Electronic Instruments (EI)
Lecturer: Dr. Cheng-Kai Lu
Phone: (02)7749-3554
Office: TD302/BAIR Lab
Email: cklu@ntnu.edu.tw
Chapter Objectives
2
At the end of this chapter, you will be able to:
3
Introduction
4
Measurement
Measurement is the process of observing and recording the observations that are collected as part of a research effort.
5
Measurement
Measurement: use of instruments to determine present state, condition or characteristic of system in quantitative terms (quantity of physical variable)
Instrument: device to determine value/magnitude of quantity/variable that includes
the sensing device, transducer element, data processing and representation
Example: DC current meter
6
Elements of Measuring System
Transducers: a combination of sensor(s) which responds to physical state/condition
to provide output as a function of the measurand(s) and variable conversion elements
Transmitters: combining signal processing, amplification and transmission capabilities
7
Application of Measurement System
Feedback Control Systems
8
Example : Temperature Control
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Units of Measurement
10
Quantity | Unit | Symbol |
Length | Meter | m |
Mass | Kilogram | kg |
Time | Second | s |
Electric Current | Ampere | A |
Thermodynamic Temperature | Kelvin | K |
Luminous Intensity candela cd | ||
Matter mole mol | ||
- Fundamental units/base units: mass, length, time
- Derived units: area, speed, acceleration etc.
Derived Units
11
Quantity | Unit | Symbol |
Area | Square meter | m2 |
Volume | Cubic meter | m3 |
Velocity | Metre per second | m/s |
Acceleration | Metre per second squared | m/s2 |
Force | Newton | N = kg‐m/s2 |
Work/Energy | Joule | J = N‐m |
Power | Watt | W = J/s |
Electric Charge | Coulomb | A‐s |
Voltage | volt | V = W/A |
Resistance | Ohm | Ω = V/A |
Magnetic Flux | Weber | Wb = V‐s |
Derived units: originate from physical law
Supplementary unit
12
Quantity | Unit | Symbol |
Angle | rad | rad |
Solid angle | sr | Sr |
Example: Electromotive Force
13
⎢ ⎥
⎣ ⎦
3
As
⎡kg.m2 ⎤
volt =
20
Emf (volt) is defined as energy required to move and electron charge
emf [volt]= workdone [Joule]
charge [Coulomb]
= Force [N]×distance [m] = mass [kg]×acceleration [m/s2 ]×distance [m] current [A]× time [s] current [A]× time [s]
Standards of Measurement
14
Centimetre–Gram–Second system of units(CGSe) Absolute System
15
Q(statcoulomb) = cm3/ 2g1/ 2s−1
= Q1Q2
r 2
F = k Q1Q2
εr 2
SI Units of Measurements
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Mass and Length
17
Time and Frequency
18
Basic Definitions
19
v [ ms−1 ]= ∂x [m]
∂t [s]
a [ ms−2 ]= ∂v [m/s]
dt[s]
−2 ] = ∂(mv)[kg ms−1 ]
F [N = kg ms
∂t [s]
p [N = kg ms
−2\1 ] =
m [ kg]
× v [ ms−1 ]
Basic Definitions
20
0
x
2 -2 ] -2 ]
⋅ x [m]
= ∫ Fdx = F [kg ms
E [J = kg m s
∂t [s]
p [watt = J s−1 ]= ∂E [J]
Facts
21
= 1.602 ×10−19 C
1
6.24 ×1018
Q =
J
1
6.24 ×1018
1 eV =
g = 9.81 m/s2
Electrical Standards
22
Ampere balance at the US National Bureau of Standards
Coils
Ohm's Law
Electrical Standards
23
New standard based on thin-film junction irradiated with microwave energy to develop the junction voltage:
Basic Definitions
24
2 -1
emf V
-2 ]= workdone [J] = workdone [kg m2 s-1 ]
charge [C] charge [As]
[ = kg m A s
=
∂I [A] ∂I [A]
∂V [V] ∂V [kg m2A-1s-3 ]
R [Ω]=
=
∂x [m] ∂x [m]
∂V [V] ∂V [kg m2A-1s-3 ]
E [V/m]=
I [A]= ∂q [C] = ∂q [A - s]
∂t [s] ∂t [s]
Electrical Standards
25
Basic Definitions
26
ε [Fs-1 ]= [kg-1 m−3 A2s4 ]
-1 -2 2 4
d [m] V [V]
−1 ] A [m2 ] = Q [C]
C [F = kg m A sec ]= ε [Fm
et[kg m2A-1s-2 ]
I [A]
L =
∂t [s]
emf [V]= −L ∂i [A]
H [A m-1 ]
μ [H/m]= B [T]
Basic Definitions
27
[ ] [ ]
l [m]
μ kg m A-2sec-2 .A m2
S [S = kg-1m-2A2sec2 ]=
S [S]
φ [W = kg m2A-1s-2 ]= −L [H] NI [A]
1
T [s]
f [Hz]=
Temperature and Luminous Intensity
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at 0.01 °C.
