PH0101 UNIT 1 LECTURE 7

1. PH0101 UNIT 1 LECTURE 7 • Introduction to Building Acoustics • Changes in the direction of sound travel • Sound Absorption and Absorption Coefficient • Reverberation and Sabine’s Formula • Factors affecting Acoustics of Building PH0101 UNIT 1 LECTURE 7

2. Introduction to Building Acoustics Building acoustics or architectural acoustics deals with sound in the built environment. Structures with acoustic implications: • Airports • Churches • Theatres • Concert and opera halls • Educational structures, including class rooms, lecture halls, libraries, music practice rooms etc., PH0101 UNIT 1 LECTURE 7

3. Phenomena related to Changes in the direction of sound travel • Sound waves change their direction of travel through four categories of phenomena : reflection, refraction, diffraction and diffusion. • These phenomena can occur when changes occur in a sound wave’s medium of travel. These physical principles are the same as those that occur in the optical world with light. PH0101 UNIT 1 LECTURE 7

4. (1) Reflection • When a sound wave encounters a sharp discontinuity in the density of a medium, some of its energy is reflected. • Reflective surfaces are typically smooth and hard. • A few common acoustic problems caused by reflections are echoes and room resonance. PH0101 UNIT 1 LECTURE 7

5. ECHOES • Echoesare caused by the limitations of our hearing mechanisms in processing sounds. • When the difference in arrival times between two sounds is less than 60 milliseconds, we hear the combination of the two sounds as a single sound. • However, when this difference exceeds 60 milliseconds, we hear the two distinct sounds. • When these two sounds are generated from the same source, this effect is known as ECHO PH0101 UNIT 1 LECTURE 7

6. When parallel surfaces are tall and fairly close to each other, a rapid succession of mid frequency echoes, known as flutter echo, can occur. FLUTTER ECHO PH0101 UNIT 1 LECTURE 7

7. ROOM RESONANCE • Room resonance occurs at specific frequencies in rooms where two reflective walls are parallel to each other. • In these cases, whole number multiples of specific half wavelengths will fit between the two walls. • Since their surfaces reflect the sound, their mirror images bounce off each wall to setup stationary pressure pattern in a room. • This phenomenon is called a single dimensional (or axial) standing wave and it is the simplest form of room resonance. PH0101 UNIT 1 LECTURE 7

8. (2) Refraction • Just as light bends through a prism, the direction of sound is altered when sound waves encounter changes in medium conditions that are not extreme enough to cause reflection, but are enough to change the speed of sound. • In addition to the speed of sound changing for different materials or media, the speed of sound changes with changes in temperature within the same medium. • This variation in sound travel direction, caused by variation in the speed of sound, is known as refraction. PH0101 UNIT 1 LECTURE 7

9. (3) Diffraction • The principle of diffraction limits the sound reduction effectiveness of any open-plan office partition or outdoor noise barrier. • Sound waves bend around and over these types of walls, independent of their material, to impose this limit. PH0101 UNIT 1 LECTURE 7

10. (3) Diffusion When a sound wave reflects off a convex or un even surface, its energy is spread evenly rather than being limited to a discrete reflection. This phenomenon, known as diffusion. PH0101 UNIT 1 LECTURE 7

11. Sound Absorption • The property of a surface by which sound energy is converted into other form of energy is known as absorption. • In the process of absorption sound energy is converted into heat due to frictional resistance inside the pores of the material. • The fibrous and porous materials absorb sound energy more, than other solid materials. PH0101 UNIT 1 LECTURE 7

12. Sound Absorption Coefficient • The effectiveness of a surface in absorbing sound energy is expressed with the help of absorption coefficient. • The coefficient of absorption `’ of a materials is defined as the ratio of sound energy absorbed by its surface to that of the total sound energy incident on the surface.  = PH0101 UNIT 1 LECTURE 7

13. A unit area of open window is selected as the standard. All the sound incident on an open window is fully transmitted and none is reflected. Therefore, it is considered as an ideal absorber of sound. • Thus the unit of absorption is the open window unit (O.W.U.), which is named a “sabin” after the scientist who established the unit. • A 1m2 sabin is the amount of sound absorbed by one square metre area of fully open window. PH0101 UNIT 1 LECTURE 7

