Section 8. Operation
305
frequency is not varying over the execution interval. The calculation returns the
average regardless of how the signal is changing.
8.1.5.4 Pulse Measurement Problems
8.1.5.4.1 Pay Attention to Specifications
The table
Example of Differing Specifications for Pulse Input Channels
(p. 305)
compares specifications for pulse-input channels to emphasize the need for
matching the proper device to application. Take time to understand signals to be
measured and compatible channels.
Table 67.
Example of Differing Specifications for Pulse-Input
Channels
Pulse Channels
P1, P2
Digital I/O Channels
C1, C2, C3, C4,
C5, C6, C7, C8
High Frequency Max
250 kHz
400 kHz
Max Input Voltage
20 Vdc
16 Vdc
State Transition
Thresholds
Count upon transition from
<0.9 to >2.2 Vdc
Count upon transition from
<1.2 to >3.8 Vdc
8.1.5.4.2 Input Filters and Signal Attenuation
Pulse-input channels are equipped with input filters to reduce spurious noise that
can cause false counts. The higher the time constant (
τ
) of the filter, the tighter
the filter. Table
Time Constants
(p. 305)
lists
τ
values for pulse-input channels. So,
while
TimerIO()
frequency measurement may be superior for clean signals, a
pulse channel filter (much higher
τ
) may be required to get a measurement on a
dirty signal.
Input filters, however, attenuate the amplitude (voltage) of the signal. The
amount of attenuation is a function of the frequency passing through the filter.
Higher-frequency signals are attenuated more. If a signal is attenuated enough, it
may not pass the state transition thresholds required by the detection device (listed
in table
Pulse-Input Channels and Measurements
(p. 39)
). To avoid over
attenuation, sensor output voltage must be increased at higher frequencies. As an
example, table
Filter Attenuation of Frequency Signals
(p. 306)
lists low-level ac
frequencies and the voltages required to overcome filter attenuation.
For pulse-input channels
P1
–
P2
, an RC input filter with an approximate 1-
μ
s
time constant precedes the inverting CMOS input buffer. The resulting amplitude
reduction is illustrated in figure
Amplitude Reduction of Pulse-Count Waveform
(p.
306).
For a 0- to 5-Vdc square wave applied to a pulse channel, the maximum
frequency that can be counted in high-frequency mode is approximately 250 kHz.
Table 68.
Time Constants (
τ
)
Measurement
τ
Pulse channel, high-frequency mode
1.2
Pulse channel, switch-closure mode
3300
Summary of Contents for CR850
Page 2: ......
Page 4: ......
Page 6: ......
Page 26: ...Table of Contents 26...
Page 30: ...Section 2 Cautionary Statements 30...
Page 32: ...Section 3 Initial Inspection 32...
Page 35: ...Section 4 Quickstart Tutorial 35 Figure 2 Wiring panel...
Page 55: ...Section 4 Quickstart Tutorial 55 Figure 24 PC200W View data utility...
Page 78: ...Section 5 System Overview 78...
Page 80: ...Section 6 CR800 Specifications 80...
Page 267: ...Section 7 Installation 267 Figure 84 Running average signal attenuation...
Page 268: ...Section 7 Installation 268...
Page 384: ...Section 8 Operation 384 Figure 113 Using the keyboard display...
Page 387: ...Section 8 Operation 387 Figure 116 Real time custom...
Page 388: ...Section 8 Operation 388 8 8 1 3 Final Storage Tables Figure 117 Final storage tables...
Page 389: ...Section 8 Operation 389 8 8 2 Run Stop Program Figure 118 Run Stop Program...
Page 390: ...Section 8 Operation 390 8 8 3 File Display Figure 119 File display...
Page 396: ...Section 8 Operation 396...
Page 402: ...Section 9 Maintenance 402...
Page 450: ...Section 11 Glossary 450...
Page 504: ...Appendix A CRBasic Programming Instructions 504...
Page 526: ...Appendix B Status Table and Settings 526...
Page 530: ...Appendix C Serial Port Pinouts 530...
Page 536: ...Appendix E FP2 Data Format 536...
Page 550: ...Appendix F Other Campbell Scientific Products 550...
Page 565: ......