Kef Reference 207/2 10″ Woofer Driver

 Note: Above picture linked from Kef’s site.

 

IMG_6602 IMG_6600

 

A fellow sent me a set of the 10″ woofer drivers from Kef’s “flagship” 207/2 speaker for me to test recently.  One 207/2 costs $9,999 via Kef direct.  So, whoever was brave enough to dismantle… thank you.  ;)

Below are my results.

Thiele-Small Parameters and Impedance

Electrical Parameters
Re 6.82 Ohm electrical voice coil resistance at DC
Le 0.662 mH frequency independent part of voice coil inductance
L2 1.014 mH para-inductance of voice coil
R2 4.3 Ohm electrical resistance due to eddy current losses
Cmes 428 µF electrical capacitance representing moving mass
Lces 64.93 mH electrical inductance representing driver compliance
Res 108.13 Ohm resistance due to mechanical losses
fs 30.2 Hz driver resonance frequency
Mechanical Parameters
(using add. mass)
Mms 48.44 g mechanical mass of driver diaphragm assembly including air load and voice coil
Mmd (Sd) 40.801 g mechanical mass of voice coil and diaphragm without air load
Rms 1.047 kg/s mechanical resistance of  total-driver losses
Cms 0.573 mm/N mechanical compliance of driver suspension
Kms 1.74 N/mm mechanical stiffness of driver suspension
Bl 10.642 N/A force factor (Bl product)
Loss factors
Qtp 0.521 total Q-factor considering all losses
Qms 8.776 mechanical Q-factor of driver in free air considering Rms only
Qes 0.553 electrical Q-factor of driver in free air considering Re only
Qts 0.52 total Q-factor considering Re and Rms only
Other Parameters
Vas 103.7157 l equivalent air volume of suspension
n0 0.496 % reference efficiency (2 pi-radiation using Re)
Lm 89.16 dB characteristic sound pressure level (SPL at 1m for 1W @ Re)
Lnom 89.85 dB nominal sensitivity (SPL at 1m for 1W @ Zn)
Sd 357.53 cm² diaphragm area

207_2  woofer Magnitude of electric impedance Z(f)

 

Large Signal Analysis with Klippel’s LSI Suite

Displacement Limits thresholds can be changed in Processing property page
X Bl @ Bl min=70% 8.2 mm Displacement limit due to force factor variation
X C @ C min=50% 8.2 mm Displacement limit due to compliance variation
X L @ Z max=17 % >8.9 mm Displacement limit due to inductance variation
X d @ d2=10% 39.3 mm Displacement limit due to IM distortion (Doppler)
Asymmetry (IEC 62458)
Ak 31.5 % Stiffness asymmetry Ak(Xpeak)
Xsym 0.57 mm Symmetry point of Bl(x) at maximal excursion

kef 207_2 woofer  Force factor Bl (X) kef 207_2 woofer  Bl Symmetry Range kef 207_2 woofer  Mechanical compliance Cms (X) kef 207_2 woofer  Stiffness of suspension Kms (X) kef 207_2 woofer  Kms Symmetry Range kef 207_2 woofer  Electrical inductance L(X, I=0) kef 207_2 woofer  Inductance over current L(X=0, I)

 

One nice plus is the relatively high sensitivity at just above 89dB @ 1w/1m.  The results show the woofer’s 20% THD limit is met by both motor and suspension at 8.2mm.  There is a near constant offset in Bl approximately 0.56mm forward.  There is a forward offset in suspension off approximately 1.0mm.  A shorting ring is used to keep inductance over excursion and inductance over current low, which is used to mitigate higher frequency distortion via intermodulation.

 

Funkin Audio FASX-380

 

 

 

IMG_6407 IMG_6408 IMG_6409

Up for test is a Funkin Audio FASX-380 15″ Subwoofer.  The sub is a dual 4ohm voice coil, though for this test only one coil was connected.

Thiele-Small Parameters

Electrical Parameters
Re 3.75 Ohm electrical voice coil resistance at DC
Le 0.312 mH frequency independent part of voice coil inductance
L2 1.962 mH para-inductance of voice coil
R2 12.84 Ohm electrical resistance due to eddy current losses
Cmes 1273 µF electrical capacitance representing moving mass
Lces 25.48 mH electrical inductance representing driver compliance
Res 13.25 Ohm resistance due to mechanical losses
fs 27.9 Hz driver resonance frequency
Mechanical Parameters
(using add. mass)
Mms 151.278 g mechanical mass of driver diaphragm assembly including air load and voice coil
Mmd (Sd) 127.892 g mechanical mass of voice coil and diaphragm without air load
Rms 8.968 kg/s mechanical resistance of  total-driver losses
Cms 0.214 mm/N mechanical compliance of driver suspension
Kms 4.66 N/mm mechanical stiffness of driver suspension
Bl 10.9 N/A force factor (Bl product)
Loss factors
Qtp 0.654 total Q-factor considering all losses
Qms 2.961 mechanical Q-factor of driver in free air considering Rms only
Qes 0.838 electrical Q-factor of driver in free air considering Re only
Qts 0.653 total Q-factor considering Re and Rms only
Other Parameters
Vas 172.4831 l equivalent air volume of suspension
n0 0.432 % reference efficiency (2 pi-radiation using Re)
Lm 88.55 dB characteristic sound pressure level (SPL at 1m for 1W @ Re)
Lnom Zn missing dB nominal sensitivity (SPL at 1m for 1W @ Zn)
Sd 753.79 cm² diaphragm area