14. The value of `’ depends on the nature of the material as well as the frequency of sound. It is a common practice to use the value of `’ at 500 Hz in acoustic designs. • If a material has the value of “” as 0.5, it means that 50% of the incident sound energy will be absorbed per unit area. • If the material has a surface area of S sq.m., then the absorption provided by that material is a = . S PH0101 UNIT 1 LECTURE 7

15. If there are different materials in a hall, then the total sound absorption by the different materials is given by A = a1 + a2 + a3 + …… A = 1S1 + 2S2 + 3S3 + …… or A = where 1, 2, 3 ………. are absorption coefficients of materials with areas S1, S2, S3, ……. PH0101 UNIT 1 LECTURE 7

16. Reverberation • Sound produced in an enclosure does not die out immediately after the source has ceased to produce it. • A sound produced in a hall undergoes multiple reflections from the walls, floor and ceiling before it becomes inaudible. • A person in the hall continues to receive successive reflections of progressively diminishing intensity. • This prolongation of sound before it decays to a negligible intensity is called reverberation. PH0101 UNIT 1 LECTURE 7

17. Reverberation Time • The time taken by the sound in a room to fall from its average intensity to inaudibility level is called the reverberation time of the room. • Reverberation time is defined as the time during which the sound energy density falls from its steady state value to its one-millionth (10-6) value after the source is shut off. PH0101 UNIT 1 LECTURE 7

18. If initial sound level is Li and the final level is Lf and reference intensity value is I ,then we can write Li = 10 log and Lf = 10 log Li – Lf = 10 log As = 10-6, Li – Lf = 10 log 106 = 60 dB Thus, the reverberation time is the period of time in seconds, which is required for sound energy to diminish by 60 dB after the sound source is stopped. PH0101 UNIT 1 LECTURE 7

19. Sabine’s Formula for Reverberation Time Prof.Wallace C.Sabine (1868-1919) determined the reverberation times of empty halls and furnished halls of different sizes and arrived at the following conclusions. • The reverberation time depends on the reflecting properties of the walls, floor and ceiling of the hall. • The reverberation time depends directly upon the physical volume V of the hall. • The reverberation time depends on the absorption coefficient of various surfaces such as carpets, cushions, curtains etc present in the hall. • The reverberation time depends on the frequency of the sound wave because absorption coefficient of most of the materials increases with frequency. PH0101 UNIT 1 LECTURE 7

20. Prof. Sabine summarized his results in the form of the following equation. Reverberation Time, T  or T = where K is a proportionality constant. It is found to have a value of 0.161 when the dimensions are measured in metric units. Thus, T = This Equation is known as Sabine’s formula for reverberation time. PH0101 UNIT 1 LECTURE 7

21. It may be rewritten as T = or T = PH0101 UNIT 1 LECTURE 7

22. Optimum Reverberation Time • Sabine determined the time of reverberation for halls of various sizes. • And from the results, he deduced the reverberation time that is likely to be most satisfactory for the purpose for which a hall is built. • Such satisfactory value is known as the optimum reverberation time. PH0101 UNIT 1 LECTURE 7

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24. Factors Affecting Acoustics of Buildings • Reverberation Time • If a hall is to be acoustically satisfactory, it is essential that it should have the right reverberation time. • The reverberation time should be neither too long nor too short. • A very short reverberation time makes a room `dead’. On the other hand, a long reverberation time renders speech unintelligible. • The optimum value for reverberation time depends on the purpose for which a hall is designed. PH0101 UNIT 1 LECTURE 7

25. Remedies • The reverberation time can be controlled by the suitable choice of building materials and furnishing materials. • Since open windows allow the sound energy to flow out of the hall, there should be a limited number of windows. They may be opened or closed to obtain optimum reverberation time. PH0101 UNIT 1 LECTURE 7

26. Remedies • Carboard sheets, perforated sheets, felt, heavy curtains, thick carpets etc are used to increase wall and floor surface absorption. Therefore, the walls are to be provided with absorptive materials to the required extent and at suitable places. • Heavy fold curtains may be used to increase the absorption. • Covering the floor with carpet also increase the absorption. PH0101 UNIT 1 LECTURE 7

27. Remedies • Audience also contribute to absorption of sound. The absorption coefficient of an individual is about 0.45 sabins. • In order to compensate for an increase in the reverberation time due to an unexpected decrease in audience strength, upholstered seats are to be provided in the hall. • Absorption due to an upholstered chair is equivalent to that of an individual. PH0101 UNIT 1 LECTURE 7

