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GOLDBERG AND MÄKIVIRTA

 

AUTOMATED IN-SITU EQUALISATION

 

 

AES 23RD CONFERENCE, May 23-25, 2003 

10 

In Figure 4 the results are pooled for all products and 
for each product type, excluding the main monitors 
where there were only three cases. The change in 
quartile difference and RMS deviation for the broad-
band and the subbands is illustrated. For all models, 
the broadband flatness is improved by 0.4 dB and the 
mean reduction in the LF subband RMS deviation is 
1.4 dB. The RMS deviation for all models pooled to-
gether has been reduced by equalisation and the larg-
est reduction is seen for the three-way systems. To 
some extent this is similar for the quartile difference 
but the small two-way and two-way systems do not 
see such large improvements due to equalisation. This 
indicates that the improvement is mainly a reduction 
of extreme magnitude values (heights of peaks and 
notches) in the low frequency response. 
 

5. DISCUSSION 

The objective of this paper is to present an automated 
system for choosing appropriate room response con-
trol settings once an in-situ frequency response meas-
urement has been made and to show that it is effec-
tive. 
The room response controls in active loudspeakers 
implement discrete filter parameter values rather than 
a continuous parameter value range. The number of 
possible filter parameter value combinations can be 
quite large and so even an experienced operator can 
find it difficult to choose the optimal settings. 
The task of the automated optimiser is to find the op-
timal combination from the possible combinations of 
discrete filter parameter values. The cost of perform-
ing a brute force search of all value combinations and 
then choosing the best among them is prohibitive in 
terms of computer processing time. The approach cho-
sen is to exploit the heuristics of experienced calibra-
tion engineers and to reduce the number of alterna-
tives by dividing the task into subsections that can re-
liably be solved independently. A significant part of 
the heuristics is the order in which these choices 
should be taken. A considerable improvement in the 
speed of optimisation was achieved relative to a full 
exhaustive search. 
The optimisation algorithm is relatively robust to a 
wide variety of situations, such as varying room 
acoustics, different sized loudspeakers with differing 
anechoic responses and varying in-situ responses [41]. 
The optimisation is efficient and so the software is fast 
enough to be used routinely at in-situ loudspeaker 
calibrations. 
A case study demonstrates the statistical changes due 
to the optimisation algorithm’s recommended room 
response control settings. The settings achieve im-
proved equalisation in the form of a smaller RMS de-

viation from the target response. The improvement is 
not limited by the optimisation method but by the 
room response controls which are not intended to cor-
rect for narrow-band deviations in the frequency re-
sponse. Examples of these are response variations re-
sulting from acoustic issues such as cancellations as-
sociated comb filtering due to reflections. These 
should be solved acoustically rather than electroni-
cally. 
The statistical analysis of 63 loudspeakers shows that 
the automated equalisation is able to systematically 
reduce the variability in the equalised responses and to 
improve the frequency response flatness relative to the 
target response. It achieves this by improving the 
broadband frequency balance relative to the target re-
sponse and by reducing the variability in the response, 
particularly in the low frequencies. Across all loud-
speaker groups the main improvement is in the reduc-
tion of extreme (outlier) values in the low frequency 
band of the response. 
It is interesting to note that the most commonly used 
room response control was the midrange level, fol-
lowed closely by the treble level and bass tilt control. 
This is explained by the fact that the algorithm in most 
stages minimises the RMS deviation, and in so doing 
affects most efficiently the extreme deviations from 
the median level. 
For all models pooled together, the broadband flatness 
was improved by equalisation. This improvement is 
mainly due to a reduction of the extreme magnitude 
values (heights of peaks and notches) in the low fre-
quency response (LF subband). 
The lack of improvement in the quartile values and 
RMS deviation in the midrange and high frequencies 
(MF and HF subbands) is because the room related 
response variation becomes narrow band. Some im-
provement in the equalisation could be obtained with 
room response controls offering a tilting or shaping of 
the response within the mid-to-high frequency range. 
The largest variability of the improvement in the low 
frequency range can be explained by the acoustics 
found in listening rooms [42]. At low frequencies the 
radiation from the loudspeaker can be considered om-
nidirectional and the sound field in the room is usually 
not very diffuse. This results in strong room effects 
and hence large variations in the magnitude response 
at these frequencies. 
The largest improvement is seen for the three-way 
systems and can be explained by two main factors. 
Firstly, the rooms in which this type of loudspeaker is 
typically installed are of a higher quality acoustical 
design, so the sound field in them is well controlled. 
Conversely, smaller loudspeakers are often installed in 
rooms with little or no acoustical design, making cor-

Summary of Contents for Frequency Response Optimisatio

Page 1: ...ce of calibrating active loud speakers Even with experienced system calibrators significant variance between calibrations can be seen Furthermore with a number of different people cali brating loudspeaker systems additional variance in results will occur For these reasons an automated calibration method was developed to ensure consis tency of calibrations Presented first in this paper is the discr...