FA FASX-380 Magnitude of electric impedance Z(f)

 

Large Signal Analysis

Displacement Limits thresholds can be changed in Processing property page
X Bl @ Bl min=70% 8.4 mm Displacement limit due to force factor variation
X C @ C min=50% >15.7 mm Displacement limit due to compliance variation
X L @ Z max=17 % 12.4 mm Displacement limit due to inductance variation
X d @ d2=10% 48.9 mm Displacement limit due to IM distortion (Doppler)
Asymmetry (IEC 62458)
Ak 47.66 % Stiffness asymmetry Ak(Xpeak)
Xsym 3.13 mm Symmetry point of Bl(x) at maximal excursion

FA FASX-380 Force factor Bl (X) FA FASX-380 Bl Symmetry Range FA FASX-380 Mechanical compliance Cms (X) FA FASX-380 Stiffness of suspension Kms (X) FA FASX-380 Kms Symmetry Range FA FASX-380 Electrical inductance L(X, I=0) FA FASX-380 Inductance over current L(X=0, I)

Airborne FR124B8-19F

The following test is for the Airborne FR124B8-19F which can be purchased from Solen here.  At the time of this test, the MSRP is approximately $51CAD ($50USD).

IMG_6406 IMG_6405

 

 

Thiele-Small Parameters

Electrical Parameters
Re 7.24 Ohm electrical voice coil resistance at DC
Le 0.203 mH frequency independent part of voice coil inductance
L2 0.25 mH para-inductance of voice coil
R2 2.11 Ohm electrical resistance due to eddy current losses
Cmes 208 µF electrical capacitance representing moving mass
Lces 18.19 mH electrical inductance representing driver compliance
Res 65.52 Ohm resistance due to mechanical losses
fs 81.8 Hz driver resonance frequency
——————
fm 53.6 Hz resonance frequency of driver with additional mass
Mechanical Parameters
(using add. mass)
Mms 5.573 g mechanical mass of driver diaphragm assembly including air load and voice coil
Mmd (Sd) 5.411 g mechanical mass of voice coil and diaphragm without air load
Rms 0.409 kg/s mechanical resistance of  total-driver losses
Cms 0.679 mm/N mechanical compliance of driver suspension
Kms 1.47 N/mm mechanical stiffness of driver suspension
Bl 5.176 N/A force factor (Bl product)
Loss factors
Qtp 0.697 total Q-factor considering all losses
Qms 7.006 mechanical Q-factor of driver in free air considering Rms only
Qes 0.774 electrical Q-factor of driver in free air considering Re only
Qts 0.697 total Q-factor considering Re and Rms only
Other Parameters
Vas 0.7183 l equivalent air volume of suspension
n0 0.049 % reference efficiency (2 pi-radiation using Re)
Lm 79.09 dB characteristic sound pressure level (SPL at 1m for 1W @ Re)
Lnom Zn missing dB nominal sensitivity (SPL at 1m for 1W @ Zn)
rmse Z 6.39 % root-mean-square fitting error of driver impedance Z(f)
Series resistor 0 Ohm resistance of series resistor
Madd 7.73 g additional mass
Sd 27.34 cm² diaphragm area

Aiborne FR124BB-19F Magnitude of electric impedance Z(f)

Large Signal Parameters

Displacement Limits thresholds can be changed in Processing property page
X Bl @ Bl min=82% 2.4 mm Displacement limit due to force factor variation
X C @ C min=75% 2.8 mm Displacement limit due to compliance variation
X L @ Z max=10 % 3.5 mm Displacement limit due to inductance variation
X d @ d2=10% 14 mm Displacement limit due to IM distortion (Doppler)
Asymmetry (IEC 62458)
Ak -9.27 % Stiffness asymmetry Ak(Xpeak)
Xsym -0.11 mm Symmetry point of Bl(x) at maximal excursion

Airborne FR124B8-19F Force factor Bl (X) Airborne FR124B8-19F Bl Symmetry Range Airborne FR124B8-19F Mechanical compliance Cms (X) Airborne FR124B8-19F Stiffness of suspension Kms (X) Airborne FR124B8-19F Kms Symmetry Range Airborne FR124B8-19F Electrical inductance L(X, I=0) Airborne FR124B8-19F Inductance over current L(X=0, I)

Frequency Response

The following measurement result is a result of merging nearfield response with farfield at 2.83v/1m to illustrate a standard 2.83v/1m measurement.

Airborne FR124B8-19F  0 30 60

 

Harmonic Distortion at 96dB/1m

FR124B8-19F 96dB HD

Airborne FR151B8-22F

The following test is for the Airborne FR151B8-22F which can be purchased from Solen here.  At the time of this test, the MSRP is approximately $69CAD ($67USD).

