Active noise control in practice: transformer station



Similar documents
Outer Diameter 23 φ mm Face side Dimension 20.1 φ mm. Baffle Opening. Normal 0.5 Watts Maximum 1.0 Watts Sine Wave.

Building Design for Advanced Technology Instruments Sensitive to Acoustical Noise

Sound absorption and acoustic surface impedance

The Sonometer The Resonant String and Timbre Change after plucking

PAGE 2. Figure 1: Difference between PWL ins and SPL 1m

Audible Alarm Basics Everything you wanted to know, but were afraid to ask by Dan O Brien, Sales Engineer, Mallory Sonalert Products, Inc.

APPLYING VIRTUAL SOUND BARRIER AT A ROOM OPENING FOR TRANSFORMER NOISE CONTROL

RX-AM4SF Receiver. Pin-out. Connections

Fire-resistant barriers: background on requirements and determination method. Reading guide for test reports.

V94 BULK TAPE DEGAUSSER

Linear Parameter Measurement (LPM)

How To Control Noise In A C7 Data Center Server Room

INTER-NOISE DECEMBER 2006 HONOLULU, HAWAII, USA

How To Reduce Noise From A Test Screen

Fluid structure interaction of a vibrating circular plate in a bounded fluid volume: simulation and experiment

LVDS Technology Solves Typical EMI Problems Associated with Cell Phone Cameras and Displays

Exhaust noise control case study for 2800 class locomotive

Sound Power Measurement

PRODUCT SHEET OUT1 SPECIFICATIONS

INTERFERENCE OF SOUND WAVES

PS 29M DUAL CHANNEL BELTPACK IN METAL CASE

Waves: Recording Sound Waves and Sound Wave Interference (Teacher s Guide)

Design of an U-slot Folded Shorted Patch Antenna for RF Energy Harvesting

Schindler 3300 / Schindler 5300 Information on noise and vibration.

4.4 WAVE CHARACTERISTICS 4.5 WAVE PROPERTIES HW/Study Packet

TOP 10 NOISE CONTROL TECHNIQUES

AIR RESONANCE IN A PLASTIC BOTTLE Darrell Megli, Emeritus Professor of Physics, University of Evansville, Evansville, IN dm37@evansville.

Interference to Hearing Aids by Digital Mobile Telephones Operating in the 1800 MHz Band.

INTERNATIONAL ASSOCIATION OF CLASSIFICATION SOCIETIES. Interpretations of the FTP

Aircraft cabin noise synthesis for noise subjective analysis

What you measure is what you get? a novel approach for specifying and controlling acoustic quality of road surfaces

Manual Analysis Software AFD 1201

X2Y Solution for Decoupling Printed Circuit Boards

INTERFERENCE OF SOUND WAVES

Calibration and Use of a Strain-Gage-Instrumented Beam: Density Determination and Weight-Flow-Rate Measurement

Waveforms and the Speed of Sound

Generic - Hearing Loop - (AFILS) U.S. System Specification

As a minimum, the report must include the following sections in the given sequence:

The Role of Acoustics in Curtain Wall Design:

2. THE TEORRETICAL OF GROUND PENETRATING RADAR:

Technical Information

Measuring Sound Insulation using Deconvolution Techniques

Part Number Structure ZT 028 L D CT R 15

Ultrasound Condition Monitoring

Testing of Partial Discharges in Generator Coil Bars with the Help of Calibrated Acoustic Emission Method

T1-40 T1-40BF T1-40V T1-38 T1-38BF T1-38V

A simple method to compute aircraft noise inside dwellings

An Experimental Study on Pixy CMUcam5 Vision Sensor

Lab Exercise 1: Acoustic Waves

Measurement of RF Emissions from a Final Coat Electronics Corrosion Module

v = fλ PROGRESSIVE WAVES 1 Candidates should be able to :

1 All safety instructions, warnings and operating instructions must be read first.

Development and optimization of a hybrid passive/active liner for flow duct applications

Noise associated with the ground water systems serving residential geothermal heat pumps

4 SENSORS. Example. A force of 1 N is exerted on a PZT5A disc of diameter 10 mm and thickness 1 mm. The resulting mechanical stress is:

Resonance in a Closed End Pipe

Assessment of low-frequency noise due to windturbines in relation to low-frequency background

Doppler Effect Plug-in in Music Production and Engineering

Constructing a precision SWR meter and antenna analyzer. Mike Brink HNF, Design Technologist.

