Assignment 1 Acoustics.

Slides:



Advertisements
Similar presentations
Angelo Farina Dip. di Ingegneria Industriale - Università di Parma Parco Area delle Scienze 181/A, Parma – Italy
Advertisements

Coulomb or Dry Friction Damping.
The Asymptotic Ray Theory
10/31/2013PHY 113 C Fall Lecture 181 PHY 113 C General Physics I 11 AM -12:15 PM TR Olin 101 Plan for Lecture 18: Chapter 17 – Sound Waves, Doppler.
Chapter 17 Compressible Flow Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel and.
Types, characteristics, properties
EEE 498/598 Overview of Electrical Engineering
Dr. Jie ZouPHY Chapter 17 Sound Waves. Dr. Jie ZouPHY Outline Sound waves in general Speed of sound waves Periodic sound waves Displacement.
Chapter 14 Sound AP Physics B Lecture Notes.
Chapter 17 Sound Waves. Introduction to Sound Waves Waves can move through three-dimensional bulk media. Sound waves are longitudinal waves. They travel.
It was assumed that the pressureat the lips is zero and the volume velocity source is ideal  no energy loss at the input and output. For radiation impedance:
1 Fall 2004 Physics 3 Tu-Th Section Claudio Campagnari Lecture 3: 30 Sep Web page:
Moza m. Al-Rabban Associate Professor of Physics
1 Sinusoidal Waves The waves produced in SHM are sinusoidal, i.e., they can be described by a sine or cosine function with appropriate amplitude, frequency,
Physics of Sound Wave equation: Part. diff. equation relating pressure and velocity as a function of time and space Nonlinear contributions are not considered.
Waves on a Flat Surface of Discontinuity
Phy 212: General Physics II
Ch 3.9: Forced Vibrations We continue the discussion of the last section, and now consider the presence of a periodic external force:
Chapter 3: Sound Wave Intensity of Periodic Sound Waves
Some general properties of waves. Summing waves The wave equation is linear A sum of waves will be the arithmetical sum of the function representing them.
Ch. 5 - Basic Definitions Specific intensity/mean intensity Flux
Waves.
Reflection A wave is reflected when it comes into contact with a barrier A wave is reflected when it comes into contact with a barrier Law of Reflection.
Laws of Radiation Heat Transfer P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Macro Description of highly complex Wave.
Physics Jeopardy 2nd Trimester Review
1 ECE 480 Wireless Systems Lecture 3 Propagation and Modulation of RF Waves.
Oscillations & Waves IB Physics. Simple Harmonic Motion Oscillation 4. Physics. a. an effect expressible as a quantity that repeatedly and regularly.
Chapter 13 - Sound 13.1 Sound Waves.
Separate branches of Mechanics and Biomechanics I. Periodic Motion. Mechanical waves. Acoustics.
Chapter 17 Sound Waves: part one. Introduction to Sound Waves Sound waves are longitudinal waves They travel through any material medium The speed of.
Chapter 15: Wave Motion 15-3 Energy Transported by Waves 15-4 Mathematical Representation of a Traveling Wave 15-5 The Wave Equation 15-6 The Principle.
Physics 1B03summer-Lecture 10 Today’s Lecture… … will start at 10:30am (and end at regular time)
Chapter 17 Sound Waves: part two HW 2 (problems): 17.22, 17.35, 17.48, 17.58, 17.64, 34.4, 34.7, Due Friday, Sept. 11.
Types of Traveling Waves
Chapter 11 Vibrations and Waves. Units of Chapter 11 Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Period and Sinusoidal Nature.
Instructor: M Sc. Eng. Nagham Ali Hasan 2 nd semester 2008/2009 University of Palestine College of Applied Engineering & Urban Planning Department of Architecture,
Oscillations About Equilibrium. 7.1 Periodic Motion.
April Second Order Systems m Spring force ky F(t) (proportional to velocity) (proportional to displacement)
Electromagnetic Waves and Their Propagation Through the Atmosphere
Mechanics Electricity & Magnetism Thermal & Modern.
The elastic wave equationSeismology and the Earth’s Deep Interior The Elastic Wave Equation  Elastic waves in infinite homogeneous isotropic media 
Waves - II Chapter 17 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
200 Physics Concepts from Delores Gende Website
Sound Waves Vibration of a tuning fork
Chapter 26 Lecture 22: Current: II
Lecture 21-22: Sound Waves in Fluids Sound in ideal fluid Sound in real fluid. Attenuation of the sound waves 1.
Oscillations About Equilibrium. 7.1 Periodic Motion.
Chapters 16, 17 Waves.
Chapter 11 Vibrations and Waves.
Sources (EM waves) 1.
Chapter 12 Sound Producing a Sound Wave Characteristics of Sound Waves The Speed of Sound Spherical and Plane Waves The.
1 Linear Wave Equation The maximum values of the transverse speed and transverse acceleration are v y, max =  A a y, max =  2 A The transverse speed.
EE Audio Signals and Systems Wave Basics Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
Ch 1.1: Basic Mathematical Models; Direction Fields Differential equations are equations containing derivatives. The following are examples of physical.
Chapter 12 Preview Objectives The Production of Sound Waves
Chapter 15: Wave Motion 15-2 Types of Waves: Transverse and Longitudinal 15-3 Energy Transported by Waves 15-4 Mathematical Representation of a Traveling.
Flow of Compressible Fluids. Definition A compressible flow is a flow in which the fluid density ρ varies significantly within the flowfield. Therefore,
Physics Mrs. Dimler SOUND.  Every sound wave begins with a vibrating object, such as the vibrating prong of a tuning fork. Tuning fork and air molecules.
Sound Waves  Sound is a longitudinal wave, meaning that the motion of particles is along the direction of propagation.  sound waves are divided into.
Chapter 17 Sound Waves 17.1 Pressure variation in Sound Waves 17.2 speed of Sound Waves 17.3 Intensity of Periodic Sound Waves 17.4 The Doppler Effect.
1 10. Harmonic oscillator Simple harmonic motion Harmonic oscillator is an example of periodic motion, where the displacement of a particle from.
Physics Section 11.3 Apply the properties of waves A wave is a periodic disturbance that transfers energy by the vibration of matter, rather than the transfer.
Momentum Equation and its Applications
The nature of radiation
Chapter 17 Sound Waves.
Lecture 11 WAVE.
Muffler Basics.
UNIT - 4 HEAT TRANSFER.
ENE 325 Electromagnetic Fields and Waves
D. GASES General Gas Law Kinetic Theory.
Presentation transcript:

Assignment 1 Acoustics

1. Which of the following options represent a sound source moving with speed of sound? (In the figures, green dot represents source and brown circles represent sound waves.) C A B D

2. Which of the following waves requires presence of a material medium for propagation? Light. Sound. X rays. Infrared rays.

3. Which of the following equations is nonlinear in ‘𝒚’ or ‘𝒙’ ? 𝜕𝑦 𝜕𝑡 =2 𝜕𝑥 𝜕𝑡 + 3 . 𝜕 4 𝑦 𝜕 𝑡 4 =2 𝜕 4 𝑥 𝜕 𝑡 4 + 3 . 𝜕𝑦 𝜕𝑡 2 =2 𝜕 2 𝑥 𝜕 𝑡 2 + 3 . 𝑦=7𝑥+9 .

4. Consider a differential equation, 𝒗 𝒊 =𝑹𝑪 𝒅 𝒗 𝒄 𝒅𝒕 + 𝒗 𝒄 4. Consider a differential equation, 𝒗 𝒊 =𝑹𝑪 𝒅 𝒗 𝒄 𝒅𝒕 + 𝒗 𝒄 . Here, 𝒗 𝒄 and 𝒗 𝒊 are functions of time and all other terms are constant. Which of the following statements is true about homogeneous and particular response of the system represented by above differential equation? Homogeneous response decays with time and particular response gives steady state solution. Both homogeneous and particular responses decay with time. Both homogeneous and particular responses grow with time. Homogeneous response gives steady state solution and particular response decays with time.

5. Consider a signal, 𝒙 𝒕 =𝑹𝒆 𝑨 𝒆 𝝅 𝟒 +𝑩−𝒋𝑪 𝒋 𝒕 5. Consider a signal, 𝒙 𝒕 =𝑹𝒆 𝑨 𝒆 𝝅 𝟒 +𝑩−𝒋𝑪 𝒋 𝒕 . What can we conclude about decay or growth of 𝒙(𝒕) ? (A,B and C are positive constants) 𝑥 𝑡 will decay with rate of decay B. 𝑥 𝑡 will grow with rate of growth B. 𝑥 𝑡 will decay with rate of decay C. 𝑥 𝑡 will grow with rate of growth C.

6. Which of the following systems decays fastest? Under damped system. Critically damped system. Over damped system. Both over damped and underdamped.

