EM375 MECHANICAL ENGINEERING EXPERIMENTATION THERMOCOUPLE LABORATORY

Similar documents
Sensors and Actuators Sensors Physics

Sensing, Computing, Actuating

ME 105 Mechanical Engineering Laboratory Spring Quarter Experiment #2: Temperature Measurements and Transient Conduction and Convection

I m. R s. Digital. R x. OhmmetersxSeries Shunt Digital. R m

Temperature Measurements

Laboratory 12: Three Thermodynamics Experiments

Lecture 36: Temperatue Measurements

Veerapong Kanchanawongkul*

Exercise 1: Thermocouple Characteristics

1) Thermo couple sensor

Temperature Scales. Temperature, and Temperature Dependent on Physical Properties. Temperature. Temperature Scale

Temperature Measurement

Experiment 5: Thermocouples (tbc 1/14/2007, revised 3/16/2007, 3/22,2007, 2/23/2009, 3/13/2011)

Temperature Measurements Using Type K Thermocouples and the Fluke Helios Plus 2287A Datalogger Artmann, Nikolai; Vonbank, R.; Jensen, Rasmus Lund

Temperature Sensors & Measurement

Temperature Measurements

SEN TRONIC AG 1 A 6 6 / "

Thermocouple Calibrations and Heat Transfer Coefficients

MEASURING INSTRUMENTS

The Underground Experimental Investigation of Thermocouples

I. Introduction and Objectives

Using a Mercury itc with thermocouples

Temperature Measurement and First-Order Dynamic Response *

ME 105 Mechanical Engineering Laboratory Spring Quarter INTRODUCTION TO TRANSIENT CONDUCTION AND CONVECTION

ASEN 2002 Experimental Laboratory 1: Temperature Measurement and an Blow Dryer Test

EA Guidelines on the Calibration of Temperature Indicators and Simulators by Electrical Simulation and Measurement

Exercise 1: Thermistor Characteristics

THERMOCOUPLE CHARACTERISTICS TRAINER

NEEL Phase Change in Chromium At the Néel Temperature

ECNG3032 Control and Instrumentation I

15. Compare the result with the value you have taken above Compare the calculated pressure value with the actual pressure value that you have

4. Thermometry. Temperature and Heat Flow Temperature Scales Thermometers

Measurement of Temperature in the Plastics Industry

Section 7. Temperature Measurement

Thermometry. History. History 1/21/18. The art or science of temperature observation

Lecture 11 Temperature Sensing. ECE 5900/6900 Fundamentals of Sensor Design

SENSORS and TRANSDUCERS

Critical parameters of

Temperature Measurement

APPENDIX ELEVEN Open Fire Temperature Measurements

Tick the box next to those resources for which the Sun is also the source of energy.

Temperature Measurement

Department of Mechanical Engineering ME 96. Free and Forced Convection Experiment. Revised: 25 April Introduction

Good practice guide containing experimental results and recommendations for the selection, preparation and calibration of the temperature sensors

T h e rm i s t o r s

Part 2. Sensor and Transducer Instrument Selection Criteria (3 Hour)

Electrical and Magnetic Properties of High Temperature Superconductors Using Varying forms of Data Acquisition

Comparing 2-D Conduction Experiments with Simulation

Experiment FT1: Measurement of Dielectric Constant

ME 365 EXPERIMENT 5 FIRST ORDER SYSTEM IDENTIFICATION APPLIED TO TEMPERATURE MEASUREMENT SYSTEMS

Community College of Allegheny County Unit 9 Page #1. Thermocouples R1 = 1K

DATA SHEET. Thermocouple module with digital I²C-Interface - THMOD-I²C. Characteristic features. Areas of application. Features.

EXPERIMENT VARIATION OF THERMO-EMF WITH TEMPERATURE. Structure. 7.1 Introduction Objectives

PHYS 352 Assignment #1 Solutions

SEMICONDUCTOR THERMAL MEASUREMENT PROCEDURE

Uncertainty Workshop: Overview of uncertainty factors in HTGHPs

Pre-Lab Quiz / PHYS 224. R-C Circuits. Your Name Lab Section

c. VH: Heating voltage between the collector and emitter.

Process Control Instrumentation Technology Curtis D. Johnson Eighth Edition

Thermocouples calibration and analysis of the influence of the length of the sensor coating

UMEÅ UNIVERSITY Department of Physics Agnieszka Iwasiewicz Leif Hassmyr Ludvig Edman SOLID STATE PHYSICS HALL EFFECT

Now let s look at some devices that don t have a constant resistance.

MECHATRONICS II LABORATORY Experiment #4: First-Order Dynamic Response Thermal Systems

Experiment 3. Electrical Energy. Calculate the electrical power dissipated in a resistor.

Week 14 The Simple Pendulum

Cryogenic Instrumentation I Thermometry OUTLINE Thermometry Pt (pure metal) Temperature Ranges of Thermometer Application Typical Resistive Thermal

Professional Article. Fire and Ice

Technical Notes. Introduction. PCB (printed circuit board) Design. Issue 1 January 2010

Slide 1. Temperatures Light (Optoelectronics) Magnetic Fields Strain Pressure Displacement and Rotation Acceleration Electronic Sensors

PURPOSE: See suggested breadboard configuration on following page!