How To Test A Fume Cupboard

Physics in Entertainment and the Arts

Solution 1: Algorithm Positioning

Cold Room & Refrigeration System (Casserole Assembly) No of units: 1

This presentation reports on the progress made during the first year of the Mapping the Underworld project. As multiple Universities and Departments

Affordable Sports Halls

EXPERIMENTAL RESEARCH ON CHARACTERISTICS OF CENTRIFUGAL PUMP NOISE IN WATER PIPE SYS- TEM

TELIKOU Intercom System. MS-500(4+1 channel) Main Station Instruction Manual

inter.noise 2000 The 29th International Congress and Exhibition on Noise Control Engineering August 2000, Nice, FRANCE

Bass Guitar Investigation. Physics 498, Physics of Music Sean G. Ely Randall Fassbinder

APPLICATION NOTE. Basler racer Migration Guide. Mechanics. Flexible Mount Concept. Housing

The Acoustical design of Mobile phones

INFRARED PARTS MANUAL

Standex-Meder Electronics. Custom Engineered Solutions for Tomorrow

Testing thermo-acoustic sound generation in water with proton and laser beams

Vibration Isolation in Data Centers

SR-M1 Single -Woofer Monitor Speaker SR-M2 Twin -Woofer Monitor Speaker AC-M1 TOA PROFESSIONAL SOUND SYSTEM FLOOR MONITOR SPEAKER SYSTEM

BNAM 2008 BERGEN BYBANE NOISE REDUCTION BY TRACK DESIGN. Reykjavik, august Arild Brekke, Brekke & Strand akustikk as, Norway

Vector Network Analyzer Techniques to Measure WR340 Waveguide Windows

How Noise is Generated by Wind Turbines The mechanisms of noise generation. Malcolm Hayes Hayes McKenzie Partnership Ltd Machynlleth & Salisbury

Sound Pressure Measurement

CHAPTER 3 MODAL ANALYSIS OF A PRINTED CIRCUIT BOARD

Direct and Reflected: Understanding the Truth with Y-S 3

Congratulations! Thank you!

DIAMOND ROOM MEASUREMENT REPORT

RF data receiver super-reactive ASK modulation, low cost and low consumption ideal for Microchip HCS KEELOQ decoder/encoder family. 0.

HP switch LP switch Discharge thermo Comp. Surface thermo

Once you know the volume of air and the static pressure of the system to be cooled, you can determine the fan specifications for your product.

Experiment 1: SOUND. The equation used to describe a simple sinusoidal function that propagates in space is given by Y = A o sin(k(x v t))

SAR ASSOCIATED WITH THE USE OF HANDS-FREE MOBILE TELEPHONES

IC+ NEW inverter compressor technology delivers energy saving, high performance cooling

Airborne Sound Insulation

Dynamic sound source for simulating the Lombard effect in room acoustic modeling software

Marine Generating Sets 3.7 to 50 kva

14.5GHZ 2.2KW CW GENERATOR. GKP 22KP 14.5GHz WR62 3x400V

CASE STUDY. University of Windsor, Canada Modal Analysis and PULSE Reflex. Automotive Audio Systems PULSE Software including PULSE Reflex, Transducers

TELIKOU Intercom System. TM-200 Main Station. Instruction Manual

Solving Signal Problems Effective shielding is key to enhancing the reliability and performance of broadcast cables.

