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INSTRUMENTATION &
MEASUREMENTS
(EE-302)
WEEK 4
UIT SPRING 20161
Anderson bridge
 Its in fact a modification of the basic Maxwell’s bridge
used to find the self inductance value using the
comparison technique.
 Used for precise measurement over a large range of
values.
UIT SPRING 20162
Anderson bridge
UIT SPRING 20163
Anderson bridge Phasor diagram
UIT SPRING 20164
Anderson bridge under balance:
UIT SPRING 20165
Under the balance condition the Anderson bridge’s
unknown parameters are:
Advantages:
 Accurate measurement of capacitance in terms of
inductance is possible.
 Requires a fixed capacitor instead of a variable capacitor.
 Bridge comparatively easier to balance with respect to
the Maxwell’s bridge.
UIT SPRING 20166
Disadvantages:
 Anderson’s bridge is more complicated than other
bridges.
 Uses more components.
 Balance equations are more complicated to drive.
 Bridge cannot be easily shielded due to additional
junction points, to avoid effect of stray capacitances.
UIT SPRING 20167
Example
UIT SPRING 20168
Example
UIT SPRING 20169
Example
UIT SPRING 201610
Hay’s Bridge
 Maxwell’s bridge is not suitable for high Q values.
 Hay’s bridge is suitable for coils having high Q values.
 In Hay’s bridge, capacitor is connected in series with the
variable resistance, a change from the Maxwell’s bridge.
 For larger phase angles, R1 is needed to be very low
which is duly practical.
 The bridge is shown below:
UIT SPRING 201611
Hay’s bridge
UIT SPRING 201612
Hay’s bridge
UIT SPRING 201613
For the balanced condition of the bridge:
Example
UIT SPRING 201614
Example
UIT SPRING 201615
Advantages and Disadvantages of
Hay’s Bridge
 Best suitable for inductances having Q factor higher than
10.
 Quite simple expression for Q factor in terms of the
bridge elements.
 Disadvantage is that it is suitable only for the
measurement of inductances with high Q factor.
UIT SPRING 201616
Schering bridge
UIT SPRING 201617
 One of the most widely used AC bridge for the
measurement of unknown capacitance, dielectric losses
and power factor.
 The Schering bridge is widely used for testing small
capacitors at low voltages with very high precision.
UIT SPRING 201618
Schering bridge and its balance
equations
Power Factor, loss angle and
dissipation factor
UIT SPRING 201619
The dissipation factor is the reciprocal of Q factor and is
given by:
High Voltage Schering bridge
UIT SPRING 201620
 A stepped up transformer is used to rectify the errors
caused by the Schering bridge low voltage
measurements. This bridge is shown here:
Wien Bridge
UIT SPRING 201621
 Primarily it is used to measure the frequency but it can
also be used to measure an unknown capacitance with
accuracy.
Wien bridge
UIT SPRING 201622
Hence 𝑓 = 1/2𝜋𝑅𝐶
Digital to Analog Conversion
UIT SPRING 201623
 For the DAC the binary input is of the form:
 And its subsequent Vout is given by the formula:
UIT SPRING 201624
The basic DAC symbol
UIT SPRING 201625
The DAC transfer characteristics
UIT SPRING 201626
DAC conversion techniques
UIT SPRING 201627
DAC: binary weighted
UIT SPRING 201628
UIT SPRING 201629
DAC: binary weighted
 Wide range of resistors are required. For an 8 bit DAC,
the largest resistor is 128 times the smallest, hence
greater chances of damaging the smallest resistor due to
heavy current flow through it.
 Integrated Circuit fabrication limitations when it comes
to so many varying resistors.
 Finite resistances of the switches disturb the resistors
values and hence cause errors.
UIT SPRING 201630
Binary Weighed DAC Limitations
Inverted R-2R ladder DAC: an
improved version
UIT SPRING 201631
Why this DAC is better?
UIT SPRING 201632
4 Bit R-2R Binary DAC
UIT SPRING 201633
UIT SPRING 201634
Resolution of the R-2R DAC
UIT SPRING 201635
Example
UIT SPRING 201636
Advantages of R-2R DAC
 Only Two resistors used, hence far more practical as
compared to binary weighed ladder.
 Any number of bits are possible by just adding more R-
2R sections.
UIT SPRING 201637
Performance Parameters of DACs
 Resolution: Could be defined in terms of the total
number of the output values that could be provided by
the DAC i.e 2n where n is the number of bits.
 It could also be defined as the change in the output
voltage of the DAC as a result of change in the LSB at
the input only. This could be defined as:
UIT SPRING 201638
 If we are using an 8 bit DAC the resolution of the DAC in
terms of the possible output states would be 28 = 256.
UIT SPRING 201639
Performance Parameters of DACs
 Accuracy: It could be defined as the difference between
the actual output voltage of the DAC and the expected
output. It is expressed in percentage. It must be ±
1
2
of
its LSB. For the full scale output of 10.2, and for an 8 bit
DAC, it could be given as:
UIT SPRING 201640
Performance Parameters of DACs
 Monotonicty: Good monotonicity means the converter is
not missing any steps while stepping through its entire
range.
 Conversion Time: Also called the setting time. It is the
time required for the conversion from application of the
digital input to the generation of final analog output
voltage.
 Settling Time: Time required by the DAC to get settled to
±
1
2
𝐋𝐒𝐁 of its final value for a given digital input voltage i.e
zero to full scale.
