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Regarding the 7A11, its designer [[John Addis]] says: | Regarding the 7A11, its designer [[John Addis]] says: | ||
<blockquote> | <blockquote> | ||
The 7A11 input capacitance is 5.8 pF from 5 mV/Div to 50 mV/Div, goes down to 3.4 pF from | The 7A11 input capacitance is 5.8 pF from 5 mV/Div to 50 mV/Div, goes down to 3.4 pF from 100 mV/Div to 1 V/Div, and down again to 2.0 pF from 2 V/Div to 20 V/Div. | ||
100 mV/Div to 1 V/Div, and down again to 2.0 pF from 2 V/Div to 20 V/Div. Because the AC | Because the AC coupling is attained with a plug-on capacitor (that adds 1.2 pF to the input C), a DC offset is supplied to reduce the need for AC coupling. | ||
coupling is attained with a plug-on capacitor (that adds 1.2 pF to the input C), a DC offset | |||
is supplied to reduce the need for AC coupling. | A nice thing about the 7A11 was that the probe cable length was adjustable in six steps to just over 7 feet in length. | ||
You just uncoil however much cable length you want. | |||
A nice thing about the 7A11 was that the probe cable length was adjustable in six steps | The 7A11 was admittedly clumsy to use because of the probe size. It had some trouble — DC drift, RF pickup at 5 mV, 100 mV and 2 V/Div. | ||
to just over 7 feet in length. You just uncoil however much cable length you want. | It was not very popular partially because it was expensive, $850 for single channel vs. dual channel [[7A12]] (105 MHz) at $700. | ||
But there was never another 1 MΩ 7000-series plugin as fast as the 7A11 ... and it was one of the originals! | |||
The 7A11 was admittedly clumsy to use because of the probe size. It had some trouble — | |||
DC drift, RF pickup at 5 mV, 100 mV and 2 V/Div. It was not very popular partially | |||
because it was expensive, $850 for single channel vs. dual channel [[7A12]] (105 MHz) at $700. | |||
But there was never another 1 MΩ 7000-series plugin as fast as the 7A11 ... and it was | |||
one of the originals! | |||
The [[7A16]] (single channel plugin) was also 150 MHz, but that was a year later. | The [[7A16]] (single channel plugin) was also 150 MHz, but that was a year later. | ||
Then the [[7904]] came out in late 1971. That made the 7A11 a 250 MHz plugin (for $950). | Then the [[7904]] came out in late 1971. That made the 7A11 a 250 MHz plugin (for $950). | ||
The [[7A16]] was then 225 MHz (for $625). The 7A16 disappeared rapidly and became the [[7A16A]], | The [[7A16]] was then 225 MHz (for $625). The 7A16 disappeared rapidly and became the [[7A16A]], still 225 MHz in 1973. | ||
still 225 MHz in 1973. | |||
In 1972, the [[485]] came out with a 250 MHz, 1 MΩ input. | In 1972, the [[485]] came out with a 250 MHz, 1 MΩ input. | ||
The 485 used a faster IC process | The 485 used a faster IC process ("[[SH2]]", 3.5 GHz) but the 1 MΩ to 50 Ω converter used only discrete devices. (See Electronics June, 1972.) | ||
("[[SH2]]", 3.5 GHz) but the 1 MΩ to 50 Ω converter used only discrete devices. | |||
(See Electronics June, 1972.) | By 1974, the 7A11 cost $950 and the new, popular [[7A26]] (dual trace) was $1,050, not counting probes. | ||
But that would still only get you to 50 mV/div with a (9.5 pF, 3 foot, × 10) probe, five years after the 7A11 introduction. | |||
[[Tom Rousseau]] designed the 7A26 which used the faster IC process and a [[155-0078-00|vertical IC I designed for the 485]]. | |||
By 1974, the 7A11 cost $950 and the new, popular [[7A26]] (dual trace) was $1,050, not | The 7A26 sold so well that Tektronix presented Tom with an entirely gold plated 7A26! | ||
counting probes. But that would still only get you to 50 mV/div with a (9.5 pF, 3 foot, × 10) | Obviously, he still has it. | ||
probe, five years after the 7A11 introduction. | |||
faster IC process and a [[155-0078-00|vertical IC I designed for the 485]]. The 7A26 sold so well that | Remember also that the 7A11 was introduced at the same show as the HP183A/1830A/1840A, faster (250 MHz), smaller, lighter, and less expensive with better triggering than 7000 series had. | ||
Tektronix presented Tom with an entirely gold plated 7A26! Obviously, he still has it. | |||
Remember also that the 7A11 was introduced at the same show as the HP183A/1830A/1840A, | |||
faster (250 MHz), smaller, lighter, and less expensive with better triggering than 7000 series had. | |||
Their secrets were Al DeVilbiss and a faster IC process. We had neither. | Their secrets were Al DeVilbiss and a faster IC process. We had neither. | ||
The star-crossed [[7A12]], which was supposed to be the dual trace flagship of the original plugins, was only 105 MHz, not the hoped-for 150 MHz. | |||
The star-crossed [[7A12]], which was supposed to be the dual trace flagship of the original plugins, | That was partially due to the fact that it used the existing Tek IC process (about 1 GHz). The HP IC process was about 3 GHz. | ||
was only 105 MHz, not the hoped-for 150 MHz. That was partially due to the fact that it used the | The 7A11 used discrete NPN and PNP transistors with 4 GHz f<sub>t</sub>. | ||