28. (2) Loudness • Sufficient loudness at every point in the hall is an important factor for satisfactory hearing. • Excessive absorption in the hall or lack of reflecting surfaces near the sound source may lead to decrease in the loudness of the sound. PH0101 UNIT 1 LECTURE 7

29. Remedies • A hard reflecting surface positioned near the sound source improve the loudness. • Low ceilings are also of help in reflecting the sound energy towards the audience. • Adjusting the absorptive material in the hall will improve the situation. • When the hall is large and audience more, loud speakers are to be installed to obtain the desired level of loudness. PH0101 UNIT 1 LECTURE 7

30. (3) Focussing • Reflecting concave surfaces cause concentration of reflected sound, creating a sound of larger intensity at the focal point. These spots are known as sound foci. • Such concentrations of sound intensity at some points lead to deficiency of reflected sound at other points. • The spots of sound deficiency are known as dead spots. The sound intensity will be low at dead spots and inadequate hearing. • Further, if there are highly reflecting parallel surfaces in the hall, the reflected and direct sound waves may form standing waves which leads to uneven distribution of sound in the hall. PH0101 UNIT 1 LECTURE 7

31. Remedies • The sound foci and dead spots may be eliminated if curvilinear interiors are avoided. If such surfaces are present, they should be covered by highly absorptive materials. • Suitable sound diffusers are to be installed in the hall to cause even distribution of sound in the hall. • A paraboloidal reflecting surface arranged with the speaker at its focus is helpful in directing a uniform reflected beam of sound in the hall. PH0101 UNIT 1 LECTURE 7

32. (4) Echoes • When the walls of the hall are parallel, hard and separated by about 34m distance, echoes are formed. Curved smooth surfaces of walls also produce echoes. Remedies • This defect is avoided by selecting proper shape for the auditorium. Use of splayed side walls instead of parallel walls greatly reduces the problem and enhance the acoustical quality of the hall. • Echoes may be avoided by covering the opposite walls and high ceiling with absorptive material. PH0101 UNIT 1 LECTURE 7

33. (5) Echelon effect • If a hall has a flight of steps, with equal width, the sound waves reflected from them will consist of echoes with regular phase difference. These echoes combine to produce a musical note which will be heard along with the direct sound. This is called echelon effect. It makes the original sound unintelligible or confusing. Remedies • It may be remedied by having steps of unequal width. • The steps may be covered with proper sound absorbing materials, for example with a carpet. PH0101 UNIT 1 LECTURE 7

34. (6) Resonance • Sound waves are capable of setting physical vibration in surrounding objects, such as window panes, walls, enclosed air etc. The vibrating objects in turn produce sound waves. The frequency of the forced vibration may match some frequency of the sound produced and hence result in resonance phenomenon. Due to the resonance, certain tones of the original music may get reinforced that may result in distortion of the original sound. Remedies • The vibrations of bodies may be suitably damped to eliminate resonance due to them by proper maintenance and selection. PH0101 UNIT 1 LECTURE 7

35. (7) Noise • Noise is unwanted sound which masks the satisfactory hearing of speech and music. • There are mainly three types of noises that are to be minimized. • They are (i) air-borne noise, (ii) structure-borne noise and (iii) internal noise. PH0101 UNIT 1 LECTURE 7

36. (i) Air-Borne Noise • The noise that comes into building through air from distant sources is called air-borne noise. • A part of it directly enters the hall through the open windows, doors or other openings while another part enters by transmission through walls and floors. Remedies • The building may be located on quite sites away from heavy traffic, market places, railway stations, airports etc. • They may be shaded from noise by interposing a buffer zone of trees, gardens etc. PH0101 UNIT 1 LECTURE 7

37. (ii) Structure-Borne Noise • The noise which comes from impact sources on the structural extents of the building is known- as the structure-borne noise. It is directly transmitted to the building by vibrations in the structure. The common sources of this type of noise are foot-steps, moving of furniture, operating machinery etc. Remedies • The problem due to machinery and domestic appliances can be overcome by placing vibration isolators between machines and their supports. • Cavity walls, compound walls may be used to increase the noise transmission loss. PH0101 UNIT 1 LECTURE 7

38. (iii) Internal Noise • Internal noise is the noise produced in the hall or office etc. • They are produced by air conditioners, movement of people etc. Remedies • The walls, floors and ceilings may be provided with enough sound absorbing materials. • The gadgets or machinery should be placed on sound absorbent material. PH0101 UNIT 1 LECTURE 7

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