 

IMG_6401 IMG_6403 IMG_6404

 

Thiele-Small Parameters

Electrical Parameters
Re 6.27 Ohm electrical voice coil resistance at DC
Krm 0.0214 Ohm WRIGHT inductance model
Erm 0.5 WRIGHT inductance model
Kxm 0.0493 Ohm WRIGHT inductance model
Exm 0.39 WRIGHT inductance model
Cmes 353 µF electrical capacitance representing moving mass
Lces 26.44 mH electrical inductance representing driver compliance
Res 62.31 Ohm resistance due to mechanical losses
fs 52.1 Hz driver resonance frequency
——————
fm 32.6 Hz resonance frequency of driver with additional mass
Mechanical Parameters
(using add. mass)
Mms 9.59 g mechanical mass of driver diaphragm assembly including air load and voice coil
Mmd (Sd) 9.217 g mechanical mass of voice coil and diaphragm without air load
Rms 0.436 kg/s mechanical resistance of  total-driver losses
Cms 0.973 mm/N mechanical compliance of driver suspension
Kms 1.03 N/mm mechanical stiffness of driver suspension
Bl 5.212 N/A force factor (Bl product)
Loss factors
Qtp 0.695 total Q-factor considering all losses
Qms 7.2 mechanical Q-factor of driver in free air considering Rms only
Qes 0.725 electrical Q-factor of driver in free air considering Re only
Qts 0.659 total Q-factor considering Re and Rms only
Other Parameters
Vas 3.145 l equivalent air volume of suspension
n0 0.059 % reference efficiency (2 pi-radiation using Re)
Lm 79.91 dB characteristic sound pressure level (SPL at 1m for 1W @ Re)
Lnom Zn missing dB nominal sensitivity (SPL at 1m for 1W @ Zn)
rmse Z 4.83 % root-mean-square fitting error of driver impedance Z(f)
Series resistor 0 Ohm resistance of series resistor
Madd 15.34 g additional mass
Sd 47.78 cm² diaphragm area

Airborne FR151B8-22F Magnitude of electric impedance Z(f)

Large Signal Analysis

Displacement Limits thresholds can be changed in Processing property page
X Bl @ Bl min=82% 2.8 mm Displacement limit due to force factor variation
X C @ C min=75% 3.7 mm Displacement limit due to compliance variation
X L @ Z max=10 %            >4.6 mm Displacement limit due to inductance variation
X d @ d2=10% 20.2 mm Displacement limit due to IM distortion (Doppler)
Asymmetry (IEC 62458)
Ak -2.28 % Stiffness asymmetry Ak(Xpeak)
Xsym -1.23 mm Symmetry point of Bl(x) at maximal excursion

Airborne FR151B8-22F Force factor Bl (X) Airborne FR151B8-22FBl Symmetry Range Airborne FR151B8-22F Mechanical compliance Cms (X) Airborne FR151B8-22F Stiffness of suspension Kms (X) Airborne FR151B8-22F Kms Symmetry Range Airborne FR151B8-22F Electrical inductance L(X, I=0) Airborne FR151B8-22F Inductance over current L(X=0, I)

Frequency Response

The following measurement result is a result of merging nearfield response with farfield at 2.83v/1m to illustrate a standard 2.83v/1m measurement.

Airborne FR151B8-22F 0 30 60

Harmonic Distortion at 96dB/1m

Airborne FR151B8-22F 96db HD

Rhythmik Audio/GR Research F12G Direct Servo Subwoofer

As a reviewer for hometheatershack.com, I just wrapped up testing on the Rythmik Audio F12G subwoofer and have posted the data here:

http://www.hometheatershack.com/forums/sub-zone-subwoofer-testing/66876-rythmik-audio-gr-research-f12g-direct-servo-subwoofer.html

 

In a nutshell, I was very impressed with with the linear excursion of the SW-12-04 subwoofer driver at just under 18mm.  At the current MSRP of $179 believe it to be a great value.  The subwoofer as a kit (enclosure, amp, and driver) perform very well and have some very nice features most other powered subs do not have.

 

- Erin

Kef R300 Midrange Drive Unit Testing

By now you’ve probably seen my testing of the Kef HTS3001SE and Q100 drive units.  I had read the next step in the Kef Uni-Q line are the drivers in the “R” series.  So, a fella let me borrow the 5 inch midrange drive unit from the R300 speaker to test.  The R300 comes with a separate woofer but I was not sent this.  The only way to obtain these drivers individually is to purchase the speakers they come with (such as the R300 or R500 speaker) and remove them.  Which brings up something worth noting.  I am testing these raw drivers as more or less for knowledge purposes.  These kind of tests tell us exactly what the basis for a speaker is (drive units + enclosure + circuit design).  If Kef is starting with a great drive unit then one can logically assume they have likewise extended efforts to use them as a speaker in a manner which reflects their ‘raw’ performance.  In other words, if the drive unit design is great, odds are so is the complete speaker it’s used in.  Now, let’s get on with it!

