Experiment A4 Sensor Calibration Procedure

Similar documents
Experiment B6 Thermal Properties of Materials Procedure

Experiment A12 Monte Carlo Night! Procedure

Experiment A11 Chaotic Double Pendulum Procedure

The RC Circuit INTRODUCTION. Part 1: Capacitor Discharging Through a Resistor. Part 2: The Series RC Circuit and the Oscilloscope

Laboratory 1: Calibration of a High-Volume Sampler

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

Electric Fields and Potentials

Electric Fields. Goals. Introduction

Empirical Gas Laws (Parts 1 and 2) Pressure-volume and pressure-temperature relationships in gases

Experiment 4. RC Circuits. Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor.

The Digital Multimeter (DMM)

PHY222 Lab 2 - Electric Fields Mapping the Potential Curves and Field Lines of an Electric Dipole

PHYS320 ilab (O) Experiment 2 Instructions Conservation of Energy: The Electrical Equivalent of Heat

Capacitance Measurement

Control Engineering BDA30703

Precalculations Individual Portion Correlation and Regression: Statistical Analysis of Trends

EE 241 Experiment #5: TERMINAL CHARACTERISTICS OF LINEAR & NONLINEAR RESISTORS 1

ENSC387: Introduction to Electromechanical Sensors and Actuators LAB 3: USING STRAIN GAUGES TO FIND POISSON S RATIO AND YOUNG S MODULUS

( ) ( ) = q o. T 12 = τ ln 2. RC Circuits. 1 e t τ. q t

Background Information for Use of Pitot Tube, Manometer, Hot Wires, and Hot Films

Lab E3: The Wheatstone Bridge

Exercise 1: Thermocouple Characteristics

PHY222 - Lab 7 RC Circuits: Charge Changing in Time Observing the way capacitors in RC circuits charge and discharge.

Electric Field Mapping

Equipotential and Electric Field Mapping

Resistivity vs. Temperature of a Superconductor WARNING

Mapping the Electric Field and Equipotential Lines. Multimeter Pushpins Connecting wires

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

Activity 1: Investigating Temperature

Lab 3: Electric Field Mapping Lab

Sudden Expansion Exercise

MECHANICAL ENGINEERING TECHNOLOGY ESSENTIALS FOR LABORATORY REPORTS

Lab: Phase Change. Introduction. Predict. Computer setup- Equipment setup- Name: Period: Date:

Apply the ideal gas law (PV = nrt) to experimentally determine the number of moles of carbon dioxide gas generated

Welcome. Functionality and application of RTD Temperature Probes and Thermocouples. Dipl.-Ing. Manfred Schleicher

Lab 12 Pressure-Temperature Relationship in Gases

Physics 1BL Electric Potentials & Fields Summer Session II 2010

Energy Conservation in Circuits Final Charge on a Capacitor. Recorder Manager Skeptic Energizer

3.14 mv ma. Objectives. Overview

Physics Lab 202P-4. Understanding Electric Potential NAME: LAB PARTNERS:

Current Balance. Introduction

Thermocouple Calibrations and Heat Transfer Coefficients

Electric Fields. Goals. Introduction

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

Laboratory #1: Inductive and Capacitive Transients Electrical and Computer Engineering EE University of Saskatchewan

Applied Fluid Mechanics

Figure 1: Capacitor circuit

Voltage Dividers, Nodal, and Mesh Analysis

Applied Fluid Mechanics

Simple circuits - 3 hr

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

ME-B41 Lab 1: Hydrostatics. Experimental Procedures

ECNG3032 Control and Instrumentation I

Science 14. Lab 1 - Potential Plotting

Equipotential and Electric Field Mapping

Name: Lab Partner: Section:

PART I: MEASURING MASS

UNIVERSITY OF MINNESOTA DULUTH DEPARTMENT OF CHEMICAL ENGINEERING ChE CONTINUOUS BINARY DISTILLATION

LAB 3: Capacitors & RC Circuits

Lab 4: The Classical Hall Effect

7/06 Electric Fields and Energy

Physics 43, Fall 1995 Lab 1 - Boltzmann's Law

Evaluation copy. The Molar Mass of a Volatile Liquid. computer OBJECTIVES MATERIALS

MCE380: Measurements and Instrumentation Lab

Lab 5a: Magnetic Levitation (Week 1)

