SlideShare una empresa de Scribd logo
1 de 11
STANDING WAVES
Sections 14.2 & 14.3 of the text
By: Harkirat Dhaliwal
WHAT ARE STANDING
WAVES?
A standing wave is a vibration of a system in which some
particular points remain fixed (such as frequency), while
other points vibrate with a maximum amplitude.
WHAT ARE NODES AND
ANTINODES?
Points of no displacement in a standing wave pattern are
referred to as nodes.
Points of maximum displacement are known as antinodes.
Exact location of nodes of a standing wave can be found
using the equation: x= m(wavelength/2) where m is 0, +-1,
+-2……..
Exact location of antinodes can be found using the equation
x = (m+0.5)(wavelength/2) where m is 0, +-1, +-2………
QUESTION 1
On the diagram above, which of the labels represents an
antinode?
A
B
C
A
B
C
QUESTION 1
On the diagram above, which of the labels represents an
antinode?
A -is the correct answer as it represents the
maximum displacement of the standing
wave
A
B
C
AMPLITUDE OF STANDING
WAVE
Amplitude of a standing wave is position dependent.
It is represented by the formula :
A(x) = 2Asin(kx) = 2A sin(2pi(x)/wavelength)
QUESTION 2
The amplitude of a standing wave is given by:
A(x) = (32.0cm)sin(4.00x)
a) Determine the amplitude and wavelength of the travelling
waves.
b) Determine the location of the first 2 nodes and first 2
antinodes along the positive x-axis.
c) Determine the first point from the origin where the
amplitude is 0.20m.
QUESTION 2-SOLUTION
A(x) = 2Asin(kx) = 2A sin(2pi(x)/wavelength)
A(x) = (32.0cm)sin(4.00x)
a) So according to equation above: 2A= 32.0 cm, so A= 32.0/2= 16.0 cm (amplitude)
Wavelength: 2pi/wavelength= 4.00 rad/m
2pi= 4 x wavelength
2pi/4 = wavelength
pi/2 m= wavelength
QUESTION 2- SOLUTION
CONTINUED
b) First 2 nodes occur when sin(2pi(x)/wavelength)= 0.
2pix/wavelength= mpi (where m= 0, 1, 2..)
x= m (wavelength/2)= m((pi/2)/2)
when m= 0, x=0m
when m=1, x= pi/2 x (1/2)= pi/4 m
So first 2 nodes occur at 0 m & 0.785 m.
QUESTION 2-SOLUTION
CONTINUED
c) Set amplitude= 0.20 m and solve for x
0.20 m= (0.32m) sin(4.00x)
0.20/0.32= sin(4.00x)
0.625m= sin(4.00x)
sin^-1(0.625) (sin inverse) = 4.00x
0.675 rad= 4x
0.675/4= x= 0.17 m
THANK YOU!

Más contenido relacionado

La actualidad más candente

Important Notes - JEE - Physics - Simple Harmonic Motion
Important Notes - JEE - Physics - Simple Harmonic MotionImportant Notes - JEE - Physics - Simple Harmonic Motion
Important Notes - JEE - Physics - Simple Harmonic MotionEdnexa
 
Application of laplace wave equation in music
Application of laplace wave equation in musicApplication of laplace wave equation in music
Application of laplace wave equation in musicLuckshay Batra
 
Applications of schrodinger equation
Applications of schrodinger equationApplications of schrodinger equation
Applications of schrodinger equationZalman Ali
 
Concepts and Problems in Quantum Mechanics, Lecture-II By Manmohan Dash
Concepts and Problems in Quantum Mechanics, Lecture-II By Manmohan DashConcepts and Problems in Quantum Mechanics, Lecture-II By Manmohan Dash
Concepts and Problems in Quantum Mechanics, Lecture-II By Manmohan DashManmohan Dash
 
Small amplitude oscillations
Small amplitude oscillationsSmall amplitude oscillations
Small amplitude oscillationsharshsharma5537
 
Simple harmonic oscillator - Classical Mechanics
Simple harmonic oscillator - Classical MechanicsSimple harmonic oscillator - Classical Mechanics
Simple harmonic oscillator - Classical MechanicsDebashis Baidya
 
