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Speaker Design Proposal Home Theatre Speakers Alison Pittsley 2012
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Design Statement

Oct 30, 2014

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Design statement for the Diamond Series Speakers
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Page 1: Design Statement

Speaker  Design  Proposal  Home  Theatre  Speakers  

Alison  Pittsley  

2012

Page 2: Design Statement

1  

Table of Contents Design Goals ....................................................................................................................... 2 Box Size Requirements ...................................................................................................... 2

SPL ...................................................................................................................................... 3 Power Requirements.......................................................................................................... 4

Frequency Response .......................................................................................................... 5 Woofers ............................................................................................................................... 6

Tweeters ............................................................................................................................ 11 Crossover .......................................................................................................................... 13

Box Shape & Materials.................................................................................................... 14 Cost.................................................................................................................................... 16

Bibliography ..................................................................................................................... 17

Page 3: Design Statement

2  

Design Goals This system consists of a stereo pair that will mainly be used for television or film sound reproduction, but may occasionally be used for music reproduction as well. Enjoyment of the listening experience, rather than critical listening, is more valuable in this design. I usually listen at fairly low SPL levels, but I also want these speakers to be close to THX standards for sound reproduction. Ideally, these speakers would have low power requirements and the frequency response would cover almost all of the audible range, but certain sacrifices are acceptable to keep the design around $500 or less. Box size is flexible, but it must be big enough to be a floor standing speaker. Achieving good low frequency response is more important than high SPL, but both are desired if possible. Since box size is flexible, cost is the most limiting factor for this design.

Box Size Requirements The size specifications for these speakers are relatively flexible since they will be placed on either side of a television that has open space around it. This home theatre setup will be fairly permanent so mobility is not a large factor. The preferable box size is smaller than 4’ tall by 1.5’ wide by 2.5’ deep, but these are arbitrary measurements assuming that these will be floor-standing speakers flanking the television. The speakers will need to have the correct size and aiming to cover the listening area in a 12’ by 16’ by 8’ room with an average listening height of 3.5 feet. A drawing and approximate values of the listening area are shown below. The walls of this room are relatively absorptive, so off axis response will not have a huge impact at the listening area; this means than that on axis response is paramount, and off axis response will not have much impact on driver choice.

Figure 1: Approximate Listening Area

Page 4: Design Statement

3  

Ear Height Max 5’ Ear Height Min 3’ (sitting in a chair) Ear Height Avg. 3.5’ (sitting on a 3’ high bed) Ideal Ear Distance From Speakers 7’ Room dimensions 14’ wide by 20’ long by 8’ high

Table 1: Approximate Listening Room Dimensions and Positions

SPL My listening levels are generally much lower than average, around 48 dBA if the noise floor is low enough. Considering that the noise floor in the intended space for these speakers is higher than the room I based my preferences on, the average listening level will probably be closer to 60 or 70 dBA. It is also important to consider that I will not be the only one listening to these speakers, so a more universal standard of SPL capabilities is beneficial. Each speaker in THX systems are calibrated to a reference level of 85 SPL with a C-weighted level meter, and have a maximum, undistorted, level of 105 SPL.1 Having speakers that are capable of THX standards is ideal, but lower SPL output is acceptable if necessary. Taking my listening preferences into mind, maximum SPL as low as 85 dBA would be acceptable. With these two values, 85 dBC and 90 dBA, and taking crest factor into account these speakers would have to be able to produce a maximum of 105 dBC and 110 dBA, respectively.

Room Level

Comfortably low listening level

Mixing Level

Rocking out to a really good song level

Beginning of discomfort

40 dBA 48 dBA 60 dBA 73 dBA 90 dBA

Table 2: My SPL preferences based on levels taken in Walker 2122

                                                                                                               

1  Tomlinson  Holman,  Sound  for  Film  and  Television,  (Focal  Press,  1997),  208-­‐209.  2  Alison  Pittsley,  experiment,  (SPL  Preferences,  Michigan  Technological  University,  Michigan  January  20,  2012).    

