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Jensen F12N Theile-Small parameters

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  • Jensen F12N Theile-Small parameters

    During the last couple of years, I've noticed several requests here and on other systems for the Theile/Small parameters for the venerable Jensen F15 and F12 series. It just so happens that I have a pristine original F12N. Having the equipment to measure such parameters, it was decided to do just that. First, a little info on the unit I have as there have been design changes made over the years.

    In this unit, the field coil has a dc resistance of 1003 ohms @ 78 deg. F. The inductance is 2.654 hy @ 60hz and 0.159 hy @ 1 khz. Field coil resistances have been noted to range from as low as 700 ohms to as high as 3500 ohms. If memory serves me well, I've seen higher. I have a 1923 Western Electric FC speaker with a field coil resistance of 3647 ohms.

    The voice coil measures 6.3 ohms and the demodulator (humbucking) coil measures 0.2 ohm.

    Since this unit was measured with filtered dc applied to the field coil, the demodulator coil serves no purpose other than the cost of about 3% in power transfer from the amplifier to the voice coil. It can be bypassed (shorted) since it is wired in series with the voice coil. This, however, is not recommended unless one has a thorough knowledge of how the speaker is wired as shorting the wrong wires can be disastrous.

    There has been much discussion on the actual power supplied to the field coil. The power ranged from 14 watts to about 25 with most recommendations being around 14 to15 watts. This unit was powered with 15w, which is about 123 vdc. The ambient temperature was noted at 78F. After an hour and 14 minutes, the field coil temperature was noted to be 121F and apparently stable. It was then decided to increase the power to 17w (130vdc); eighteen minutes later, the temperature of the field coil was noted to be 126F. Considering the age of the speaker, this level was abandoned.

    Tests were made with 10w applied to the field coil and Theile-Small parameters determined. The biggest difference noted was less than a 1 dB drop in the calculated SPL at 1w1m. It is, therefore, my humble opinion that the power to the field coil be kept around 10-11 watts.

    Common sense prevails. Keep in mind these speakers are 50 years old or older. The adhesives holding the voice coil wire to the coil form and the cone to voice coil are considerably aged. There is also the effect of time on the paper cone; it dries and becomes very brittle.

    Anyway, here's the Theile-Small parameters for an 8 ohm Jensen F12N with 15w (dc) applied to the field coil. Included are piccies of normalised amplitide response curves in various size cabinets, closed and vented.

    Since there are virtually an infinite number of alignments, internal volumes were kept to about 3 ft^3 or less. Higher low frequency output can be achieved with a vented enclosure of 7 to 10 cubic feet but that size is impractical. The old electric organs typically used such volumes and a lot were essentially open back or covered with a thin panel of about 0.25 inch or thinner. The one exception of which I can think is the Leslie.

    As a side note, don't be concerned about the original sound of 50 years ago; it can't be reproduced knowingly. To do that, one would need a time machine to go back to the 40's or 50's and hear a new unit. Suffice it to say that any vintage speaker, especially one with a pristine original cone will sound different than it did back then and in all probability it'll sound different that anything else today. Let's face it, it's all about nostalgia and take it from a 71 year old, that's priceless,.


    These next four were determined with 15w to the field coil. (15wFC)

    Driver Properties Red curve
    Name: F12N 15wFC
    Type: Standard one-way driver
    Company: JENSEN
    No. of Drivers = 1
    Fs = 49.77 Hz
    Qms = 23.84
    Vas = 200.1 liters
    Cms = 548.9 µm/N
    Mms = 18.63 g
    Rms = 0.539 lb/s
    Xmax = 2 mm
    Xmech = 0.118 in
    P-Dia = 10 in
    Sd = 0.0507 sq.m
    P-Vd = 0.00358 cu.ft
    Qes = 0.455
    Re = 6.9 ohms
    Le = 0.535 mH
    Z = 8.28 ohms
    BL = 9.4 Tm
    Pe = 50 watts
    Qts = 0.446
    no = 5.184 %
    1-W SPL = 99.35 dB
    2.83-V SPL = 99.99 dB
    -----------------------------------------
    Box Properties
    Name:
    Type: Closed Box
    Shape: Prism, square
    Vb = 0.783 cu.ft
    Qtc = 0.933
    QL = 19.94
    F3 = 111.4 Hz
    Fill = heavy