 Stability: The performance of the converter changes with
temperature, age and power supply variations. Hence the
relevant parameters such as offset, gain, linearity, error and
monotonicity must be within a certain limit during the entire
operating range of temperature and supply fluctuations.
This constitute to stability.
UIT SPRING 201641
Performance Parameters of DACs

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Week 4

  • 2. Anderson bridge  Its in fact a modification of the basic Maxwell’s bridge used to find the self inductance value using the comparison technique.  Used for precise measurement over a large range of values. UIT SPRING 20162
  • 4. Anderson bridge Phasor diagram UIT SPRING 20164
  • 5. Anderson bridge under balance: UIT SPRING 20165 Under the balance condition the Anderson bridge’s unknown parameters are:
  • 6. Advantages:  Accurate measurement of capacitance in terms of inductance is possible.  Requires a fixed capacitor instead of a variable capacitor.  Bridge comparatively easier to balance with respect to the Maxwell’s bridge. UIT SPRING 20166
  • 7. Disadvantages:  Anderson’s bridge is more complicated than other bridges.  Uses more components.  Balance equations are more complicated to drive.  Bridge cannot be easily shielded due to additional junction points, to avoid effect of stray capacitances. UIT SPRING 20167
  • 11. Hay’s Bridge  Maxwell’s bridge is not suitable for high Q values.  Hay’s bridge is suitable for coils having high Q values.  In Hay’s bridge, capacitor is connected in series with the variable resistance, a change from the Maxwell’s bridge.  For larger phase angles, R1 is needed to be very low which is duly practical.  The bridge is shown below: UIT SPRING 201611
  • 13. Hay’s bridge UIT SPRING 201613 For the balanced condition of the bridge:
  • 16. Advantages and Disadvantages of Hay’s Bridge  Best suitable for inductances having Q factor higher than 10.  Quite simple expression for Q factor in terms of the bridge elements.  Disadvantage is that it is suitable only for the measurement of inductances with high Q factor. UIT SPRING 201616
  • 17. Schering bridge UIT SPRING 201617  One of the most widely used AC bridge for the measurement of unknown capacitance, dielectric losses and power factor.  The Schering bridge is widely used for testing small capacitors at low voltages with very high precision.
  • 18. UIT SPRING 201618 Schering bridge and its balance equations
  • 19. Power Factor, loss angle and dissipation factor UIT SPRING 201619 The dissipation factor is the reciprocal of Q factor and is given by:
  • 20. High Voltage Schering bridge UIT SPRING 201620  A stepped up transformer is used to rectify the errors caused by the Schering bridge low voltage measurements. This bridge is shown here:
  • 21. Wien Bridge UIT SPRING 201621  Primarily it is used to measure the frequency but it can also be used to measure an unknown capacitance with accuracy.
  • 22. Wien bridge UIT SPRING 201622 Hence 𝑓 = 1/2𝜋𝑅𝐶
  • 23. Digital to Analog Conversion UIT SPRING 201623
  • 24.  For the DAC the binary input is of the form:  And its subsequent Vout is given by the formula: UIT SPRING 201624
  • 25. The basic DAC symbol UIT SPRING 201625
  • 26. The DAC transfer characteristics UIT SPRING 201626
  • 28. DAC: binary weighted UIT SPRING 201628
  • 29. UIT SPRING 201629 DAC: binary weighted
  • 30.  Wide range of resistors are required. For an 8 bit DAC, the largest resistor is 128 times the smallest, hence greater chances of damaging the smallest resistor due to heavy current flow through it.  Integrated Circuit fabrication limitations when it comes to so many varying resistors.  Finite resistances of the switches disturb the resistors values and hence cause errors. UIT SPRING 201630 Binary Weighed DAC Limitations
  • 31. Inverted R-2R ladder DAC: an improved version UIT SPRING 201631
  • 32. Why this DAC is better? UIT SPRING 201632
  • 33. 4 Bit R-2R Binary DAC UIT SPRING 201633
  • 35. Resolution of the R-2R DAC UIT SPRING 201635
  • 37. Advantages of R-2R DAC  Only Two resistors used, hence far more practical as compared to binary weighed ladder.  Any number of bits are possible by just adding more R- 2R sections. UIT SPRING 201637
  • 38. Performance Parameters of DACs  Resolution: Could be defined in terms of the total number of the output values that could be provided by the DAC i.e 2n where n is the number of bits.  It could also be defined as the change in the output voltage of the DAC as a result of change in the LSB at the input only. This could be defined as: UIT SPRING 201638
  • 39.  If we are using an 8 bit DAC the resolution of the DAC in terms of the possible output states would be 28 = 256. UIT SPRING 201639 Performance Parameters of DACs
  • 40.  Accuracy: It could be defined as the difference between the actual output voltage of the DAC and the expected output. It is expressed in percentage. It must be ± 1 2 of its LSB. For the full scale output of 10.2, and for an 8 bit DAC, it could be given as: UIT SPRING 201640 Performance Parameters of DACs
  • 41.  Monotonicty: Good monotonicity means the converter is not missing any steps while stepping through its entire range.  Conversion Time: Also called the setting time. It is the time required for the conversion from application of the digital input to the generation of final analog output voltage.  Settling Time: Time required by the DAC to get settled to ± 1 2 𝐋𝐒𝐁 of its final value for a given digital input voltage i.e zero to full scale.  Stability: The performance of the converter changes with temperature, age and power supply variations. Hence the relevant parameters such as offset, gain, linearity, error and monotonicity must be within a certain limit during the entire operating range of temperature and supply fluctuations. This constitute to stability. UIT SPRING 201641 Performance Parameters of DACs