Module 1 Units 3,4,5

Transducer. A device to which change or converts physical quantity in a more easily measurable quantity. Transducer. (Input) Sensor.

Base metal thermocouples drift rate dependence from thermoelement diameter

Experiment A4 Sensor Calibration Procedure

EMRP ENG05 Metrology for Solid State Lighting D2.4.1 Report on junction temperature vs. voltage characteristics for the selected SSL

CHAPTER 4 THERMAL CONDUCTIVITY AND VISCOSITY MEASUREMENTS

Study of Resistance Components

TEST METHOD FOR STILL- AND FORCED-AIR JUNCTION-TO- AMBIENT THERMAL RESISTANCE MEASUREMENTS OF INTEGRATED CIRCUIT PACKAGES

Resistivity and Temperature Coefficients (at 20 C)

Harnessing the Power of Arduino for the Advanced Lab

Lab 1f Boiling Heat Transfer Paradox

Pin Fin Lab Report Example. Names. ME331 Lab

Control Engineering BDA30703

AE 3051, Lab #16. Investigation of the Ideal Gas State Equation. By: George P. Burdell. Group E3

ME 4/549 Lab Assignment 5: Single Block Experiment Spring 2006 due 1 June 2006

Measurement of Electrical Resistance and Ohm s Law

Module 4 : THERMOELECTRICITY Lecture 21 : Seebeck Effect

Chapter 1. Blackbody Radiation. Theory

Measurement in Engineering

PHYS208 RECITATIONS PROBLEMS: Week 2. Gauss s Law

MCP9700/9700A MCP9701/9701A

Sensors and Actuators Sensors Physics

Making Temperature Measurements

An Electronic Thermal Transducer

Chemistry 212 Lab, Spring Design of the Experiment: Standard and Non-Standard Reduction Potentials For Metal/Metal Ion Half-Cells

Thermal Characterization of Packaged RFIC, Modeled vs. Measured Junction to Ambient Thermal Resistance

MODEL FOR UNCERTAINTY ESTIMATION IN COMPARISON CALIBRATION OF THERMOCOUPLES

ELECTRICITY UNIT REVIEW

Experiment 12: Superconductivity

Review of Ohm's Law: The potential drop across a resistor is given by Ohm's Law: V= IR where I is the current and R is the resistance.

Transcription:

EM375 MECHANICAL ENGINEERING EXPERIMENTATION THERMOCOUPLE LABORATORY PURPOSE The objective of this laboratory is to introduce the student to the manufacture and use of thermocouples. Thermocouples will be modeled as a first order system, and students will explore the transient response characteristics of their thermocouples. Particular attention will be focused on the concept of the time constant. BACKGROUND In 1821 Thomas Seebeck discovered that when two wires of different metals were joined together at each end and the junction at one end was heated, a small, continuous electrical current flowed in the circuit. The current is very small, and rather than measuring current we now connect the wires to a high input impedance meter and measure the resulting voltage. The magnitude of this Seebeck effect increases as the temperature difference between the junctions increases and we can use the measured voltage to determine the temperature difference. The phenomenon, though, is not linear. The most rudimentary thermocouple circuit we can use to measure temperature consists of two dissimilar metals joined at a junction at one end (marked hot in the illustration below) and to a high impedance meter at the other. The main problem with this arrangement is that the meter reading (Seebeck effect) depends upon the temperature difference between the hot junction and the wiring connectors at the meter. Without reference junction temperature compensation this device will measure the difference between the hot temperature and the temperature of the meter. Many thermocouple meters have reference junction temperature compensation which may use internal thermistors to measure the temperature of the wiring block, or alternatively compensating IC. These types of meter or DAQ system make it seem that we only need a single junction to make a working thermocouple. A better wiring arrangement that can give more accurate temperature measurements is shown below. This circuit has two active junctions (HOT and REFERENCE) and two parasitic junctions where the Metal B connects to the wiring block at the meter. The reference junction is maintained at a fixed temperature (e.g., by using an ice bath). The temperature difference between the two junctions can now be used to determine the temperature of the hot junction.

There are many different wiring configurations for thermocouples. However they all rely on the Seebeck effect increasing as the temperature difference between junctions also increases. Discussion of those many other approaches is beyond the scope of this course. THEORY You will be making K-type thermocouples which use the metals chromel and alumel 1 for the two wires in each junction. You will then verify the thermocouples are working. This is not a calibration, rather more a field check. You do this by testing your thermocouples at 0 C (melting Ice Cubes in a water bath) and at 100 C (steam). You will also check the zero-point by inserting your thermocouples into a calibrator, which is maintained very accurately at 0 C. RECORD ALL THREE FIELD-CHECK RECORDINGS. Time constant, ττ After you have verified your thermocouples work, you will test one of them to determine its time constant in air. The time constant depends upon several different parameters that include the thermocouple itself (size and materials), and the environment in which it is being used. The theoretical time constant can be estimated from the equation: ττ = ρρcc vvvv haa 1 Chromel and Alumel are trademarks of the Hoskins Manufacturing Company. Chromel is approximately 90%nickel and 10% chromium. Alumel is approximately 95% nickel, 2% manganese, 2% aluminum and 1% silicon.