SECTION 1 - WHAT IS A BTU METER? BTU's = Flow x ΔT Any ISTEC BTU Meter System consists of the following main components:

Physics 208 Fall 2008 Lab 4: Electric Fields and Electric Potentials

General Physics II Lab EM2 Capacitance and Electrostatic Energy

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

Experiment 2: THE DENSITY OF A SOLID UNKNOWN AND CALIBRATION WITH DATASTUDIO SOFTWARE

ENGR 101 Electroplating

Combinational logic systems

SC125MS. Data Sheet and Instruction Manual. ! Warning! Salem Controls Inc. Stepper Motor Driver. Last Updated 12/14/2004

Rotational Motion. Figure 1: Torsional harmonic oscillator. The locations of the rotor and fiber are indicated.

Temperature Measurement and First-Order Dynamic Response *

Prepare for this experiment!

2 One-dimensional motion with constant acceleration

Lab 4 RC Circuits. Name. Partner s Name. I. Introduction/Theory

farads or 10 µf. The letter indicates the part tolerance (how close should the actual value be to the marking).

Name Date Time to Complete

Properties of Liquids

DUBLIN INSTITUTE OF TECHNOLOGY Kevin Street, Dublin 8.

Old Dominion University Physics 112N/227N/232N Lab Manual, 13 th Edition

In this experiment, the concept of electric field will be developed by

FUNDAMENTAL STUDIES OF THE CATALYTIC IGNITION PROCESS

Lab Section Date. ME4751 Air Flow Rate Measurement

Siddharth Institute of Engineering & Technology

Designing a Thermostat Worksheet

Industrial Electricity

(Refer Slide Time: 01:16)

8 Enthalpy of Reaction

Experiment 5 Voltage Divider Rule for Series Circuits

Critical parameters of

Safety Barriers Series 9001, 9002 Standard Applications

I. Introduction and Objectives

EXPERIMENT 5A RC Circuits

Capacitors GOAL. EQUIPMENT. CapacitorDecay.cmbl 1. Building a Capacitor

CHARGED PARTICLES IN FIELDS

E80. Fluid Measurement The Wind Tunnel Lab. Experimental Engineering.

Exercise 4-3. Titration of Weak Acids EXERCISE OBJECTIVE DISCUSSION OUTLINE. The 5% rule DISCUSSION

Transcription:

Experiment A4 Sensor Calibration Procedure Deliverables: Checked lab notebook, Brief technical memo Safety Note: Heat gloves and lab coats must be worn when dealing with boiling water. Open-toed shoes are strictly prohibited. Overview In this lab, you will learn how to implement modern electronic transducers. In the first part, you will perform a 2-point calibration of a resistive temperature device (RTD). In the second part, you will perform a multipoint calibration of a capacitive pressure transducer using a manometer as a calibration standard. You will also use a Pitot probe to measure the velocity of a jet of air and a flowmeter or rotameter to measure flow rate.. Part 1: RTD Calibration As discussed in lecture, the resistivity of a metallic strip increases with temperature, and this phenomenon can be exploited to create an electronic transducer known as a resistive temperature device (RTD). In this exercise, you will calibrate a resistive temperature device (RTD) probe. The tip of the RTD probe contains a thin strip of platinum wire, and the resistance of the platinum probe wire R S is related to temperature by R S (T ) = R 0 1+ α T ( T T 0 ), (1) where α T is the temperature coefficient of resistance and R 0 is the resistance of the probe at a temperature T 0 = 0 C. Please follow the steps listed below to experimentally determine R 0 and α T. Tektronix DC Power Supply i = 0.02 A V+ V- Extech DMM A V Keysight DMM R S (RTD) Black wires Figure 1 A schematic of the RTD circuit. A4 Calibrations 1 Last Revision: 2/12/18