 

Kef R300_2 Kef R300_1 Kef R300_3

 

Like the Q100, this driver has a very large motor structure and basket.  For a midrange, this is a HUGE drive unit, relative to other mids I’ve used.  You’ll also notice the motor and frame are a bolt together design.  The spider is below the cone on a tier sitting above where conventional speakers’ spiders are.  The surround of this driver has a curved shape to it, I assume to help it act more like a waveguide as with the cone’s shape.  The voice coil diameter is roughly 45-47mm (I had to spitball this so please take it as only an estimate).  OD is approximately 130mm.  Surface area (minus the tweeter assembly/waveguide) is about 98.01cm².  Actual effective surface area, noting the moving portion of the driver’s cone is 25cm²; the tweeter housing/waveguide is roughly 49mm in diameter.

 

Tweeter Thiele-Small Parameters

I didn’t have much time to perform full T/S parameter measurements (Vas, Bl, Mms, etc) so I have only the most basic parameters posted below.

Re 3.04 Ohm electrical voice coil resistance at DC
fs 1250 Hz driver resonance frequency
Qms 0.65 mechanical Q-factor of driver in free air considering Rms only
Qes 2.31 electrical Q-factor of driver in free air considering Re only
Qts 0.51 total Q-factor considering Re and Rms only

Woofer Thiele-Small Parameters

I didn’t have much time to perform full T/S parameter measurements (Vas, Bl, Mms, etc) so I have only the most basic parameters posted below.

Re 3.18 Ohm electrical voice coil resistance at DC
fs 178 Hz driver resonance frequency
Qms 3.01 mechanical Q-factor of driver in free air considering Rms only
Qes 0.94 electrical Q-factor of driver in free air considering Re only
Qts 0.72 total Q-factor considering Re and Rms only

Klippel LSI

Klippel LSI testing of this speaker has not yet been performed simply due to lack of time.  I do plan to perform this testing so check back here from time to time.

 

Tweeter Frequency Response

0, 30, and 60 degrees.  2.83v/1m; Nearfield & Farfield merged at 1800hz.

Kef R300 Drive Unit Tweeter Frequency Response 0 30 60

 

Woofer Frequency Response

0, 30, and 60 degrees.  2.83v/1m; Nearfield & Farfield merged at 500hz.

Kef R300 Drive Unit Woofer Frequency Response 0 30 60

 

Tweeter Harmonic Distortion at 90dB/1m and 96dB/1m

kef r300 tweeter Fundamental + Harmonic distortion components (90dB1m) r300 tweeter Fundamental + Harmonic distortion components (96dB1m)

Woofer Harmonic Distortion at 90dB/1m and 96dB/1m

kef r300 woofer Fundamental + Harmonic distortion components (90dB1m) kef r300 woofer Fundamental + Harmonic distortion components (96dB1m)

Miscellaneous Testing

I took some time to do a bit of additional testing with this driver just for fun using REW software and my calibrated mic.

I used an active crossover with a 3khz/LR2 crossover point between the mid and tweeter.  I then measured the driver at 0, 30, 45, 60, and 90 degrees to see how the response of the driver with this crossover applied measures in all angles.  The results are overlaid below in 1/12 resolution.

NOTE:  SPL is not indicative of any particular test method.  I just applied power to the driver and tested in various axes.  In other words, this is NOT indicative of 1w/1m or 2.83v/1m test standards.  The following is for the sake of seeing the driver’s performance in all axes with a 3khz/LR2 crossover.

drive unit sound power

Now, averaged them together for a single plot average of all the above points:

drive unit average

Same result as above, but in 1/3 octave:

drive unit average one-third

Another bit of testing I did was to see how the peak between 5-6khz could be tamed.  So, I applied some DSP correction and did a comparison.  The result below is a measurement of the raw woofer response vs the EQ’d response taken on axis (0 degrees).

This isn’t to say it’s needed.  It’s just something I did because I had some time and thought I’d share.  ;)

r300 woofer raw vs eq

I failed to save the results from the off-axis measurements with the DSP included, but suffice it to say, the EQ cuts added to tame this peak worked and were shown to have diminished greatly in the off-axis measurements as well as the on-axis measurement shown above.

Impulse Response Note

Being this is called a coincident driver and the benefit of these are they are supposed to emanate sound from the sound point, I measured the tweeter and midrange drive units separately and evaluated the arrival of the impulse response.  The two impulse response lined up to a ‘T’.  Unfortunately, I didn’t save this measurement because I simply forgot to before I had to shut down the computer so am unable to post the results.