APPLICATION NOTE PROFESSIONAL LOUDSPEAKERS BUILDING AN EFFECTIVE, HIGH PERFORMANCES, 2 WAY, 12 LOUDSPEAKER SYSTEM

Transcription:

Active noise control in practice: transformer station Edwin Buikema 1 ; Fokke D. van der Ploeg 2 ; Jan H. Granneman 3 1, 2, 3 Peutz bv, Netherlands ABSTRACT Based on literature and extensive measurements at a specific transformer two concepts regarding anti noise have been developed. These concepts have been tested in the Peutz acoustical laboratory, and on site with an experimental setup for anti noise at large transformers. Noise measurements show that a reduction of 5 db can be achieved in all directions. Additionally, by directing the noise emission, a reduction of 10 db can be achieved in one specific direction. This experimental project was part of a broader demonstration project regarding the practical application of different types of sensor technology. 1. INTRODUCTION From literature few examples of application of anti noise in real practical situations are available. Therefore the practical application of anti noise was introduced in the so-called Sensor City program. The aim of this program is to stimulate the use of sensors in a broad scope (not only for sound) and in a variety of practical cases, and if possible in combination with each other. This anti noise projects fits within this research program because of the application of sensors for measuring sound and vibration. 2. AIM OF THE RESEARCH The aim of this specific research was to obtain an understanding into the effects of anti noise at large noise sources and at long distances by the application of specific sensor techniques. At present no commercially available anti noise systems designed especially for large transformers are known. 2.1 Noise measurements Figure 1 gives an impression of the transformer used in the test. 1 2 3 e.buikema@peutz.nl f.vanderploeg@peutz.nl j.granneman@peutz.nl Inter-noise 2014 Page 1 of 10

Page 2 of 10 Inter-noise 2014 Figure 1 Transformer Figure 2 shows typical noise spectra of a transformer, at respectively approximately 2 m and 200 m. Figure 2 Measuring results: A-weighted noise spectra At a short distance frequencies of 100 Hz and 200Hz are dominant but also the higher modes (300, 400 and 500 Hz) are clearly present. At a further distance mainly the mode of 100 Hz and although slightly less - the 200 Hz are dominant. Because of the measurement results at further distance the focus was on reducing noise around 100 Hz. 2.2 Origin of transformer noise The main installations in transformer stations are the transformers themselves. Often so-called three-phase-transformers are used. These consist of three coils, each fitted with an iron core. There are two major sources for transformer noise. The characteristic noise of transformers is caused by magnetostriction: the expansion and contraction within the stacked iron core (laminates) due to the magnetic effect of alternating current flowing through the transformer coils. These extensions and contractions will occur twice during Page 2 of 10 Inter-noise 2014

Inter-noise 2014 Page 3 of 10 each complete cycle of the alternating current flowing through the coil. This causes an audible hum. To some extent magnetostriction can be reduced by adequate transformer design, but it cannot be totally eliminated. The other cause of noise are mechanical vibrations. This usually results from vibrations emanating from the core that are transferred to parts of the installation that are attached to it. In general there are different ways to reduce the noise emission of transformers from a manufacturing point of view, such as: Reduce the flux density by increasing the amount of steel in the core. This is the most effective but also the most expensive method to reduce noise. Apply a suitable adhesive between the layers of, for instance, epoxy or polyurethane with a low viscosity. The basic idea behind this is to reduce the ability of movement and the extent to which the laminates can extend and contract when the core is magnetized. This is considerably less expensive but means extra effort in stacking the core. The adapted system should have some resiliency and should not be rigid. A less expensive alternative is the application of an adhesive to the edges of the laminates in the stacked core. The low viscosity is required for penetration, at least to some extent, between the sheets of laminates in the core. Thereby laminates are bond together near the edges and vibrate less when magnetized. Noise due to vibration caused by magnetostriction transferred to other parts of the transformer causing mechanical noise can be reduced by appropriate cushioning. Flexible mounting of components will reduce the transfer of vibrations and thereby reduce noise emission. 2.3 Anti noise The noise reducing provisions as mentioned above have limited effect on new transformers and are not directly suitable for many of the existing transformers. Therefore anti noise is an interesting alternative to reduce the noise emission of transformers. The principle of anti noise is to apply a second noise source near the original one, radiating noise in anti phase and with the same magnitude. Interference of the sound radiated by both sources causes reduction of the total noise emission. The amount of reduction depends on frequency and the distance between both sources. Only with a secondary source at a distance of 1/10 of the wave length a significant reduction, of approximately 10 db, can be expected from a theoretical point of view. As a consequence, for 100 Hz the distance between both sources should be 34 cm or less. Also the noise sources should be small compared to the wavelength of interest. In practice, most noise sources do not match with these theoretical criteria. This is especially true for transformers. Transformers are used to reduce the electrical voltage from the main transportation network (grid) to lower values before entering urban or industrial areas. A transformer is a complex noise source. Different parts of its housing radiate sound in a different way and magnitude. Also, a transformer is not small compared to the wave length of the radiated sound. So the location of speakers to produce anti noise effectively has to be selected carefully. Furthermore there are practical and important safety issues. Fans can be installed in front of the transformer to cool the oil. This is the reason no sound screen is possible in front of the transformer: it would obstruct the air flow too much. Also the top has to be open for the same reason. Loudspeakers have to be placed at a safe distance from high voltage cables to avoid electrocution. So the possibilities to apply anti noise to transformers have to be tested in practice. 3. TEST SET-UP 3.1 General Based on a close look on the noise characteristics of the specific transformer, literature study and detailed noise measurements of a transformer two concepts of anti noise were designed. At first, both concepts were tested under laboratory conditions in the Peutz laboratory. Then the test was continued in practice at a transformer station. Because of the spectrum of the noise levels near dwellings at about 100 m distance the focus was on 100 Hz. 3.2 Laboratory tests The practical possibilities of anti noise were tested with two small loudspeakers, at short distance from each other. Figure 3 shows the principle, figure 4 the practical set-up. Inter-noise 2014 Page 3 of 10