Chapter 2 lecture 2 mechanical vibration
Chapter 2  lecture 2 mechanical vibrationChapter 2  lecture 2 mechanical vibration
Chapter 2 lecture 2 mechanical vibrationBahr Alyafei
 
Lagrangian Mechanics
Lagrangian MechanicsLagrangian Mechanics
Lagrangian MechanicsAmeenSoomro1
 
Maths partial differential equation Poster
Maths partial differential equation PosterMaths partial differential equation Poster
Maths partial differential equation PosterEr. Ashish Pandey
 
Physics Quantum mechanics
Physics Quantum mechanicsPhysics Quantum mechanics
Physics Quantum mechanics2569294Mohan
 
On Application of Unbounded Hilbert Linear Operators in Quantum Mechanics
On Application of Unbounded Hilbert Linear Operators in Quantum MechanicsOn Application of Unbounded Hilbert Linear Operators in Quantum Mechanics
On Application of Unbounded Hilbert Linear Operators in Quantum MechanicsBRNSS Publication Hub
 
Electromagnetic oscillation
Electromagnetic oscillationElectromagnetic oscillation
Electromagnetic oscillationMumuKhan1
 
Structure Design-I (Moments)
Structure Design-I (Moments)Structure Design-I (Moments)
Structure Design-I (Moments)Simran Vats
 
Bound states in 1d, 2d and 3d quantum wells
Bound states in 1d, 2d and 3d quantum wellsBound states in 1d, 2d and 3d quantum wells
Bound states in 1d, 2d and 3d quantum wellsAhmed Aslam
 
Schrödinger wave equation
Schrödinger wave equationSchrödinger wave equation
Schrödinger wave equationHARSHWALIA9
 

La actualidad más candente (20)

Important Notes - JEE - Physics - Simple Harmonic Motion
Important Notes - JEE - Physics - Simple Harmonic MotionImportant Notes - JEE - Physics - Simple Harmonic Motion
Important Notes - JEE - Physics - Simple Harmonic Motion
 
Application of laplace wave equation in music
Application of laplace wave equation in musicApplication of laplace wave equation in music
Application of laplace wave equation in music
 
Applications of schrodinger equation
Applications of schrodinger equationApplications of schrodinger equation
Applications of schrodinger equation
 
Concepts and Problems in Quantum Mechanics, Lecture-II By Manmohan Dash
Concepts and Problems in Quantum Mechanics, Lecture-II By Manmohan DashConcepts and Problems in Quantum Mechanics, Lecture-II By Manmohan Dash
Concepts and Problems in Quantum Mechanics, Lecture-II By Manmohan Dash
 
Small amplitude oscillations
Small amplitude oscillationsSmall amplitude oscillations
Small amplitude oscillations
 
Cross Section
Cross SectionCross Section
Cross Section
 
Lecture19
Lecture19Lecture19
Lecture19
 
Simple harmonic oscillator - Classical Mechanics
Simple harmonic oscillator - Classical MechanicsSimple harmonic oscillator - Classical Mechanics
Simple harmonic oscillator - Classical Mechanics
 
schrodinger equation Pooja
schrodinger equation Poojaschrodinger equation Pooja
schrodinger equation Pooja
 
Chapter 2 lecture 2 mechanical vibration
Chapter 2  lecture 2 mechanical vibrationChapter 2  lecture 2 mechanical vibration
Chapter 2 lecture 2 mechanical vibration
 
Lagrangian Mechanics
Lagrangian MechanicsLagrangian Mechanics
Lagrangian Mechanics
 
Quantum
QuantumQuantum
Quantum
 
Maths partial differential equation Poster
Maths partial differential equation PosterMaths partial differential equation Poster
Maths partial differential equation Poster
 
Physics Quantum mechanics
Physics Quantum mechanicsPhysics Quantum mechanics
Physics Quantum mechanics
 
Vector Calculus.
Vector Calculus.Vector Calculus.
Vector Calculus.
 
