Lindab Group We simplify construction

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1 Lindab Group We simplify construction Lindab Acoustics Tuomas Veijalainen Product Manager Acoustic Mikkeli, Finland

2 Agenda Acoustic theory What are sound and noise? A-weighting db db(a) Sound pressure sound power Cross talk Sound insulation sound attenuation Sound sources in ventilation Sound attenuators Testing of silencers Materials Lindab silencers Sound measurements Sound calculations by DIMsilencer Questions and comments

3 Sound Sound is a variation of pressure. It travels forward in zones of negative and positive pressure. It is of longitudinal wave motion i.e.. vibration. Movement of sound requires a certain material; air, water, concrete, wood etc. Sonic speed 344 m/s (at sea level, +20 C)

4 Sound The simplest vibration is sine wave (pure tone) Frequency is the number of occurrences per time unit The Unit is Hertz (HZ = 1/s) lindab we simplify construction

5 pressure 0104 lindab we simplify construction Wave Length - Frequency Wavelength l: Distance between two pressure maxima. Frequency f: number of pressure variations pr second Speed of sound c relates frequency and wavelength atmospheric pressure distance c [m/s] = f It follows from this that: low frequency sound has a long wavelength. Therefore low frequency sound is difficult to attenuate. Ventilations systems are normally assessed in eight frequency bands, from 63 to 8000 Hz. These are called octave bands f Frequency [Hz] Wavelength [m]

6 Noise What is noise? That sounds like a pretty simple question, but noise is a perceived value. You may think of noise as anything you can hear, but we will define noise as any unwanted sound. Sound becomes noise when it Is too loud: the sound is uncomfortable or makes speech difficult to understand Is duct rumble created by a fan Contains unwanted pure tones (e.g., a whine, whistle, or hum) Contains unwanted information or is distracting (e.g., an adjacent telephone conversation or undesirable music) Is unexpected (e.g., the sound of breaking glass} Is uncontrolled (e.g., a neighbor s lawn mower) Happens at the wrong time (e.g., a door slamming in the middle of the night) Is unpleasant (e.g., a dripping faucet)

7 Noise L p (SPL) These small pressure waves send a signal to the brain, through the ear, which recognises it as sound Unit: decibel (db) Sound pressure level Lp db Sound Pressure p Pa Sound Source 0 0,00002 Normal hearing level 50 0,006 Quiet conversation Scream; 1 m Jet engine

8 Noise L p (SPL) Pressure waves cause the eardrum and microphone of the sound level meter to react in the same way and the meter will register the sound pressure level. When noise is in a certain place e.g. room, yard etc. We talk about Sound Pressure Level.

9 Weighting Curves A-weighting compensates the human s sense of hearing and it is most commonly used. Ventilation noise is normally A-weighted Frequency [Hz] B-weighting (e.g. Cars) C-weighting compensates almost un-weighted sound (used mainly frequency range Hz) D- weighting is standard for aircraft noise A- weighting [db] B- weighting [db] C- weighting [db] 63-26,2-9,3-0, ,1-4,2-0, ,6-1, ,2-0, ,2-0,1-0, ,0-0,7-0, ,1-2,9-3,0

10 Sound weighting [db(a)] & [db(c)] Often requirements for a system is stated as a single value in stead of in the 8 octave bands. This is done by adding a filter value to each octave band and add the octave bands logarithmically. The human ear can perceive frequencies from Hz. However a sound pressure of for instance 30 db at 63 Hz is perceived as less annoying than 30 db at 1000 Hz. This is the reason that db(a) filters are used. There are large negative filter values in the low frequencies as shown in the graph. Sometimes there are stricter requirements in the low frequencies. In these cases the C-filter is used. Frequecy [Hz] A- weighting [db] B- weighting [db] C- weighting [db] 63-26,2-9,3-0, ,1-4,2-0, ,6-1, ,2-0, ,2-0,1-0, ,0-0,7-0, ,1-2,9-3, C-filter 1,2 1-0,8-0, ,2-0,8-1,1-3,2-3 -9,6 A-filter -16,1-26,2 63 Hz 125 Hz 250 Hz 500 Hz 1000 Hz 2000 Hz 4000 Hz 8000 Hz Example of db(a) value calculation. Sound db A-weighting A-weighted db(a)

11 Sound level [db] 0104 lindab we simplify construction Sound Weighting ( NR & NC - curves) Both NR and NC value are found in a similar way. The sound level is drawn in the NR/NC diagram. The highest NR/NC value is read from the curves. NR 68 NR (found kurver at 500 Hz) NC 69 (found NC kurver at 500 Hz) Lydniveau [db] Sound level [db] NR 80 NR 70 NR 60 NR 50 NR 40 NR 30 NR 20 NR 10 Lydniveau [db] NC 80 NC 70 NC 60 NC 50 NC 40 NC 30 NC 20 NC Frequency Frekvens [Hz] [Hz] frequency Frekvens [Hz] [Hz]

12 Sound Power L w Noise levels for sound technical calculations must be given as sound power levels. In sound calculations we use the Sound Power Levels (L w ) from the fan manufacturer. Sound power is measured inside the duct. Compare to sound pressure level which is measured outside the duct (room or in a open space).

