Why put a step-down transformer after a vacuum tube in an a valve amplifier?

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I'm researching valve amplifiers. I found this schematic for one:



image



So the input is amplified by the first valve, and then the amplified signal is amplified again by the second valve, right?



My question is, why is the voltage being stepped down before going to the speaker? It seems pointless to me, increasing the voltage with the valves and then decreasing it again. All the schematics I can find online do this. Why?



(Is the 300V rail at the top related to the transformer? If not, what's it for?)










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    up vote
    5
    down vote

    favorite












    I'm researching valve amplifiers. I found this schematic for one:



    image



    So the input is amplified by the first valve, and then the amplified signal is amplified again by the second valve, right?



    My question is, why is the voltage being stepped down before going to the speaker? It seems pointless to me, increasing the voltage with the valves and then decreasing it again. All the schematics I can find online do this. Why?



    (Is the 300V rail at the top related to the transformer? If not, what's it for?)










    share|improve this question























      up vote
      5
      down vote

      favorite









      up vote
      5
      down vote

      favorite











      I'm researching valve amplifiers. I found this schematic for one:



      image



      So the input is amplified by the first valve, and then the amplified signal is amplified again by the second valve, right?



      My question is, why is the voltage being stepped down before going to the speaker? It seems pointless to me, increasing the voltage with the valves and then decreasing it again. All the schematics I can find online do this. Why?



      (Is the 300V rail at the top related to the transformer? If not, what's it for?)










      share|improve this question













      I'm researching valve amplifiers. I found this schematic for one:



      image



      So the input is amplified by the first valve, and then the amplified signal is amplified again by the second valve, right?



      My question is, why is the voltage being stepped down before going to the speaker? It seems pointless to me, increasing the voltage with the valves and then decreasing it again. All the schematics I can find online do this. Why?



      (Is the 300V rail at the top related to the transformer? If not, what's it for?)







      amplifier vacuum-tube






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      asked 54 mins ago









      Jacob Garby

      262




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          2 Answers
          2






          active

          oldest

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          up vote
          8
          down vote













          It's a question of impedance.



          The anode (plate) voltage of the tube varies over a wide range, while the current varies over a much smaller range. If you define output impedance as



          $$Z_out = fracDelta VDelta I$$



          This usually works out to a fairly high number for a typical vacuum tube, on the order of thousands of ohms.



          On the other hand, most speakers have a low impedance — on the order of 4 to 16 Ω — which means they want a relatively higher current change coupled with a relatively smaller voltage change.



          Note that in both cases, you're talking about the same amount of power (voltage × current), which is what the amplifer is really achieving — an increase in signal power from input to output.



          The transformer provides this impedance change. It trades off a high voltage swing for a high current swing. Without it, you'd get only a tiny fraction of the available signal power actually delivered to the speaker, limited by the relatively low current in the tube.




          From a comment:




          Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?




          The 300V power supply is required for much the same reason: The output of the impedance of the tube is inherently high.



          The 6V6 tube is rated for 50 mA plate current (average), which means that the signal current swing must be less than about ±40 mA (peak). Similarly, the tube is rated for a plate voltage of 250 V (nominally, but it is frequently overdriven in this respect), so the signal voltage needs to be less than about ±120 V (peak).



          The signal power available at the output is therefore the RMS current multiplied by the RMS voltage, or:



          $$frac40 mAsqrt2 cdot frac120 Vsqrt2 = frac4.8 W2 = 2.4 W$$



          If you use a lower plate voltage, the available power is reduced proportionally.



          Note that this works out to an output impedance of:



          $$Z_out = frac120 V40 mA = 3000 Omega$$



          To drive an 8Ω speaker, you'd use a 3000Ω:8Ω transformer (19.4:1 turns ratio), which would give you 4.38 VRMS and 548 mARMS at the speaker.






          share|improve this answer


















          • 1




            So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
            – Jacob Garby
            30 mins ago










          • Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
            – Dave Tweed♦
            28 mins ago











          • Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
            – Jacob Garby
            25 mins ago






          • 1




            See edit above.
            – Dave Tweed♦
            9 mins ago

















          up vote
          5
          down vote













          In addition to what Dave Tweed said (+1), the transformer in this case also eliminates the DC bias current from going to the speaker, and decouples the common mode input and output voltages.



          The plate current of V1 sits at a center value when idle. The input signal causes the plate current to go both up and down from the center value according to the peaks and troughs of the input signal.