Where ρρ is the density of the thermocouple bead (average of the two metal densities), CC vv is the thermal capacitance, VV is the volume of the bead, AA is the surface area of the bead, and h is the convective heat transfer coefficient between the thermocouple and its surroundings. Your experiment is to subject a thermocouple to a step change in temperature and measure the resulting temperature versus time data. The thermocouple is a first order system. One of the mathematical formulations for the transient response of a first order system subject to a step input is: TT(tt) = TT (TT TT 0 )ee (tt tt 0 )/ττ In this equation, TT 0 is the initial temperature of the thermocouple at time t0, TT is the actual temperature after the step input (the measurand in this case) and TT(tt) is the temperature recorded by the thermocouple system as a function of time. You will be required to process your temperature vs. time data to determine the time constant for the thermocouple and also to determine the temperature of a hot aluminum block. This is a nonlinear regression which can be achieved using a similar method to the one you used for the elastomer lab. PROCEDURE Each group will make two K-type thermocouples; a twisted wire thermocouple and a welded thermocouple. Both thermocouples will be tested to verify they are working. The twisted wire thermocouple will then be inserted in a protection tube (shroud) and brought to room temperature. Shrouds are commonly used for thermocouples; they provide mechanical protection and also change the time constant. After the thermocouple has reached thermal equilibrium you will subject it to a step change in temperature by inserting it into a hot aluminum block. From the measured temperature versus time data, you will determine the time constant for your thermocouple, and also the actual temperature of the calibrator. The detailed procedure will be given in class, and is summarized below: 1. The twisted wire thermocouple is made by stripping about half-inch of the insulation from the ends of the thermocouple wire and twisting the bare ends together. 2. The welded thermocouple is made by stripping the insulation from the ends of the thermocouple wire and joining them using a Helicarc welder. 3. Both thermocouples are verified with field checks with the thermocouples attached to a thermocouple voltmeter. How accurate was your thermocouple when it was placed in the calibrator? How accurate was your thermocouple when it was placed in melting ice? How accurate was your thermocouple when it was placed in steam? 4. Allow the thermocouple to come to room temperature. Make sure it is dry. 5. Insert one of the thermocouples into the shroud. Observe the temperature and ensure it is reasonably stable (not changing) and is close to room temperature. 6. Activate the digital recorder and record a few seconds of ambient temperature data.

7. While still recording, quickly lower the measuring junction into the hot aluminum block. Continue to record the temperature as a function of time for about 3 minutes. ANALYSIS and REPORT REQUIREMENTS The data collection, reduction, and report writing will be done in groups. Your report should ONLY include the transient temperature test. DO NOT include manufacturing details, but do report the field check temperatures for all the thermocouples your team manufactured. Your Matlab code should, as a minimum: 1. Plot the entire measured temperature vs. time data set. 2. Select a start point where the transient response is clean and use this to define the start of a reduced data set. Also look at the end of the data set to identify whether any of the trailing recordings need to be eliminated (for example, if you continued to record as you pulled the thermocouple out of the aluminum block). 3. Look at the raw data and estimate an initial estimate for the time constant ττ. Include this value in your report and explain how you obtained it. 4. Conduct a least squares nonlinear regression and determine the initial temperature TT 0, thermocouple time constant ττ and the actual temperature of the aluminum block, TT You will need to write a Matlab function that takes parameters of initial temperature, final temperature and time constant. It should also accept a vector of time values. It will return the temperatures calculated using the parameters and time values. You will then need to program the use of Matlab functions nlinfit and nlparci. You may want to refer back to the code you wrote for the elastomers lab. t0 will be the time of the first point in your reduced data set Use the temperature at this time as your initial guess for TT 0 Use the last temperature in your retained data set as your initial guess for TT What should you use as your initial guess for the time constant? 5. Plot the measured (full data set with all recorded values) temperature data. Overlay the theoretical transient response using your regressed parameters. Only plot the overlay for the time covered by your reduced data set. See the end of this handout for a sample plot. Note that the plot of measured data includes the initial part at ambient temperature. Those values need to be excluded for the analysis, but must be plotted for comparison. The main body of your report should include as a minimum: 1. A statement that gives the calculated time constant and its uncertainty.

2. A statement that gives the final temperature time TT and its uncertainty. 3. The plot from Matlab (4) above 4. A discussion about the possible accuracies and errors in the experiment. 5. A discussion about how you could change the time constant of your thermocouple, and why you might want to change it (i.e., make it smaller or larger). 6. Calculations for the following scenario: The thermocouple/shroud you made is initially at room temperature (20 C) and then is plunged into a source at 180 C. What will the thermocouple read after 1 minute? 35 30 Measured Curve Fit 25 20 Temperature (deg C) 15 10 5 0-5 0 20 40 60 80 100 120 140 160 180 200 Time (s) Sample plot for a thermocouple tested in a source close to 0 C