On Application of Unbounded Hilbert Linear Operators in Quantum Mechanics
On Application of Unbounded Hilbert Linear Operators in Quantum MechanicsOn Application of Unbounded Hilbert Linear Operators in Quantum Mechanics
On Application of Unbounded Hilbert Linear Operators in Quantum Mechanics
 
Electromagnetic oscillation
Electromagnetic oscillationElectromagnetic oscillation
Electromagnetic oscillation
 
Structure Design-I (Moments)
Structure Design-I (Moments)Structure Design-I (Moments)
Structure Design-I (Moments)
 
Bound states in 1d, 2d and 3d quantum wells
Bound states in 1d, 2d and 3d quantum wellsBound states in 1d, 2d and 3d quantum wells
Bound states in 1d, 2d and 3d quantum wells
 
Schrödinger wave equation
Schrödinger wave equationSchrödinger wave equation
Schrödinger wave equation
 

Similar a Standing Waves LO

Standing waves Explanation in Depth
Standing waves Explanation in DepthStanding waves Explanation in Depth
Standing waves Explanation in DepthRick Grootes
 
Standing waves
Standing wavesStanding waves
Standing wavesJenny He
 
Harmonic waves
Harmonic wavesHarmonic waves
Harmonic wavesJenny He
 
Janzen hui lo2 standing waves
Janzen hui lo2   standing wavesJanzen hui lo2   standing waves
Janzen hui lo2 standing wavesJanzen Hui
 
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...Pooja M
 
Standing waves
Standing wavesStanding waves
Standing wavesdegaa
 
Harmonic waves
Harmonic wavesHarmonic waves
Harmonic wavesAlison Wu
 
Learning objects 1
Learning objects 1Learning objects 1
Learning objects 1Bowen Zhu
 
Standing Waves on a String
Standing Waves on a StringStanding Waves on a String
Standing Waves on a Stringayshaab
 
Harmonic Waves
Harmonic WavesHarmonic Waves
Harmonic WavesRyan Koon
 
Standing Waves on a String
Standing Waves on a String Standing Waves on a String
Standing Waves on a String Alykhan Devsi
 
Standing Waves LO6 physics 101- Alvin Parappilly
Standing Waves LO6 physics 101- Alvin ParappillyStanding Waves LO6 physics 101- Alvin Parappilly
Standing Waves LO6 physics 101- Alvin ParappillyAlvin Parappilly
 

Similar a Standing Waves LO (20)

Lo 2
Lo 2Lo 2
Lo 2
 
Standing waves Explanation in Depth
Standing waves Explanation in DepthStanding waves Explanation in Depth
Standing waves Explanation in Depth
 
Lo6
Lo6Lo6
Lo6
 
Standing waves
Standing wavesStanding waves
Standing waves
 
Harmonic waves
Harmonic wavesHarmonic waves
Harmonic waves
 
Janzen hui lo2 standing waves
Janzen hui lo2   standing wavesJanzen hui lo2   standing waves
Janzen hui lo2 standing waves
 
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
 
Standing waves
Standing wavesStanding waves
Standing waves
 
Standing Waves
Standing WavesStanding Waves
Standing Waves
 
Chapter 3 wave_optics
Chapter 3 wave_opticsChapter 3 wave_optics
Chapter 3 wave_optics
 
Harmonic waves
Harmonic wavesHarmonic waves
Harmonic waves
 
Wave Motion Theory 6/ Advanced Theory
Wave Motion Theory 6/ Advanced TheoryWave Motion Theory 6/ Advanced Theory
Wave Motion Theory 6/ Advanced Theory
 
15Waves ppt 1.pdf
15Waves ppt 1.pdf15Waves ppt 1.pdf
15Waves ppt 1.pdf
 
Learning objects 1
Learning objects 1Learning objects 1
Learning objects 1
 
Standing Waves on a String
Standing Waves on a StringStanding Waves on a String
Standing Waves on a String
 
Harmonic Waves
Harmonic WavesHarmonic Waves
Harmonic Waves
 
Standing wave lo5
Standing wave lo5Standing wave lo5
Standing wave lo5
 
Standing Waves on a String
Standing Waves on a String Standing Waves on a String
Standing Waves on a String
 
Standing Waves LO6 physics 101- Alvin Parappilly
Standing Waves LO6 physics 101- Alvin ParappillyStanding Waves LO6 physics 101- Alvin Parappilly
Standing Waves LO6 physics 101- Alvin Parappilly
 