Page 5: Design Statement

4  

Power Requirements Ideally, power requirements would remain low, with driver sensitivities 85 dB or above. Given that the listening area is about 2 meters away from each speaker, 1 watt of power would be enough to deliver the average listening SPL; higher sensitivities would easily allow smaller amplifiers to produce maximum SPLs over 100 dBA. Having high driver sensitivity is a very important since many home theater receivers do not provide more than 100 W per channel. Assuming a maximum of 100 W, 20 dBW is the most that could be gained by using more power so a driver with the sensitivity of 85 dB would have a maximum of 105 dB after considering the crest factor. To reach the maximum of 105 dBC for a THX system, the sensitivity of the drivers would have to be 105 dB or above; considering sensitivities above approximately 92 dB are less common and more expensive, a good balance of power capabilities and cost must be found for each driver.

___ Watts (W) to deliver ___ SPL (dBA) at ___ Meters (M) dBW 1 79 2 0 2 82 2 3 4 85 2 6 8 88 2 9 16 91 2 12 32 94 2 15 64 97 2 18 128 100 2 21 256 103 2 24 512 106 2 27

Table 3: Example power requirement chart, driver sensitivity = 85 dB 1W/1m

___ Watts (W) to deliver ___ SPL (dBA)

at ___ Meters (M) dBW

1 84 2 0 2 87 2 3 4 90 2 6 8 93 2 9 16 96 2 12 32 99 2 15 64 102 2 18 128 105 2 21

Table 4: Example power requirement chart, driver sensitivity=90 dB 1W/1m 3

                                                                                                               

3  Christopher  Plummer,  lecture,  (course  on  Transducer  Theory,  Michigan  Technological  University,  Michigan  January  11,  2012).    

Page 6: Design Statement

5  

Frequency Response Given that this system will be used mainly for television or films, some might think that the low frequency limit could be high because vocal frequencies wouldn’t be affected until around 300 Hz, the vocal frequency range for humans being about 300 Hz to 3.5 kHz.4 Though dialogue is usually considered, on the surface, to be the driving force in TV and films, there is so much more sound involved in communicating stories, much of it outside the vocal range. Knowing this, but not knowing how much low frequency usage is common in film mixing, I used THX standards for an idea of the required frequency response for films and TV. Speakers in THX systems are calibrated to the X-curve, which begins to roll off around 50 Hz and is about 4 dB down around 25 Hz.5

Figure 2: X Curve5

In addition to finding the THX standards, I also did an experiment to find my own low frequency extension preferences while listening to music. For this experiment I loaded four songs that represent the kind of music I like to listen to into Logic Pro and put a high pass filter on all of them. Playing each song and my preferred listening level, I swept the filter higher until I noticed significant change in the quality of the music. Doing this I found the frequencies where I thought that low frequency loss was acceptable, and the point at which I thought the loss was not acceptable (results of this experiment are shown on the next page). Using this information, and keeping the THX standards in mind, the highest low frequency limit that could be considered is around 75 Hz, with 43 Hz being the middle ground, and 20 Hz being ideal.

                                                                                                               

4  Ken  Ellis,  “Sound  and  Light  SALT  Manual,”  Last  modified  05  19,  2001,  http://www.kodachrome/salt/sunderst.htm.    5  Brian  Florian,  “Learning  from  History:  Cimema  Sound  and  EQ  Curves.”  Last  modified  06,  2002.  Accessed  January  21,  2012.  http://www.hometheatrehifi.com/volume_9_2/feature-­‐article-­‐curves-­‐6-­‐2002.html.  

Page 7: Design Statement

6  

Song Title (Artist)

Maximum loss (Hz)

Acceptable loss (Hz)

Thunderstruck (AC/DC)

81 49

Circle the Drain (Katy Perry)

63 43

Juke Box Hero (Foreigner)

87 49

The Luckiest (Ben Folds)

142 112

Table 5: My low frequency extension preferences6

Woofers To begin the woofer selection process I searched for woofers in my price range that had large frequency ranges and high sensitivities. With these parameters, I came up with the following list to compare.

Woofer Cost sen. power

(W) Max SPL

(dB) Q_ts F_s (Hz)

Box Volume V_b (ft^3)

f_3 (Hz)

Seas CA18RLY $71.55 88 80 107 0.45 40 1.187713006 43.312 Aura

NS6-255-8A $11.50 91 50 108 0.55 55 0.838113058 53.9825 Seas CA12RCY $66.40 86 60 103.5 0.31 57 0.084420221 106.7268

