PHY1110L Calorimetry Instructions

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Wright State University *

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1110

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Chemistry

Date

Dec 6, 2023

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docx

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4

Uploaded by ProfBeaver3142

EXPERIMENT: CALORIMETRY [Equipment List: Computer Laptop, Computer Interface, Temperature Probe, Double- Walled Calorimeter, Stirrer, Water, Ice] Overview: When heat energy is added to a body it may cause the temperature of the body to rise or the phase of the body to change (for example, solid to liquid). When heat energy is removed from a body the reverse processes may occur. When a change of phase from solid to liquid occurs (as we are concerned with in this experiment) the amount of heat energy Q needed to melt the material is related to the mass, m , of the material melted by Q = mL , where L is called the latent heat of fusion. When a material exchanges energy but does not go through a phase change the change in energy is related to the change in temperature by Q = mc T , where c is the specific heat of the material and T is the change in temperature. If materials at different temperatures are in contact with each other, and no energy flows into or out of the system, heat energy is given up by the hotter component and absorbed by the cooler one, until the parts of the system come to a common temperature. In this experiment, we use a calorimeter that approximates an adiabatic situation. (Heat transfer by radiation, conduction, and convection, can be impeded but never prevented). The specific heats of the materials of the calorimeter are known, and the latent heat of ice is determined. Temperature Probe Lid Cable to Interface Inner Cup Non- Conducting Ring Outer Cup Water Air Insulation Stirrer figure 1 1
The general method for measuring the latent heat of fusion for ice is to measure the initial temperature of the water in the calorimeter cup, ease the ice into the calorimeter cup, and determine how much the temperature of the water decreases. The chief source of systematic error in calorimetric experiments lies in the exchange of heat between the calorimeter and its surroundings by radiation and convection (not truly adiabatic). In this experiment the simplest way to correct for this is to start with the initial temperature of the receiver (can and water) as far above room temperature as the final temperature will be below it. This way the heat lost by the calorimeter to the surroundings during the first half of the experiment (before the ice is added), will be approximately compensated by the heat gained by the calorimeter from the surroundings in the second half of the experiment (after the ice is added). Measure the masses of the calorimeter cup and the stirrer and record these on the Excel worksheet. The cup is aluminum and the stirrer is nickel-plated brass. The specific heat of aluminum is 0.224 cal/(gm o C) , and of nickel plated brass is 0.090 cal/gm o C . Trial 1: Fill the calorimeter can 2/3 full of water that is about 5 o C above room temperature and determine the mass of the water. Record the mass of the water onto the Excel worksheet. The specific heat of water is 1.000 cal/(gm·°C) . Assemble the calorimeter with the stirrer and temperature probe. Record the temperature of the water using the temperature probe readout on the computer. While gently agitating the water with the stirrer, allow about 30 seconds to go by to establish a cooling curve showing the loss of heat to the surroundings. Carefully add 1 ice cube and continue taking the temperature and gently agitating the water with the stirrer. The specific heat of ice is 0.500 cal/(gm·°C) . Be sure that the ice is as dry as possible before placing it in the calorimeter. Extra water will have adverse effects to the results. After the final warming trend is clearly established, determine the mass of ice added by subtracting the mass of the system before from the mass of the system after, making this calculation on the Excel worksheet. 2 Temperature Ice Introduced Cooling Curve Room Temperature Equilibrium between water and ice reached Heating Curve Time Figure 2
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