Ch16 ssm
Ch16 ssmCh16 ssm
Ch16 ssm
 

Último

Pests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdfPests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdfPirithiRaju
 
GBSN - Biochemistry (Unit 1)
GBSN - Biochemistry (Unit 1)GBSN - Biochemistry (Unit 1)
GBSN - Biochemistry (Unit 1)Areesha Ahmad
 
module for grade 9 for distance learning
module for grade 9 for distance learningmodule for grade 9 for distance learning
module for grade 9 for distance learninglevieagacer
 
9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service
9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service
9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Servicenishacall1
 
Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...
Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...
Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...Sérgio Sacani
 
GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)Areesha Ahmad
 
FAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and SpectrometryFAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and SpectrometryAlex Henderson
 
Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...
Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...
Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...Monika Rani
 
Nightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43b
Nightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43bNightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43b
Nightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43bSérgio Sacani
 
9654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 6000
9654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 60009654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 6000
9654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 6000Sapana Sha
 
Chemistry 4th semester series (krishna).pdf
Chemistry 4th semester series (krishna).pdfChemistry 4th semester series (krishna).pdf
Chemistry 4th semester series (krishna).pdfSumit Kumar yadav
 
Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)
Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)
Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)Joonhun Lee
 
Call Girls Alandi Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Alandi Call Me 7737669865 Budget Friendly No Advance BookingCall Girls Alandi Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Alandi Call Me 7737669865 Budget Friendly No Advance Bookingroncy bisnoi
 
Hire 💕 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire 💕 9907093804 Hooghly Call Girls Service Call Girls AgencyHire 💕 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire 💕 9907093804 Hooghly Call Girls Service Call Girls AgencySheetal Arora
 
GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...
GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...
GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...Lokesh Kothari
 
SCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptx
SCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptxSCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptx
SCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptxRizalinePalanog2
 
Botany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdfBotany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdfSumit Kumar yadav
 
Factory Acceptance Test( FAT).pptx .
Factory Acceptance Test( FAT).pptx       .Factory Acceptance Test( FAT).pptx       .
Factory Acceptance Test( FAT).pptx .Poonam Aher Patil
 
Nanoparticles synthesis and characterization​ ​
Nanoparticles synthesis and characterization​  ​Nanoparticles synthesis and characterization​  ​
Nanoparticles synthesis and characterization​ ​kaibalyasahoo82800
 

Último (20)

Pests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdfPests of cotton_Sucking_Pests_Dr.UPR.pdf
Pests of cotton_Sucking_Pests_Dr.UPR.pdf
 
GBSN - Biochemistry (Unit 1)
GBSN - Biochemistry (Unit 1)GBSN - Biochemistry (Unit 1)
GBSN - Biochemistry (Unit 1)
 
module for grade 9 for distance learning
module for grade 9 for distance learningmodule for grade 9 for distance learning
module for grade 9 for distance learning
 
9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service
9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service
9999266834 Call Girls In Noida Sector 22 (Delhi) Call Girl Service
 
Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...
Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...
Discovery of an Accretion Streamer and a Slow Wide-angle Outflow around FUOri...
 
GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)GBSN - Microbiology (Unit 1)
GBSN - Microbiology (Unit 1)
 
CELL -Structural and Functional unit of life.pdf
CELL -Structural and Functional unit of life.pdfCELL -Structural and Functional unit of life.pdf
CELL -Structural and Functional unit of life.pdf
 
FAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and SpectrometryFAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
FAIRSpectra - Enabling the FAIRification of Spectroscopy and Spectrometry
 
Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...
Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...
Vip profile Call Girls In Lonavala 9748763073 For Genuine Sex Service At Just...
 
Nightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43b
Nightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43bNightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43b
Nightside clouds and disequilibrium chemistry on the hot Jupiter WASP-43b
 
9654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 6000
9654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 60009654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 6000
9654467111 Call Girls In Raj Nagar Delhi Short 1500 Night 6000
 
Chemistry 4th semester series (krishna).pdf
Chemistry 4th semester series (krishna).pdfChemistry 4th semester series (krishna).pdf
Chemistry 4th semester series (krishna).pdf
 
Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)
Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)
Feature-aligned N-BEATS with Sinkhorn divergence (ICLR '24)
 
Call Girls Alandi Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Alandi Call Me 7737669865 Budget Friendly No Advance BookingCall Girls Alandi Call Me 7737669865 Budget Friendly No Advance Booking
Call Girls Alandi Call Me 7737669865 Budget Friendly No Advance Booking
 
Hire 💕 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire 💕 9907093804 Hooghly Call Girls Service Call Girls AgencyHire 💕 9907093804 Hooghly Call Girls Service Call Girls Agency
Hire 💕 9907093804 Hooghly Call Girls Service Call Girls Agency
 
GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...
GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...
GUIDELINES ON SIMILAR BIOLOGICS Regulatory Requirements for Marketing Authori...
 
SCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptx
SCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptxSCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptx
SCIENCE-4-QUARTER4-WEEK-4-PPT-1 (1).pptx
 
Botany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdfBotany 4th semester file By Sumit Kumar yadav.pdf
Botany 4th semester file By Sumit Kumar yadav.pdf
 
Factory Acceptance Test( FAT).pptx .
Factory Acceptance Test( FAT).pptx       .Factory Acceptance Test( FAT).pptx       .
Factory Acceptance Test( FAT).pptx .
 
Nanoparticles synthesis and characterization​ ​
Nanoparticles synthesis and characterization​  ​Nanoparticles synthesis and characterization​  ​
Nanoparticles synthesis and characterization​ ​
 

Standing Waves LO

  • 1. STANDING WAVES Sections 14.2 & 14.3 of the text By: Harkirat Dhaliwal
  • 2. WHAT ARE STANDING WAVES? A standing wave is a vibration of a system in which some particular points remain fixed (such as frequency), while other points vibrate with a maximum amplitude.
  • 3. WHAT ARE NODES AND ANTINODES? Points of no displacement in a standing wave pattern are referred to as nodes. Points of maximum displacement are known as antinodes. Exact location of nodes of a standing wave can be found using the equation: x= m(wavelength/2) where m is 0, +-1, +-2…….. Exact location of antinodes can be found using the equation x = (m+0.5)(wavelength/2) where m is 0, +-1, +-2………
  • 4. QUESTION 1 On the diagram above, which of the labels represents an antinode? A B C A B C
  • 5. QUESTION 1 On the diagram above, which of the labels represents an antinode? A -is the correct answer as it represents the maximum displacement of the standing wave A B C
  • 6. AMPLITUDE OF STANDING WAVE Amplitude of a standing wave is position dependent. It is represented by the formula : A(x) = 2Asin(kx) = 2A sin(2pi(x)/wavelength)
  • 7. QUESTION 2 The amplitude of a standing wave is given by: A(x) = (32.0cm)sin(4.00x) a) Determine the amplitude and wavelength of the travelling waves. b) Determine the location of the first 2 nodes and first 2 antinodes along the positive x-axis. c) Determine the first point from the origin where the amplitude is 0.20m.
  • 8. QUESTION 2-SOLUTION A(x) = 2Asin(kx) = 2A sin(2pi(x)/wavelength) A(x) = (32.0cm)sin(4.00x) a) So according to equation above: 2A= 32.0 cm, so A= 32.0/2= 16.0 cm (amplitude) Wavelength: 2pi/wavelength= 4.00 rad/m 2pi= 4 x wavelength 2pi/4 = wavelength pi/2 m= wavelength
  • 9. QUESTION 2- SOLUTION CONTINUED b) First 2 nodes occur when sin(2pi(x)/wavelength)= 0. 2pix/wavelength= mpi (where m= 0, 1, 2..) x= m (wavelength/2)= m((pi/2)/2) when m= 0, x=0m when m=1, x= pi/2 x (1/2)= pi/4 m So first 2 nodes occur at 0 m & 0.785 m.
  • 10. QUESTION 2-SOLUTION CONTINUED c) Set amplitude= 0.20 m and solve for x 0.20 m= (0.32m) sin(4.00x) 0.20/0.32= sin(4.00x) 0.625m= sin(4.00x) sin^-1(0.625) (sin inverse) = 4.00x 0.675 rad= 4x 0.675/4= x= 0.17 m