SlideShare a Scribd company logo
1 of 8
Damp Oscillation
Tiffany Yang
18422148
•Supposed that a damped mass-spring oscillator
loses 4% of its energy during each cycle. If the
period is 2.0 s, the mass is 0.20 kg, and the initial
amplitude is 0.30m
Question 1: What is the value of the
damping constant
Explanation
• Damped oscillator oscillates at a lower frequency, and the
damped amplitude decreases over time. We combined the
amplitude and a exponential term to express a relationship
between amplitude and time passes.
• Key equation: A(t)=Ae^(-bt/2m)
Calculation:• the initial amplitude is 0.3
• Amplitude of the oscillator
after 1 oscillation: 0.3*(1-
4%)=0.288
• We know that T=2.0, and
mass is= 0.20
• We can then plug in all the
values into the equation:
A(t)=Ae^(-b/m)
0.3*e^(-bt/2m)=0.288
e^(-bt/2m)=0.94
ln94=-bt/2m
b=-2m/t*ln(0.95)
b=-0.20*2/2.0*ln(0.94)
b=0.0124kg/s
Question 2: How many cycles elapsed before
the amplitude reduces to 0.20m?
• We can also apply the key equation A(t)=Ae^(-bt/2m) in this question.
• We can use this equation to calculate the time elapsed.
Calculation of t:
A(t)=Ae^(-bt/(2m))
A(t)/A=e^(-bt/(2m))
ln(0.2/0.3)=-bt/(2m)
ln(3/2)=bt/(2m)
t=ln(2/3)*2m/b
t=2*0.20/(0.0124)*ln(2/3)
t=13.08s
Number of cycle=time/period
•t/T=13.08/2.0
•t/T=6.54
•Therefore, around 6.54cycles elapsed before
amplitude reaches to 0.20
Extended Question(no calculation is
required):
• 1. Would it take the same number of circles to reduce
the amplitude from 0.2 to 0.1?
• 2. How would the number of circles change if you
decrease the damping constant.
Answers:
• 1. No. According to the equation A(t)=Ae^(-bt/2m), the amplitude
decreases exponentially not linear. So it takes different amount of
time to reduce the amplitude from 0.2 to 0.1.
• 2. Number of circles will increase. Damping constant measures the
strength of the drag force. So as you decreases the constant, the drag
force decreases. Number of circles oscillate increases. Also, you can
observe the relationship from the equation A(t)=Ae^(-bt/2m) that t
and k are inversely proportional.

More Related Content

What's hot

Website newton's first and second
Website   newton's first and secondWebsite   newton's first and second
Website newton's first and secondstephm32
 
Standing Waves on a String
Standing Waves on a StringStanding Waves on a String
Standing Waves on a StringIreneNg8
 
Lo2: Damped Oscillations
Lo2: Damped OscillationsLo2: Damped Oscillations
Lo2: Damped OscillationsMichelle Wu
 
13.1.1 Shm Simple Pendulums
13.1.1 Shm Simple Pendulums13.1.1 Shm Simple Pendulums
13.1.1 Shm Simple PendulumsChris Staines
 
Mechanical vibration lab_manual
Mechanical vibration lab_manualMechanical vibration lab_manual
Mechanical vibration lab_manualRajnish kumar
 
derivation of Wave equation
derivation of Wave equationderivation of Wave equation
derivation of Wave equationUCP
 
UBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.Acceleration
UBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.AccelerationUBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.Acceleration
UBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.AccelerationAustere_J
 
Time Independent Perturbation Theory, 1st order correction, 2nd order correction
Time Independent Perturbation Theory, 1st order correction, 2nd order correctionTime Independent Perturbation Theory, 1st order correction, 2nd order correction
Time Independent Perturbation Theory, 1st order correction, 2nd order correctionJames Salveo Olarve
 
Chapter 2 lecture 2 mechanical vibration
Chapter 2  lecture 2 mechanical vibrationChapter 2  lecture 2 mechanical vibration
Chapter 2 lecture 2 mechanical vibrationBahr Alyafei
 
Chapter1
Chapter1Chapter1
Chapter1jluoaa
 
Physics lo1
Physics lo1Physics lo1
Physics lo1book1126
 

What's hot (20)

Website newton's first and second
Website   newton's first and secondWebsite   newton's first and second
Website newton's first and second
 
Lo1
Lo1Lo1
Lo1
 
Standing Waves on a String
Standing Waves on a StringStanding Waves on a String
Standing Waves on a String
 