Peerless HDS Nomex $76.67 89.7 NA 0.38 30 1.880061394 40.368

Peerless HDS 4" GF Cone $38.33 85.9 30 100.4 0.58 89 0.175989137 79.032

Peerless HDS PPB 4" Midwoofer $37.23 87 NA 0.54 77.6 0.183771032 71.974

Peerless HDS 5.25" GF Cone $47.30 87 30 101.5 0.49 66 0.329939471 65.8878 Peerless HDS

5.25" Alu Cone $53.67 86.1 30 100.6 0.65 72 0.524224879 60.4944 Peerless HDS PPB 5.25" Midwoofer $43.42 88.3 NA 0.41 56.1 0.337695505 67.83051

Peerless SDS 5.25" Midwoofer $19.14 87 NA 0.54 62.4 0.563564499 57.876 Seas L15RLY/P $78.25 86 80 105 0.35 44 0.26612409 67.3772

W5-1685 $65.70 86 45 103 0.46 50 0.525404181 52.925 Dayton RS225-8 $57.42 86.2 80 105.2 0.36 27.6 1.461003082 40.38432

Table 6: Woofer Spec Spreadsheet

                                                                                                               

6  Alison  Pittsley,  experiment,  (Low  Frequency  Extension  Preferences,  Michigan  Technological  University,  Michigan  January  20,  2012).    

Page 8: Design Statement

7  

Using Win Speakers, I modeled the system frequency response of all these drivers assuming a SBB_4 alignment (box volume and f_3 shown in above table). From these models I easily chose five drivers to examine more closely. They were:

• Seas CA18RLY • Aura NS6-255-8A • Seas L15RLY/P • TB W5-1685 • Dayton RS225-8

From this point I closely examined frequency response of the drivers and of the system. The qualities I took into account were, in order:

1. Lowest extending/flattest system response 2. Flattest driver response 3. Highest driver response (as least 3000Hz for crossover at 2000Hz) 4. High sensitivity (All drivers meet minimum sensitivity requirement)

Figure 3: W5-1685 Frequency Response Figure 4: Seas L15RLY/P Frequency Response Figure 5: Seas CA18RLY Frequency Response

Frequency [Hz]

L15RLY/P

H1141L15RLY/P is a 15 cm (5’’) cone driver, developed for use as a long throwhigh fi delity woofer or woofer/midrange unit.

Stiff, yet light aluminium cone and low loss rubber surround show no sign of the familiar 500-1500 Hz cone edge resonance and distortion associated with soft cones.

Large magnet system , together with very long, and light weightcopper clad aluminium voice coil allow for extreme coil excursion with lowdistortion and good transient response.

Extremely stiff and stable injection moulded metal basket, keeps the critical compo-nents in perfect alignment. Large windows in the basket both above and below the spider reduce sound refl ection, air fl ow noise and cavity resonances to a minimum.

The frequency responses above show measured free fi eld sound pressure in 0, 30, and 60 degrees angle using a 7L closed box. Input 2.83 VRMS, microphone distance 0.5m, normalized to SPL 1m.The dotted line is a calculated response in infi nite baffl e based on the parameters given for this specifi c driver. The impedance is measured in free air without baffl e using a 2V sine signal.

SPL [

dB]

Imped

ance [o

hm

]

W15-411Jul 2007-1 *IEC 268-5SEAS reserves the right to change technical data

10 100 1 000 10 000

100

95

90

85

80

75

70

65

60

55

50

50

40

30

20

10

0

Nominal Impedance 8 Ohms Voice Coil Resistance 5.5 Ohms

Recommended Frequency Range 45 - 3000 Hz Voice Coil Inductance 0.84 mH

Short Term Power Handling * 200 W Force Factor 5.7 N/A

Long Term Power Handling * 80 W Free Air Resonance 44 Hz

Characteristic Sensitivity (2,83V, 1m) 86 dB Moving Mass 8.1 g

Voice Coil Diameter 26 mm Air Load Mass In IEC Baffl e 0.38 g

Voice Coil Height 16 mm Suspension Compliance 1.6 mm/N

Air Gap Height 6 mm Suspension Mechanical Resistance 1.12 Ns/m

Linear Coil Travel (p-p) 10 mm Effective Piston Area 75 cm2

Maximum Coil Travel (p-p) 20 mm VAS 12 Litres

Magnetic Gap Flux Density 1.1 T QMS 2.10

Magnet Weight 0.42 kg QES 0.43

Total Weight 1.28 kg QTS 0.35

RoHS compliant product www.seas.no

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Page 9: Design Statement

8  

Figure 6: Dayton RS225-8 Frequency Response

Figure 7: Aura NS6 Frequency Response

Figure 8: W5-1685 SBB_4 Response Figure 9: Seas L15RLY/P SBB_4 Response

Last Revised: 9/16/2010

RS225-8

RS

22

5-8

8" Reference Woofer

8"