1. Make sure the RTD is not yet connected. 2. Turn on the Tektronix DC power supply, and turn both the current knobs as low (counterclockwise) as they will go, then turn both the voltage knobs as high as they will go. 3. Construct the circuit shown in Fig. 1. a. Connect one of the black wires on the RTD to the negative terminal of the DC power supply with a black banana-to-grabber cable. b. Connect the positive terminal of the DC power supply to the VΩmA receptacle on the Extech DMM with a red banana-to-banana cable. c. Connect the red wire on the RTD to the COM receptacle on the Extech DMM with a red banana-to-grabber cable. d. Set the Extech DMM to 200mA mode. e. Connect the HI (red) cable of the Precision DMM to the red wire of the RTD with a red banana-to-grabber cable. f. Connect the LO (black) cable to the other black wire of the RTD with a black banana-to-grabber cable. 4. Compare the circuit you constructed to Figure 1 to make sure it is correct. Ask the instructor to check if you are unsure. 5. Turn on the Keysight Precision DMM and press the DCV button to measure DC voltage. 6. Slowly turn up the fine current knob on the DC power supply until you get close to 20 ma on the Extech DMM. CAUTION: If you turn up the current to high, it will burn out the probe! 7. Record the current on the Extech DMM and the voltage on the Keysight Precision DMM in your lab notebook. The measured resistance of the RTD at any given temperature can be calculated by dividing the voltage V by the current i, i.e. R S = V/i. 8. Fill a beaker with ice water. Mount the RTD probe in the beaker clamp and dangle it in the ice water. You should notice a change in the voltage. After the voltage reaches steady state, record it in your lab notebook. 9. Fill another beaker with about an inch of distilled water and place it on the hot plate. Turn on the hot plate and allow the water to reach a slow boil. 10. Put on the heat gloves, remove the RTD probe from the ice bath, and submerge it in the boiling water. You should notice a change in the voltage. After the voltage reaches steady state, record it in your lab notebook. 11. Turn off the hot plate. 12. Turn off the DC Power supply. Turn all four knobs as low as they will go (counterclockwise). A4 Calibrations 2 Last Revision: 2/12/18

13. Using the voltage you measured in the ice bath, calculate the resistance R 0 at T 0 = 0 C by dividing the measured voltage V by the measured current i, i.e. R S (0 C) = V/i. 14. Using the voltage you measured in the boiling water, calculate the resistance at T = 100 C by dividing the voltage V by the current i, i.e. R S (100 C) = V/i. 15. Then, use your value for R 0, your resistance at 100 C, and Eq. (1) to determine the temperature coefficient of resistance α T. (Note: α T should have units of 1/ C.) 16. Compare your values for R 0 and α T with the values given on the RTD data sheet and Omega website. (The exact part number for the RTD can be found in the appendix of this handout.) Part II: Pressure Transducer and Pitot Probe In this exercise, you will simultaneously calibrate a capacitive pressure transducer using a manometer and use a pitot probe to determine the speed of an air jet. Theoretical Background Calibrating the Pressure Transducer Shown in Fig. 2 is a schematic of the capacitive pressure transducer. This analog sensor outputs a DC voltage V out that is linearly related to the differential pressure P = P 2 P 1, such that V out ( P) = k P + V 0 (2) where k is the sensitivity coefficient and V 0 is the offset voltage. In this exercise, you will experimentally determine the calibration curve, which is the inverse of Eq. (2). Pinout: 1. Not Connected 2. V supply = +5V (RED) 3. V out (BLUE) 4. GND (BLACK) Figure 2 The pinout for the capacitive pressure transducer. Note that the pin numbers go left to right when looking at the side with letters printed on it. A4 Calibrations 3 Last Revision: 2/12/18

Measuring Airspeed Shown in Figure 3 is a schematic of the overall experimental set-up. As you calibrate the pressure transducer, you will simultaneously measure the airspeed of a jet as a function of flow rate. Theoretically, the average velocity <u> is related to the flow rate Q by the equation <u> = Q/A, (3) where A is the cross sectional area of the nozzle. You will measure the airspeed using a Pitot Static Probe, which measures pressure using the Bernoulli effect. Bernoulli s equation says that the airspeed u is related to the pressure differential ΔP = P 2 P 1 via where ρ A is the density of air. u = 2ΔP ρ A, (4) T connector P 2 Pitot probe P 1 Pressure transducer Air jet P 2 P 1 P 2 P 1 V out Manometer Rotameter Compressed Air in Figure 3 A schematic of the experimental setup for calibrating the capacitive pressure transducer and measuring airspeed with the Pitot probe. Experimental Procedure 1. Make sure the breadboard is turned off. 2. Plug the pressure transducer into the breadboard such that each wire is in a separate row. Make sure the tubes are securely fastened to the barbed connectors on the transducer. 3. Refer to the pin-out in Figure 2. Use the breadboard s built-in +5V DC power supply to connect Pin 2. Pin 4 should be connected to ground. CAUTION: Make sure the sensor is properly connected before you turn on the power supply. If you are unsure, ask the lab instructor for help. Mixing up +5V DC with ground will burn out the sensors! 4. Turn on the breadboard. A4 Calibrations 4 Last Revision: 2/12/18