7. Which of the following statements is not true about Bode plots? Help to study linear systems. They are plots of the time response of a linear system. Shows asymptotic behavior of a transfer function. Not used for nonlinear systems

8. Which of the following is true about the axes for Bode phase plots? x-axis y-axis a) b) c) d)

9. Which physical quantity is used to characterize sound pressure level in dB? Amplitude of pressure produced due to pressure wave, radiated to atmosphere with rest pressure Po. Amplitude of absolute pressure in atmosphere when sound is produced. RMS value of pressure produced due to pressure wave radiated to atmosphere with rest pressure Po. RMS value of absolute pressure produced in atmosphere when sound is produced.

10. Which of the following options is not required for deriving the 1-D Wave Equation? Newton’s 2nd law of motion. Conservation of mass. Equilibrium of moment. Gas law.

11. The linearized equation of momentum for 1D wave propagation is_______? 𝜕𝑝 𝜕𝑥 = 𝜌 𝑜 𝜕𝑢 𝜕𝑡 . 𝜕𝑝 𝜕𝑥 = −𝜌 𝑜 𝜕𝑢 𝜕𝑡 . 𝜕𝑢 𝜕𝑥 = 𝜌 𝑜 𝜕𝑝 𝜕𝑡 . 𝜕𝑢 𝜕𝑥 = −𝜌 𝑜 𝜕𝑝 𝜕𝑡 .

12. Which of the following thermodynamic processes accurately captures the behavior of gas when an acoustic wave passes through it? Isobaric process. Isochoric process. Isothermal process. Adiabatic process.

13. _____ is the expression for speed of sound in fluids? 𝑐= 𝛾 𝑝 𝑜 𝜌 𝑜 . 𝑐= 𝑝 𝑜 𝛾𝜌 𝑜 . 𝑐= 𝛾 𝑝 𝑜 2 𝜌 𝑜 . 𝑐= 2 𝑝 𝑜 𝛾 𝜌 𝑜 .

14. Which of the following options can be a suitable solution for the wave equation, 𝝏 𝟐 𝒑 𝝏 𝒙 𝟐 = 𝟏 𝒄 𝟐 𝝏 𝟐 𝒑 𝝏 𝒕 𝟐 ? 𝑓 𝑡− 𝑥 𝑐 . 𝑓(𝑡+ 𝑥 𝑐 ). Both a) and b). None of the above.

15. Which of the following statements can be made for an infinitely long tube excited by a piston, for the position x=0? P+ = P- P+ = -P- P- = 0 P+ = 0 x=0

16. Which of the following relations explicitly shows that ‘c’ represents the speed of sound wave? 𝜕 2 𝑝 𝜕 𝑥 2 = 1 𝑐 2 𝜕 2 𝑝 𝜕 𝑡 2 𝑐= 𝛾 𝑝 𝑜 𝜌 𝑜 𝑐= 𝑝 𝑜 𝛾𝜌 𝑜 𝑝 𝑥,𝑡 =𝑓 𝑡− 𝑥 𝑐 +𝑓 𝑡+ 𝑥 𝑐

17. Which of the following is the transmission line equation for 1-D planar sound waves propagating in loss-less medium? 𝑝(𝑥,𝑡) 𝑢(𝑥,𝑡) = 𝑃 + 𝑃 − 𝑃 + 𝑧 𝑜 𝑃 − 𝑧 𝑜 𝑒 − 𝑠𝑥 𝑐 𝑒 𝑠𝑥 𝑐 𝑒 𝑠𝑡 𝑝(𝑥,𝑡) 𝑢(𝑥,𝑡) = 𝑃 + 𝑃 − 𝑃 + 𝑧 𝑜 − 𝑃 − 𝑧 𝑜 𝑒 − 𝑠𝑥 𝑐 𝑒 𝑠𝑥 𝑐 𝑒 𝑠𝑡 𝑝(𝑥,𝑡) 𝑢(𝑥,𝑡) = 𝑃 + − 𝑃 − 𝑃 + 𝑧 𝑜 𝑃 − 𝑧 𝑜 𝑒 − 𝑠𝑥 𝑐 𝑒 𝑠𝑥 𝑐 𝑒 𝑠𝑡 𝑝(𝑥,𝑡) 𝑢(𝑥,𝑡) = 𝑃 + − 𝑃 − 𝑃 + 𝑧 𝑜 − 𝑃 − 𝑧 𝑜 × 𝑒 − 𝑠𝑥 𝑐 𝑒 𝑠𝑥 𝑐 × 𝑒 𝑠𝑡

18. Which of the following acoustical property varies with position in a medium? Driving point impedance Specific acoustic impedance Characteristic impedance Options ‘a’ and ‘b’

19. Which of the following instruments can be used for characterizing acoustic properties of a material? Kundt’s tube. Seismometer. Muffler. Accelerometer.