Re

fere

nc

e W

oo

fer

86.340.8327.61.440.480.3633.80.99

211.2147.9

8.861.87.0

38.586.280

28 - 2,200

Lightweight black anodized aluminum cone Attractive 6-hole cast frame Advanced low distortion

motor design Solid aluminum phase plug Rubber surround

50

45

40

35

30

25

20

15

10

5

0

180°

90°

0 deg

-90°

-180°

1 2 5 10 20 50 100 200 500 1kHz 2k 5k 10k 20k

Algo Sound, Inc.2335 Alaska Ave., El Segundo, CA 90245 310.643.5300 310.643.9463 fax

www.aurasound.comTM TM

TM Model NS6-255-8A6” Loudspeaker

• High Sensitivity

• Compact - Light Weight

• NO Stray Magnetic Fields

Nominal Diameter (Ø) . . . . . . . . . . . 6 inches (156.4 mm)Nominal Impedance (Z) . . . . . . . . . . 8 OhmsSensitivity, 1W/1m (E) . . . . . . . . . . . 91 dBPower Capacity, RMS (Pe) . . . . . . . . 50 WPower Capacity, Peak . . . . . . . . . . . 100 WFrequency Range (-10dB) . . . . . . . . Fo - 5.5 kHzMinimum Impedance . . . . . . . . . . . . 8 OhmsVoice Coil Diameter (Ø) . . . . . . . . . . 25.5 mmVoice Coil Winding Length (h) . . . . . 11.3 mmVoice Coil Number of Layers (n) . . . . 2Voice Coil Former Material . . . . . . . . KaptonVoice Coil Wire Composition . . . . . . CopperMotor Reference . . . . . . . . . . . . . . . N255-C08-127CMagnetic Material . . . . . . . . . . . . . . Neodymium radialStray Flux Shielding . . . . . . . . . . . . . InherentMagnetic Gap Depth (He) . . . . . . . . 12.7 mmCone Material . . . . . . . . . . . . . . . . . PaperSurround Material . . . . . . . . . . . . . . FoamPolarity, Outward Motion . . . . . . . . . Po s i t i ve voltage on (+) tabNet Weight . . . . . . . . . . . . . . . . . . . . 0.484 kg

Thiele / Small Parameters

Resonant Frequency (Fo) - Fs . . . . . 55 HertzVoice Coil DC Resistance - Re . . . . . 6 OhmsTotal Q - Qts . . . . . . . . . . . . . . . . . . 0.55Mechanical Q - Qms . . . . . . . . . . . . 10.8Electrical Q - Qes . . . . . . . . . . . . . . 0.58Equivalent Volume of Air - Vas . . . . . 16.48 LRadiating Piston Area - Sd . . . . . . . . 126.0 cm2

Electrical / Mechanical Parameters

Flux Density x Length - BL . . . . . . . . 6.10 Tesla-metersCompliance - Cms . . . . . . . . . . . . . . 900 µm/NTotal Mass - Mms . . . . . . . . . . . . . . 9.30 grams

Impedance

Frequency Response (1W, 1m)

Distortion (1W, 1m)

TM

4/2/02

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

6

8

10

mmExc

Linear Exc Limit

0

2

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Pha 0°

90°

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msDly

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15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

5086500.460.533.330.44500456.100

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

0.52540.6251502.25000.84697

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

1121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

TB W5-1685 (SBB4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

6

8

10

mmExc

Linear Exc Limit

0

2

4

6

8

10

12

14

16

18

20

22

24

26

28

30

Pha 0°

90°

180°

270°

360°

450°

msDly

0

1

2

3

4

5

6

7

8

9

10

11

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15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

5086440.350.432.10.423800801000

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

0.26610.5635440.823001.5937

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

1121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

Seas L15RLY/P (SBB4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

Page 10: Design Statement

9  

Figure 10: Seas CA18RLY SBB_4 Response Figure 11: Dayton RS225-8 SBB_4 Response

Figure 12: Aura NS6 SSB_4 Response

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

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mmExc

Linear Exc Limit

0

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msDly

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15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