5. Using the Keysight Precision DMM, measure the voltage difference between Pin 3 V out and ground. 6. The tubes from the transducer should be connected to a couple of T s, which split the gas flow between the Pitot probe and manometer. Connect the other tubes from the T to the manometer and Pitot probe, as shown in Fig. 3. 7. Ask the Lab Instructor for a pair of dial calipers. Use them to measure the diameter of the brass nozzle D. Use this to then calculate the area of the nozzle A. 8. Mount the nozzle to the lab stand using the beaker clamp, such that it is facing upward. 9. Mount the Pitot probe above the nozzle using the other beaker clamp, such that it is directly facing the nozzle. 10. Use the knob on the manometer to zero the fluid level. (Turn the knob until the red line of fluid ends at zero.) Note that the manometer measures pressure in units of inches of water. 11. Slowly open the needle valve on the rotameter. You should hear air flow, see the bead begin to levitate, the fluid level in the manometer should change, and the voltage from the transducer should change. Once you have confirmed this, close the needle valve on the rotameter. 12. Gradually open the needle valve and record the flow rate, manometer pressure in inches of water, and transducer voltage in a table in your lab notebook. (The flow rate should be measured from the center of the bead. Use the flowmeter calibration sheet to convert the bead height to a flow rate in L/min.) Do this for at least 8 different flow rates. Be sure to include units! 13. Make a calibration plot of the differential pressure P in units of Pascal as a function of the output voltage V out. Apply a linear curve fit to determine the calibration equation. 14. Use Bernoulli s Eq. to calculate the velocity of the air jet based on the measured pressure differential. Make a plot of the velocity in m/s as a function of the flow rate in m 3 /s. (Double check that your units are correct!) A4 Calibrations 5 Last Revision: 2/12/18

Data Analysis and Deliverables Create plots and other deliverables listed below. Save the plots as PDFs, import them into either Microsoft Word or LaTeX, and add an intelligent, concise caption. Make sure the axes are clearly labeled with units. Plots with multiple data sets on them should have a legend. Additionally, write 1 3 paragraphs describing the items below. Any theoretical formula you used in your analysis should be included as a numbered equation within these paragraphs. 1. Make a table containing the voltage, current, and RTD resistance you measured for both of the temperatures, 0 C and 100 C. 2. Make a table including the parameters R 0 and α T that you measured for the RTD probe compared with the values reported by the manufacturer. 3. Make plot of the measure differential pressure P (in units of Pa) as a function of the transducer voltage V out with a linear curve fit. 4. Report the calibration equation determined by from the linear curve fit from the previous deliverable. The Equation should be of the form P = av out + b. 5. What is the sensitivity coefficient k = dv out /dp? 6. Make a plot of the measure velocity of the air jet u in m/s as a function of the flow rate Q in m 3 /s. The measured velocity should be determined from the manometer pressure using Eq. (4). Plot the theoretical curve for the average velocity given by Eq. (3) on top of your data. A4 Calibrations 6 Last Revision: 2/12/18

Appendix A Equipment Part I RTD Calibration Omega General Purpose RTD probe (PR-10-2-100-1/4-6-E) Keysight 34465A Precision Digital Multimeter (DMM) o One black banana-to-grabber cable Extech Handheld Digital Multimeter o One red banana-to-banana cable DC power supply o One black banana-to-grabber cable Hot plate Lab coats Heat gloves 2x 100mL beakers Ice bath (solid water floating in liquid water) Lab stand with one beaker clamp Part II Calipers Pitot probe Capacitive pressure transducer (Honeywell HSCSAAN010NDAA5) Keysight 34465A Precision Digital Multimeter (DMM) o One black banana-to-grabber cable DC power supply Inclined manometer Rotameter (0 24,000 L/min) o Long tube with quick-connect going to drop-down compressed air o Short tube with nozzle Two T s with tubes connected Lab stands with two beaker clamps A4 Calibrations 7 Last Revision: 2/12/18