Differential Scanning Calorimetry and Thermogravimetric Analysis (DSC-TGA) of Quail Egg Shell M. Dzulfahmi Ramadhan – 6137442 SCCH/M SCCH 778 Physico Chemical Technique (Aj. Siwaporn M. Smith) Introduction Thermal analytical techniques particularly have both diverse and dynamic in its current field. Normally, almost any sample in chemical experiments whether its solid, semisolid or liquid can be analyzed and mainly characterized using thermal analytical techniques. In general, materials such as food, pharmaceuticals, polymers, organic and inorganic compounds can simply be measured the change of material properties in terms of function of temperature. Thus allows researchers unable to access information related to matter theories, for instance, equilibrium and irreversible thermodynamics and kinetics. The basic principal of Differential Scanning Calorimetry (DSC), is simply derived from DTA instruments, but DSC has different technique in allowing measurement of a change in enthalpy. Controlled temperature applied in both sample and reference with no phase change, increase or decrease, particularly will lead into a point that undergo a phase change. Subsequently, this change can be determined as endothermic or exothermic process when specific heating rate is applied (heating or cooling respectively), and the difference in temperature can be also recorded. Heat flow recorded from DSC instrument is based on equation of ππ» ππ = πΆπ ππ‘ ππ‘ where H is amount of enthalpy evolved, Cp is heat capacity, T is the absolute temperature, and t is time, thus it can be stated that dT/dt is the heating rate applied. While thermal analysis using Thermogravimetric Analysis allows measurement of changes in weight in relation to changes in temperature. The measured weight loss curve of specific sample will give information of changes in sample composition, thermal stability and also kinetic parameters for chemical reactions in the sample. Theoretically, the mechanism of weight loss change in TGA has particular scheme for each sample, it could be decomposition, which is caused from breaking apart of chemical bonds; evaporation, caused by the loss of volatile compounds in sample after being applied within elevated temperature; reduction, as the matter of interaction atmosphere (hydrogen, ammonia, etc) and also desorption, composition to be released out from the sample. Figure 1. Thermobalance scheme in TGA instrument of sample to a reducing which allows particular Simultaneous TGA and DSC analysis from a single sample has also been widely used for time saving and convenient method of thermal analysis experiments. This DSC-TGA method measures both heat flow and weight changes in a material as a function of temperature or time in a controlled atmosphere. Concurrent measurement of these two material properties not only improves productivity but also simplifies interpretation of the results. The Figure 2. DSC-TGA instrument design complimentary information obtained allows differentiation between endothermic and exothermic events which have no associated weight loss, such as melting and crystallization, and those which involving weight loss. Interpretation of DSC-TGA result may differ based on typical case for each sample used. As the temperature sensitive instrument can be controlled exclusively, the sample of solid, semi-solid and liquid can be analyzed its properties such as oxidative or thermal stability of materials, composition of multi-component systems, melting and boiling points, transition temperatures, heats of fusion and reactions, also decomposition kinetics of materials as well. In experiment, it is also possible to decomposition Figure 3. Typical DSC-TGA kinetics of some polymeric materials. When the sample is Results for Various Case heated using several different heating rate conditions will allow change decomposition time scale for typical component. Applying high value of heating rate causes the higher the given decomposition temperature becomes. The Distributed Activation Energy Model can be used to estimate the activation energy corresponds to the decomposition of materials for each thermal transition. Basically, DAEM model assumes the existence of an infinite number associated with various activation energy. This theory than become simpler with the help of Arrhenius equation, to be written simply as π π0 π πΈπ 1 ln ( 2 ) = ln ( ) + 0.6075 − π πΈπ π π where a is heating rate (K/s), Ea is activation energy (J/mol), k0 is frequency factor, R universal constant (J/mol K), T is temperature applied in thermal transition. Experimental methods In this work, we use material sample of quail egg shell which contains of hard part (presumably CaCO3) and soft part (maybe protein and moisture). This material was placed in a small crucible pan with a half amount fill. The sample then was placed inside container that connected through sensitive analytical balance. For temperature control, oxygen gas was also applied during experiment at the ambient temperature, then scanned the sample in interval of 25 – 800 oC. In this experiment, both sample and reference were applied different heating rates as following number of 6, 8, 10, 15, 20 oC/min which normally caused weigh loss of some composition of egg shell. The mass loss might be caused by typical process such as evaporation, since we know that the sample may contain some water vapors, degradation, decomposition, or even chemical reaction. DSC data analysis would allow us to get information about specific temperature for crystallization and melting process of egg shell components. While TGA would give information about thermal transition of material decomposition of egg shell. The influence of heating rate and decomposition range will be discussed using TG information later on. Result and discussion Thermal transition of quail egg shell component was typically represented with decomposition process. As the main component of hard part of the egg shell is composed by calcium carbonate elements, then proposed transitions for this component is written by CaCO3 (s) CaO (s) + CO2 (g) This decomposition reaction gives conclusion that after high temperature applied during heating process, calcium carbonate would decay gradually at some points to form white solid of CaO along with the evaporation of CO2. Here in this experiment, we could get information about decomposition from Thermogravimetric Analysis. When the temperature was heated up with typical heating rate condition, first, the moisture began to vapored out from the sample, which gave small percentage of weight loss. Secondly, around 500 oC the composition degraded with larger number of weight loss which can be concluded that there were some organic compounds