6091550.550.5810.80.58200503.0500

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

1.0550.6851552.06000.55157

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

1121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

Aura NS6-255-8A (SC4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

6

8

10

mmExc

Linear Exc Limit

0

2

4

6

8

10

12

14

16

18

20

22

24

26

28

30

Pha 0°

90°

180°

270°

360°

450°

msDly

0

1

2

3

4

5

6

7

8

9

10

11

12

13

14

15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

6.5088400.450.581.941.0600801000

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

1.1880.619406.1000.89247

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

1121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

Seas CA18RLY (SBB4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

6

8

10

mmExc

Linear Exc Limit

0

2

4

6

8

10

12

14

16

18

20

22

24

26

28

30

Pha 0°

90°

180°

270°

360°

450°

msDly

0

1

2

3

4

5

6

7

8

9

10

11

12

13

14

15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

8086.227.60.360.481.442.1820080700

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

1.460.568627.62.9001.4957

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

1121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

Dayton RS225-8 (SBB4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

Page 11: Design Statement

10  

From these choices I cut the drivers that had an f_3 above 50Hz. The final two options were the Aura NS6-255-8A and the Seas CA18RLY; I chose the Aura because it had a higher sensitivity, a higher frequency extension, and the Seas low frequency response was not superior enough to outweigh the benefits of the Aura. When choosing drivers I left the prices out of my spreadsheet so they would not affect my decisions; once I finally looked up the prices, I realized that I had chosen a driver that was only $11.50 and thought I must have made a mistake. I did; I had entered 40Hz as the f_B when it was really 55Hz; this factor had been a huge part in my decision-making process. The correct system response, as seen above in Figure 12, is not nearly as attractive as the one that was incorrect. With the correct system response, the Aura is not as attractive as the Seas in terms of low and flat frequency response, but all the qualities I liked about the Aura initially were still there, so deciding whether to keep the Aura, or use the Seas, was very difficult. Initially when comparing the final drivers, I used f_Bs for SSB_4 alignments because it is the best in terms of low tuning and transient response, with the SC_4 coming just below it in quality.7 After I realized that I chose the Aura’s based on the lower f_B of 40, I noticed that the Aura’s f_B with the SC_4 alignment is 42Hz. Given that this alignment gave the type of f_B I needed to get a nice system response and keep the high sensitivity and high frequency extension, I decided to stick with the Aura’s. Using the Aura’s, I experimented with the number of drivers and box volume to see if I could come up with a better response. With this, I decided to use four woofers in each speaker, separating the drivers into two spaces, with two drivers in each space.

Figure 13: Aura NS6 SC_4 Response Figure 14: Aura NS6 Double Driver Response

                                                                                                               

7  Vance  Dickanson,  Loudspeaker  Design  Cookbook,  (Peterborough,  New  Hampshire:  Audio  Amateur  Press,  2006),  62.  

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

6

8

10

mmExc

Linear Exc Limit

0

2

4

6

8

10

12

14

16

18

20

22

24

26

28

30

msDly

0

1

2

3

4

5

6

7

8

9

10

11

12

13

14

15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

6091550.550.5810.80.58200503.0500

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

30.648426.3000.3887

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

2121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

Aura NS6-255-8A (SC4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

20 50 100Hz 200 500 1k 2kMag -20

-18

-16

-14

-12

-10

-8

-6

-4

-2

0 dB

2

4

6

8

10

mmExc

Linear Exc Limit

0

2

4

6

8

10

12

14

16

18

20

22

24

26

28

30

msDly

0

1

2

3

4

5

6

7

8

9

10

11

12

13

14

15TATATATA

Driver ParametersDriver ParametersDriver ParametersDriver Parameters Box ParametersBox ParametersBox ParametersBox ParametersDriver:

Nominal DiameterNominal PowerSensitivity (1W/1m)Free Air ResonanceTotal QElectrical QMechanical QEquivalent VolumeNominal ImpedanceDC ResistanceMax Thermal PowerMax Linear ExcursionMax ExcursionVoice Coil Diam.

D =P =

SPL =f(s) =

Q(ts) =Q(es) =Q(ms) =V(as) =

Z =R(e) =P(t) =

X(max) =X(lim) =D(vc) =

6091550.550.5810.80.58200503.0500

inWattsdB SPLHz

cu ftOhmsOhmsWattsmmmmmm

Driver Notes:

NOTE: X(max) was estimated based on the nominal driver diameter.NOTE: S(D) was estimated based on the nominal driver diameter.

