CRE7: Mass transfer aspects of a gas-solid non catalytic reaction
AIM: To determine the effective diffusion coefficient for the non-catalytic gas-solid reaction of
calcium carbonate decomposition.
APPARATUS:
 Furnace: Used to provide controlled high temperatures.
 Holders: Containers to hold the chalk pellets.
 Microbalance: Instrument to measure precise weights of samples.
 Stopwatch: Tool to measure reaction times.
 Crucibles: Containers to hold samples during the reaction.
 Vernier scale: Used for measuring dimensions accurately.
 Chemicals: Chalk (calcium carbonate).
CHEMICALS:
 Calcium carbonate powder or chalk
PREPARATION:
 Cut the chalk into cylindrical shapes and weigh them to ensure precise weight measurement.
 Measure the diameter and thickness of the chalk pellets and note the readings.
PROCEDURE:
     I. Number the pellets for identification.
    II. Raise the furnace temperature to the desired reaction temperature (750°C and 800°C).
   III. Place all the pellets in the furnace simultaneously. Ensure they have similar
        dimensions and initial weights.
   IV.  Remove each pellet after different reaction times and transfer them to a desiccator for
        cooling.
    V.  Measure the weight loss of the pellets corresponding to different reaction times.
   VI.  Perform the experiment at both 750°C and 800°C. Take four chalk samples at each
        temperature.
  VII.  Maintain a time gap of 15 minutes between readings for both 750°C and 800°C.
THEORY:
In the context of gas-solid reactions, diffusion plays a
crucial role in transporting reactant molecules from the bulk gas phase to the solid
surface where the reaction occurs. Fick's Law of Diffusion can be used to describe this
process. The effective diffusion coefficient takes into account the complex nature of diffusion in
heterogeneous systems like gas-solid reactions. It considers factors such as pore
structure, surface area, and possible hindrances to diffusion due to interactions between
reactant molecules and the solid surface. The effective diffusion coefficient is not a
constant value, but rather a parameter that varies depending on the conditions and
characteristics of the system. The Arrhenius equation relates the rate constant of a reaction to
temperature. It's commonly used to describe the temperature dependence of reaction rates.
                              CaCO3 → CaO + CO2
The reaction is assumed to proceed according to the shrinking core model.
At the high temperature rate of reaction will be high but the mass transfer is controlling.
DERIVATION:
DATA AND CALCULATIONS
For 750°C
                    Initial
 Initial D final D  W        Final W Initial L Final L  Time
      9.81     8.85   1.9587   1.5425   32.55     30.12      15
       9.5     8.27   2.3807   1.8743   41.22      36.4      30
      9.78     8.21   2.0988   1.6521   35.39     30.54      45
      9.62     7.75   2.2413   1.7638   38.47     31.89      60
For 800°C
                    Initial
 Initial D final D  W        Final W Initial L Final L   Time
      9.67     8.45    2.198   1.7298   36.42     32.93       10
      9.76     7.98   2.4444   1.9235   39.21     32.82       20
      9.72     7.46   2.1544   1.6953   36.56     29.77       30
      9.56     7.32   2.1321   1.6776   36.89         29      40
Theoretical Effective Diffusivity Calculation:
For 750°C
 Initial                     True           Bulk
 Volume         Final Volume Density        Density      Porosity
 2460.248009    1852.812151       2.711     0.81432877   0.699621
 2921.763635    1955.249953       2.711     0.88670738   0.672922
  2658.57033    1616.758781       2.711     0.90565308   0.665934
 2796.161243    1504.346243       2.711     0.98701633   0.635922
                                            0.89842639      0.6686
For 800°C
 Initial                   True       Bulk
 Volume       Final Volume Density    Density    Porosity
 2674.747381 1846.69439         2.711 0.87923029 0.67568
    2933.5018 1641.474879       2.711 1.00254117 0.630195
 2712.867597 1301.20694         2.711 1.04850427 0.613241
 2647.977686 1220.422038        2.711 1.08989347 0.597974
                                       1.0050423 0.629272
Experimental Effective Diffusivity Calculation:
                           Initial
 Initial D final D         W        Final W Initial L Final L  Time    X        t/X
      9.81     8.85          1.9587   1.5425   32.55     30.12      15 0.482927 31.0606
       9.5     8.27          2.3807   1.8743   41.22      36.4      30 0.483433 62.05616
      9.78     8.21          2.0988   1.6521   35.39     30.54      45 0.483718 93.02942
      9.62     7.75          2.2413   1.7638   38.47     31.89      60 0.484195 123.9169
                                       t/X v/s X
        140
        120                                             y = 74892x - 36138
        100
                                                                                           Chalk       DAB
         80
                                                                                                   1   5.373059
  min
         60                                                                                        2   0.851482
         40                                                                                        3   0.857101
                                                                                                   4   0.832361
         20
                                                                                                       1.978501
          0
          0.4828   0.483    0.4832   0.4834   0.4836   0.4838   0.484    0.4842   0.4844
