harmonic Motion (SHM): If x(t=0) = A then x(t ) = A cos(ωt ) v x (t ) = −ωA sin(ωt ) a x (t ) = −ω 2 A cos(ωt ) xmax = A vmax = ωA amax = ω 2 A k a x (t ) = −ω x(t ) = − x(t ) spring m 2 ω = spring k m The period T is the time is takes for one circular revolution: Time t R. Field 11/7/2013 University of Florida T= 2π ω T = period (in s) 1 f = T f = frequency (in Hz) PHY 2053 ω = 2πf ω = angular frequency (in rad/sec) Page 2 SHM: Graphical Representation If x(t=0) = A then x(t ) = A cos(ωt ) v x (t ) = −vmax sin(ωt ) a x (t ) = −amax cos(ωt ) xmax = A vmax = ωA amax = ω 2 A T= R. Field 11/7/2013 University of Florida PHY 2053 2π ω 1 f = T ω = spring k m ω = 2πf Page 3 SHM: General Solution If the acceleration ax(t) and the position x(t) are related as follows: a x (t ) = −Cx(t ) where C is some constant then x(t ) = A cos(ωt + φ ) v x (t ) = −vmax sin(ωt + φ ) a x (t ) = −amax cos(ωt + φ ) If x(t=0) = A then φ = 0: xmax = A k C = spring m ω= C vmax = C A 2π amax = CA T = C 1 f = ω = 2πf T If x(t=0) = 0 and vx(t=0) > 0 then φ = π/2: x(t ) = A cos(ωt ) x(t ) = A sin(ωt ) v x (t ) = −vmax sin(ωt ) a x (t ) = −amax cos(ωt ) v x (t ) = vmax cos(ωt ) a x (t ) = − amax sin(ωt ) cos( A + B ) = cos A cos B + sin A sin B R. Field 11/7/2013 University of Florida PHY 2053 Page 4 SHM: General Solution • Angular Oscillations SHM: If the angular acceleration α(t) and the angular position θ(t) are related as follows: α (t ) = −Cθ (t ) where C is some constant then θ (t ) = A cos(ξt + φ ) ω (t ) = −ωmax sin(ξt + φ ) α (t ) = −α max cos(ξt + φ ) R. Field 11/7/2013 University of Florida θ max = A ξ= C ωmax = C A 2π = T α max = CA 1 f = ω = 2 π f C T PHY 2053 Page 5 The Pendulum: Small Oscillations SHM • Simple Pendulum: axis Small pendulum bob with mass m on string of lengh L and negligible mass. Calculate the torque about the axis of rotation as follows: τ = Iα = −mgL sin θ I = mL α (t ) = −Cθ (t ) 2 mgL g α (t ) = − 2 sin θ → − θ (t ) θ <<1 L mL SHM with period T given by T = L 2π = 2π g C g C= L θ(t) L m θ mg (simple pendulum) • Physical Pendulum: Moment of inertia, I, Length L, mass m, distance from axis of rotation to the center-of-mass, dcm. Calculate the torque about the axis of rotation as follows: mgd cm mgd cm − θ (t ) τ = Iα = −d cm mg sin θ α (t ) = − I sin θ θ→ <<1 I mgd cm α (t ) = −Cθ (t ) C = ω 2 = I I 2π T = = 2 π SHM with period T given by C R. Field 11/7/2013 University of Florida PHY 2053 mgd cm (physical pendulum) Page 6 SHM: Example Problems • A simple harmonic oscillator consists of a block of mass 2 kg attached to a spring of spring constant 200 N/m. If the speed of the block is 40 m/s when the displacement from equilibrium is 3 m, what is the amplitude of the oscillations? Answer: 5m E = kA = mv + kx 1 2 A= 2 1 2 2 x 1 2 A2 = 2 m 2 v x (t ) + x 2 (t ) k m 2 (2kg ) v x (t ) + x 2 (t ) = (40m / s ) 2 + (3m) 2 = 5m k (200 N / m) • A simple pendulum has a length L. If its period is T when it is on the surface of the Earth (gravitational acceleration g ), what is its period when it is on the surface of a planet with gravitational acceleration equal to g/4? Answer: 2T L T = 2π g R. Field 11/7/2013 University of Florida Tnew = 2π L L = 2 × 2π = 2T ( g / 4) g PHY 2053 Page 7 SHM: Example Problems • Two blocks (m = 5 kg and M = 15 kg) and a spring (k = 196 N/m) are arranged on a horizontal frictionless surface. If the smaller block begins to slip when the amplitude of the simple harmonic motion is greater than 0.5 m, what is the coefficient of static friction between the two blocks? Answer: 0.5 f s = ma x ≤ μ s mg μs = R. Field 11/7/2013 University of Florida amax = μ s g 2 amax = ω spring A= k A ( M + m) k 196 N / m A= (0.5m) = 0.5 ( M + m) g (20kg )(9.8m / s ) PHY 2053 Page 8