System/Product Atlas Model/Module Atlas Calorimeter Subject Type Measuring the Specific Heat Capacity (Cp) for components and mixtures Subject Version 1.0 Author Yann Lecouturier Date 21st December 2011 Technical Note: Measuring the Specific Heat Capacity (Cp) for components and mixtures with the Atlas Calorimeter 1 Introduction There are a number ways of measuring Cp which may be more or less appropriate depending on cost/availability of materials, reactivity etc. This document describes two methods which are simple to do using the Atlas Calorimeter. • Method 1: Measuring Cp using one single PCC experiment– Direct method • Method 2: Measuring Cp using two PCC experiments at 2 different temperatures – Indirect method Before explaining the details of both methods of measurement, it is important to clarify what we are measuring and calculating. 1.1 Specific Heat Capacity: The objective of this technical note is to measure Cp, the Specific Heat Capacity. Therefore the following terms should be clarified: • Heat Capacity or Thermal Capacity is the measurable physical quantity that characterizes the amount of heat required to change a substance's temperature by a given amount. In the International System of Units (SI), heat capacity is expressed in units of Joule(s) (J) per Kelvin (K). • Specific Heat Capacity (J/g/K): It is the Heat Capacity per gram of the component studied. (Called Cp in this document) Technical note-Measuring Cp for components and mixtures.doc Measuring Cp for components and mixturesPage 1 of 6 • Molar Heat Capacity (J/mol/K): It is the Heat Capacity per mole of the component studied. Specific Heat Capacity and Molar Heat Capacity are commonly used in scientific papers. NOTE: The Calorimetry analysis section in the Atlas Reporting Software requires Specific Heat Capacity for calculations. I will therefore describe two methods to calculate the Specific Heat Capacity referred to as Cp in the rest of this document. 1.2 Equations and enthalpies involved in the calculation of Cp. Q is the overall Enthalpy of the whole process. This is what is seen and measured by the Atlas Calorimeter. This is not the Enthalpy of Reaction. The Enthalpy of Reaction ( ∆HR ) has to be calculated from the Overall Enthalpy Q. The Overall Enthalpy measured is the addition of several aspect of the reaction. They can be defined as three different enthalpies: • Enthalpy of Reaction ( ∆HR ): This is thermal energy released/absorbed by a chemical reaction. This is linked with the molecular/chemical transformation. • Enthalpy of Addition ( ∆Hadd ): This is simply due to the difference of temperature between the two solutions (components) mixed together. The software calculates the Enthalpy of Addition using Cp values entered in the software. The majority of chemist use Cp given in the literature but Cp can be measured as described in this document. The Cp is calculated using the following equation: ∆Hadd = Cp ⋅ M X ⋅ (Tf − Ti ) Mx (g)is the mass of component x added. Ti (°K) is the initial temperature of X and Tf is final temperature of the system after addition. • Enthalpy of Solvation ( ∆HX ): Also called enthalpy of dissolution. This the energy released/absorbed due to the physical effect of mixing a component into another one. In other words, this is the energy involved in the process of forming a solution, i.e. dissolving a solute in a solvent. This is linked with hydrogen bonding, interaction dipole-dipole, anionic interaction etc. This is equal to ZERO when the same component is added to itself as there is no dissolution happening. So the Overall Enthalpy Q can be expressed as the addition of the three enthalpies described above. Q = ∆HR + ∆Hadd + ∆HX Technical note-Measuring Cp for components and mixtures.doc Measuring Cp for components and mixturesPage 2 of 6 2 Experimental Methods 2.1 Method 1: Measuring Cp using one single PCC experiment – Direct method The simplest method is a single experiment where we mimic the calorimetry of reaction. In this case we add a component X to a large volume of the same component X at a single temperature (TR). We just need to run a standard Power Compensation Calorimetry experiment on Atlas Software. 1. In the reactor: Large amount of Compound X 2. Running standard PCC at a given temperature TR 3. Addition of small amount Mx of compound X (X being at ambient temperature) 4. Getting the Overall Enthalpy Q value using Atlas Reporting software. This PCC experiment will give us the Overall Enthalpy Q after the baseline correction in Atlas reporting software. The calculation of the Enthalpy of Reaction are irrelevant here. We are only interested in the Overall Enthalpy value Q. Technical note-Measuring Cp for components and mixtures.doc Measuring Cp for components and mixturesPage 3 of 6 We are adding the component X to itself so: Enthalpy of Reaction ( ∆HR ) = 0 and Enthalpy of Solvation ( ∆HX ) = 0 Therefore Q is simplified as follow: Q = ∆Hadd = Cp ⋅ M X ⋅ (Tf − Ti ) Tf in this case is the temperature of “reaction” or the temperature chosen for the calorimetry experiment TR. In principle the compound added will be at ambient temperature so Ti = Tamb . So, Q = Cp ⋅ M X ⋅ (TR − Tamb ) . We can then isolate Cp: Cp = Q M X ⋅ (TR − Tamb ) It is important to note that Cp here is the average value of Cp over the temperature interval. This temperature interval cannot be too small, otherwise the Enthalpy of Addition detected would be too small to give an accurate result. However, this interval cannot be too large either, otherwise an average Cp over a large temperature would be irrelevant. You can use this method to estimate Cp for mixtures. Simply replace X with the mixture of interest • Advantage of method 1: It is a simple and quick method to use. • Disadvantage of method 1: It may require large amounts of the component X. It requires Tamb to be accurately measured. 