20. The definition of standing wave ratio(𝝆) is: 𝜌= 𝑚𝑖𝑛𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 𝑚𝑎𝑥𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 𝜌= 𝑚𝑎𝑥𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 𝑚𝑖𝑛𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 𝜌= 2×𝑚𝑖𝑛𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 𝑚𝑎𝑥𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 𝜌= 𝑚𝑖𝑛𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒 2×𝑚𝑎𝑥𝑖𝑚𝑢𝑚 𝑝𝑟𝑒𝑠𝑠𝑢𝑟𝑒 𝑎𝑚𝑝𝑙𝑖𝑡𝑢𝑑𝑒

21. If the Which of the following is the appropriate statement about the velocity of sound derived by assuming adiabatic and isothermal processes? Velocity of sound derived with adiabatic process is higher than that of isothermal process. Velocity of sound derived with adiabatic process is lower than that of isothermal process. Velocity of sound derived with adiabatic process is equal to that of isothermal process. Velocity of sound derived with adiabatic process may be higher or lower than that of isothermal process.

Cross sectional Area = Ao 22. A cylinder-piston arrangement is at its equilibrium position. If we give a small disturbance to piston, the gas in the cylinder will act as spring. What will be the expression for the spring stiffness of such a spring? Assume that the volume of gas in the cylinder, when the piston is in equilibrium is 𝑽𝑶. Volume = Vo Cross sectional Area = Ao Piston Cylinder 𝐾= 𝑑𝑝 𝑑𝑉 𝑉 𝑜 2 𝐾= 𝑑𝑝 𝑑𝑉 𝐴 2 𝐾= 𝑑𝑝 𝑑𝑉 𝐴 −2 𝐾= 𝑑𝑝 𝑑𝑉 𝑉 𝑜 −2

23. Two long metallic plates are kept in parallel and the potential difference across them is 𝑽 𝒕 . What is the boundary condition at x=0? 𝑥=0 𝑥= -𝑙 𝑉(𝑡) ~ At 𝑥=0, current = ∞ At 𝑥=0, current = 0 At 𝑥=−𝑙, current = ∞ At 𝑥=−𝑙, current = 0

24. A sound wave with an incident complex magnitude 𝑷 + enters another medium. The complex magnitude for reflected and transmitted sound waves is 𝑷 − and 𝑷 𝐓 , respectively. What is the attenuation factor for such a wave as it enters into the second medium?? 𝑃 𝑇 𝑃 + 𝑃 𝑇 𝑃 + 2 𝑃 𝑇 𝑃 + 1 2 𝑃 𝑇 𝑃 + −2 𝑃 + 𝑃 𝑇 𝑃 − Medium 1 Medium 2

25. What is the definition for transmission loss (𝑻𝑳), for a sound wave propagating from one medium into another? 𝑇𝐿=10 log 10 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑡 𝑤𝑎𝑣𝑒 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑡𝑟𝑎𝑛𝑠𝑚𝑖𝑡𝑡𝑒𝑑 𝑤𝑎𝑣𝑒 𝑇𝐿=−10 log 10 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑡 𝑤𝑎𝑣𝑒 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑡𝑟𝑎𝑛𝑠𝑚𝑖𝑡𝑡𝑒𝑑 𝑤𝑎𝑣𝑒 𝑇𝐿=20 log 10 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑡 𝑤𝑎𝑣𝑒 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑡𝑟𝑎𝑛𝑠𝑚𝑖𝑡𝑡𝑒𝑑 𝑤𝑎𝑣𝑒 𝑇𝐿=−20 log 10 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑡 𝑤𝑎𝑣𝑒 𝐼𝑛𝑡𝑒𝑛𝑠𝑖𝑡𝑦 𝑜𝑓 𝑡𝑟𝑎𝑛𝑠𝑚𝑖𝑡𝑡𝑒𝑑 𝑤𝑎𝑣𝑒

Average transmission loss (dB) 26. The following graph depicts transmission loss for a planar wall with respect to varying frequency. In this graph, which region is “mass controlled”? A B Average transmission loss (dB) Frequency (Hz) A B Both A and B None of the above