Parting Thoughts

The benefit of having a coincident design is excellent.  I’ve toyed with a few here and there, though, I felt the companies’ never quite got it right.  So, when I first started testing the Kef drive units I didn’t expect much, to be honest.  However, the previous Kef Uni-Q units I’ve tested (HTS3001SE & Q100) have proven to be very well designed.  My results for the R300 drive unit show the same standard of performance.  I took the time to listen to these along with the Q100 speakers I have and must say that I am now sold on Kef’s coincident driver engineering.  I was extremely impressed by these (two) drive units’ performance in my listening tests.  People tend to get caught up in subjective ‘analysis’ whereas I fall in to a very objective analyzer category.  I tend to ignore subjective reviews in whole and often advise others to use them lightly, unless there is objective data to correlate.  This is why it’s rare I comment on the sound of a speaker/driver.  But, I can unequivocally say, after about 3 weeks of listening to these R-series mids and the Q100 speakers – against my coveted DIY speakers and countless other drive units – these truly are the best drive units I’ve laid ears on.  And, for the price, the Q100 speaker is what I would consider an excellent value for the critical listener on a real-world budget.  In fact, I intended to sell my Q100′s after testing the drive units but I have since decided to use the Q100′s as portable reference system.

Bohlender Graebenar Neo10 Planar Transducer

A fellow on tech-talk sent me four of these drivers to test and check for consistency.  I normally don’t see the need but figured it’d be interesting so I obliged.

I tested each driver’s impedance, frequency response and relative harmonic distortion. I added each driver’s respective result to the same graph for comparison purpose.  I then chose one of the drivers to do further testing on.  So what we have is the typical suite of data plus unit-to-unit comparison data.  I hope you enjoy!

 

IMG_5354 IMG_5359

 

Driver Comparison Testing

Let’s first start with the comparison data. All four drivers were tested in the exact same fashion.  One was tested, then removed from the baffle and the next was added.  The mic never moved and all the impulse responses were windowed to the exact same time(s).  Therefore, the only variant in each test is the driver itself.

Impedance Comparison

As stated above, I received (4) of these drivers to test.  However, I didn’t sweep the first driver sample for impedance so there are only (3) samples in the impedance data.

BG Neo10 - Impedance Comparison

 

Frequency Response Comparison

The comparison testing for FR & HD was done at one-half meter, with 2.83v input signal.  The results on the FR below were each attenuated 6dB in order to provide a normalized 2.83v/1meter response SPL.

This response is in the horizontal plane only.  I did not test repeatability in the vertical plane.

Neo10 Frequency Response Comparison

Harmonic Distortion Comparison

Neo10 - Total Harmonic distortion Comparison

End of Comparison Testing….

———————————————————————————————————————————————

Single Driver Testing:  Sample 3

After completing the comparison testing above, I chose Sample 3 to test further as it seemed to have the better response in FR and HD.  Yes, this is cherry picking but you’ve seen the variance above.

Thiele-Small Parameters

Electrical Parameters
Re 6.28 Ohm electrical voice coil resistance at DC
Le 0.006 mH frequency independent part of voice coil inductance
L2 0.01 mH para-inductance of voice coil
R2 0.29 Ohm electrical resistance due to eddy current losses
Cmes 1264 µF electrical capacitance representing moving mass
Lces 0.77 mH electrical inductance representing driver compliance
Res 1.1 Ohm resistance due to mechanical losses
fs 161.2 Hz driver resonance frequency
Loss factors
Qtp 1.194 total Q-factor considering all losses
Qms 1.403 mechanical Q-factor of driver in free air considering Rms only
Qes 8.032 electrical Q-factor of driver in free air considering Re only
Qts 1.194 total Q-factor considering Re and Rms only

Frequency Response: Horizontal Axis

Neo10 Horizontal Frequency Response 0 30 60

Frequency Response: Vertical Axis

Neo10 Vertical Frequency Response 0 30 60

Harmonic Distortion (Horizontal Axis)

Note the response rises throughout.  Therefore, the SPL level used to determine 96dB/1m was based on the fundamental mean SPL from 300hz to 5khz.  This is the same as I do on all my tests, albeit with some more wiggle room here by a couple dB.  Overall, this is comparable to my other test results.

Fundamental + Harmonic distortion components (96dB1m)

Cumulative Spectral Decay

Neo10 Cumulative spectral decay 2

End

Scan Speak 10F/4424G00 Discovery 4″ Midrange (4 ohm version)

Up for test is the Scan Speak Discover 10F midrange.  This driver features a neo magnet to keep its weight down.  Accompanied with the extremely small form factor, this is a top choice for many in car audio and home audio alike.  While this is noted as a 4″ midrange, seeing it in person makes it appear to be closer to the 3.5″ driver family relative to other 4 inch drivers.  This is a driver I often recommend for its price vs performance, though I’ve never gotten the chance to test one until now…