Lo2: Damped Oscillations
Lo2: Damped OscillationsLo2: Damped Oscillations
Lo2: Damped Oscillations
 
13.1.1 Shm Simple Pendulums
13.1.1 Shm Simple Pendulums13.1.1 Shm Simple Pendulums
13.1.1 Shm Simple Pendulums
 
Wave Motion QA 2
Wave Motion QA 2Wave Motion QA 2
Wave Motion QA 2
 
GENERAL DYNAMICS
GENERAL DYNAMICSGENERAL DYNAMICS
GENERAL DYNAMICS
 
Mechanical vibration lab_manual
Mechanical vibration lab_manualMechanical vibration lab_manual
Mechanical vibration lab_manual
 
The wave equation
The wave equationThe wave equation
The wave equation
 
derivation of Wave equation
derivation of Wave equationderivation of Wave equation
derivation of Wave equation
 
Statics
Statics Statics
Statics
 
Lecture21
Lecture21Lecture21
Lecture21
 
UBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.Acceleration
UBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.AccelerationUBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.Acceleration
UBC.PHYS101.LO2.Simple.Pendulum.in.Uniform.Acceleration
 
All experiments 1
All experiments 1All experiments 1
All experiments 1
 
4Torque
4Torque4Torque
4Torque
 
Time Independent Perturbation Theory, 1st order correction, 2nd order correction
Time Independent Perturbation Theory, 1st order correction, 2nd order correctionTime Independent Perturbation Theory, 1st order correction, 2nd order correction
Time Independent Perturbation Theory, 1st order correction, 2nd order correction
 
Free vibration
Free vibrationFree vibration
Free vibration
 
Chapter 2 lecture 2 mechanical vibration
Chapter 2  lecture 2 mechanical vibrationChapter 2  lecture 2 mechanical vibration
Chapter 2 lecture 2 mechanical vibration
 
Chapter1
Chapter1Chapter1
Chapter1
 
Physics lo1
Physics lo1Physics lo1
Physics lo1
 

Viewers also liked

The dropper effect
The dropper effectThe dropper effect
The dropper effectTiffany Yang
 
Raspberry pi - Node js - Drupal
Raspberry pi - Node js - DrupalRaspberry pi - Node js - Drupal
Raspberry pi - Node js - DrupalMark Corben
 
Lo mine sher l2 e
Lo mine sher l2 eLo mine sher l2 e
Lo mine sher l2 epianomine
 
plagiarism-hacking-software_piracy
plagiarism-hacking-software_piracyplagiarism-hacking-software_piracy
plagiarism-hacking-software_piracyAbhishek Shukla
 
Cromoterapie
CromoterapieCromoterapie
CromoterapieAna-Gri
 
Tipuri de flori
Tipuri de floriTipuri de flori
Tipuri de floriAna-Gri
 
Fenomene
FenomeneFenomene
FenomeneAna-Gri
 
Animalele
AnimaleleAnimalele
AnimaleleAna-Gri
 
Vreausastiu
VreausastiuVreausastiu
VreausastiuAna-Gri
 
Legenda florii soarelui
Legenda florii soareluiLegenda florii soarelui
Legenda florii soareluiAna-Gri
 
секреты привлечения клиентов в условиях кризиса
секреты привлечения клиентов в условиях кризисасекреты привлечения клиентов в условиях кризиса
секреты привлечения клиентов в условиях кризисаDmitry Lisakovskiy
 
Influenta factorilor de_mediu_asupra_corpurilor_cu_viata
Influenta factorilor de_mediu_asupra_corpurilor_cu_viataInfluenta factorilor de_mediu_asupra_corpurilor_cu_viata
Influenta factorilor de_mediu_asupra_corpurilor_cu_viataAna-Gri
 

Viewers also liked (15)

The dropper effect
The dropper effectThe dropper effect
The dropper effect
 
Lo2
Lo2Lo2
Lo2
 
hands-on training certificate
hands-on training certificatehands-on training certificate
hands-on training certificate
 
Raspberry pi - Node js - Drupal
Raspberry pi - Node js - DrupalRaspberry pi - Node js - Drupal
Raspberry pi - Node js - Drupal
 
Lo mine sher l2 e
Lo mine sher l2 eLo mine sher l2 e
Lo mine sher l2 e
 
MVR Profile (+Wave)
MVR Profile (+Wave)MVR Profile (+Wave)
MVR Profile (+Wave)
 
plagiarism-hacking-software_piracy
plagiarism-hacking-software_piracyplagiarism-hacking-software_piracy
plagiarism-hacking-software_piracy
 