existing Tek IC process (about 1 GHz). The HP IC process was about 3 GHz. The 7A11 used discrete | |||
NPN and PNP transistors with 4 GHz f<sub>t</sub>. | There is one noteworthy point I would like to make about the 7A11. In those days, the different V/div settings were generally attained using fixed high impedance attenuators, usually stacked one after another and few with more than ×10 attenuation. | ||
I wanted the 7A11 to be able to handle the full useful range of sensitivites that other plugins attained when adding a ×10 probe ... that meant going to 20 V/Div. | |||
But you could certainly get to 5 mV/Div, which you could not attain with a 5 mV/Div plugin and a ×10 passive probe. | |||
There is one noteworthy point I would like to make about the 7A11. In those days, the different | |||
V/div settings were generally attained using fixed high impedance attenuators, usually stacked one | But using that scheme, if the 7A11 went to 20 V/Div, it would have to stack three ×10 attenuators inside the probe, making it a behemoth, and even if you did, that would still leave the ×2 and ×5 attenuations up to gain switching in the amplifier. | ||
after another and few with more than ×10 attenuation. I wanted the 7A11 to be able to handle the | |||
full useful range of sensitivites that other plugins attained when adding a ×10 probe ... that | Problem with gain switching is, the bandwidth and transient response tend to change when you change amplifier gain. | ||
meant going to 20 V/Div. But you could certainly get to 5 mV/Div, which you could not attain with | The greater the gain change, the greater the bandwidth/transient response change in the amplifier. | ||
a 5 mV/Div plugin and a ×10 passive probe. | The more gain settings you had, the worse it got due to longer leads and more parasitics. | ||
To get a 1-2-5 sequence from 5 mV/Div to 20 V/Div, it had the worst of all possible worlds. | |||
But using that scheme, if the 7A11 went to 20 V/Div, it would have to stack three ×10 attenuators | The 7A11 needed two ×20 attenuators in the probe and that meant that it needed not just ×1, ×2 and ×5 gains in the amplifier, but ×1, ×2, ×2.5, ×4, ×5 and ×10! | ||
inside the probe, | This had not been done before, but the 7A11 does it without any change in transient response! | ||
attenuations up to gain switching in the amplifier. | |||
The secret is three entirely passive, [[miniature relays | relay-switched]], O-pad attenuators: ×2, ×2, and ×2.5 in a balanced transmission line environment. | |||
Stack them up (as you can do with matched pads) and you get all the combinations you need: ×1, ×2, ×2.5, ×4, ×5, and ×10. From 5 mV/Div to 20 V/Div, twelve different V/div settings, more than any other high speed plug in! | |||
Problem with gain switching is, the bandwidth and transient response tend to change when you change | |||
amplifier gain. The greater the gain change, the greater the bandwidth/transient response change in | I got a patent on the variable attenuator, which was just a JFET shunting the O-pads. | ||
the amplifier. The more gain settings you had, the worse it got due to longer leads and more parasitics. | The patent had to do with making the gain vs. control rotation linear, which does not simply happen with linear gate-source voltage control. | ||
The JFET causes a small change in transient response, but not a bad one. | |||
To get a 1-2-5 sequence from 5 mV/Div to 20 V/Div, it had the worst of all possible worlds. The 7A11 | |||
needed two ×20 attenuators in the probe and that meant that it needed not just ×1, ×2 and ×5 gains in | |||
the amplifier, but ×1, ×2, ×2.5, ×4, ×5 and ×10! This had not been done before, but the 7A11 does it | |||
without any change in transient response! | |||
The secret is three entirely passive, [[miniature relays | relay-switched]], O-pad attenuators: ×2, ×2, and ×2.5 in a | |||
balanced transmission line environment. Stack them up (as you can do with matched pads) and you get | |||
all the combinations you need: ×1, ×2, ×2.5, ×4, ×5, and ×10. From 5 mV/Div to 20 V/Div, twelve | |||
different V/div settings, more than any other high speed plug in! | |||
I got a patent on the variable attenuator, which was just a JFET shunting the O-pads. The patent had | |||
to do with making the gain vs. control rotation linear, which does not simply happen with linear | |||
gate-source voltage control. The JFET causes a small change in transient response, but not a bad one. | |||
[[Ron Peltola]] (of [[Peltola connector]] fame) designed the probe. I helped on the probe's amplifier. | [[Ron Peltola]] (of [[Peltola connector]] fame) designed the probe. I helped on the probe's amplifier. | ||
</blockquote> | </blockquote> | ||
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|align=right| $2,700 | |align=right| $2,700 | ||
|- | |- | ||
! | ! 2023 value | ||
|align=right| $ | |align=right| $6,400 | ||
|align=right| $ | |align=right| $6,400 | ||
|align=right| $ | |align=right| $7,900 | ||
|- | |- | ||
|} | |} |