    Driver Properties Orange curve
    Optimum closed box alignment (Qtc=0.707)
    Name: F12N 15wFC
    Type: Standard one-way driver
    Company: JENSEN
    No. of Drivers = 1
    Fs = 49.77 Hz
    Qms = 23.84
    Vas = 200.1 liters
    Cms = 548.9 µm/N
    Mms = 18.63 g
    Rms = 0.539 lb/s
    Xmax = 2 mm
    Xmech = 0.118 in
    P-Dia = 10 in
    Sd = 0.0507 sq.m
    P-Vd = 0.00358 cu.ft
    Qes = 0.455
    Re = 6.9 ohms
    Le = 0.535 mH
    Z = 8.28 ohms
    BL = 9.4 Tm
    Pe = 50 watts
    Qts = 0.446
    no = 5.184 %
    1-W SPL = 99.35 dB
    2.83-V SPL = 99.99 dB
    -----------------------------------------
    Box Properties
    Name:
    Type: Closed Box
    Shape: Prism, square
    Vb = 1.835 cu.ft
    Qtc = 0.707
    QL = 17.62
    F3 = 96.44 Hz
    Fill = heavy




    Driver Properties Green curve
    Name: F12N 15wFC
    Type: Standard one-way driver
    Company: JENSEN
    No. of Drivers = 1
    Fs = 49.77 Hz
    Qms = 23.84
    Vas = 200.1 liters
    Cms = 548.9 µm/N
    Mms = 18.63 g
    Rms = 0.539 lb/s
    Xmax = 2 mm
    Xmech = 0.118 in
    P-Dia = 10 in
    Sd = 0.0507 sq.m
    P-Vd = 0.00358 cu.ft
    Qes = 0.455
    Re = 6.9 ohms
    Le = 0.535 mH
    Z = 8.28 ohms
    BL = 9.4 Tm
    Pe = 50 watts
    Qts = 0.446
    no = 5.184 %
    1-W SPL = 99.35 dB
    2.83-V SPL = 99.99 dB
    -----------------------------------------
    Box Properties
    Name:
    Type: Vented Box
    Shape: Prism, square
    Vb = 2.065 cu.ft
    Fb = 63.57 Hz
    QL = 6.772
    F3 = 79.94 Hz
    Fill = normal
    No. of Vents = 1
    Vent shape = round
    Vent ends = one flush
    Dv = 4.558 in
    Lv = 0.75 in




    Driver Properties Yellow curve
    Name: F12N 15wFC
    Type: Standard one-way driver
    Company: JENSEN
    No. of Drivers = 1
    Fs = 49.77 Hz
    Qms = 23.84
    Vas = 200.1 liters
    Cms = 548.9 µm/N
    Mms = 18.63 g
    Rms = 0.539 lb/s
    Xmax = 2 mm
    Xmech = 0.118 in
    P-Dia = 10 in
    Sd = 0.0507 sq.m
    P-Vd = 0.00358 cu.ft
    Qes = 0.455
    Re = 6.9 ohms
    Le = 0.535 mH
    Z = 8.28 ohms
    BL = 9.4 Tm
    Pe = 50 watts
    Qts = 0.446
    no = 5.184 %
    1-W SPL = 99.35 dB
    2.83-V SPL = 99.99 dB
    -----------------------------------------
    Box Properties
    Name:
    Type: Vented Box
    Shape: Prism, square
    Vb = 3.23 cu.ft
    Fb = 55.93 Hz
    QL = 6.772
    F3 = 67.58 Hz
    Fill = normal
    No. of Vents = 1
    Vent shape = round
    Vent ends = one flush
    Dv = 5.398 in
    Lv = 0.75 in

    These next two were determined with 10w to the field coil. (10wFC)

    Driver Properties Pink curve
    Name: F12N 10wFC
    Type: Standard one-way driver
    Company: JENSEN
    No. of Drivers = 1
    Fs = 49.63 Hz
    Qms = 22.96
    Vas = 201.4 liters
    Cms = 552.3 µm/N
    Mms = 18.62 g
    Rms = 0.558 lb/s
    Xmax = 2 mm
    Xmech = 0.118 in
    P-Dia = 10 in
    Sd = 0.0507 sq.m
    P-Vd = 0.00358 cu.ft
    Qes = 0.501
    Re = 6.6 ohms
    Le = 0.533 mH
    Z = 7.92 ohms
    BL = 8.746 Tm
    Pe = 50 watts
    Qts = 0.49
    no = 4.698 %
    1-W SPL = 98.92 dB
    2.83-V SPL = 99.75 dB
    -----------------------------------------
    Box Properties
    Name:
    Type: Closed Box
    Shape: Prism, square (optimum)
    Vb = 2.389 cu.ft
    Qtc = 0.707
    QL = 16.41
    F3 = 87.87 Hz
    Fill = heavy