System Type: 4th Order Vented Box

Box VolumeClosed Box QBox FrequencyMin Rec Vent AreaVent Surface AreaVent LengthCompliance RatioBox Loss Q

V(B) =Q(tc) =F(B) =

S(vMin) =S(v) =L(v) =

alpha =Q(B) =

3.1090.599342.151.58000.18727

cu ft

Hzsq insq inin

System ParametersSystem ParametersSystem ParametersSystem Parameters

No. of DriversIsobaric FactorInput PowerSPL Distance

N =I =

P(in) =D =

1121

System Notes:

(1=normal, 2=iso)Wattsm

My CompanyMy CompanyMy CompanyMy CompanyMy Address, line 1My Address, line 2My Country My Phone

Aura NS6-255-8A (SC4)

4th Order Vented Box

System Name:

Designer:

Title:

Rev Date: Rev:

My NameMy Title

Page 12: Design Statement

11  

Tweeters To begin the tweeter selection process I searched for tweeters in my price range that extended lower than 2000Hz (assuming a crossover at 2000Hz) and with high sensitivities. With these parameters, I came up with the following list to compare.

Tweeter Cost F_s sensitivity power

(W) f_3

(Hz) impedence

(ohms) Max SPL

(dB)

Dayton DCS8F-8 $18.00 637.2 89 50 8 106

Seas H1189 $42.40 550 90 90 6 109

Seas H1212 $45.35 550 92 90 6 111

Vifa BC25TG15-04 $17.00 1130 87.8 50 4 104.8

Vifa BC25SC55-04 $19.80 1400 89.3 100 4 109.3

Vifa XT25SC90-04 $27.20 825 89.9 100 4 109.9

Vifa D27TG-06 $31.17 720 87.4 100 6 107.4

Vifa XT25TG30-04 $34.25 436 110 4 NA

Vifa XT19TD00-04 $38.75 763 87.7 120 900 4 108.7

Vifa XT25BG60-04 $40.10 589 91.5 100 900 4 111.5

Fostex FT48D $96.25 93 50 1000 8 110

ScanSpeak D2608/9130 $81.40 700 91.3 80 1500 8 110.3

ScanSpeak D2606/9220 $51.90 850 91.4 100 1000 6 111.4

ScanSpeak D2606/9200 $36.65 1100 91.4 100 900 6 111.4

Fostex FT28D $68.20 90 40 1500 8 106

Audax TW034X0 $72.05 800 93 70 700 8 88.5

Morel CAT 328-104 $90.80 650 90 200 1700 8 223

Morel MDT 32S $80.40 650 90 200 1500 8 223

Dayton DCS8FS-8 $26.75 812.9 89 50 8 106

Dayton RS28A-4 $54.75 592.2 88 100 4 108 Table 7: Tweeter Spec Spreadsheet

Page 13: Design Statement

12  

Looking at the specs for these tweeters I cut the ones with the least flat responses and highest frequency extensions first, as well as any tweeter with a nominal impedance below 6 ohms, and ended up with the following to compare more closely: • Fostex FT48D • ScanSpeak D2608/9130 • Audax TW034X0

Figure 15: Fostex Frequency Response Figure 16: Audax Frequency Response

Figure 17: ScanSpeak Frequency Response

Page 14: Design Statement

13  

Of these tweeters, I chose the one that I thought had the best balance between: 1. Low frequency extension 2. Smooth low frequency roll off 3. Flat high frequency extension through 20kHz 4. Off axis response close to on axis response 5. High sensitivity (All drivers meet minimum sensitivity requirement) With the idea of a first order crossover in mind, it was important to have low frequency extension with a smooth roll off. Two of the three of the final tweeters had really smooth roll offs so I had to take flatness of the high frequencies, off axis response, and sensitivity into higher account for my final selection. I I ended up choosing the ScanSpeak D2608/9130, even though the off axis response is very inconsistent at high frequencies, because it has flat response on axis and a high sensitivity; because the room these will be placed is non-reverberant the off axis response will not have a very big impact on the listening area.