IMG_5348 IMG_5350 IMG_5349

Small Signal Analysis

Electrical Parameters
Re 3.18 Ohm electrical voice coil resistance at DC
K 0.0098 LEACH inductance model
n 0.52 LEACH inductance model
Cmes 208 µF electrical capacitance representing moving mass
Lces 6.58 mH electrical inductance representing driver compliance
Res 9.58 Ohm resistance due to mechanical losses
fs 136.1 Hz driver resonance frequency
Mechanical Parameters
(using add. mass)
Mms 3.524 g mechanical mass of driver diaphragm assembly including air load and voice coil
Mmd (Sd) 3.266 g mechanical mass of voice coil and diaphragm without air load
Rms 1.768 kg/s mechanical resistance of  total-driver losses
Cms 0.388 mm/N mechanical compliance of driver suspension
Kms 2.57 N/mm mechanical stiffness of driver suspension
Bl 4.116 N/A force factor (Bl product)
Loss factors
Qtp 0.447 total Q-factor considering all losses
Qms 1.704 mechanical Q-factor of driver in free air considering Rms only
Qes 0.566 electrical Q-factor of driver in free air considering Re only
Qts 0.425 total Q-factor considering Re and Rms only
Other Parameters
Vas 0.764 l equivalent air volume of suspension
n0 0.327 % reference efficiency (2 pi-radiation using Re)
Lm 87.34 dB characteristic sound pressure level (SPL at 1m for 1W @ Re)
Lnom 88.34 dB nominal sensitivity (SPL at 1m for 1W @ Zn)
Sd 37.28 cm² diaphragm area

10f impedance

Large Signal Analysis with Klippel’s LSI Module

Displacement Limits thresholds can be changed in Processing property page
X Bl @ Bl min=82% 1.4 mm Displacement limit due to force factor variation
X C @ C min=75% 1.7 mm Displacement limit due to compliance variation
X L @ Z max=10 % >2.2 mm Displacement limit due to inductance variation
X d @ d2=10% 8.8 mm Displacement limit due to IM distortion (Doppler)
Asymmetry (IEC 62458)
Ak 8.89 % Stiffness asymmetry Ak(Xpeak)
Xsym 0.95 mm Symmetry point of Bl(x) at maximal excursion
Xpse 2.7 mm

Scan Speak 10F Force factor Bl (X) Scan Speak 10F Bl Symmetry Range Scan Speak 10F Kms Symmetry Range Scan Speak 10F Stiffness of suspension Kms (X) Scan Speak 10F Mechanical compliance Cms (X) Scan Speak 10F Electrical inductance L(X, I=0) Scan Speak 10F Inductance over current L(X=0, I)

Frequency Response with Klippel’s TRF Module

Scan Speak 10F4424G00 0 30 60

Harmonic Distortion with Klippel’s TRF Module

The following is HD results at both 90dB/1m and 96dB/1m equivalent.

10f hd 90 10f hd 96

Cumulative Spectral Decay

10f Cumulative spectral decay

Thoughts

As this is a pure midrange, the xmax values provided by LSI aren’t frightening.  If you want to cross low, there’s not a lot of displacement so it’s best to use this with a woofer and cross above 300hz.  Judging by the rolloff, toward an Fs of 136hz, you’ll likely need to EQ assist the response below 400hz. Another benefit of this driver is it doesn’t require a large enclosure.  My measured Vas is approximately 0.7L, and the lower Qts of 0.45 allows you to go a tad below the Vas value to reach a Qtc of 0.707.

The overall frequency response of this driver is pretty nice, maintaining a fairly flat response in what I would call two ‘sectors’ of response; divided by 1.5khz.  At this point, the response dips a bit and increases by about 3dB to 2khz where it is fairly flat.  I’ve never been one to propose using wideband or fullrange drivers due to the lack of top end response and typical varying response above the pistonic range (aka: tweeterless) but in this case, I think one would be OK to do so given the extension through 20khz and smooth, controlled off-axis response.  There are no major nodal issues to speak of here; it seems the nomex cone is doing a good job of keeping break up to a minimum.

In line with that, THD results suggest a crossover above 300hz.  The bump in HD around 400hz is a driver-borne result.  I tested it a couple times in a couple different manners to see if it showed up consistently and there is nothing in the setup that would be the cause.  3rd order HD is quite nice, staying well below the 1% threshold above 200hz.  Subsequent even and odd-order distortion is very low.

All in all, not the world’s best results but as a midrange in a 3-way system crossed above 300hz or (as high as 500hz) this makes a very fine driver.  If one wanted, they could build a very nice 2-way speaker with this as well and let this driver handle everything above 300-500hz.

Kef Q100 Speaker Drive Unit Testing

As with the Kef HTS3001SE I tested, I ordered a set of the Kef Q100 speakers in order to remove and review the raw Q100 driver itself.  I really wanted to see how this coaxial design performed.  Zaph had already tested this one but I wanted to do Klippel LSI testing on it to see how the suspension performed.  He actually mentioned this in his writeup and I thought it would be cool to provide the results.  Of course, since I had it on the test baffle I did some other standard measurements as well.  The one I was interested in, but didn’t perform on the HTS3001SE driver was tweeter frequency response performance with movement of the woofer.  I don’t necessarily have an easy way to test this so I did something a bit different: I used a 9v battery to statically ‘fix’ the woofer either in the coil out or coil in position and measured the response.  I then compared this to the woofer at rest performance of the tweeter and did a direct comparison.  This is discussed further below.