          Even if there was a speaker that was impedance-matched to the plate of the 6V6, the DC bias current thru it would not be desirable. The transformer also blocks DC, while passing the relevant AC parts of the signal.



          Note that impedance matching is still the primary reason. Since a transformer is required for that anyway, the designer of the circuit made use of the fact that it also blocks DC, and that the common mode input and output voltages are decoupled. This latter fact allows one side of the speaker to be grounded, even though the transformer primary is tied to 300 V.






          share|improve this answer




















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            2 Answers
            2






            active

            oldest

            votes








            2 Answers
            2






            active

            oldest

            votes









            active

            oldest

            votes






            active

            oldest

            votes








            up vote
            8
            down vote













            It's a question of impedance.



            The anode (plate) voltage of the tube varies over a wide range, while the current varies over a much smaller range. If you define output impedance as



            $$Z_out = fracDelta VDelta I$$



            This usually works out to a fairly high number for a typical vacuum tube, on the order of thousands of ohms.



            On the other hand, most speakers have a low impedance — on the order of 4 to 16 Ω — which means they want a relatively higher current change coupled with a relatively smaller voltage change.



            Note that in both cases, you're talking about the same amount of power (voltage × current), which is what the amplifer is really achieving — an increase in signal power from input to output.



            The transformer provides this impedance change. It trades off a high voltage swing for a high current swing. Without it, you'd get only a tiny fraction of the available signal power actually delivered to the speaker, limited by the relatively low current in the tube.




            From a comment:




            Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?




            The 300V power supply is required for much the same reason: The output of the impedance of the tube is inherently high.



            The 6V6 tube is rated for 50 mA plate current (average), which means that the signal current swing must be less than about ±40 mA (peak). Similarly, the tube is rated for a plate voltage of 250 V (nominally, but it is frequently overdriven in this respect), so the signal voltage needs to be less than about ±120 V (peak).



            The signal power available at the output is therefore the RMS current multiplied by the RMS voltage, or:



            $$frac40 mAsqrt2 cdot frac120 Vsqrt2 = frac4.8 W2 = 2.4 W$$



            If you use a lower plate voltage, the available power is reduced proportionally.



            Note that this works out to an output impedance of:



            $$Z_out = frac120 V40 mA = 3000 Omega$$



            To drive an 8Ω speaker, you'd use a 3000Ω:8Ω transformer (19.4:1 turns ratio), which would give you 4.38 VRMS and 548 mARMS at the speaker.






            share|improve this answer


















            • 1




              So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
              – Jacob Garby
              30 mins ago










            • Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
              – Dave Tweed♦
              28 mins ago











            • Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
              – Jacob Garby
              25 mins ago






            • 1




              See edit above.
              – Dave Tweed♦
              9 mins ago














            up vote
            8
            down vote













            It's a question of impedance.



            The anode (plate) voltage of the tube varies over a wide range, while the current varies over a much smaller range. If you define output impedance as



            $$Z_out = fracDelta VDelta I$$



            This usually works out to a fairly high number for a typical vacuum tube, on the order of thousands of ohms.



            On the other hand, most speakers have a low impedance — on the order of 4 to 16 Ω — which means they want a relatively higher current change coupled with a relatively smaller voltage change.



            Note that in both cases, you're talking about the same amount of power (voltage × current), which is what the amplifer is really achieving — an increase in signal power from input to output.



            The transformer provides this impedance change. It trades off a high voltage swing for a high current swing. Without it, you'd get only a tiny fraction of the available signal power actually delivered to the speaker, limited by the relatively low current in the tube.




            From a comment:




            Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?




            The 300V power supply is required for much the same reason: The output of the impedance of the tube is inherently high.



            The 6V6 tube is rated for 50 mA plate current (average), which means that the signal current swing must be less than about ±40 mA (peak). Similarly, the tube is rated for a plate voltage of 250 V (nominally, but it is frequently overdriven in this respect), so the signal voltage needs to be less than about ±120 V (peak).



            The signal power available at the output is therefore the RMS current multiplied by the RMS voltage, or:



            $$frac40 mAsqrt2 cdot frac120 Vsqrt2 = frac4.8 W2 = 2.4 W$$



            If you use a lower plate voltage, the available power is reduced proportionally.