Crossover A first order crossover is the “only conventional crossover whose combined output reconstruct the input waveform.”8 This is the reason I put such high value on having a woofer and tweeter that extended above and below 2000 Hz, respectively. With the ScanSpeak D2608/9130 tweeter and the Aura NS6-255-8A woofer a first order crossover at 2000 Hz makes a smooth roll off of both the highs and lows, making for a smooth transition between the tweeter and the woofer. However, a second order crossover gives a much safer drop in dB at the tweeter resonant frequency and will probably allow the tweeter a longer life than a first order crossover.

Figure 18: Crossover model of ScanSpeak D2608/9130 tweeter and Aura NS6-255-8A woofer

                                                                                                               

8  Philip  Newell,  and  Keith  Holland,  Loudspeakers  for  Music  Recording  and  Reproduction,  (Elsevier  Ltd.,  2007),  132.  

-­‐100  

-­‐50  

0  

50  

200   2000  

Relative  dB  

Frequency  Response  (Hz)  

Crossover  Model  

Tweeter  1st  order  ailter   Woofer  1st  order  ailter  

Zeroed  Tweeter  Resonse   Zeroed  Woofer  Resonse  

Tweeter  2nd  order  ailter   Woofer  2nd  order  ailter  

Page 15: Design Statement

14  

For these reasons, I decided to go with a second order Linkwitz-Riley crossover, which sums to a flat magnitude.9 As stated before, in the woofer section, these speakers will have four drivers split into two sections. This provides an opportunity to extend low frequency response by compensating for the baffle step loss with a .5 crossover on the low end. Two woofers will cover the low and mid frequencies, and the other two will only cover low frequencies. This makes the speakers more consistent on the vertical axis.10 With the .5 crossover added on the low end, the final design will be a second order Linkwitz-Riley 2.5 way crossover.

Figure 19: Example 2.5 Way Crossover11 Figure 20: Example 2.5 Filter Response

Box Shape & Materials The boxes are intended to be floor standing, approximately 3.5ft tall by 1.5ft deep by 1.5ft wide. I had originally planned on making rectangular speakers with rounded edges to reduce edge diffraction, but the effectiveness of this is rather limited.12 With a rectangular design, the drivers were to be placed different distances from the edges of the speakers, which makes a big improvement in the diffraction loss.13 I opted for the more complex diamond shape because I like the look, and because the 45-degree angles off the front baffle help to reduce diffraction loss a great deal more than rounded or chamfered edges. With the symmetrical look of the diamond shape, I chose to keep the drivers center on the baffle to keep the symmetrical look.

                                                                                                               

9  Vance  Dickanson,  Loudspeaker  Design  Cookbook,  (Peterborough,  New  Hampshire:  Audio  Amateur  Press,  2006),  162.  10  Christopher  Plummer,  lecture,  (course  on  Transducer  Theory,  Michigan  Technological  University,  Michigan  Feburary,  15  2012).  11  Paul  Spencer,  Red  Spade  Audio  Blog,  "Etude  TL  crossover."  Last  modified  06  29,  2011.  Accessed  April  26,  2012.  http://redspade-­‐audio.blogspot.com/2011/06/etude-­‐tl-­‐crossover.html.  12  Linkwitz  Lab,  “Diffraction  from  baffle  edges.”  Last  modified  10/04/2011.  Accessed  January  29,  2012.  http://www.linkwitzlab.com/diffraction.htm.  13  John L. Murphy, Introduction to Loudspeaker Design, (Andersonville, TN: True Audio, 1998), 71.

Posted by Paul Spencer

keep the efficiency up.

The inductor (L2) provides the low pass, while R2 and capacitor C2 provideimpedance equalisation. This means the inductor sees the driver as having aconstant impedance. C5 is needed only where low cost electro caps are used.

You may notice that the low pass filter is applied at a lower point than the acousticcrossover point of 3.5k. The acoustic response of the driver is combined with the filterto give the desired crossover point.

3. Woofer network

Theinductor(L1) has agreatervalue toapply agentle

first order low pass above 200 Hz. This network essentially provides bafflestepcompensation. It compensates for the loss of efficiency below a point determined bybaffle width. A 2 way design has both drivers reproducing midrange and bass butuses EQ to allow for bafflestep.

If there is one criticism of this crossover, it would be that the tweeter crossover is alittle high. The result is off axis lobing. Generally, a speaker with a 6.5" mid and 1"dome with a 105mm face plate should cross around 2.4k to avoid this problem. As aresult, I suggest keeping the vertical spacing as close as you can without lookingcramped. The higher crossover results in greater power handling, but at 3.5k the midis starting to beam. At the crossover point the dispersion will rapidly shift since thetweeter has much wider dispersion. This is always a problem with conventionalspeakers such as this, but the high crossover point makes it a little worse.