Page 2: ...al to significantly improve perceived sound quality The practical challenge is the selection of the best settings for the low order in situ equaliser Despite advances in psychoacoustics it is difficult to quantify what the listener actually perceives the sound quality to be or to optimise equalisation based on that evaluation 13 15 Because of this in situ equalisa tion typically attempts to obtain...

Page 3: ...re determined by the crossover filters The bass tilt control compensates for a bass boost seen when the loudspeaker is loaded by large nearby boundaries 33 36 This typically happens when a loudspeaker is placed next to or mounted into an acoustically hard wall This filter is a first order shelv ing filter The bass roll off control compensates for a bass boost often seen at the very lowest frequenc...

Page 4: ...her than using a least squares type objective function is that the bass roll off tends to assume maximum attenuation to minimise the RMS deviation This type of objective function does not yield the best setting as subjectively a loss of bass extension is perceived This stage of the optimiser algorithm takes six filtering steps three for small two way models 3 2 2 Midrange Level to Treble Level Rat...

Page 5: ...tics of experienced calibration engineers The resulting num ber of filtering steps has been dramatically reduced for the larger systems Table 9 and even the relatively simple two way systems show a substantial improve ment when compared to the number of filtering steps needed by direct search method as summarised in Table 5 There are two main reasons for the improve ment the constraint of not allo...

Page 6: ... there is also a 3 dB roll off with 50 Hz being down by 1 dB and 40 Hz by 2 dB Tolerance lines are set to 3 dB with additional leeway at low and high fre quencies 1 An example of the room equaliser settings output for the large system optimised in Figure 1 is shown in Figure 2 The optimised result is displayed in green and dark grey boxes The green boxes are room re sponse controls that should be ...

Page 7: ...d tonal bal ance improvement This is indicated by a reduction of the median value differences 4 2 Example of Statistical Data Analysis Figure 7 in Appendix C shows a case example where room response control settings are calculated accord ing to the optimisation algorithm The equalisation target is a flat magnitude response straight line at 0 dB level The in situ frequency response of the loudspeak...

Page 8: ...subbands show no changes or a slight increase of the RMS deviation Three way systems show a clear reduction in most cases of both the quartile difference Figure 13 and RMS deviation Figure 14 for the broadband and LF subband Slight and equal numbers of increases and reductions are seen for MF and HF subbands A similar trend is seen for the three large systems in cluded in this study Figure 15 16 M...

Page 9: ...n the median level for the LF subband A similar outcome is noted sepa rately for each loudspeaker type However only in the three way systems is an improvement seen also in the MF and HF subband variance 25 to 75 Percentile Difference Change due to Equalisation All models 3 2 1 0 1 Broadband LF MF HF Level dB RMS Deviation Change due to Equalisation All models 5 4 3 2 1 0 1 Broadband LF MF HF Level...

Page 10: ...d room response control settings The settings achieve im proved equalisation in the form of a smaller RMS de viation from the target response The improvement is not limited by the optimisation method but by the room response controls which are not intended to cor rect for narrow band deviations in the frequency re sponse Examples of these are response variations re sulting from acoustic issues suc...

Page 11: ...Thesis at the Helsinki University of Technol ogy 41 8 REFERENCES 1 Genelec Oy http www genelec com 2003 Feb 2 Walker R Equalisation of Room Acoustics and Adaptive Systems in the Equalisation of Small Rooms Acoustics Proc 15th Int Conf paper 15 005 1998 Oct 3 Cox T J and D Antonio P Determining Op timum Room Dimensions for Critical Listening Envi ronments A New Methodology presented in 110th Conv A...

Page 12: ...2001 Sep 29 Mäkivirta A Antsalo P Karjalainen M and Välimäki V Low Frequency Modal Equalisation of Loudspeaker Room Responses presented in 111th Conv Audio Eng Soc preprint 5480 2001 Sept 30 Karjalainen M Esquef P A A Antsalo P Mäkivirta A and Välimäki V Frequency Zooming ARMA Modelling of Resonant and Reverberant Sys tems J Audio Eng Soc vol 50 pp 1012 1029 2002 Dec 31 Moore B C J Glasberg B R Pl...

Page 13: ...User Inputs Model Database Stored Measurement Microphone Compensation CTRL M Measurement Dump Reset Graph and Outputs Get Model Number Apply Mic Compensation Remove DC Window FFT and Smooth Load Impulse Response Set DIPtimisation Range Display Original Freq Response Display Target Response Calculate Target Resp Stored Measurement CLOSE DIPtimiser 1 2 Figure 5 Software flow chart part 1 CLOSE Set F...

Page 14: ...5 2003 14 Is Large System Is Small System Load Filters Model Filters Preset BRO Find ML TL Ratio Set BL BT wrt ML TL Reset BRO Set TT Display Final Tone Control Settings Display Final Frequency Response Set BT Is 3 way System 1 2 Figure 5 continued Software flow chart part 2 Y N N Y ...

Page 15: ...GOLDBERG AND MÄKIVIRTA AUTOMATED IN SITU EQUALISATION AES 23RD CONFERENCE May 23 25 2003 15 APPENDIX B SOFTWARE GRAPHICAL USER INTERFACE Figure 6 Software graphical user interface at start up ...