Heat vs Temperature
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IEEE Standards
30
36
Measurement methods
31
Active and Passive Instruments
32
Passive pressure gauge
Float-type tank level gauge
Null-Type and Deflection-Type
33
Passive pressure gauge
Dead-weight pressure gauge
Analog and Digital
34
Display methods
Instrument Characteristics
35
Properties of Instruments
Static Characteristics
36
Accuracy of Measurement
37
Accuracy of Measurement
38
Sensitivit y = Δ instrument output
Δ measured variable
Example: Pressure Measurement
39
Pressure Gauge:
measurement range 0 -10 bar
fs ±1.0%
Full‐scale reading precision:
emax = ±1.0% ×10 bar = ±0.1bar
Maximum error:
1 bar
= (1± 0.1 bar ) −1 bar ×100 = ±10%
1bar
e
Measurement error for reading 1 bar (in %):
% error = measured value − true value ×100%
true value
Example: Tolerance
40
Resistors:
pack of resistors with R = 1000 Ω
± 5%
tolerance:
Minimum value:
Maximum value:
Rmin = 1000 Ω − 5% = 950 Ω
Rmax = 1000 Ω + 5% = 1050 Ω
Linearity and Measurement Sensitivity
41
Linearity
Sensitivity:
Sensitivity = Scale deflection = Slope
Value
Linearity and Deviations
42
Sensitivity to Disturbance
43
Zero Drift
Sensitivity Drift
zero drift and sensitivity drift
Example 1: Measurement Sensitivity
44
Platinum resistance thermometers:
resistivity measured at varying temperatures
Measurement sensitivity:
30o C
= 0.233 Ω /o C
7Ω
Rsens =
R | T |
307 | 200 |
314 | 230 |
321 | 260 |
328 | 290 |
305
310
315
330
325
320
0
50
100
150
200
250
300
350
Resistance
Example 2: Measurement Sensitivity
45
Measurement sensitivity:
1 kg
20 mm
sens
= 20 mm / kg
D (20 C) =
0
Load (kg) | 0 | 1 | 2 | 3 |
Deflect (mm) | 0 | 20 | 40 | 60 |
Spring Balance:
calibrated at 20°C
used at 30°C
Load (kg) | 0 | 1 | 2 | 3 |
Deflect (mm) | 5 | 27 | 49 | 71 |
20
10
0
70
60
50
40
30
80
0
1
2
3
Sensitivity
Deflection (mm)
Deflection (mm)
1 kg
sens
D (300 C) = 22 mm = 22 mm / kg
Zero drift = 5 mm Sensitivity drift = 2 mm/kg
Zero drift coefficient = 5 mm/10 °C = 0.5 mm /°C Sensitivity drift coefficient = 2 (mm/kg)/10 °C
= 0.2 (mm/kg) /°C
Statistical Analysis of Measurement
46
Statistical Analysis of Measurement
47
where x = measured value,
n = number of reading / measurement
0 Average reading the most likely value for measured variable
0 Average amount of measurement error
x
n
n
i
∑
=
x =
i=1
n
x1 + x2 +·+ xn
d1 = x1 − x d2 = x2 − x · dn = xn − x
Statistical Analysis of Measurement
48
0 random errors that lie scattered within 50% probability region around mean; A range within one probable error on either side of the mean will include 50% of the data values