Page 4 of 10 Inter-noise 2014 Figure 3 anti noise by means of two loudspeakers at short distance from each other Figure 4 Test set-up with two identical loudspeakers Both loudspeakers were connected to a computer by which frequency, phase and amplitude could be regulated. The distance between the loudspeakers was varied, and the noise reduction was measured in three directions. The achieved noise reduction varied between 8 and 13 db; the latter value if the loudspeakers were facing each other. In another experiment in the laboratory vibrations were generated in a plasterboard panel by means of an exciter. This plasterboard panel (dimensions 0.45 x 0.45 m, thickness 12.5 mm) was meant to simulate a vibrating part of the transformer. The dimension of this panel was chosen in such a way that the whole panel would vibrate in phase when excited at 100 Hz. Figure 5 shows some pictures of the laboratory test set-up. Page 4 of 10 Inter-noise 2014

Inter-noise 2014 Page 5 of 10 Figure 5 Laboratory test set-up with vibrating panel with exciter Both a small and a large loudspeaker were placed near this vibrating panel. Figure 6 shows the test with the smaller loudspeaker. Inter-noise 2014 Page 5 of 10

Page 6 of 10 Inter-noise 2014 Figure 6 Laboratory test set-up with smaller loudspeaker From these tests it appeared that reduction of the noise emission was possible with both types of loudspeaker, reaching the values that could be achieved theoretically. Reductions of 8 to 9 db were measured. The tests as described above are not adaptive. In practice, with transformer variations due to changes in load and/or temperature influence the noise emission to the environment. So an adaptive system is required, with a unit that regulates both phase and amplitude (feed forward). A possible location of the microphone for this purpose is between the vibrating panel and the loudspeaker. The optimal location of the microphone appeared to be at the center between the vibrating panel and the loudspeaker. 4. TESTS IN PRACTICE 4.1 First concept For the purposes of the first concept, a number of small loudspeakers are applied at a distance of approximately 30 centimeters from the loudest parts of the housing of the transformer. In figure 7 two loudspeakers are shown. Page 6 of 10 Inter-noise 2014