            Note that this works out to an output impedance of:



            $$Z_out = frac120 V40 mA = 3000 Omega$$



            To drive an 8Ω speaker, you'd use a 3000Ω:8Ω transformer (19.4:1 turns ratio), which would give you 4.38 VRMS and 548 mARMS at the speaker.






            share|improve this answer


















            • 1




              So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
              – Jacob Garby
              30 mins ago










            • Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
              – Dave Tweed♦
              28 mins ago











            • Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
              – Jacob Garby
              25 mins ago






            • 1




              See edit above.
              – Dave Tweed♦
              9 mins ago












            up vote
            8
            down vote










            up vote
            8
            down vote









            It's a question of impedance.



            The anode (plate) voltage of the tube varies over a wide range, while the current varies over a much smaller range. If you define output impedance as



            $$Z_out = fracDelta VDelta I$$



            This usually works out to a fairly high number for a typical vacuum tube, on the order of thousands of ohms.



            On the other hand, most speakers have a low impedance — on the order of 4 to 16 Ω — which means they want a relatively higher current change coupled with a relatively smaller voltage change.



            Note that in both cases, you're talking about the same amount of power (voltage × current), which is what the amplifer is really achieving — an increase in signal power from input to output.



            The transformer provides this impedance change. It trades off a high voltage swing for a high current swing. Without it, you'd get only a tiny fraction of the available signal power actually delivered to the speaker, limited by the relatively low current in the tube.




            From a comment:




            Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?




            The 300V power supply is required for much the same reason: The output of the impedance of the tube is inherently high.



            The 6V6 tube is rated for 50 mA plate current (average), which means that the signal current swing must be less than about ±40 mA (peak). Similarly, the tube is rated for a plate voltage of 250 V (nominally, but it is frequently overdriven in this respect), so the signal voltage needs to be less than about ±120 V (peak).



            The signal power available at the output is therefore the RMS current multiplied by the RMS voltage, or:



            $$frac40 mAsqrt2 cdot frac120 Vsqrt2 = frac4.8 W2 = 2.4 W$$



            If you use a lower plate voltage, the available power is reduced proportionally.



            Note that this works out to an output impedance of:



            $$Z_out = frac120 V40 mA = 3000 Omega$$



            To drive an 8Ω speaker, you'd use a 3000Ω:8Ω transformer (19.4:1 turns ratio), which would give you 4.38 VRMS and 548 mARMS at the speaker.






            share|improve this answer














            It's a question of impedance.



            The anode (plate) voltage of the tube varies over a wide range, while the current varies over a much smaller range. If you define output impedance as



            $$Z_out = fracDelta VDelta I$$



            This usually works out to a fairly high number for a typical vacuum tube, on the order of thousands of ohms.



            On the other hand, most speakers have a low impedance — on the order of 4 to 16 Ω — which means they want a relatively higher current change coupled with a relatively smaller voltage change.



            Note that in both cases, you're talking about the same amount of power (voltage × current), which is what the amplifer is really achieving — an increase in signal power from input to output.



            The transformer provides this impedance change. It trades off a high voltage swing for a high current swing. Without it, you'd get only a tiny fraction of the available signal power actually delivered to the speaker, limited by the relatively low current in the tube.




            From a comment:




            Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?




            The 300V power supply is required for much the same reason: The output of the impedance of the tube is inherently high.



            The 6V6 tube is rated for 50 mA plate current (average), which means that the signal current swing must be less than about ±40 mA (peak). Similarly, the tube is rated for a plate voltage of 250 V (nominally, but it is frequently overdriven in this respect), so the signal voltage needs to be less than about ±120 V (peak).



            The signal power available at the output is therefore the RMS current multiplied by the RMS voltage, or:



            $$frac40 mAsqrt2 cdot frac120 Vsqrt2 = frac4.8 W2 = 2.4 W$$



            If you use a lower plate voltage, the available power is reduced proportionally.



            Note that this works out to an output impedance of:



            $$Z_out = frac120 V40 mA = 3000 Omega$$



            To drive an 8Ω speaker, you'd use a 3000Ω:8Ω transformer (19.4:1 turns ratio), which would give you 4.38 VRMS and 548 mARMS at the speaker.







            share|improve this answer














            share|improve this answer



            share|improve this answer








            edited 2 mins ago

























            answered 41 mins ago









            Dave Tweed♦

            108k9129232




            108k9129232







            • 1




              So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
              – Jacob Garby
              30 mins ago










            • Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
              – Dave Tweed♦
              28 mins ago











            • Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
              – Jacob Garby
              25 mins ago






            • 1




              See edit above.
              – Dave Tweed♦
              9 mins ago












            • 1




              So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
              – Jacob Garby
              30 mins ago










            • Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
              – Dave Tweed♦
              28 mins ago











            • Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
              – Jacob Garby
              25 mins ago






            • 1




              See edit above.
              – Dave Tweed♦
              9 mins ago







            1




            1




            So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
            – Jacob Garby
            30 mins ago




            So am I right in thinking the the transformer basically reduces the impedance, to one which is correct for the speaker?
            – Jacob Garby
            30 mins ago












            Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
            – Dave Tweed♦
            28 mins ago





            Yes, that's the idea. The impedance ratio is the square of the turns ratio. For example if you need a 1000:1 impedance ratio, you'd want roughly a 32:1 turns ratio.
            – Dave Tweed♦
            28 mins ago













            Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
            – Jacob Garby
            25 mins ago




            Thanks, got it! Any idea what the 300V rail is for? Is it simply a power supply for the valves? Why is it so high-voltage?
            – Jacob Garby
            25 mins ago




            1




            1




            See edit above.
            – Dave Tweed♦
            9 mins ago




            See edit above.
            – Dave Tweed♦
            9 mins ago












            up vote
            5
            down vote













            In addition to what Dave Tweed said (+1), the transformer in this case also eliminates the DC bias current from going to the speaker, and decouples the common mode input and output voltages.



            The plate current of V1 sits at a center value when idle. The input signal causes the plate current to go both up and down from the center value according to the peaks and troughs of the input signal.



            Even if there was a speaker that was impedance-matched to the plate of the 6V6, the DC bias current thru it would not be desirable. The transformer also blocks DC, while passing the relevant AC parts of the signal.



            Note that impedance matching is still the primary reason. Since a transformer is required for that anyway, the designer of the circuit made use of the fact that it also blocks DC, and that the common mode input and output voltages are decoupled. This latter fact allows one side of the speaker to be grounded, even though the transformer primary is tied to 300 V.






            share|improve this answer
























              up vote
              5
              down vote













              In addition to what Dave Tweed said (+1), the transformer in this case also eliminates the DC bias current from going to the speaker, and decouples the common mode input and output voltages.



              The plate current of V1 sits at a center value when idle. The input signal causes the plate current to go both up and down from the center value according to the peaks and troughs of the input signal.



              Even if there was a speaker that was impedance-matched to the plate of the 6V6, the DC bias current thru it would not be desirable. The transformer also blocks DC, while passing the relevant AC parts of the signal.



              Note that impedance matching is still the primary reason. Since a transformer is required for that anyway, the designer of the circuit made use of the fact that it also blocks DC, and that the common mode input and output voltages are decoupled. This latter fact allows one side of the speaker to be grounded, even though the transformer primary is tied to 300 V.






              share|improve this answer






















                up vote
                5
                down vote










                up vote
                5
                down vote









                In addition to what Dave Tweed said (+1), the transformer in this case also eliminates the DC bias current from going to the speaker, and decouples the common mode input and output voltages.



                The plate current of V1 sits at a center value when idle. The input signal causes the plate current to go both up and down from the center value according to the peaks and troughs of the input signal.



                Even if there was a speaker that was impedance-matched to the plate of the 6V6, the DC bias current thru it would not be desirable. The transformer also blocks DC, while passing the relevant AC parts of the signal.



                Note that impedance matching is still the primary reason. Since a transformer is required for that anyway, the designer of the circuit made use of the fact that it also blocks DC, and that the common mode input and output voltages are decoupled. This latter fact allows one side of the speaker to be grounded, even though the transformer primary is tied to 300 V.






                share|improve this answer












                In addition to what Dave Tweed said (+1), the transformer in this case also eliminates the DC bias current from going to the speaker, and decouples the common mode input and output voltages.



                The plate current of V1 sits at a center value when idle. The input signal causes the plate current to go both up and down from the center value according to the peaks and troughs of the input signal.



                Even if there was a speaker that was impedance-matched to the plate of the 6V6, the DC bias current thru it would not be desirable. The transformer also blocks DC, while passing the relevant AC parts of the signal.



                Note that impedance matching is still the primary reason. Since a transformer is required for that anyway, the designer of the circuit made use of the fact that it also blocks DC, and that the common mode input and output voltages are decoupled. This latter fact allows one side of the speaker to be grounded, even though the transformer primary is tied to 300 V.







                share|improve this answer












                share|improve this answer



                share|improve this answer










                answered 26 mins ago









                Olin Lathrop

                276k28328774




                276k28328774



























                     

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