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Energy of adsorption of an adsorbent in solving environmental problems

The article presents the results of the study of the adsorption energy, thermodynamic parameters of adsorbents, which serve to solve the problems of ecology and environmental protection.Based on the results obtained, the adsorption mechanism of the pargaz activated carbon adsorbent on the basis of tree wood and waste stem was studied.The energy of the adsorption process of the adsorbent is obtained on the basis of data on the full thermodynamic parameters of the field of application of adsorbents. The paper examines the differential heat content, adsorption isotherm, entropy, and kinetics of PPAU-A experimentally. This article uses adsorption microcalorimetric methods of analysis. Paulownia tomentosa tree coal adsorbents according to the adsorption amounts of water molecules in thermally and steam-gas activated carbon adsorbents based on tree stems is as follows: PPAU-A> BAU-A.The value of the adsorption value of water vapor in PPAU-Ada Beryoze activated carbon was found to be 1.4 times higher than BAU-A.


Introduction
There are a number of factors leading to the conflicting state of ecology and environmental protection by industrial and manufacturing enterprises, the development of adsorbents with active surface, active adsorption properties to solve these problems, the study of their adsorption energy is one of the urgent problems. One of the main problems of ecology is the problem of environmentally hazardous wastes and atmospheric air pollution. Extraction of secondary raw materials from waste and its use in the elimination of environmental problems serve as a solution to the above problems.Therefore, in this research work, the aim was to obtain an activated adsorbent based on tree waste and to study their adsorption energy. As a result of studying the thermodynamics of the adsorption process in adsorbents, we obtain accurate information about their active surface area, adsorption mechanisms and complete thermodynamic parameters. In the study of thermodynamic processes, we gain insights into the mechanism of adsorption mainly by studying the adsorption heat, isotherm, kinetics, and entropy.
In adsorbents, the adsorption process is observed in the state of physical and chemical adsorption.
In both the physical adsorption process and the chemical adsorption process, a thermal effect is observed, in which the amount of heat is released as the adsorption event occurs by an exothermic process, i.e. heat dissipation. The amount of heat released during the course of chemical adsorption is very close to the thermal effect of chemical reactions. In the case of physical adsorption, the amount of heat released is mainly measured using a microcalorimeter device.
In this case, the results obtained as a result of the experiment have an approximate value, because the adsorption process and the time of heat dissipation last for a certain period of time. The thermal effect occurring in the adsorption phenomenon is analyzed by concepts such as integral heat and differential heat of adsorption, as well as formulas for their determination by mathematical operations.

Literature Review
Adsorption heat can be determined using microcalorimetric devices based on a very sensitive adiabatic process [1 ]. The exact values of the adsorption isotherms and the differential heat of adsorption can be used to determine the differential molar entropy (∆Sd) of adsorption using the Gibbs-Helmholtz equation [2][3][4].
Adsorption of benzene and toluene vapor as adsorbents from organic substances to natural mineral compounds, ie bentonites, mainly from adsorbents, as well as thermodynamic parameters were studied [5-10] defined. In the adsorption of synthetic zeolites, the full thermodynamic parameters of the adsorption of benzene, water and SO2 gas vapors from adsorbates were studied and the adsorption mechanism was determined on their basis [11][12][13]. However, to date, the literature does not provide accurate information on the adsorption and thermodynamic parameters of adsorbents based on the tree, the mechanism of adsorption.
Studies on adsorbents obtained as a result of activation of various tree species make up a very small amount [14][15][16][17][18][19][20][21]. As a result of determining the adsorption mechanism using thermodynamic parameters of adsorbents, experimental studies were carried out on a high-vacuum adsorption microcalorimetric device in order to obtain information about their active surface surfaces and selective adsorption capacity.The adsorbent mechanism of water quadrupol molecule vapors belonging to the class of aromatic hydrocarbons to the carbon adsorbent obtained by steam-gas activation method on the basis of Paulownia tomentosa tree stem was obtained, energy characteristics of molecular interactions between adsorbent-adsorbate and adsorbateadsorbate. The following authors [22][23][24][25][26] have dealt with the issues of energy, electrical mechanisms and the energy of adsorption of the adsorbent.

Research methods
This article uses adsorption microcalorimetric methods of analysis. In determining the thermodynamic parameters of adsorbents with high adsorption activity, the process of studying the adsorption mechanism used a universal high-vacuum adsorption device at a temperature of 303 K and a system of differential microcalorimeter type Tiana-Kalve DAK-1-1A connected to it.
Using the device, the values of the isotherm, differential heat content, entropy and kinetics of water vapor adsorption on the adsorbent PPAU-A (Paulownia pargaz activated carbon adsorbent) were obtained.