–  Side Note:  I’d really like to get my hands on the R300 or R500 midrange to test and compare against this Q100.  However, in order to do so, I have to own a set or at least have the serial numbers from the speakers.  This is the same story for the Q100 so I bit the bullet and bought a set.  A set of the R300 speakers runs more than $900 and I just can’t spend that kind of money on a set of speakers I’ll dismantle just to test a drive unit.  So, if anyone reading this happens to have a set of the R-series speakers from Kef and thinks they could help me out with this, please let me know.  –

On to the testing…

 

Up first, obligatory pictures:

IMG_5291  IMG_5288 IMG_5289 IMG_5290

This driver is quite the little beast.  A very large motor and pretty substantial surround make this one of the largest 5.25″ drivers I’ve personally seen.  Although I didn’t weigh it, it is fairly heavy due to the woofer’s ferrite magnet as opposed to neodymium.  This results in large and heavy.  I can’t exactly measure the voice coil but comparing it to the tweeter assembly, it appears to be a few mm larger in radius so I’d estimate VC diameter at roughly 55mm.  It is best to rear mount this driver given the very tall surround at approximately 12mm, but for the purpose of my test I front mounted it.

If you look at the ‘Tangerine’ waveguide/lens/whatever you want to call it, you’ll notice there’s actually a phase plug on the tweeter.  The HTS3001SE does not have this.

For those who want to read about the Tangerine waveguide, click this link (PDF format).  There’s also discussion on the radial ribbing of the other Uni-Q cones, which this driver doesn’t employ.

 

 

Raw Driver Physical Measurements

First off, given this isn’t sold as an individual driver, I have taken my own measurements.  These are rough measurements taken with my not-so-recently calibrated calipers, but should be good within +/-1mm.

Outer Diameter 143 mm
Mounting Diameter 120 mm
Mounting Depth   83 mm
Effective Piston Diameter* 109 mm
Effective Piston Diameter**   60 mm
Flange Thickness 0.34 mm
Mounting Tab Thickness 0.65 mm
*Half surround to half surround; including space consumed by coincident tweeter.
**Half surround to half surround; NOT including space consumed by coincident tweeter.

Test Results

To make things a bit easier to manage, I’ve broken down the test results in to two sections:

  1. Woofer Testing
  2. Tweeter Testing

Part I: Woofer Testing

Woofer Thiele-Small Parameters and Impedance

Note:  When determining the full suite of T/S parameters, the effective diameter of the driver is needed to calculate Vas, Bl, etc.  Most of the time this can simply be measured by measuring the diameter of the driver from half-surround to half-surround since the motor must control the entire cone area.  However, in this case, the entire cone does not move.  Therefore, the effective diameter (and resulting Sd) is not the entire diameter of the driver.  The effective diameter here is determined by subtracting the static tweeter assembly from the overall effective diameter of the woofer.  See physical measurements section above for all values.

Electrical Parameters
Re 3.03 Ohm electrical voice coil resistance at DC
K 0.0087 LEACH inductance model
n 0.68 LEACH inductance model
Cmes 348 µF electrical capacitance representing moving mass
Lces 23.03 mH electrical inductance representing driver compliance
Res 51.73 Ohm resistance due to mechanical losses
fs 56.2 Hz driver resonance frequency
——————
fm 42 Hz resonance frequency of driver with additional mass
Mechanical Parameters
(using add. mass)
Mms 11.914 g mechanical mass of driver diaphragm assembly including air load and voice coil
Mmd (Sd) 11.744 g mechanical mass of voice coil and diaphragm without air load
Rms 0.662 kg/s mechanical resistance of  total-driver losses
Cms 0.673 mm/N mechanical compliance of driver suspension
Kms 1.49 N/mm mechanical stiffness of driver suspension
Bl 5.851 N/A force factor (Bl product)
Loss factors
Qtp 0.376 total Q-factor considering all losses
Qms 6.359 mechanical Q-factor of driver in free air considering Rms only
Qes 0.373 electrical Q-factor of driver in free air considering Re only
Qts 0.352 total Q-factor considering Re and Rms only
Other Parameters
Vas 0.7611 l equivalent air volume of suspension
n0 0.035 % reference efficiency (2 pi-radiation using Re)
Lm 77.63 dB characteristic sound pressure level (SPL at 1m for 1W @ Re)
Lnom 78.83 dB nominal sensitivity (SPL at 1m for 1W @ Zn)
rmse Z 5.55 % root-mean-square fitting error of driver impedance Z(f)
Series resistor 0 Ohm resistance of series resistor
Madd 11.06 g additional mass
Sd 28.27 cm² diaphragm area

Q100 Magnitude of electric impedance Z(f)

Woofer Large Signal Analysis with Klippel’s LSI Module

Displacement Limits thresholds can be changed in Processing property page
X Bl @ Bl min=82% >4.8 mm Displacement limit due to force factor variation
X C @ C min=75% 1.8 mm Displacement limit due to compliance variation
X L @ Z max=10 % 2.9 mm Displacement limit due to inductance variation
X d @ d2=10% 18.9 mm Displacement limit due to IM distortion (Doppler)
Asymmetry (IEC 62458)
Ak 37.52 % Stiffness asymmetry Ak(Xpeak)
Xsym 0.25 mm Symmetry point of Bl(x) at maximal excursion
Xpse 6.1 mm

Kef Q100 Drive Unit Force factor Bl (X) Kef Q100 Drive UnitBl Symmetry Range Kef Q100 Drive Unit Stiffness of suspension Kms (X) Kef Q100 Drive Unit Kms Symmetry Range Kef Q100 Drive Unit Mechanical compliance Cms (X) Kef Q100 Drive Unit Electrical inductance L(X, I=0) Kef Q100 Drive Unit Inductance over current L(X=0, I)

Woofer Frequency Response

Measured at 2.83v/1m.  Stitched with a nearfield measurement at approximately 500hz.

