lecture 18: elasticity and oscillations i l simple harmonic motion: definition l springs: forces l...

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Lecture 18: Lecture 18: Elasticity and Elasticity and Oscillations I Oscillations I Simple Harmonic Motion: Definition Springs: Forces Springs: Energy Simple Harmonic Motion: Equations

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Springs: Forces l Hooke’s Law: l Hooke’s Law: The force exerted by a spring is proportional to the distance the spring is stretched or compressed from its relaxed position. è F X = -k xWhere x is the displacement from the relaxed position and k is the constant of proportionality. relaxed position (equilibrium position) F X = 0 +x x=0

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Page 1: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Lecture 18:Lecture 18: Elasticity and Oscillations I Elasticity and Oscillations I

Simple Harmonic Motion: Definition

Springs: Forces

Springs: Energy

Simple Harmonic Motion: Equations

Page 2: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Simple Harmonic MotionSimple Harmonic Motion

VibrationsVocal cords when singing/speakingString/rubber band

Simple Harmonic MotionRestoring force proportional to displacementSprings: F = -kx

Page 3: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Springs: ForcesSprings: Forces Hooke’s Law:Hooke’s Law: The force exerted by a spring is

proportional to the distance the spring is stretched or compressed from its relaxed position.

FX = -k x Where x is the displacement from the relaxed position and k is the

constant of proportionality.

relaxed position (equilibrium position)

FX = 0+x

x=0

Page 4: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Springs: ForcesSprings: Forces Negative displacement:

Positive forcePositive acceleration

Zero displacement (at equilibrium):Zero forceZero acceleration

Positive displacement:Negative forceNegative acceleration

+x

Page 5: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Springs: EnergySprings: Energy Force of spring is Conservative:

F = -k x W = ½ k x2

Work done only depends on initial and final position.Potential Energy: Uspring = ½ k x2

A mass oscillating on a spring: Energy = U + K = constant

½ k x2 + ½ m v2 = total energym

xx=0

0 x

U

Page 6: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Maximum Negative displacement:Maximum potential energyZero kinetic energy

Zero displacement (at equilibrium):Zero potential energyMaximum kinetic energy

Maximum Positive displacement:Maximum potential energyZero kinetic energy

+x Springs: EnergySprings: Energy

Page 7: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Simple Harmonic MotionSimple Harmonic Motion

x(t) = [A]cos(t)v(t) = -[A]sin(t)a(t) = -[A2]cos(t)

x(t) = [A]sin(t)v(t) = [A]cos(t)a(t) = -[A2]sin(t)

xmax = A

vmax = A

amax = A2

Period = T (seconds per cycle)Frequency = f = 1/T (cycles per

second)Angular frequency = = 2f = 2/TFor spring: 2 = k/m

OR

Page 8: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Spring ExampleSpring Example A mass of m = 4 kg is attached to a spring with k = 16 N/m and

oscillates with an amplitude A = 0.15 m. What is the magnitude of the acceleration of the mass when the potential energy stored in the spring is equal to the kinetic energy of the mass?

First, use energy to find x where U = K:» U + K = constant

Second, use Hooke’s Law to find force on the mass:» F = -k x

Third, use Newton’s Second Law to find acceleration of mass:» F = m a

Page 9: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Spring ExampleSpring Example A mass of m = 4 kg is attached to a spring with k = 16 N/m and

oscillates with an amplitude A = 0.15 m. What is the magnitude of the acceleration of the mass when the potential energy stored in the spring is equal to the kinetic energy of the mass?

First, use energy to find x where U = K:» U + K = constant» U + K = ½ k A2 (since total energy is ½ k A2)» U + U = ½ k A2 (since K = U when they are equal)» k x2 = ½ k A2 (since U = ½ k x2 when they are equal)» x2 = ½ A2 (simplify)

2

21 Ax = 0.106 m

Page 10: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Spring ExampleSpring Example A mass of m = 4 kg is attached to a spring with k = 16 N/m and

oscillates with an amplitude A = 0.15 m. What is the magnitude of the acceleration of the mass when the potential energy stored in the spring is equal to the kinetic energy of the mass?

Second, use Hooke’s Law to find force on the mass:

» F = k x (we are only concerned with magnitude)

2

21 AkF = 1.70 N

Page 11: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Spring ExampleSpring Example A mass of m = 4 kg is attached to a spring with k = 16 N/m and

oscillates with an amplitude A = 0.15 m. What is the magnitude of the acceleration of the mass when the potential energy stored in the spring is equal to the kinetic energy of the mass?

Third, use Newton’s Second Law to find acceleration of mass:

» F = m a (we are only concerned with magnitude)

2

21 A

mka = 0.424 m/s2

Page 12: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

Young’s ModulusYoung’s Modulus Spring F = k x

What happens to “k” if cut spring in half?1) ½ 2) same 3) 2

k is inversely proportional to length! Define

Strain = L / LStress = F/A

NowStress = Y Strain F/A = Y L/Lk = Y A/L from F = k x

Y (Young’s Modules) independent of L

15

Page 13: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

What does moving in a circle have to do with moving back & forth in a straight line ??

y

x

-R

R

0

1 12 2

3 3

4 45 5

6 62

R

8

7

8

7

23

x

Moviex = R cos = R cos (t)

since = t

46

Page 14: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

(A) (B) (C)

Page 15: Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs:…

(A) (B) (C)