27. In stiffness controlled region , expression for attenuation for an acoustic wave incident from random direction ‘𝜽’ is given by _________? 1 1+ cos 𝜃 2 𝑍 𝑜 𝑐𝜔 2 1 1+ sin 𝜃 2 𝑍 𝑜 𝑐𝜔 2 1 1+ 1 2 𝑍 𝑜 𝑐𝜔 2 1 1+ 1 2 𝑍 𝑜 𝑐𝜔

28. The value of incident and transmitted sound power intensity on a plane wall of thickness 30 cm is 130 dB and 80 dB, respectively. Thus, the reduction of sound intensity across the wall is by a factor of ____ . 10000 100000 1000 100

29. If for an ISO frequency band the central frequency is p, then it’s band number would be : 20log10 𝑝 40log10 𝑝 10log10 𝑝 None of above

30. Acoustical average power per cycle is not zero for: An undamped infinitely long tube. A short undamped open tube. A short undamped close tube. None of the above.

31. If power correction factor for a system is 1, then it’s transmission loss will be _________. Maximum Minimum Infinite None of above

32. For a monopole sound source which of the following is true. 𝜕𝑝 𝜕𝑟 = 0; 𝜕𝑝 𝜕θ = 0 and 𝜕𝑝 𝜕φ ≠ 0 𝜕𝑝 𝜕𝑟 = 0; 𝜕𝑝 𝜕θ ≠ 0 and 𝜕𝑝 𝜕φ = 0 𝜕𝑝 𝜕𝑟 ≠ 0; 𝜕𝑝 𝜕θ = 0 and 𝜕𝑝 𝜕φ = 0 None of above Note: p= Pressure r = Radial direction θ = Azimuthal angle φ=Zenith angle

33. The magnitude of pressure at point P, which is at a distance r from a simple monopole sound source is proportional to _________. 𝑟 1 𝑟 1 𝑟 2 1 𝑟

34. The value of specific acoustical impedance, Z(r,ω) for a monopole sound source becomes approximately equal to the characteristic impedance, Z0, of the medium at a radial distance, r, when ____. r≫ λ 2π r≪ λ 2π Never None of the above

35. Volume velocity of a sound source is defined as: Dot product of pressure of sound source and velocity of sound source. Dot product of velocity of sound source and area of sound source. Dot product of pressure of sound source and area of sound source. None of the above

36. Near-field for a monopole sound source refers to the zone for which the radial distance (r) is in the range of ____. 0 to 2 times ( λ 2π ) 0 to 3 times ( λ 2π ) 0 to 4 times ( λ 2π ) 0 to 5 times ( λ 2π )

37. At a particular angular position P, two monopole sound sources separated by a distance of 𝝀 𝟒 produce minimum pressure amplitude. If the magnitude of volume velocity of both of these sources is same, and the phase difference their volume velocities is π/2 radians, then, what will be the angular position of point P. 0 degree 90 degree 180 degree 270 degree

38. The ratio of specific characteristic impedance for a spherical and planar wave fronts, i.e. 𝒁 𝒓𝒂𝒅𝒊𝒂𝒍 𝒁 𝒑𝒍𝒂𝒏𝒂𝒓 is: 1 1+ ( λ 2π𝑟 ) 2 1 1+ ( λ π𝑟 ) 2 1 1+ ( λ 4π𝑟 ) 2 None of above

39. A small spherical sound dissipates 12 W of acoustical power 39. A small spherical sound dissipates 12 W of acoustical power. Calculate the sound intensity level in air at a point, which is 70 cm away from the sound source. Assume free-field conditions. 100 dB 122 dB 136 dB 146 dB

40. The relation for volume-velocity for a monopole sound source is: Volume-velocity = ____. 4𝜋𝑟 𝑝(𝑟,𝜔) 3𝑗 𝜔 𝜌 𝑒 −( 𝑗𝜔𝑟 𝑐 ) 4𝜋 𝑝(𝑟,𝜔) 𝑗 𝜔 𝑟 𝜌 𝑒 −( 𝑗𝜔𝑟 𝑐 ) 4𝜋𝑟 𝑝(𝑟,𝜔) 𝑗 𝜔 𝜌 𝑒 −( 𝑗𝜔𝑟 𝑐 ) None of above

41. Calculate the sound pressure level for the following signal. The medium of propagation is air at STP. 105 dB 104 dB 103 dB 102 dB