r = ±0.6745σ
(✓)
Normal Error Distribution
49
Probable error:
r = ±0.6745σ
Deviation σ | | Fraction Area |
0.6745 | | 0.5000 |
1.0 | | 0.6828 |
2.0 | | 0.9546 |
3.0 | | 0.9972 |
D2
D1
1
P(D1 ≤ D ≤ D2 ) =
1
F(x) =
e[−D2 / 2σ 2 ]dD
e[−( x−m)2 / 2σ 2 ]
2π
∫ σ
σ 2π
Example 3: Statistical Analysis
50
Reading | | Deviation | |
R (Ω) | | d | d2 |
100.2 | | 0.2 | 0.04 |
100.3 | | 0.3 | 0.09 |
99.8 | | ‐0.2 | 0.04 |
100.5 | | 0.5 | 0.25 |
99.3 | | 0.7 | 0.49 |
100.4 | | 0.4 | 0.16 |
100.1 | | 0.1 | 0.01 |
99.5 | | ‐0.5 | 0.25 |
99.7 | | 0.3 | 0.09 |
99.7 | | 0.3 | 0.09 |
=
∑
= 100.0 Ω
999.5
10 10
10
ave
i=1
i
R
R =
Determine:
Range = Rmax − Rmin = 100.5 − 99.3 = 1.2 Ω
c) Deviation, d
- as shown in table -
Precision: ONE decimal
Example 3: Statistical Analysis
51
Reading | | Deviation | |
R (Ω) | | d | d2 |
100.2 | | 0.2 | 0.04 |
100.3 | | 0.3 | 0.09 |
99.8 | | ‐0.2 | 0.04 |
100.5 | | 0.5 | 0.25 |
99.3 | | 0.7 | 0.49 |
100.4 | | 0.4 | 0.16 |
100.1 | | 0.1 | 0.01 |
99.5 | | ‐0.5 | 0.25 |
99.7 | | 0.3 | 0.09 |
99.7 | | 0.3 | 0.09 |
= 0.4 Ω
1.51
2
n −1 10 −1
d
n
i=1 =
∑ i
σ =
Determine:
d) standard deviation
e) probable error
Probable error, r = ±0.6745σ = ±0.2763 Ω
Example 4: Statistical Analysis
52
Number of measuremen t, n = 11
Average (mean) reading = 409
∑deviation2 = 1370
10
1370
137 = 11.7
= 137
=
n −1
Probable error, r = ±0.6745σ = ±7.89
Standard deviation, σ =
∑deviation 2
Variance, σ 2 =
Hysteresis
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Hysteresis:
Dead Space
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Types of Errors
55
0 Instrumental: inherent to measuring eqpt.
x Static: limitation of device
x Dynamic: inability to respond to change in measured variable
0 Environmental: due to change in external conditions (temperature, pressure, humidity, magnetic/electric fields)
Gross Errors
56
Other Examples
Reduction Methods
Caused by human error due to incorrect use of equipment, wrong observation, carelessness etc.
calculations
Estimation
Systematic Errors
57
Can come from 2 sources:
1. Instrumental: inherent to measuring equipment
x Static: limitation of device
x Dynamic: inability to respond to change in measured variable
2. Environmental: due to change in external conditions (temperature, pressure, humidity, magnetic/electric fields)
Systematic Errors
58
1. Instrumental: inherent to measuring equipment
Examples
Estimation
Reduction Methods
Systematic Errors
59
2. Environmental: due to change in external conditions
Estimation
Reduction Methods
Random Errors
60
Sources of Errors
61
inaccurate/incorrect methods.
