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#1
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I wonder whether someone can help me to clear an issue regarding AM signals
produced by a (class-C) tube transmitter. It is well known that the peak-envelope power of a carrier 100%-modulated by a pure sine wave is four times the unmodulated carrier power. This is simply because, according to the Ohm's law, doubling voltage power gets four times higher. I would have no problem if a tube would behave like a normal resistor. But a tube instead behaves like a differential resistor, and this makes a lot of difference. If you consider the plate characteristic of a typical pentode, you see that plate current does not change much increasing plate voltage. So, doubling the plate voltage, power would not get four times higher, but just a little more that two times. The triode plate current is instead much more dependent on plate voltage so that, doubling plate voltage, power would grow probably at least three times. But definitely not four times. Can someone pinpoint what I am missing? 73 Tony I0JX |
#2
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On Feb 16, 8:47*pm, "Antonio Vernucci" wrote:
I wonder whether someone can help me to clear an issue regarding AM signals produced by a (class-C) tube transmitter. It is well known that the peak-envelope power of a carrier 100%-modulated by a pure sine wave is four times the unmodulated carrier power. This is simply because, according to the Ohm's law, doubling voltage power gets four times higher. I would have no problem if a tube would behave like a normal resistor. But a tube instead behaves like a differential resistor, and this makes a lot of difference. If you consider the plate characteristic of a typical pentode, you see that plate current does not change much increasing plate voltage. So, doubling the plate voltage, power would not get four times higher, but just a little more that two times. The triode plate current is instead much more dependent on plate voltage so that, doubling plate voltage, power would grow probably at least three times. But definitely not four times. Can someone pinpoint what I am missing? 73 Tony I0JX You could be a bit mixed up ... the final is acting as a high level mixer ... you end up with a spectrum .. not a single carier .. in fact the carrier amplitude is not changed by the process (should not be ...) that is , the additional power is in the sidebands G .. |
#3
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![]() "Antonio Vernucci" I wonder whether someone can help me to clear an issue regarding AM signals produced by a (class-C) tube transmitter. It is well known that the peak-envelope power of a carrier 100%-modulated by a pure sine wave is four times the unmodulated carrier power. This is simply because, according to the Ohm's law, doubling voltage power gets four times higher. I would have no problem if a tube would behave like a normal resistor. But a tube instead behaves like a differential resistor, and this makes a lot of difference. If you consider the plate characteristic of a typical pentode, you see that plate current does not change much increasing plate voltage. So, doubling the plate voltage, power would not get four times higher, but just a little more that two times. The triode plate current is instead much more dependent on plate voltage so that, doubling plate voltage, power would grow probably at least three times. But definitely not four times. Can someone pinpoint what I am missing? ** I'll give it a go. In a class C stage, the grid is overdriven with RF voltage so the output tube is biased either fully conducting or off - as a result, the plate voltage stays fairly low whenever the tube is conducting, which is less than 50 % of each RF cycle. However, the actual current flow through the tube depends on the ratio of the external circuit impedance ( ie a tuned load) to the B+ voltage. Since the tuned load does not vary in impedance, the B+ voltage controls how much RF current flow there is. IOW, the output voltage from a well designed class C stage follows the B+ voltage linearly over a wide range cos to a large degree, the plate voltage / plate current characteristics of the tube have been rendered irrelevant. ...... Phil |
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