Page 16: ... AND MÄKIVIRTA AUTOMATED IN SITU EQUALISATION AES 23RD CONFERENCE May 23 25 2003 16 APPENDIX C CASE EXAMPLE STATISTICAL GRAPHS Figure 7 Case example optimisation results Figure 8 Case example statistical output ...

Page 17: ...5 4 0 3 5 3 0 2 5 2 0 1 5 1 0 0 5 0 0 0 5 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB Low Frequency 25 to 75 Percentile Difference Before Equalisation 0 2 4 6 8 10 12 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB Low Frequency 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 1029A 1029A 1029A 1029A 1029A 1029A...

Page 18: ...2 0 1 5 1 0 0 5 0 0 0 5 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB High Frequency 25 to 75 Percentile Difference Before Equalisation 0 2 4 6 8 10 12 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB High Frequency 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 102...

Page 19: ...to Equalisation 7 6 5 4 3 2 1 0 1 2 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB Low Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB Low Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB ...

Page 20: ...Equalisation 7 6 5 4 3 2 1 0 1 2 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB High Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB High Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A 1029A Level dB H...

Page 21: ...ence Before Equalisation 0 2 4 6 8 10 12 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB Low Frequency 25 to 75 Percentile Difference Change due to Equalisation 4 5 4 0 3 5 3 0 2 5 2 0 1 5 1 0 0 5 0 0 0 5 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB Broadband 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 1030A 1030A 1031A...

Page 22: ... 3 0 2 5 2 0 1 5 1 0 0 5 0 0 0 5 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB High Frequency 25 to 75 Percentile Difference Before Equalisation 0 2 4 6 8 10 12 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB High Frequency 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A ...

Page 23: ...ange due to Equalisation 7 6 5 4 3 2 1 0 1 2 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB Low Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB Low Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB Low Frequ...

Page 24: ...e due to Equalisation 7 6 5 4 3 2 1 0 1 2 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB High Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB High Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 1030A 1030A 1031A 1031A 1031A 1031A 1031A 1031A 1031A 1032A 1032A Level dB High Frequ...

Page 25: ...tion 0 2 4 6 8 10 12 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB Low Frequency 25 to 75 Percentile Difference Change due to Equalisation 4 5 4 0 3 5 3 0 2 5 2 0 1 5 1 0 0 5 0 0 0 5 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB Broadband 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 ...

Page 26: ... 0 5 0 0 0 5 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB High Frequency 25 to 75 Percentile Difference Before Equalisation 0 2 4 6 8 10 12 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB High Frequency 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 S30D S30D S30D S30D 1037B 1037B 10...

Page 27: ...tion 7 6 5 4 3 2 1 0 1 2 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB Low Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB Low Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 10...

Page 28: ...n 7 6 5 4 3 2 1 0 1 2 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB High Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 1038A 1038A 1038A 1039A Level dB High Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 S30D S30D S30D S30D 1037B 1037B 1037B 1037B 1037B 1038A 1038A 103...

Page 29: ...evel dB Low Frequency 25 to 75 Percentile Difference Before Equalisation 0 2 4 6 8 10 12 1036A 1036A 1036A Level dB Low Frequency 25 to 75 Percentile Difference Change due to Equalisation 4 5 4 0 3 5 3 0 2 5 2 0 1 5 1 0 0 5 0 0 0 5 1036A 1036A 1036A Level dB Broadband 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 1036A 1036A 1036A Level dB Low Frequency 25 to 75 Percentile Diff...

Page 30: ...ifference Change due to Equalisation 4 5 4 0 3 5 3 0 2 5 2 0 1 5 1 0 0 5 0 0 0 5 1036A 1036A 1036A Level dB High Frequency 25 to 75 Percentile Difference Before Equalisation 0 2 4 6 8 10 12 1036A 1036A 1036A Level dB High Frequency 25 to 75 Percentile Difference After Equalisation 0 2 4 6 8 10 12 1036A 1036A 1036A Level dB High Frequency 25 to 75 Percentile Difference Change due to Equalisation 4 ...

Page 31: ... 1036A 1036A Level dB Broadband RMS Deviation Change due to Equalisation 7 6 5 4 3 2 1 0 1 2 1036A 1036A 1036A Level dB Low Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 1036A 1036A 1036A Level dB Low Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 1036A 1036A 1036A Level dB Low Frequency RMS Deviation Change due to Equalisation 7 6 5 4 3 2 1 0 1 2 1036A 1036A 1036A Level dB Fig...

Page 32: ...036A 1036A Level dB Midrange RMS Deviation Change due to Equalisation 7 6 5 4 3 2 1 0 1 2 1036A 1036A 1036A Level dB High Frequency RMS Deviation Before Equalisation 0 2 4 6 8 10 1036A 1036A 1036A Level dB High Frequency RMS Deviation After Equalisation 0 2 4 6 8 10 1036A 1036A 1036A Level dB High Frequency RMS Deviation Change due to Equalisation 7 6 5 4 3 2 1 0 1 2 1036A 1036A 1036A Level dB Fig...

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