decayed due to the higher temperature point. Then the decomposition would lead into the removal of CO2 gases which occurred in the last step around 700 oC. Therefore, composition of the sample has only about a half of total weight, which specifically is CaO solid left. This hypothesis was also strengthened with the presence of white solid when the thermal analysis process had already ended. And quantitatively, we can also get this information from molecular mass ratio for calcium carbonate decomposition reaction. Even we do not have the specific mass, we still can predict that the total of CaO may occur left in the sample after decomposition is around 56% (CaO = 56 g/mol, CaCO3 = 100 g/mol). In fact, actual value is obtained from TGA data which specifically give us information that if the value of CaO left in the last thermal transition is higher, then there might be also another inorganic compound that cannot be removed. While if the value of weight loss occurs higher than normally does, it might be caused by some hydrate or organic compounds which typically sensitive with the high temperature analysis. Thermal transitions occurred in this experiment are summarized in table 1. Heating rate (oC/min) 6 8 10 15 20 1st transition 5.831 6.163 5.433 9.043 6.275 Water/moisture Weight loss (%) 2nd transition 2.841 5.099 13.16 7.716 44.82 Organic compound (protein) 3rd transition 40.14 38.12 34.01 36.70 21.73 CO2 Approximate Residue (%) 50 50 47 45 27 CaO (s) Table 1. Summarizes of thermal decomposition of quail egg shell components in various heating rates The removal of CO2 has the main effect of this decomposition, which leading into high value of weight loss (almost 40%). And the maximum weight value of CO2 can be removed approximately 48% according to the molecular mass ratio. Heating rate gives the influence for the decomposition process in terms of thermal transition. Theoretically, increasing heating rate will cause the decomposition yield higher value. Hence it is can be optimally achieved when applying optimum condition of heating rates. Nevertheless, if the heating rates is increased further can cause the decomposition to result in small residue, this may because the higher heating rate also possibly can make the kinetic energy of thermal transition to be more than the composition could bear. As we can see, for quail egg shell sample which contains of mainly calcium carbonate was degraded excessively when it comes to heating rate of 20 oC/min. The composition of residue obtained after thermal process is much lower than expected, in this case, we can conclude that there was also some calcium oxide decayed from the total composition. Thermal transitions occurred in the quail egg shell decomposition are mainly divided into two major process, which are crystallization, showed by peak up, and melting process showed by peak down. For both two processes, there were no reaction but physical properties change. The crystallization occurred from exothermic process which also proceed some enthalpy differences in thermal transition, while the melting represented endothermic process. The various heating rates applied in this experiment make it unable to calculate the activation energy for each using The Distribution of Activation Energy Model (DAEM). On the basic principle of Arrhenius equations, we can simplify DAEM in order to get the approximate values of activation energy and the corresponding frequency factor, k0. π π0 π πΈπ 1 ln ( 2 ) = ln ( ) + 0.6075 − π πΈπ π π DAEM equation unable approximation to be done from linear regression from various heating rates and temperature. Once we pot ln(a/T2) versus 1/T for various heating rates at specific thermal transition, we can get graph as following and then using linearization result, we can calculate the activation energy E, from its slope, which defined by (-Ea/R), while the frequency factor can be calculated using intercept quantitatively. Figure 4. Graphic plot of DAEM Model to calculate the activation energy for each thermal transition in various heating rates Activation energy occurs for each crystallization and melting transition based on DSC graph. Here we get the linear equation of y = -3981.2x + 2.9834 for the first transition and y = 5772.x -1.8389. After considering the gas constant R for calculation, the activation energy obtained for crystallization process is 33.1 kJ/mol and for melting is 48 kJ/mol. Conclusion Simultaneous thermal analysis using DSC-TGA is considered to be used effectively to observe physical properties of some materials. This instrument generally refers to one sample and reference measurement using thermal energy application to measure both heat flow and weight changes in a material as a function of temperature or time in a controlled atmosphere. This hybrid method allows measurement to increase productivity and simplify interpretation of the results. The complimentary information obtained allows differentiation between endothermic and exothermic events which have no associated weight loss, such as melting and crystallization, and those which involving weight loss. In this experiment quail egg shell is mainly composed of few proteins and some calcium carbonate which is more dominant in forming the shell to become hard and stiff. The decomposition of the sample was leading into removal of moisture, organic compounds, and CO2 and leaving residue of CaO from TGA data. While from DSC data, thermal transition occurred in two ways, exothermic crystallization and endothermic melting process. In addition, activation energy for each thermal transition also can be achieved using DAEM model, resulting 33.1 kJ/mol and 48 kJ/mol respectively. Reference 1. Hongbo Y, Meiling C, Xu W, Hong G. Thermal analysis on the kinetics of magnesiumaluminum layered double hydroxides in different heating rates. Arch Metall Mater. 2015;60(2):1357–9. 2. Soria-Verdugo A, Garcia-Gutierrez LM, Blanco-Cano L, Garcia-Hernando N, RuizRivas U. Evaluating the accuracy of the Distributed Activation Energy Model for biomass devolatilization curves obtained at high heating rates. Energy Convers Manag. 2014;86:1045. 3. Stodghill, Steven. Thermal Analysis – A Review of Techniques and Applications in the Pharmaceutical Sciences. American Pharmaceutical Review. 2010:13:2. 4. Wellen Renate, Eduardo L., Canedo. On the Kissinger equation and the estimate of activation energies for non-isothermal cold crystallization of PET. ScienceDirect Elsevier. 2014:40:33-38. 5. Royal Society of Chemistry. Accessed internet 24 Nov, from http://www.rsc.org/learnchemistry/resource/res00000704/thermal-decomposition-of-calciumcarbonate?cmpid=CMP00005970 Differential Scanning Calorimetry Data Thermogravimetric Analysis Data