13 Sound Power of a Fan, L w Sound power of a fan is dependent on the type of fan. Noise is caused mainly by two ways; mechanical noise and air flow noise.

14 Sound Power of a Fan, L w Specifying sound power by exact calculations is not possible. It must always be measured. Corrections for external influences must be corrected after the measurement & calculation

15 Sound Power of a Fan, L w Sound power levels must be declared so that their are divided to different frequencies per octave band is precisely specified.

16 Sabine room attenuation Many producers gives sound pressure levels for air-devices in Sabine 10 m² room Sound power level is in this case +4 db(a)

17 Sound Attenuation Sound Isolation Sound attenuation; e.g. Reduce of sound power level caused by a fan or regulation damper etc. Sound isolation; e.g. prevention of noise travelling from one room to the other.

18 Sound Movement Between Rooms - Through walls Via holes in the walls / floors etc. Via water and heating pipes Via ventilation ducts Round duct is always better than rectangular if we want to avoid sound travelling via ducts Cross Talk

19 Attenuation Between Rooms Sometimes we must prevent noise travelling from one room to the next. The most effective way of achieving this is through the use of silencers.

20 Sound sources of Ventilation systems; Air handling unit (fan) Grilles Roof hoods Valves & diffusers Dampers Air flow Compressors and condensers Attenuators

21 Sound Moving Inside The Duct Sound is progressing in duct same way as flowing air. Airflow direction is not relevant ; sound will travel in either direction

22 Sound Attenuation of Duct System In sheet metal ducts, and concrete ducts with smooth surface, the sound attenuation is very low only db / m. That attenuation is usually ignored in measurement and design. It s just for additional assurance.

23 Distribution of Sound Power Distribution of sound power is according to areas of duct branch L w = L w -10 lg (A/A ) db For example, if the duct splits into a branch this results in a reduction of 3 db in sound power level. i.e. if the ducts reduces from 500 mm2 to 2 pieces 250 mm2 the result is a constant reduction of 3 db. L w = L w -10 lg 2 db = L w 3 db

24 Sound Attenuation Attenuators are used for reducing the sound emissions of fans, dampers and other sources.

25 Lindab Acoustic Own test laboratory IT-solutions, calculation tools DIMsilencer, LindQST etc. Technical support Effective production Wide product range Short delivery times

26 Lindab Acoustic Laboratory lindab we simplify construction

27 Grevie and Boliden, Sweden Karlovarska. Czech Republic Haderslev, Denmark Jyväskylä, Finland Tallinn, Estonia Silencer Production lindab we simplify construction

28 The Principle of Attenuation When noise passes through the attenuator, it is absorbed by attenuation material (sound is converted into heat) Attenuation material is normally some soft material like mineral wool or polyester (Acutec) The level of attenuation depends on the model of attenuator and attenuation material. The silencer model will be selected according to the need of attenuation in the space

with surface and sometimes also with perforated

29 Attenuation Materials Mineral wool: Mineral wool - plate or mat Rock wool or glass wool Always covered with surface and sometimes also with perforated plate Polyester (Acutec): Coated plate or moulded element

Round Sound Attenuator Traditional attenuator with many benefits and low price Can be equipped with baffle or central pod style attenuation element.

30 Round Sound Attenuator Traditional attenuator with many benefits and low price Can be equipped with baffle or central pod style attenuation element. Mineral wool or Acutec polyester Small pressure loss The Principle is based on sound absorption to attenuation material Used on ducts or with axial fan SLXU, SLU, SLCU, SLBU, SLGPU, PVA, PVAP, PVD, PVDP, TAO, AKS

Small pressure loss The Principle is based on sound absorption

31 Rectangular Silencer with Round Connections Effective attenuation Can be installed in lower ceiling voids. Small pressure loss The Principle is based on sound absorption to attenuation material Used on ducts and residential AHU LRCA, LRCB, LRBCB, KVAP / KVDP

32 Sound Attenuation Comparison Value can be added for the customer to compare different products. LRCA Hz 125 Hz 250 Hz 500 Hz SLGU Hz 125 Hz 250 Hz 500 Hz x SLU Hz 125 Hz 250 Hz 500 Hz

33 Round Bend Silencers Small pressure loss The Principle is based on sound absorption to attenuation material Sizes Ø mm 50 or 100 mm insulation Used on ducts BSLU and BSLCU

34 Flexible Sound Attenuator Aluminium or plastic outer duct Aluminium inner duct Easy to install Absorption + sound go thru duct SLFA, SLFU, AKUCOM, FSA, TAO-S FLEX