2.2 Method 2: Measuring Cp using two PCC experiments at 2 different temperatures – Indirect method We just need to run 2 standard Power Compensation Calorimetry experiment on Atlas Software. 1. In the reactor: Large amount of H2O or another suitable solvent (it cannot react with the compound X added !) 2. Running standard PCC at a given temperature T1 3. Addition of small amount MXof compound X 4. Getting the Overall Enthalpy QT1 value using Atlas Reporting software. Technical note-Measuring Cp for components and mixtures.doc Measuring Cp for components and mixturesPage 4 of 6 5. Running a similar PCC at a different temperature T2, addition of the same quantity MX of compound X and getting QT2. These PCC experiments will give us the Overall Enthalpy QT1 and QT2 after the correction of the baseline in Atlas reporting software. The calculation of Enthalpy of Reaction are irrelevant here. We are only interested in the Overall Enthalpy value QT1 and QT2. We are adding the component X to h2O (or any suitable solvent not reacting with X itself), so: Enthalpy of Reaction ( ∆HR ) = 0, Therefore Q is simplified as follow: Q = ∆Hadd + ∆HX = Cp ⋅ M X ⋅ (Tf − Ti ) + ∆HX Tf in this case is the temperature chosen for the calorimetry experiment: T1 or T2. The component added will be at ambient temperature so Ti = Tamb . So, we can write the following 2 equation for both experiment at T1 or T2. Q(T ) = M X ⋅ Cp ⋅ (T1 − Tamb ) + ∆H x 1 Q(T ) = M X ⋅ Cp ⋅ (T 2 − Tamb ) + ∆H x 2 ΔHx is the heat of solvation of X in a large excess of water (or other suitable solvent). It is independent of temperature of the experiment and so constant in these two experiments as long as the amount of compound X added is the same: MX in both cases. If we isolate ΔHx in both equation above we get: ∆HX = Q( T ) − M X ⋅ Cp ⋅ (T1 − Tamb ) 1 ∆HX = Q(T ) − M X ⋅ Cp ⋅ (T2 − Tamb ) 2 ΔHx being the same in both experiments we can write the following, rearrange and finally isolate Cp as follow: Q(T ) − M X ⋅ Cp ⋅ (T1 − Tamb ) = Q( T ) − M X ⋅ Cp ⋅ (T2 − Tamb ) 1 2 ⇔ M X ⋅ Cp ⋅ (T1 − Tamb ) − M X ⋅ Cp ⋅ (T2 − Tamb ) = Q( T ) − Q( T ) 1 2 ⇔ Cp = Q( T ) − Q( T ) 1 2 M X ⋅ (T1 − T2 ) Technical note-Measuring Cp for components and mixtures.doc Measuring Cp for components and mixturesPage 5 of 6 As for method 1, it is important to note that Cp here is the average value of Cp over the temperature interval between T1 and T2. This temperature interval cannot be too small, otherwise the Enthalpy of Addition detected would be too small to give an accurate result. However, this interval cannot be too large either, otherwise an average Cp over a large temperature would be irrelevant. You can use this method to estimate Cp for mixtures. Simply replace X with the mixture of interest. • Advantage of method 2: It only requires a small amount of component X and Tamb does not need to be known. • Disadvantage of method 2: It is not as quick as method 1. 2.3 Important note to apply these methods successfully with the Atlas Software. Calorimetry of reaction is usually done to assess the risk associated with exothermic reactions. Therefore, the Enthalpy of Reaction measured should be negative as we are talking about exothermic reactions. However, the Atlas Reporting software gives positive values of Enthalpies of Exothermic Reaction for ease of use. This means the following for the Overall Enthalpies values measured in Method 1 and 2: • Any positive Q value given by the Calorimetry software is in fact negative and therefore an Exothermic process. It should be used a negative values in Cp calculations. • Any negative Q value given by the Calorimetry software is in fact postive and therefore an Endothermic process. Method 1: It is likely that the TR chosen will be higher than Tamb. For example: TR = 30°C and Tamb = 20°C: In this case, because we are adding an amount of X at a colder temperature than the large amount of X in the reactor, the overall process will be endotermic, therefore Q used in calculation of Cp should be positive. The Atlas reporting software will show a negative Overall Enthalpy value. Method 2: The process can be Endothermic or Exothermic. This depends on T1 and T2 chosen and the amount of energy released/absorbed by the dissolution ΔHx. Technical note-Measuring Cp for components and mixtures.doc Measuring Cp for components and mixturesPage 6 of 6