Return to main TL speaker page

If you already have the JV60, I have some suggestions for upgrades.

Continue to crossover upgrades

Recommend this on Google

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Red Spade Audio: Etude TL crossover http://redspade-audio.blogspot.com/2011/06/etude-tl-crossover.html

2 of 6 4/26/12 12:37 AM

Page 16: Design Statement

15  

The box material needed to be stiff enough so that the speakers will not resonate with the drivers. To achieve stiffness of the box I decided to use two layers of wood. On the outside, ¾” birch plywood with the highest ply possible to increase rigidity, and on the inside, ¾” MDF which is heavy and will vibrate less in tandem with the driver.14 The MDF will also be used a brace that separates the box into two sealed enclosures (besides the ports). Each box will have two tuning ports, one for each enclosure. These ports will be located on the back diagonal of the boxes so that the box noise will not be directed at the listening area, nor will it be reflected off the wall behind it. Once the boxes are constructed, the unique shape and wood grain will create a nice aesthetic. I plan to keep this natural look by using natural wood stain, and possibly a clear glossy coat to a more finished look.

Figure 21: 3D Rendering of Speaker Design

                                                                                                               

14  Philip  Newell,  and  Keith  Holland,  Loudspeakers  for  Music  Recording  and  Reproduction,  (Elsevier  Ltd.,  2007),  87.  

Page 17: Design Statement

16  

Cost The budget for these speakers is around $500, with limited flexibility for better quality. My initial thought was that each driver could cost no more than $100, which was one of the limiting factors when finding drivers to compare. This would have left about $100, which would not have been enough to cover wood and crossover costs. The low cost of the woofers and tweeters leaves enough money for wood and crossover materials, in addition to less significant costs like shipping, glue, and stain.

Quantity Cost Total

Woofer 8 $11.50 $92.00

Tweeter 2 $81.40 $162.80

Baltic Birch 4x8 2 $60.00 $120.00

MDF 4x8 2 $40.00 $80.00

Total: $454.80

Table 8: Current Speaker Budget

Page 18: Design Statement

17  

Bibliography

Custom Car Stereo, "Xover Calculators." Accessed April 26, 2012. http://ccs.exl.info/calc_cr.html

Dickanson, Vance. Loudspeaker Design Cookbook. Peterborough, New Hampshire: Audio Amateur Press, 2006.

Ellis, Ken. “Sound and Light SALT Manual.” Last modified 05 19, 2001. http://www.kodachrome/salt/sunderst.htm.

Florian, Brian. “Learning from History: Cimema Sound and EQ Curves.” Last modified 06, 2002. Accessed January 21, 2012. http://www.hometheatrehifi.com/volume_9_2/feature-article-curves-6-2002.html.

Holman ,Tomlinson. Sound for Film and Television. Focal Press, 1997.

King, Martin J. Simple Sizing of the Components in a Baffle Step Correction Circuit. 2005.

Linkwitz Lab, “Diffraction from baffle edges.” Last modified 10/04/2011. Accessed January 29, 2012. http://www.linkwitzlab.com/diffraction.htm.

McCarthy, Bob. Sound Systems: Design and Optimization. Burlington, MA: Elsevier Ltd., 2010.

Murphy, John L. Introduction to Loudspeaker Design. Andersonville, TN: True Audio, 1998.

Newell, Philip, and Keith Holland. Loudspeakers for Music Recording and Reproduction. Elsevier Ltd., 2007.

Pittsley, Alison. Experiment, (Low Frequency Extension Preferences, Michigan Technological University, Michigan January 20, 2012).

Pittsley, Alison. Experiment, (SPL Preferences, Michigan Technological University, Michigan January 20, 2012).

Plummer , Christopher. Lecture, (course on Transducer Theory, Michigan Technological University, Michigan January 11, 2012).

Plummer , Christopher. Lecture, (course on Transducer Theory, Michigan Technological University, Michigan Feburary, 15 2012).

Spencer, Paul. Red Spade Audio Blog, "Etude TL crossover." Last modified 06 29, 2011. Accessed April 26, 2012. http://redspade-audio.blogspot.com/2011/06/etude-tl-crossover.html.