35 Exhaust Air Terminal Devices For big air volumes SLKNU combination of silencer and take-off cone EXAD, combination of DIRU damper, silencer and take-off cone Conic inlet with mesh / wire guard (option in EXAD)

Rectangular Sound Attenuator Effective sound attenuation Sizes

alternatives The air flow must be noticed The Principle is based on

36 Rectangular Sound Attenuator Effective sound attenuation Sizes according to customer s needs 400x300 mm Various baffle and split alternatives The air flow must be noticed The Principle is based on sound absorption to attenuation material and End Reflection i.e. Sound waves cancel each other out Used with AHU or on ducts SLRS, TUNE-S, DLD, MINKA, DACKA, TAP Splitters SLRA, TUNE-A Low build models LRLB and LRLS 150x x400 mm

noticed The Principle is based on sound absorption to attenuation material and End

37 Rectangular Bend silencers Effective sound attenuation Sizes according to customer s needs 400x300 mm Various baffle and split alternatives The air flow must be noticed The Principle is based on sound absorption to attenuation material and End Reflection i.e. Sound waves cancel each other out Used with AHU or on ducts SLRB, BDLD

38 Reactive Attenuator Measurement must be performed separately in each case. Principle is based on Reflection i.e. Sound waves cancel each other out Used when specific attenuation to achieve a certain frequency

39 Industrial projects and products Calculation as standard products Special materials (stainless steel, aluminium, painted steel etc. Material thickness 1,2 5,0 mm Flange connections Used especially to lower the noise to surroundings

40 Industrial projects and products Attenuation baffles Calculating as whole silencers lindab we simplify construction

41 Industrial projects and products Bend silencers

42 Industrial projects and products Round attenuator

43 Sound calculations by DIMsilencer Required information for sound calculations: Air volume l/s, m 3 /s or m3/h Maximum pressure loss Pa Sound power levels by Hz Required attenuation, sound power or sound pressure level db(a) Lay out (fan size, space for silencer) Material of the silencer Galvanized steel, EN1.4404, EN1.4301, S235 with epoxy paint Thickness of the steel (seamed or welded structure) Material of insulation Should we use mineral wool or polyester fibre Operation temperature Other requirements if any

44 Sound Calculations by DIMsilencer

45 Sound Calculations by DIMsilencer Available in Downloads Free of charge.

46 Be Aware for These Many sound sources(two equal source of noise causes 3 db increase in noise level) Using different equipment than what was in the original drawings Moving of sound via structures & services of the building Regulation using wrong methods. First adjusting fan to right air volume then balancing airflow by regulation dampers, valves or diffusers. Too small ducts too high velocity / pressure Wrong selection of diffusers Wrong connection between fan and duct system and / or wrong kind of bend on rectangular duct system.

47 Fan connection lindab we simplify construction

48 Low Pressure Loss = Low Noise Level Less turbulence = less pressure loss less noise

49 Sound Measurements Only use meters calibrated in accordance to local standards Usually A-weight in ventilation On the meter select the time setting F (Fast) for more accurate result

50 Sound Measurements First measuring background sound. NB! Maybe different between rooms Measuring mainly in the middle of the room. 1,2 1,5 meters above floor level. In big rooms several measurements required. Take the average from measuring places.

51 Typical Mistakes In Sound Measuring Discreet background noise. Difference between ventilation noise and background noise must be at least 10 db. Noisy building site Measuring too close to the diffuser Measuring inside the duct or fan unit Doors are open to the other rooms Microphone too close to the device

52 Examples from Summation of Sound Background noise is 31 db(a) and measured noise is 35 db(a) noise from ventilation = 33 db(a) Background noise is 25 db(a) and measured noise is 35 db(a) noise from ventilation = 35 db(a)

53 0505 On the following pages these symbols will be used: = Logarithmic addition = Logarithmic subtraction = Logarithmic multiplication = Logarithmic division lindab we simplify construction Difference added to the highest db value [db] Ltot Addition L1 L2 Ln log ( ) Difference between the values [db] Subtraction from higher value [db] Subtraction Ltot Differense between values [db] L1 L log (10 10 ) Multiplication Division Sound Level increase [db] Ltot L 10log( n) 1 10 Number of Sound Sources (n) Sound Level decrease [db] Ltot L 10log( n) 1 10 Number of Sound Sources (n)

54 Multiplication Multiplication Sound Level increase [db] Number of Sound Sources (n)

55 QUESTIONS? lindab we simplify construction

56 Thank you! Good luck for studies and have a nice spring! Photo: Pasi Koukkula

EXPERIMENTAL INVESTIGATION OF NOISE PARAMETERS IN HVAC SYSTEMS

EXPERIMENTAL INVESTIGATION OF NOISE PARAMETERS IN HVAC SYSTEMS The 40 th International Conference on Mechanics of Solids, Acoustics and Vibrations & The 6th International Conference on Advanced Composite Materials Engineering ICMSAV2016& COMAT2016 Brasov, ROMANIA,