arrow_back_ios

Main Menu

See All Software See All Instruments See All Transducers See All Vibration Testing Equipment See All Electroacoustics See All Acoustic End-of-Line Test Systems See All Academy See All Resource Center See All Applications See All Industries See All Services See All Support See All Our Business See All Our History See All Global Presence
arrow_back_ios

Main Menu

See All nCode - Durability and Fatigue Analysis See All ReliaSoft - Reliability Analysis and Management See All Test Data Management See All DAQ Software See All Drivers & API See All Utility See All Vibration Control See All High Precision and Calibration Systems See All DAQ Systems See All S&V Hand-held Devices See All Industrial Electronics See All Power Analyzer See All S&V Signal Conditioner See All Acoustic See All Current and Voltage Sensors See All Displacement See All Force sensors See All Load Cells See All Pressure See All Strain Gauges See All Temperature Sensors See All Torque Sensors See All Vibration See All Accessories for Vibration Testing Equipment See All Vibration Controllers See All Measurement Exciters See All Modal Exciters See All Power Amplifiers See All LDS Shaker Systems See All Test Solutions See All Actuators See All Combustion Engines See All Durability See All eDrive See All Production Testing Sensors See All Transmission & Gearboxes See All Turbo Charger See All Training Courses See All Acoustics See All Asset & Process Monitoring See All Custom Sensors See All Data Acquisition & Analysis See All Durability & Fatigue See All Electric Power Testing See All NVH See All Reliability See All Smart Sensors See All Vibration See All Weighing See All Automotive & Ground Transportation See All Calibration See All Installation, Maintenance & Repair See All Support Brüel & Kjær See All Release Notes See All Compliance See All BKSV Worldwide Contacts
arrow_back_ios

Main Menu

See All API See All Microphone Cartridges See All Microphone Sets See All Microphone Pre-amplifiers See All Sound Sources See All Acoustic Calibrators See All Special Microphones See All Accessories for acoustic transducers See All Experimental testing See All Transducer Manufacturing (OEM) See All Piezoelectric Charge Accelerometers See All Piezoelectric CCLD (IEPE) accelerometers See All Electroacoustics See All Noise Source Identification See All Environmental Noise See All Sound Power and Sound Pressure See All Noise Certification See All Industrial Process Control See All Structural Health Monitoring See All Electrical Devices Testing See All Electrical Systems Testing See All Grid Testing See All High-Voltage Testing See All Vibration Testing with Electrodynamic Shakers See All Structural Dynamics See All Machine Analysis and Diagnostics See All Dynamic Weighing See All Vehicle Electrification See All Calibration Services for Transducers See All Calibration Services for Handheld Instruments See All Calibration Services for Instruments & DAQ See All On-Site Calibration See All Resources See All Software License Management

Accurate Measurement Results at High and Low Temperatures

null

To ensure accurate measurement results even under changing ambient conditions, temperature compensation of quarter bridge strain gauge applications need to be established. Several different temperature factors influence the physical strain on its way to digitalization, such as:

  • The mutual influence of thermal material expansion differences on substrate/base material and strain gauge grid material
  • The ohmic resistance of the lead wires
  • The temperature dependency of the gauge factor by self-heating of the strain gauge
  • The temperature dependency of the Youngs modulus

These temperature influences can be corrected by using software packages designed for strain gauge applications such as catman Easy/AP from HBK. We will give you a clear and understandable link between theory and practice of temperature compensation for quarter bridge strain gauge applications.

Strain gauges from HBK are shipped with a data sheet, containing all relevant parameters to ensure the accuracy of the measurement. The HBK strain gauge data sheet has the following layout and displays the parameters for compensation in a chart and formula. Annotation: In this example, two curves are displayed in the data sheet. One curve represents the thermal response of the strain gauge itself while the other curve represents the thermal behavior of the gauge including 2-wire leads. 