    Driver Properties Blue curve
    Name: F12N 10wFC
    Type: Standard one-way driver
    Company: JENSEN
    No. of Drivers = 1
    Fs = 49.63 Hz
    Qms = 22.96
    Vas = 201.4 liters
    Cms = 552.3 µm/N
    Mms = 18.62 g
    Rms = 0.558 lb/s
    Xmax = 2 mm
    Xmech = 0.118 in
    P-Dia = 10 in
    Sd = 0.0507 sq.m
    P-Vd = 0.00358 cu.ft
    Qes = 0.501
    Re = 6.6 ohms
    Le = 0.533 mH
    Z = 7.92 ohms
    BL = 8.746 Tm
    Pe = 50 watts
    Qts = 0.49
    no = 4.698 %
    1-W SPL = 98.92 dB
    2.83-V SPL = 99.75 dB
    -----------------------------------------
    Box Properties
    Name:
    Type: Vented Box
    Shape: Prism, square (optimum)
    Vb = 2.661 cu.ft
    Fb = 68.85 Hz
    QL = 6.642
    F3 = 72.83 Hz
    Fill = normal
    No. of Vents = 1
    Vent shape = round
    Vent ends = one flush
    Dv = 6.59 in
    Lv = 0.75 in


    In the attached piccie, the trace colors correspond to the colors listed after Driver Properties

    The piccy has been enlarged in PhotoShop to facilitate reading the traces.

    The vents have been normalised for a tunnel depth of 0.75 inch and are consistent with maximum power tuning.

    Another consideration worthy of mention; this is NOT a bass guitar speaker despite it's original use in an electric organ. Those old organ amps delivered about 15 watts and organ tones are not percussive. The transient of a percussive signal fed through a 100 watt or arc welder type amplifier will destroy this unit in short order.

    This file can also be seen in my website. F12N


    For some reason, the piccy of the alignments response curves won't upload. This attempt failed on two XP and one WIN 8 machine. If you go to the above link, this whole file can be viewed along with the alignment picky as well as 3 of the F12N.

  • #2
    Click image for larger version

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    Here it is and THANKS A LOT for posting
    Juan Manuel Fahey

    Comment


    • #3
      Thank you very much for the thumbs up and your affixing the graph. Robert. (klipschorn)

      Comment


      • #4
        I finally got my old Jensen F12N powered up today. I put together an adjustable 100V DC filtered power supply to power the field coil - 680 ohms resistance. It has the original cone from 1957 in excellent shape. I mounted the speaker in a Hammond Tone cabinet - large open back cab. The speaker really sounds great, powered by a Deluxe Reverb clone. It also seems to be a fairly sensitive speaker with a lot of volume per watt. The residual magnetism in the speaker iron horseshoe is strong enough that I can play above bedroom level even without powering the field coil. I'm going to reverse the connections to the field coil to see if I can demagnetize it. As I turn down the field coil voltage, the speaker starts to distort a good bit at low volumes. I'm wondering if the low field in the gap is letting the voice coil get out of control?

        Comment


        • #5
          Yes.
          That's what Fluxtone speakers do, vary flux density to achieve lower acoustic output.
          Juan Manuel Fahey

          Comment


          • #6
            Originally posted by J M Fahey View Post
            Yes.
            That's what Fluxtone speakers do, vary flux density to achieve lower acoustic output.
            Thanks J M. I was expecting the volume drop like the Fluxtone speakers, but I wasn't expecting to get more distortion from the speaker as the field voltage was reduced. The distortion seems to be greatest at low note E-string guitar frequencies. I read that Fluxtone uses a tighter voice coil gap (.040 inch) than traditional speakers (.060 inch). I didn't check the VC gap on the Jensen F12N, since it's the original cone. I'm wondering about the cause for the distortion, since I don't hear it in the Fluxtone videos. Do you think it's the different gap? I have another F12N speaker that I'm going to experiment with today, to see if behaves in a similar fashion. I also have a Rola field coil speaker that I must recone before testing. Thanks in advance for any advice. Perhaps Mr.Coil will pop in for a visit and straighten me out?

            Comment


            • #7
              Narrow gap is one ticket to killer sound, because magnetic field focuses so much better, but then speakers become very difficult to build.

              I'm using 0.045" , no problem with guitar speakers but getting lots of rejects with Bass ones.
              Juan Manuel Fahey

              Comment


              • #8
                I have always thought that, yes, the narrower the VC/ Magnet gap, the more 'efficient' the speaker will be.

                But, as always, there is a trade off.
                The narrower the gap, the less power that the speaker can handle.
                (VC heating/ expansion, the need to precisely align the VC.)

                So a real high power speaker is inherently inefficient, needing a wider VC/ magnet gap.

                Comment


                • #9
                  I hooked up my second Jensen F12N speaker yesterday, and it sounds just like my first one. The cones and dust caps appear identical too. My two speakers have corrugated spiders like most modern speakers. I noticed that the OP, Klipschorn - Robert, had an F12N with the vintage-style flat phenolic spider. So perhaps, the Thiele parameters he measured, are different from my speakers.

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