Kef Q100 Drive Unit (Woofer) 0 30 60

Woofer Harmonic Distortion

kef q100 woofer FR HD 96dB

Part II: Tweeter Testing

Tweeter Frequency Response

Kef Q100 Drive Unit (Tweeter Only) 0 30 60

Tweeter Harmonic Distortion

Kef Q100 Tweeter FR HD 96dB

Tweeter Response vs Woofer Position

I thought it would be interesting to see how the position of the woofer cone impacts the frequency response of the tweeter.  This matters when you’re listening to music and isn’t captured by a standard sine sweep.  To measure this performance I simply connected a 9v battery to the woofer’s terminals in positive polarity, then negative polarity which resulted in an approximate +/-3mm shift in cone direction.  I ran a sine sweep over the tweeter while the woofer was a) at rest, b) fixed out, and c) fixed in.  The pictures below show illustrate this.

Woofer at rest:

Q100 Woofer At Rest

Woofer fixed out:

Q100 Woofer Out

Woofer fixed in:

Q100 Woofer In

The following results are of the three positions discussed above overlaid on one another.  The lines are labeled per the woofer position.

Note: The SPL level is not absolute here.  I performed the test at the same volume level throughout but it is not intended to reference any set test paraemter such as 2.83v/1m or 1w/1m.

Kef Q100 Drive Unit Woofer Displacement on Tweeter Response Example

End

If you have any specific questions or you have feedback on the performance of this driver, feel free to post to my page.

If you like what you see here and what to help me out, there’s a Paypal Contribute button at the bottom of each page.  Every little bit does help.  Remember, I don’t get paid a dime to do this stuff.  I do it on my own for the love and entertainment but it is nice not to have to pay out of pocket to purchase things to test or gear to test with.  I’m looking to buy a new high-SPL capable mic for subwoofer testing so any donations in the near future will go toward that.

 

Thanks!

 

 

EDIT, 01/16/2013:

I was asked for a picture of the crossover that comes with the Q100 speaker.  Here it is:

IMG_5312

Kef HTS3001SE Speaker Test

IMG_5164

 

I recently purchased a set of Kef HTS3001SE speakers with the sole intention of testing the raw drive units only.  You can view the data here.  I had no intentions on testing the speaker because my curiosity ended at the drive unit itself.  However, at the request of quite a few people, I have decided to go further and test the speaker itself, in the ‘Egg’ enclosure.  The Kef speaker comes with the rear port stuffed, and thus, the option to remove the stuffing from the port enabling the listener to use them in a sealed or ported fashion, depending on placement and preference.  The data below is broken up in to two sections to reflect this.

 

On with the results…

 

Sealed Option Testing

Impedance and Magnitude

sealed kef impedance

Frequency Response at 0, 30, and 60 Degrees

2.83v/1m

Kef HTS3001SE Speaker (Sealed) 0 30 60

Harmonic Distortion

Approximately 96dB/1m Equivalent.  Windowed to 200hz as measurement was taken at one-half meter.

kef 3001 sealed HD 96dB Final

Ported Option Testing

Impedance

kef 3001 ported impedance

Frequency Response at 0, 30, and 60 Degrees

Kef HTS3001SE Speaker (Ported) 0 30 60

Harmonic Distortion

I did not perform HD testing for the ported option.

Frequency Response Comparison of Sealed vs Ported Option

Kef HTS3001SE Speaker Sealed vs Ported Comparison

Thoughts

The average output is approximately 81dB at 2.83v/1m.  Below 400hz, there’s a rise in response to a 3dB peak at 150hz possibly tied to woofer Q+enclosure Q.  The frequency response above 200hz remains fairly neutral.  There is a 2dB bump in response from about 2khz to 4khz and a rise in response above 8khz with a peak of 4dB from nominal at 10khz.  A bit of EQ should be able to tame this easily.  Off-axis response at 30 degrees looks pretty well behaved.  Harmonic Distortion looks quite nice, staying under 1% above 200hz with a small bump at 6khz and a rise above 8khz in 2nd order.  3rd order distortion stays pretty above 1khz, though it rides closely along 2nd order below 1khz.  Overall, pretty nice speakers with an aesthetically pleasing exterior.  Given these are intended as ‘satellite’ home theater speakers, I think they’d make a good option for music and desktop speakers depending on the price you can snag them for and your relative use of the word “value”.