Error Reduction
62
Maximum and Likely Errors
63
THREE separate sources of error are identified:
Maximum possible error =
± (1.2 + 0.8 + 0.5)% = ±2.5%
Likely error =
± 1.22 + 0.82 + 0.52 %
= ±1.53%
Aggregated Errors (1)
64
±ay and ±bz respectively, - where a and b are errors fractions - the sum
/ difference S is
S = ( y ± z) ± e
where likely error, e = (ay)2 + (bz)2
Error in a sum / difference
Note: Here e is the absolute error.
Example 5: Errors in a Sum
65
The total resistance of 2 resistors (to 3 significant figures) each with a tolerance of:
Solution:
THREE significant figures
R1 = 99.3 ±1.0%
R2 = 46.123 ± 6.5%
= 145.423 ± 3.158 Ω
= 145 Ω ± 2.2%
= (R1 + R2 ) ± e
e = ± (0.01× 99.3)2 + (0.065× 46.123)2
= ± 0.986 + 8.988 = ±3.158
∴ RT
Note: a = 0.01, b = 0.065
error fractions
Example 6 : Errors in a Difference
e = ± (0.01×100)2 + (0.05× 80)2
= ± 1+16 = ±4.123
∴VT = (V1 −V2 ) ± e
= 20 ± 4.123 V
= 20 V ± 20.6%
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Solution:
The maximum likely error,
Note: The percentage error increases for difference between measurements.
The difference between 2 voltage measurements, VD:
V1 = 100 V ± 1%
V2 = 80 V ± 5%
Aggregated Errors (2)
67
±ay and ±bz respectively, the product P is
and the quotient Q is
Q = y ± e
z
Error in a product / quotient
P = yz ± e
where e = a2 × b2
Note: Here e is the fraction/percentage error.
Example 7: Errors in a Product
68
If the density of a substance is calculated from measurements of its mass and volume, where the respective errors are 2% and 3%, find the maximum likely error in the density value.
Solution:
V
Since density is mass per unit volume ρ = m , then the likely error is
e = 0.022 × 0.032
= ± 0.0013 = ±0.036
Propagation of Uncertainties
69
n
i
i n
∂x
∂x ∂x
∂x
dy = ∂y dx + ∂y dx +· + ∂y dx +· ∂y dx
1 2
1 2
y = f (x1 , x2 ,., xi , ,., xn )
Consider: General equations and difference
2
2
2
2
2
1
1 2
⎥⎦
⎤1/ 2
⎟
⎞2
⎛ ∂
⎞2
⎛ ∂
⎞2
⎛ ∂
⎟
⎞2
⎡⎛ ∂
xn
xi
x 2
x1
y
xn
xi
i n
x 2
x1
y max
xn
xi
i n
x 2
y x1
(U ) ⎥
⎝ ∂xn ⎠
y
⎝ ∂xi ⎠
y
⎝ ∂x2 ⎠
y
(U ) + ⎜ ⎟
⎢⎣⎝ ∂x1 ⎠
y
U = ⎢⎜
∂x
∂x
∂x
) + ∂y (U
∂x
= ∂y (U
U
∂x
∂x
∂x ∂x
U = ∂y (U ) + ∂y (U
(U ) +· + ⎜
(U ) +· + ⎜ ⎟
) +· + ∂y (U ) +·+ ∂y (U )
) +· + ∂y (U ) +· + ∂y (U )
Uncertainties: Due to difference in each components
Dynamic Characteristics
70
dy
d n y an dt n
d n−1 y
d m x + dx +
dt m · + b1 dt b0 x
+· + a1 dt + a0 y = bm
where
x = input
y = output
a, b = coefficient
Dynamic Inputs
71
Periodic input
Transient input
Random signal
Periodic Signals
72
Periodic input
∞
f (t) = a0 / 2 + ∑ an cos nωt + bn sin nωt
n=1
∫
T
n
T
0
a = 2
f (t) cos nωtdt
∫
T
n
T
0
a = 2
f (t) cos nωtdt
Dynamic Characteristics
73
Zero order
where K is the instrument sensitivity.
a
0
b
a0 y = b0 x or y = 0 x = Kx
Frequency Response
74
Response to sinusoidal input
Frequency Response
75
Magnitude (log dB)
Frequency (log)
Response to sinusoidal input
76
END