The temperature response of a strain gauge depends on:

  • The temperature expansion coefficients of the substrate/material
  • The temperature expansion coefficient (CTE) of the strain gauge grid
  • The temperature coefficient of the ohmic resistance of the strain gauge grid
  • The temperature coefficient of the gauge factor k

In practice, the thermal output strain is simply measured and extracted in a temperature chamber under accurate conditions. The result of this measurement reflects:

  • The compensation of temperature expansion of the substrate/material by the strain gauge properties
  • A residual error that cannot be compensated but corrected for highly accurate measurement demands

The residual error can be determined from the measurement and represented by a polynomial εs, which ideally would always give zero as the result, regardless of temperature. But in practice there is a range around the reference temperature, where it is optimised close to zero during production of the strain gauge.

null

Application Example

We will perform an example calculation to demonstrate how thermal compensation in quarter bridges can be established considering the most important influences. We take the following setup:

  • Transducer: Strain gauge of type 1-LY11-10/120 installed on a material in a test chamber with the test condition of 100 deg. C. To connect the transducer with the amplifier, 10mm leads, a solder terminal and a 4-wire cable are used.
  • Amplifier: Strain is measured in a quarter bridge configuration by the DAQ module QuantumX MX1615B with DC or carrier frequency excitation value depending on the ambient electromagnetic environment.
  • Software: catman Easy/AP DAQ software, installed on a PC or running in the data recorder, is used to correct the temperature influences by online math.

1. Correction of Strain Value With Polynomial

null

The thermal polynomial is plotted on each data sheet. The general layout is as follows - please be aware, that the polynomial can vary:

Thermal Polynomial

In catman Easy/AP the thermal compensation for the strain gauge can easily be added by clicking on “Adaption” in the ribbon bar of the DAQ channels. All parameters can be found in the data sheet.

In some cases, the polynomial includes further contributors that influence the strain signal if the temperature changes:

  • Influence of leads (εl): In this specific example the measurement uncertainty and the influence of 2-wire strain gauge leads connected to the measurement grid is added as well. Generally, the influence of leads must be considered as well, but it might differ between gauge types and manufacturers. If you are using our HBM-patented 3- or 4-wire technology this compensates all cable resistances, but in some cases, there is a residual 2-wire part which cannot be compensated automatically.
  • Measurement Uncertainty (εu): The measurement uncertainty is a general part which should be considered in the total calculation. Even the polynomial has some scatter which leads to this uncertainty part.

The adapted polynomial is as follows:

Thermal polyinomial including inclunce of leads and measurement uncertainty

Focusing on our application example it looks like:

Thermal polyinomial including inclunce of leads and measurement uncertainty

Let’s assume that the temperature during the strain measurement is constantly 100 °C (T = 100 °C) and the length of leads is 10 mm (L = 10 mm). Please be aware that the length of leads can vary. Looking at the polynomial, it demonstrates that the thermal strain has a significant impact on the result, since it is higher than 100 μm/m!

Thermal polynomial

To calculate the thermal output strain, deploy the temperature and the length of leads into the polynomial:

Calculation thermal output strain

The result fits quite well to the polynomial displayed on the data sheet. By considering the polynomial the most significant influences are taken into account, whereas only very long 2-wire cables can impact the result additionally. Since we use the 3- and 4-wire technology that compensates the impact of cable resistance, this part of the calculation is not relevant!

Superimposing the thermal strain on the measured strain now gives the corrected strain value, which only takes the mechanical strain into account:

Corrected Strain Value without thermal strain


2. Gauge Factor Adjustment

The polynomials of most manufacturers are measured with a fixed gauge factor (or k-factor) of k = 2, whereas the real measured k-factor typically differs. This effect is mainly visible in extreme conditions, such as high and low temperatures or high strains. To compensate the variations which can influence the temperature compensation, the gauge factor printed on the data sheet should be considered.

Therefore, multiplicate the quotient of the gauge factors printed on the data sheet to correct the thermal output that can be expected with the strain gauge. In this case we have the following gauge factors:

Thermal polynomial with gauge factor adjustment

Of course, the thermal strain correction is only applied to the polynomial and must not be applied to additionally contributing factors as measurement uncertainty or the influence of leads:

Thermal strain correction by gauge factor adjustment

In this case, we have two gauge factors (kpolynomial = 2.0 and kdata_sheet = 2.12). The thermal strain correction would be:

Thermal strain correction by gauge factor adjustment

The corrected strain signal would change to:

Corrected Strain Signal by Gauge Factor Adjustment

To establish this correction in catman DAQ software a new calculation channel needs to be created which consider all factors. A computation channel can be added by clicking on "New Computation Channels" and "Create a new Channel". The strain signal can be corrected by inserting the thermal strain correction polynomial into the "Edit Expression" of the new computation channel. 

null

3. Deviating Temperature Coefficient of Substrate Material

In this theoretical test case, the temperature coefficient of the strain gauge matches the material perfectly. Nevertheless, in practice, there might be slight deviations between temperature coefficient of the substrate material and the temperature coefficient to which the strain gauge has been adapted. An approximate adjustment to correct the measured strain value is given by the following formula. In this case, we assume that a strain gauge adapted to ferritic steel (10.8 ppm/K) was used on an aluminium (23 ppm/K):
Deviating Temperature Coefficient of Substrate Material

The temperature difference must be calculated from the reference temperature and the temperature during test. The reference temperature is the temperature the strain gauge data sheet refers to and for which the parameters have been measured:

Deviating Temperature Coefficient of Substrate Material

This will lead to the following correction factor:

Deviating Temperature Coefficient of Substrate Material

null

If this is considered for the corrected strain value, the overall equation is obtained:

Deviating Temperature Coefficient of Substrate Material

To establish this correction in catman DAQ software a new calculation channel needs to be created or an already existing calculation channel needs to be adapted. In this application example, the already existing computation channel needs to be adjusted by the updated thermal strain correction polynomial. 


4. Gauge Factor Variation By Temperature (Optional)

In chapter 2, the strain correction was performed via the polynomial and the gauge factor fitting. This is sufficient for most experimental tests. Nevertheless, the gauge factor (k-factor) additionally varies approximately linearly with temperature over a wide range. Therefore, a correction of the gauge factor can be considered in the uncorrected strain signal (not to be considered in the polynomial, since the temperature dependence of the gauge factor is already included in the polynomial). The temperature coefficient can be positive or negative, depending on the grid material (Constantan or CrNi (Modco).

To easily calculate the temperature adjusted gauge factor, the HBK data sheet displays the temperature coefficient as well as the needed gauge factor (kdata_sheet = 2.12).  Please check first, if the linear behaviour is valid even at extreme temperatures. In this case the temperature coefficient of the gauge factor is:

Gauge Factor Variation By Temperature

The correction formula of the gauge factor is as follows (T = 100 °C):
Gauge Factor Variation By Temperature

It is obvious that this effect is very small and might not be considered in the measurement since the effect is neglectable.

The temperature dependency of the gauge factor can be easily considered as part of the complete formula in catman DAQ software by adjusting the already existing computation channel.

null

5. The Ultimate Thermal Correction Formula

Considering all effects described in this Tech Note, the formula for correcting the strain value is as follows:

null

Glossary

ε Strain signal without any temperature correction
εs Thermal output polynomial from strain gauge data sheet 
εc Strain value including thermal correction
εf Mismatch correction of temperature coefficient
αR Temperature coefficient of the gauge resistance [1/K]
αS Temperature coefficient of the substrate/structure [1/K]
αM Temperature coefficient of the strain gauge metal grid [1/K]
k Gauge factor of the strain gauge
kdata_sheet Gauge factor printed on the data sheet
kdata_sheet(T) Gauge factor printed on the data sheet including temperature correction
kpolynomial Gauge factor which was used to determine the polynomial (typically 2.00)
αk Temperature coefficient of the gauge factor
a0 a0 coefficient of polynomial
a1 a1 coefficient of polynomial
a2 a2 coefficient of polynomial
a3 a3 coefficient of polynomial
∆T Temperature difference of temperature during strain measurement and reference temperature printed on strain gauge data sheet
Tref  Reference temperature printed on the strain gauge data sheet
αsubstrate     Temperature coefficient of material on which the strain gauge is applied
αstrain_gauge  Temperature coefficient of the strain gauge

Legal Disclaimer: TECH NOTEs from HBK are designed to provide a quick overview to a specific topic beside the usual documentation. TECH NOTEs are continuously improved and so change frequently. HBM assumes no liability for the completeness of the descriptions. We reserve the right to make changes to the features and/or the descriptions at any time without prior notice.


Support Content