Cromoterapie
CromoterapieCromoterapie
Cromoterapie
 
Tipuri de flori
Tipuri de floriTipuri de flori
Tipuri de flori
 
Fenomene
FenomeneFenomene
Fenomene
 
Animalele
AnimaleleAnimalele
Animalele
 
Vreausastiu
VreausastiuVreausastiu
Vreausastiu
 
Legenda florii soarelui
Legenda florii soareluiLegenda florii soarelui
Legenda florii soarelui
 
секреты привлечения клиентов в условиях кризиса
секреты привлечения клиентов в условиях кризисасекреты привлечения клиентов в условиях кризиса
секреты привлечения клиентов в условиях кризиса
 
Influenta factorilor de_mediu_asupra_corpurilor_cu_viata
Influenta factorilor de_mediu_asupra_corpurilor_cu_viataInfluenta factorilor de_mediu_asupra_corpurilor_cu_viata
Influenta factorilor de_mediu_asupra_corpurilor_cu_viata
 

Similar to Damp oscillation

Damped harmonic oscillator - LO2
Damped harmonic oscillator - LO2Damped harmonic oscillator - LO2
Damped harmonic oscillator - LO2preetg92
 
VIBRATIONS AND WAVES TUTORIAL#2
VIBRATIONS AND WAVES TUTORIAL#2VIBRATIONS AND WAVES TUTORIAL#2
VIBRATIONS AND WAVES TUTORIAL#2Farhan Ab Rahman
 
Learning object 1
Learning object 1Learning object 1
Learning object 1Alex Law
 
Travelling Harmonic Waves
Travelling Harmonic Waves Travelling Harmonic Waves
Travelling Harmonic Waves Harley Ma
 
Harley ma learning object
Harley ma learning objectHarley ma learning object
Harley ma learning objectHarley Ma
 
ClassExamplesPeriodicMotionWaves.pdf
ClassExamplesPeriodicMotionWaves.pdfClassExamplesPeriodicMotionWaves.pdf
ClassExamplesPeriodicMotionWaves.pdfPatrickSibanda3
 
Simple Harmonic & Circular Motion
Simple Harmonic & Circular MotionSimple Harmonic & Circular Motion
Simple Harmonic & Circular MotionPaula Mills
 
Fourier Series for Continuous Time & Discrete Time Signals
Fourier Series for Continuous Time & Discrete Time SignalsFourier Series for Continuous Time & Discrete Time Signals
Fourier Series for Continuous Time & Discrete Time SignalsJayanshu Gundaniya
 
2014 st josephs geelong physics lecture
2014 st josephs geelong physics lecture2014 st josephs geelong physics lecture
2014 st josephs geelong physics lectureAndrew Smith
 
Module 4_spring 2020.pdf
Module 4_spring 2020.pdfModule 4_spring 2020.pdf
Module 4_spring 2020.pdfMohammad Javed
 
Topic 2 damped oscillation
Topic 2 damped oscillationTopic 2 damped oscillation
Topic 2 damped oscillationGabriel O'Brien
 
Simple harmonic motion
Simple harmonic motionSimple harmonic motion
Simple harmonic motionaulia rodlia
 
Physics of nuclear medicine.pptx
Physics of nuclear medicine.pptxPhysics of nuclear medicine.pptx
Physics of nuclear medicine.pptxAbdulla866778
 
Waves and oscillation undergraduates .pptx
Waves and oscillation undergraduates .pptxWaves and oscillation undergraduates .pptx
Waves and oscillation undergraduates .pptxrajnishkumar361716
 

Similar to Damp oscillation (20)

Damped harmonic oscillator - LO2
Damped harmonic oscillator - LO2Damped harmonic oscillator - LO2
Damped harmonic oscillator - LO2
 
Maths 3 ppt
Maths 3 pptMaths 3 ppt
Maths 3 ppt
 
VIBRATIONS AND WAVES TUTORIAL#2
VIBRATIONS AND WAVES TUTORIAL#2VIBRATIONS AND WAVES TUTORIAL#2
VIBRATIONS AND WAVES TUTORIAL#2
 
Learning object 1
Learning object 1Learning object 1
Learning object 1
 
Travelling Harmonic Waves
Travelling Harmonic Waves Travelling Harmonic Waves
Travelling Harmonic Waves
 
