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1 the input settling time constant – Campbell Scientific CR510 Basic Datalogger User Manual

Page 148

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SECTION 13. CR510 MEASUREMENTS

13-4

FIGURE 13.3-1. Input Voltage Rise and Transient Decay

13.3.1 THE INPUT SETTLING TIME CONSTANT

The rate at which an input voltage rises to its full
value or that a transient decays to the correct
input level are both determined by the input
settling time constant. In both cases the
waveform is an exponential. Figure 13.3-1
shows both a rising and decaying waveform
settling to the signal level, Vso. The rising input
voltage is described by Equation 13.3-1 and the
decaying input voltage by Equation 13.3-2.

V

s

= V

so

(1-e-t/R

o

C

T

), rise

[13.3-1]

V

s

= V

so

+ (V

eo

-V

so

) e-t/R

o

C

T

, decay

[13.3-2]

where V

s

is the input voltage, V

so

the true signal

voltage, V

eo

the peak transient voltage, t is time

in seconds, R

o

the source resistance in ohms,

and C

T

is the total capacitance between the

signal lead and ground (or some other fixed
reference value) in farads.

The settling time constant,

τ

in seconds, and the

capacitance relationships are given in
Equations 13.3-3 through 13.3-5,

τ

= R

o

C

T

[13.3-3]

C

T

= C

f

+ C

w

L

[13.3-4]

C

f

= 3.3 nfd

[13.3-5]

where C

f

is the fixed CR510 input capacitance

in farads, C

w

is the wire capacitance in

farads/foot, and L is the wire length in feet.

Equations 13.3-1 and 13.3-2 can be used to
estimate the input settling error, V

e

, directly.

For the rising case, V

s

= V

so

-V

e

, whereas for

the decaying transient, V

s

= V

so

+V

e

.

Substituting these relationships for V

s

in

Equations 13.3-1 and 13.3-2, respectively,
yields expressions in V

e

, the input settling error:

V

e

= V

so

e-t/R

o

C

T

, rise

[13.3-6]

V

e

= V

e'o

e-t/R

o

C

T

, decay

[13.3-7]

Where V

e'o

= V

eo

-V

so

, the difference between

the peak transient voltage and the true signal
voltage.

NOTE: Since the peak transient, V

eo

,

causes significant error only if it is several
times larger than the signal, V

so

, error

calculations made in this section
approximate V

e'o

by V

eo

; i.e., V

eo

= V

eo

-V

so

.

If the input settling time constant,

τ

, is known, a

quick estimation of the settling error as a
percentage of the maximum error (V

so

for

rising, V

e'o

for decaying) is obtained by knowing

how many time constants (t/

τ

) are contained in

the 450 µs CR510 input settling interval (t). The
familiar exponential decay relationship is given
in Table 13.3-1 for reference.

TABLE 13.3-1. Exponential Decay, Percent

of Maximum Error vs. Time in Units of

τ

Time

%

Time

%

Constants

Max. Error Constants

Max. Error

0

100.0

5

0.7

1

36.8

7

0.1

3

5.0

10

0.004

Before proceeding with examples of the effect
of long lead lengths on the measurement, a
discussion on obtaining the source resistance,
R

o

, and lead capacitance, C

w

L, is necessary.