39,717
edits
No edit summary |
|||
Line 42: | Line 42: | ||
It was requested that we change the design to be a TM500 plug-in module instead. | It was requested that we change the design to be a TM500 plug-in module instead. | ||
The AM503 front panel still looks like a scope’s plug-in. | The AM503 front panel still looks like a scope’s plug-in. | ||
The AC/DC switch and | The AC/DC switch and 5 MHz bandwidth switch, for example, were left on the front panel from the oscilloscope design. | ||
There are still some remnants of the oscilloscope circuits, such as the [[cam switch]] that interfaced to a circuit board that sets the scope’s readout in amps/div. | There are still some remnants of the oscilloscope circuits, such as the [[cam switch]] that interfaced to a circuit board that sets the scope’s readout in amps/div. | ||
The square pin header connector on the back of the circuit board was for the readout, but not used. | The square pin header connector on the back of the circuit board was for the readout, but not used. | ||
Line 51: | Line 51: | ||
The AM503 was also intended to work with future higher frequency probes, like the [[P6022]] with an added hall device for DC measurements. | The AM503 was also intended to work with future higher frequency probes, like the [[P6022]] with an added hall device for DC measurements. | ||
The smaller P6022 had a 120 MHz bandwidth, whereas the [[P6302]] was only 50 MHz. | The smaller P6022 had a 120 MHz bandwidth, whereas the [[P6302]] was only 50 MHz. | ||
The design engineer (actually only an R&D technician) | The design engineer (actually only an R&D technician) moved to the TM500 engineering and evaluation group before this probe was created. | ||
The AM503 was being developed in the Accessories division in Beaverton, since that’s where the other current probes were designed. | The AM503 was being developed in the Accessories division in Beaverton, since that’s where the other current probes were designed. | ||
That was unusual as all the other plug-ins were being designed by the TM500 group on Walker Road, near Hillsboro. | That was unusual as all the other plug-ins were being designed by the TM500 group on Walker Road, near Hillsboro. | ||
Line 59: | Line 59: | ||
<br> | <br> | ||
There were some innovations that were incorporated in this design: | There were some innovations that were incorporated in this design: | ||
The [[cam switch]] with replaceable laser trimmed attenuator resistors, a | The [[cam switch]] with replaceable laser trimmed attenuator resistors, a 1 GHz Gilbert cell op amp (actually developed by Howard Jones in 1963). | ||
This IC, [[155-0078-xx]], was being developed by Tek’s IC department. | This IC, [[155-0078-xx]], was being developed by Tek’s IC department. | ||
(At the same time these IC designers were teaching the technology at the University of Portland as part of Tek’s excellent education and training program.) | (At the same time these IC designers were teaching the technology at the University of Portland as part of Tek’s excellent education and training program.) | ||
Line 76: | Line 76: | ||
The Hall device used for the DC measurements used a vacuum deposition process with indium antimonide. | The Hall device used for the DC measurements used a vacuum deposition process with indium antimonide. | ||
The cores were lapped and polished to a few Fresnel lines flatness to minimize the gap on the sliding ferrite. | The cores were lapped and polished to a few Fresnel lines flatness to minimize the gap on the sliding ferrite. | ||
The L/R time constant affects the point where the Hall device and | The L/R time constant affects the point where the Hall device and coils’ bandwidths crossover. | ||
<br> | <br> | ||
<br> | <br> | ||
An interesting aspect of the design was trying to find a way to test and calibrate the peak current pulse on the larger P6303. | An interesting aspect of the design was trying to find a way to test and calibrate the peak current pulse on the larger P6303. | ||
Luckily we had the tube lab. We developed an argon filled thyratron that could discharge a | Luckily we had the tube lab. We developed an argon filled thyratron that could discharge a 4 kV charge line into a 4 Ω load. | ||
The load resistor was designed and built by Tektronix. A large rectangular ceramic plate was coated with a metal film resistor. | The load resistor was designed and built by Tektronix. A large rectangular ceramic plate was coated with a metal film resistor. | ||
It had a voltage divider tap to allow for a safer measurement point. It was laser trimmed for accuracy. | It had a voltage divider tap to allow for a safer measurement point. It was laser trimmed for accuracy. | ||
The current probe would measure the current to ground through this resistor, so the voltage was near zero for the user. | The current probe would measure the current to ground through this resistor, so the voltage was near zero for the user. | ||
The | The 4 kV supply was charged into a 4 Ω transmission line so a clean high current pulse would be generated. | ||
This concept was taken from Tek’s [[109]] pulse generator. | This concept was taken from Tek’s [[109]] pulse generator. | ||
A trigger circuit was designed to fire the grid. It was based on the xenon flash circuit of the C5 camera flash, also in the Accessories group. | |||
A trigger circuit was designed to fire the grid. It was based on the xenon flash circuit of the [[C-5|C5 camera]] flash, also in the Accessories group. | |||
The first prototype I made arced across the laser trim lines in the metal film resistor as they were cut perpendicular to the current flow. | The first prototype I made arced across the laser trim lines in the metal film resistor as they were cut perpendicular to the current flow. | ||
This caused high voltage gradients across the film and thus the arcing across the cuts. | This caused high voltage gradients across the film and thus the arcing across the cuts. | ||
Line 93: | Line 94: | ||
<br> | <br> | ||
<br> | <br> | ||
Also interesting, the P6303 | Also interesting, the P6303 required special potting epoxy developed by 3M. | ||
The epoxy used in other current probes put excessive stress on the larger ferrite that caused the inductance to drop to zero. | The epoxy used in other current probes put excessive stress on the larger ferrite that caused the inductance to drop to zero. | ||
due to the magnetostriction property of ferrite. | |||
The epoxy could even also cause shear fractures in the ferrite. | The epoxy could even also cause shear fractures in the ferrite. | ||
</blockquote> | </blockquote> |