                                                X
 DAB = 0. 859114 cm2/s
                           Initial
 Initial D final D         W        Final W Initial L Final L   Time    X        t/X
      9.67     8.45           2.198   1.7298   36.42     32.93       10 0.484118 20.65613
      9.76     7.98          2.4444   1.9235   39.21     32.82       20 0.484317 41.2953
      9.72     7.46          2.1544   1.6953   36.56     29.77       30 0.484315 61.94311
      9.56     7.32          2.1321   1.6776   36.89         29      40 0.484478 82.56317
                                         t/X
        90
        80
                                                                                      Chalk       DAB
                                                        y = 170997x - 82763
        70                                                                                    1   2.316319
        60                                                                                    2    0.39259
        50                                                                                    3   0.358822
  min
        40
        30
                                                                                              4   0.359118
        20                                                                                        0.856712
        10
         0
         0.48405 0.4841 0.48415 0.4842 0.48425 0.4843 0.48435 0.4844 0.48445 0.4845
                                             X
DAB = 0. 374146 cm2/s
RESULTS AND CONCLUSION:
         Theoretical vs. Experimental Diffusion Coefficient: we used complex calculations
          involving various process parameters to determine the theoretical diffusion coefficient
          (Dtheo). However, there is a difference between the theoretical and experimental
          diffusion coefficient (Dexp) values. This difference is attributed to variations between the
          assumptions of the theoretical model and the actual experimental conditions.
         Shrinking Core Model: The Shrinking Core model, which assumes that the rate of mass
          transfer within the unreacted core controls the rate of reaction, was selected to represent
          the reaction mechanism. This choice was reasonable considering the observed
          breakdown process characteristics in your experiment.
         Temperature Effects: Normally, higher temperatures lead to increased kinetic energy and
          higher diffusion coefficients. However, our experiment's results did not entirely align with
          this expectation.
         Internal Diffusion-Limiting Factors: The diffusion rate of carbon dioxide gas through the
          unreacted core of the particles significantly affects the overall reaction rate.
         Complexity of Real-World Reactions: Despite the observed discrepancies between
          theoretical predictions and practical results, our experiment sheds light on the complexity
          of real-world reactions. This emphasizes the importance of accurate experimental
          methods and the understanding that real reactions can be influenced by numerous
          factors beyond theoretical considerations
PRECAUTION AND SOURCES OF ERROR:
      Temperature Control: Ensure accurate and consistent temperature control throughout
       the experiment to avoid variations in reaction rates due to temperature fluctuations.
      Pellet Uniformity: Maintain uniform pellet dimensions and weights to minimize
       discrepancies in mass transfer rates and reaction kinetics.
      Pellet Handling: Handle pellets carefully to avoid damage or irregularities that could
       affect the experiment's results.
      Gas Flow: Ensure proper gas flow and distribution around the pellets to prevent localized
       variations in gas concentration.
      Pressure Changes: Monitor and control pressure conditions to prevent deviations from
       standard atmospheric pressure, which can impact gas-solid interactions.
      Data Collection: Accurately record weight and time data, minimizing human errors during
       measurements and data logging.
SCOPE FOR IMPROVEMENT:
      Advanced Instrumentation: Employ advanced equipment for more precise
       measurements, such as high-resolution thermocouples and advanced gas flow control
       systems.
      Real-time Monitoring: Use real-time monitoring techniques to continuously track weight
       changes and reactions, enhancing data accuracy and capturing dynamic behaviors.
      Variability Analysis: Investigate the effect of variations in pellet properties on
       experimental outcomes through systematic studies.
      Gas Mixture Control: Experiment with different gas mixtures and compositions to
       understand their impact on mass transfer and reaction kinetics.
INDUSTRIAL APPLICATION:
      Catalyst Development: Insights from these experiments can aid in the design and
       optimization of catalysts and solid reactants for various industrial processes.
      Chemical Production: Understanding mass transfer and reaction kinetics is crucial for
       optimizing chemical reactions and production processes, leading to improved yield and
       efficiency.
      Environmental Control: Knowledge of gas-solid reactions can be applied to
       environmental control technologies, such as air pollution control systems and carbon
       capture processes.
      Material Synthesis: These principles are essential in industries involving material
       synthesis, where controlling reactions between gases and solids leads to tailored
       material property.