Chapter 6 Temperature Scales and Thermometers 6.1 Purpose Temperature is an important property of physical systems. It was not well understood until the latter 1800’s. Today there are many different types of temperature measuring devices. In this lab we will experiment with one of the oldest but most straightforward thermometers, a copper bulb containing a gas. The bulb’s temperature is determined from the pressure of the enclosed gas. We will then construct a temperature scale and determine absolute zero temperature at which molecular motion ceases. 6.2 Introduction Throughout history, a variety of mechanical devices for measuring temperature have been used. You are probably most familiar with the ordinary red-liquid thermometers and simple dial thermometers, which are most often seen. You may also have seen older, glass medical thermometers, which have a mercury column in a glass tube. Each of these types of thermometers makes use of the expansion or contraction of certain substances when changes in temperature occur. The substance, which expands in the usual red-liquid thermometer and thus indicates higher temperatures, is most often alcohol with red dye. The ordinary dial thermostat, which we see in daily use, have within them a ’bi-metal’ element. This is two pieces of different metals joined together. They have differing rates of thermal expansion and contraction and thus a metallic coil formed of such metal pairs will tend to wind or unwind with temperature changes. Electronic thermometers make use of the fact that some materials have very well-defined electrical resistance which varies predictably as temperature varies. In addition to a device to measure and display temperature, one needs certain standards with which to compare temperatures and to calibrate various temperature-measuring devices. You are probably most familiar with the Fahrenheit scale which defines an ice + water mixture as 32 and defines boiling water (at an atmospheric pressure equal to sea level) as 212. You are undoubtedly aware of the Celsius scale, which defines those two temperature 29 The Pascal: The Torr: The lb/in2 (psi) 1 Pa = 1 N/m2 1 Torr = 1 mm Hg 1 lb/in2 = 6870.8 Pa 1atm = 1.01 x 105 Pa 1 atm = 760 Torr 1 atm = 14.7lb/in2 Table 6.1: Units for Pressure standards as 0 and 100 respectively. A constant-volume gas thermometer consists of a fixed volume of gas connected a pressure gauge. Pressure is the force per unit area that the gas molecules exert on the container as they collide with the walls of the container. Pressure in this experiment will be measured in Torr. A table of common pressure units is shown in Table 6.1 In a gas bulb thermometer the pressure, p, increases with the temperature, T, of the gas if the volume, Vconstant , is constant. The ideal gas law: pVconstant = nRT (6.1) describes the relationship between pressure (p), temperature (T) and volume (Vconstant ) which is constant in this case. In addition, n is the number of moles of gas and R is the J ). ’ideal gas law constant’ (8.315 molK Equation 6.1 displays the proportionality between p and T. We can rewrite equation 6.1 as p=( nR Vconstant )T = CT (6.2) where C is a constant since the volume is constant. As temperature decreases, molecular velocities decrease. Absolute zero is that temperature for which the molecular velocities reach zero and molecular motion ceases. (In quantum mechanics, there is a small residual molecular motion even at absolute zero.) Figure 6.1 displays the p and T behavior of equation 6.1. Note that as p → 0, then T → absolute zero. 6.3 Equipment: Gas thermometer, helium supply, vacuum pump, 3 temperature baths, graph paper. 6.4 Procedure Special Cautions: • The temperature of liquid nitrogen is 77 K (-196o C). Direct contact with skin will burn. 30 pressure −273 oC o temperature ( C) Figure 6.1: Plot of temperature vs pressure for an ideal gas Figure 6.2: The gas thermometer with the pressure gauge. • Do not exceed a pressures of 1060 Torr in the gas thermometer. Hold the stem or handle of the bulb firmly while it is in the bath. In this experiment we will show the linear dependence of p on T for the gas bulb thermometer. We will also find the numerical value (in degrees Celsius) of absolute zero temperature. The gas thermometer is shown in figure 6.2 • With the help of your teaching assistant, pump out and fill the gas thermometer with helium. Attach the gas thermometer to the vacuum pump hose. Open the valve, turn on the vacuum pump and remove the air from the gas thermometer. When the pressure reads zero, close the valve and remove the vacuum pump hose. Attach the helium regulator hose to the gas thermometer and fill the gas thermometer to a pressure of 1060 Torr. • Record the initial (room-temperature) pressure of the helium filled gas thermometer. • Place the bulb of the thermometer in each of the three baths beginning with the liquid nitrogen and ending with the boiling water. This avoids formation of a layer of ice around the bulb that could result in errors. Jiggle the bulb around the bath until it reaches thermal equilibrium. Record the reading of the pressure gauge in each bath in a table like Table 6.2. 31 Bath liquid nitrogen ice water boiling water Kelvin(K) Celsius (o C) 77 -196 273 0 373 100 Pressure Table 6.2: Table of temperature and pressure values Pressure Temperature (K) Tap Water Room Air Table 6.3: Table for temperature measurements • Using graph paper, plot pressure on the y-axis and temperature on the x-axis. Draw the ’best fit’ straight line for the three data points. Extrapolate the line to zero pressure. The value where the pressure is extrapolated to zero is absolute zero (-273o or 0 K). Calculate the percentage error of the standard value of absolute zero (-273o) and your extrapolated value. • Now use your gas thermometer to measure the temperature of tap water. Read first the pressure of the bulb when placed in tap water and then use your graph to tell you the waters temperature. Record the values in a table like Table 6.3. Next use your gas thermometer to measure the temperature of the room air. Wait for a few minutes for your gas thermometer to come to equilibrium with the room air. Record the pressure and find the temperature from your graph. 6.5 Questions • What would our graph look like if we had filled the bulb with a gas which condenses at, say, 10C ? • Why do you think helium was used in our thermometer? 32