Inter-noise 2014 Page 7 of 10 Figure 7 Loudspeaker positions near parts of transformer These loudest parts of the transformer are determined based on sound-intensity measurements. These sound-intensity measurements have been performed several times on different days and at different times. It has been found that the location of the loudest parts of the housing does not change either under various conditions and changing load of the transformer. Thus, there is no shift to be seen where other sub-faces are more important for the noise emission at different times. This allows speakers to be applied at a short distance and at fixed positions from the loudest parts of the transformer. For the purpose of the test set-up, five loudspeakers were used. Each loudspeaker is driven on the basis of its own vibration sensor and microphone. In the overall arrangement there were five loudspeakers, five microphones and five vibration sensors. Data acquisition cards have been used to digitize the signals from the microphones and vibration sensors. These digitized signals are the input signals for the control system which is installed on a laptop. Finally the system drives the loudspeakers. Based on the signal from the vibration sensor, the phase and the frequency are determined. This vibration sensor is mounted on the housing of the transformer, at the loud part just in front of the loudspeaker. Important fact is that the system should be able to respond rapidly to frequency changes. It has been found that the frequency of the transformer is not stable but that it fluctuates relatively rapidly in time at around 100 Hz (band width of only about 0.2 Hz). If the system does not respond fast enough beating of the sound arises (the noise cancellation is not offered at the exact same frequency), which makes the noise situation rather more annoying. The microphone is placed between the casing of the transformer and the loudspeaker. Based on the information from the microphone the volume of the loudspeaker is set. This set-up requires a less quick response because the noise from the casing of the transformer is relatively constant over time and slowly fluctuates around an average value. Since each loudspeaker used is controlled autonomously, the system can easily be expanded with multiple loudspeakers. In practice it has been found that the systems hardly influence each other. Therefore, even if two sound reducing loudspeakers are located at a short distance next to each Inter-noise 2014 Page 7 of 10

Page 8 of 10 Inter-noise 2014 other, there is no question of mutual influence and this has no effect on the overall sound reduction. In fact, if more loudspeakers are used, the final reduction will be higher. 4.2 Second concept The second concept consists of a single loudspeaker located on a stand with a height of approximately 2 m at a distance of about 8 m from the transformer; see figure 8. Figure 8 Loudspeaker at larger distance from transformer The frequency is determined by the signal from a vibration sensor, mounted on the housing of the transformer. A microphone is placed at a distance of approximately 15 meters from the loudspeaker, in the direction of the nearest dwellings. Based on the signal from this microphone, the phase and volume are set, the target is to minimize the sound pressure level at 100 Hz at the location of this microphone. Based on measurements the area with effective noise reduction by anti noise can be determined. It can be argued that such a system is only suitable if a significant "quiet area" is created by anti noise from which one or more dwellings could benefit. A disadvantage of this second concept is that Page 8 of 10 Inter-noise 2014

Inter-noise 2014 Page 9 of 10 the sound level can increase at other locations. 4.3 Results With the first concept (five small loudspeakers at short distance from the transformer) the obtained reduction at 100 Hz was 3 to 6 db in all directions. However, more reduction is possible if more loudspeakers are used because more radiating parts of the transformer can be treated by such a system. With the second concept (loudspeakers at further distance) an additional average reduction of 5 db was obtained at 100 m distance. Measurements were performed in a straight line over a distance of about 50 m with mutual distance of approximately every 3 m; see figure 9. Figure 9 - Dwellings at about 100 m from transformer; average effect 5 db at 100 Hz The reductions at these positions varied between 3 to 15 db, on average 5 db. So reduction is achieved in a significant area and not only at a specific point. Figure 10 shows results of anti noise. Inter-noise 2014 Page 9 of 10

Page 10 of 10 Inter-noise 2014 Figure 10 - Results of anti noise in practice; left without anti noise, right with anti noise at 100 Hz 5. CONCLUSIONS Anti noise creates a significant reduction of transformer noise. With the combination of both concepts (loudspeakers at short respectively longer distance from the transformer) a reduction of 10 db at 100 Hz can be obtained at certain dwellings at about 100 m distance. 6. ACKNOWLEDGMENT This project has been made possible by the European Union, European Fund of Regional Development, Dutch Ministry of Economical Affairs and Koers Noord as part of the project Sensor City. A special acknowledgment to Tennet for their assistance in the practical part of this study. Page 10 of 10 Inter-noise 2014