Harley ma learning object
Harley ma learning objectHarley ma learning object
Harley ma learning object
 
Unit step function
Unit step functionUnit step function
Unit step function
 
ClassExamplesPeriodicMotionWaves.pdf
ClassExamplesPeriodicMotionWaves.pdfClassExamplesPeriodicMotionWaves.pdf
ClassExamplesPeriodicMotionWaves.pdf
 
Simple Harmonic & Circular Motion
Simple Harmonic & Circular MotionSimple Harmonic & Circular Motion
Simple Harmonic & Circular Motion
 
Oscillation & Oscillatory Motion
Oscillation & Oscillatory MotionOscillation & Oscillatory Motion
Oscillation & Oscillatory Motion
 
Vibration lab manual 1
Vibration lab manual 1Vibration lab manual 1
Vibration lab manual 1
 
Fourier Series for Continuous Time & Discrete Time Signals
Fourier Series for Continuous Time & Discrete Time SignalsFourier Series for Continuous Time & Discrete Time Signals
Fourier Series for Continuous Time & Discrete Time Signals
 
unit.pptx
unit.pptxunit.pptx
unit.pptx
 
2014 st josephs geelong physics lecture
2014 st josephs geelong physics lecture2014 st josephs geelong physics lecture
2014 st josephs geelong physics lecture
 
Module 4_spring 2020.pdf
Module 4_spring 2020.pdfModule 4_spring 2020.pdf
Module 4_spring 2020.pdf
 
Physicalquantities
PhysicalquantitiesPhysicalquantities
Physicalquantities
 
Topic 2 damped oscillation
Topic 2 damped oscillationTopic 2 damped oscillation
Topic 2 damped oscillation
 
Simple harmonic motion
Simple harmonic motionSimple harmonic motion
Simple harmonic motion
 
Physics of nuclear medicine.pptx
Physics of nuclear medicine.pptxPhysics of nuclear medicine.pptx
Physics of nuclear medicine.pptx
 
Waves and oscillation undergraduates .pptx
Waves and oscillation undergraduates .pptxWaves and oscillation undergraduates .pptx
Waves and oscillation undergraduates .pptx
 

Damp oscillation

  • 2. •Supposed that a damped mass-spring oscillator loses 4% of its energy during each cycle. If the period is 2.0 s, the mass is 0.20 kg, and the initial amplitude is 0.30m Question 1: What is the value of the damping constant
  • 3. Explanation • Damped oscillator oscillates at a lower frequency, and the damped amplitude decreases over time. We combined the amplitude and a exponential term to express a relationship between amplitude and time passes. • Key equation: A(t)=Ae^(-bt/2m)
  • 4. Calculation:• the initial amplitude is 0.3 • Amplitude of the oscillator after 1 oscillation: 0.3*(1- 4%)=0.288 • We know that T=2.0, and mass is= 0.20 • We can then plug in all the values into the equation: A(t)=Ae^(-b/m) 0.3*e^(-bt/2m)=0.288 e^(-bt/2m)=0.94 ln94=-bt/2m b=-2m/t*ln(0.95) b=-0.20*2/2.0*ln(0.94) b=0.0124kg/s
  • 5. Question 2: How many cycles elapsed before the amplitude reduces to 0.20m? • We can also apply the key equation A(t)=Ae^(-bt/2m) in this question. • We can use this equation to calculate the time elapsed. Calculation of t: A(t)=Ae^(-bt/(2m)) A(t)/A=e^(-bt/(2m)) ln(0.2/0.3)=-bt/(2m) ln(3/2)=bt/(2m) t=ln(2/3)*2m/b t=2*0.20/(0.0124)*ln(2/3) t=13.08s
  • 6. Number of cycle=time/period •t/T=13.08/2.0 •t/T=6.54 •Therefore, around 6.54cycles elapsed before amplitude reaches to 0.20
  • 7. Extended Question(no calculation is required): • 1. Would it take the same number of circles to reduce the amplitude from 0.2 to 0.1? • 2. How would the number of circles change if you decrease the damping constant.
  • 8. Answers: • 1. No. According to the equation A(t)=Ae^(-bt/2m), the amplitude decreases exponentially not linear. So it takes different amount of time to reduce the amplitude from 0.2 to 0.1. • 2. Number of circles will increase. Damping constant measures the strength of the drag force. So as you decreases the constant, the drag force decreases. Number of circles oscillate increases. Also, you can observe the relationship from the equation A(t)=Ae^(-bt/2m) that t and k are inversely proportional.