On Fri, 26 Jul 2013 10:37:02 -0700 (PDT), George Herold
<
ghe...@teachspin.com> wrote:
>Yeah.. So like twenty years ago I did a 20 MHz pulse amp for an NMR system.
>It looked something like those pictures.. not at all easy to do.
>(Well at least it took me a while. I was learning RF at the same time.)
We may have been competitors. I did an NMR driver and power amp
system using then new VMOS devices. My guess(tm) was about 1979.
Getting ultra low distortion of -60dB 3rd order IM at rated power gave
me headaches and nightmares.
>> If OP wants 10 watts of distortion and
>> intermod free output, which is likely if he's feeding it with a
>> function generator, he's likely to get only about 15% amplifier
>> efficiency with class A. That means he has to burn 67 watts of heat
>> in order to get 10 watts of clean output.
>Hmm is it that bad?
It's always worse, never better.
>(the efficiency) I was thinking about just
>biasing the transistor at the mid current point. And then the
>sine wave turns it on or off.. but the average power loss still
>looks to be about 1/2.
>So ideally 50% efficiency.. but of course it will be a bit worse
>than that in practice. (I may be making some huge blunder here,
>but then (hopefully) I'll be corrected and learn something.)
The problem is linearity. If I setup the amplifier for best
efficiency, I end up driving the output from rail to rail. That's
fine for getting the maximum output from the device, but not so fine
for getting the best linearity, lowest intermod, and minimum
distortion. Generally, the output swing needs to stay away from the
rails. A safe guess(tm) would be about 50% voltage swing, which is
1/4th of the maximum output power. For example, for 10 watts of clean
output, I would need an amp capable of producing 40 watts. Of course,
if one doesn't care about distortion, intermod, and such, a 10 watt
amp would do just fine.
As a side note, the bandwidth should be at least 3 times the maximum
usable frequency. If the function generator is expected to be usable
to 10 MHz, the amp has to go up to at least 30 Mhz in order to amplify
the 3rd harmonic necessary for something resembling a square wave.
I dunno about using the LT1210. From the data sheet:
<
http://cds.linear.com/docs/en/datasheet/1210fa.pdf>
the maximum output swing is +/- 11.5V. Into a 50 ohm load, that's:
(22.5v / 2 * 0.707)^2 / 50 = 0.4 watts rms
So much for direct drive. 0.4 watts seems a bit less than the
required 10 watts output power.
However, the LT1210 can drive a 10 ohm load with a 22.5v swing. Using
a 4:1 impedance ratio output transformer, the maximum output would be:
(22.5 / 2 * 0.707)^2 / 12.5 ohms = 1.6 watts rms
which is still shy of 10 watts by a large amount.
In my never humble opinion, getting rid the transformers and ferrites
is a necessity. To deliver 10 watts into 50 ohms, one needs:
(10 * 50)^0.5 = 22.4 v rms * 2.828 = 63.3 volts p-p
which means a +/- 50v power supply and output swing.
>Upon further reflection, (sorry for thinking out loud) I was
>picturing an opamp->transistor, voltage to current source for
>driving the inductor, since that's what I often use for driving coils.
>Hey, if the OP's load is a coil then he may want a current source.
>(no change in the B-field as the coil warms up.)
All I know about the load is that it's a "physics package" which is
the common term for rubidium and cesium fountains used in frequency
standards. I don't recall the excitation frequency (and am too lazy
to Google for the numbers).