Time-to-Digital-Converters by Acam
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Time to Digital Converters

TDC - GP1
TDC - GP2
TDC - GPX
Time-to-Digital Applications
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PICOSTRAIN®

Time to Digital Converters for Digital Strain Gage

PICOSTRAIN® PS08
PICOSTRAIN® PS081
PICOSTRAIN® PS021
Strain Gage Applications
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PICOCAP®

Time to Digital Converters for Capacitance Measurement

PICOCAP® PS021
PICOCAP® PSA21
Capacitance Applications
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PICOTURN®

Time to Digital Converters for Speed Sensors

PICOTURN® 2G
PICOTURN® BM/SM
Speed Sensor Applications
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Time-to-Digital - TDC Cookbook

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time-to-digital converters
TDC - Cookbook
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PS021 - Digital Amplifier for Strain Gage - Capacitor

Capacitor Choice

PS021 Circuits

The Capacitor

For correct operation it is necessary to select the right capacitor value and the right capacitor material. Following the recommendation for the comparator circuit, the discharge time is about comparator

In measurement range 2 the time interval measurement uses not only the high-speed unit of the TDC but also the reference clock (pre-divider). Doing this the measurement range of the TDC is extended to 100 µs. This allows update rates up to 10 kHz. For higher update rates the discharge time must be reduced. At update rates higher than 10 kHz measurement range 1 is recommended.

The following values are recommended for measurement range 2:

R SG C Load
1 kOhm 68 nF
350 Ohm 220 nF
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PS021 - Capacitor Material

Capacitor material

The capacitor is an important part of the circuit and has direct influence on the quality of the measurement and the stability with temperature.

We recommend the following materials (group 1):

  • CFCAP (Multilayer ceramic from Taiyo-Yuden)
  • C0G or NP0 ceramics
  • Polystyrene
  • Polyvenylsulfid

Also these materials may be used but with some small losses in temperature stability (group 2):

  • X7R
  • Polyester

The following materials must not be used (group 3):

  • Z0G
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PS021 - Comparator

The Comparator

The comparator significantly influences the quality of the measurement. It is not integrated in the PSØ21. It is possible to get results of outstanding quality using a very simple bipolar comparator circuit as shown in the figure. The circuit is very insensitive to low supply voltage. When driving the chip with Vcc and Vio at the lower limit of 1.8 V, the absolute noise is still less than with 5 V - a proof of the power and robustness of this simple and low-cost measuring principle.

This comparator with its 5 transistors in parallel shows the lowest noise. In many applications 1 transistor might be sufficient. It has a quiescent current of about 180 µA at 3 V supply voltage.

The PSØ21 can fully control the comparator on time. The comparator current can be reduced at low resolution and low update rates to a few µa allowing even solar cell driven systems

comparator

strain gage comparator

 
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