Results and discussion
In the adsorption-calorimetric method, an adsorbent sample with a dispersion of 2-5 mm, which is activated in the study of thermodynamic characteristics of adsorbents water vapor adsorption, is placed in a glass ampoule, and in turn the finished ampoule is connected to the calorimeter.
Initially, the vacuum is connected to the vacuum pump at a temperature of 423K for 4 hours until a residual pressure of 10 -5 Pa is reached. The quadrupol water molecule selected as the adsorbate was first frozen and then the dissolved gases were removed using a vacuum pump at room temperature. The adsorption process is carried out at a temperature of 303K. The results of the differential thermal adsorption of pargaz activated carbon adsorbent are shown in Figure 1. In the PPAU-Ada water adsorption heat in the initial saturation areas, when the adsorption amount a = 0.14 mmol/g, the Qd differential heat value started from 74.0 kJ/mol, a sharp decrease was observed, and the Qd value was equal to 50.51 kJ/mol. In the subsequent adsorption stages, the process changes in a stepwise manner through the maximum.
The results of the experimental study showed that with increasing value of the amount of adsorbent in the adsorbent, the differential heat at a = 0.83 mmol/g reaches the value of Qd = 49.1 kJ/mol, and a small saturation of the first step passes through the maximum. The reason for the high heat at such small saturations is due to the formation of p-complexes with water molecules with small amounts of rare metal cations in the carbon adsorbent sample. As the amount of adsorption in the adsorbent increased to a = 1.65 mmol/g, a stepwise decrease in the amount of differential heat was observed to Qd = 46.78 kJ/mol. In such a saturation state, the electron acceptor formed during the vapor-gas activation of the carbon adsorbent falls into the field of formation due to the interaction of carbon atoms with water molecules. Then, in the next stage, the amount of differential heat decreases to Qd = 45.4 kJ/mol when the amount of adsorption increases in the range a = 1.65÷2.94 mmol/g, and then the differential heat of adsorption increases when the amount of adsorption increases to a = 3.60 mol/kg. An insignificant decrease was observed through the maximum to Qd = 45.0 kJ/mol. Then, as a result of the change in the amount of adsorption in the range a = 5.2÷6.55 mmol/g, the change in the differential heat of adsorption to Qd = 44.87÷42.13 kJ/mol was observed with a high maximum, while the amount of differential heat Qd = 55.6 kJ/mol as a result of rising to the top was observed a sharp high maximum. During the next stages of the adsorption process, a decrease in the amount of heat of adsorption was observed between small maxima in the range Qd= 42.13÷40.13 kJ/mol in the range of adsorption amount a = 6.55 mmol/g to 9.1 mmol/g. At the end of the adsorption, when the amount reached a = 9.56 mmol/g, a decrease in the heat value of condensation was observed. Such a decrease in the heat of adsorption corresponds to a decrease in the potential energy in the adsorbent due to the occurrence of adsorption on the micro-, and meza-pores in the empty state of the adsorbent, as well as the filling of the pores with adsorbent molecules. Since the porosity of carbon-based adsorbents is very small, sunken mensk is formed in such pores. In these mensks, the adsorbent vapors condense at pressures below the saturation pressure (Ps) on the flat surface.
At this time, the adsorbent initially forms polymolecular layers on the capillary walls, which accumulate and become a liquid that moistens the capillary and fills it. In this case, capillary condensation occurs not under the influence of adsorption forces, but under the influence of the force of attraction of vapor molecules to the spherical surface of the liquid. In the last saturation areas of adsorption, the adsorption heat was observed to decrease in the range a = 9.56 mmol/g to Qd = 36.65 kJ/mol. This indicates that the final stages of adsorption occur due to the adsorbate-adsorbate interaction, where the thermal value of the adsorption is small. The results of the adsorption isotherm of PPAU-A based on experiments at 303 K are shown in Figure 2.
The differential entropy value of adsorption describes the motion of a certain number of adsorbed molecules in the adsorbent, the state function. The entropy curve of the PPAU-A and H2O system has a wavy appearance according to the adsorbent saturation values, and the quadrupol molecule selected as the adsorbate in the adsorbent provides information on the location of the water (Fig. 3). The maximum level of differential entropy value expressed in molar value of adsorption in the adsorbent was in the range of positive entropy value ∆S = 22.6 J/(mol*K) in the areas of formation of p-complexes. It was then observed that in the PPAU-A-H2O system at negative values of adsorption entropy, the amount of adsorption between 0.5 and 4.96 mmol / g passes through small minimum rings with entropy value ∆S = -19.02 J/(mol*K).
This state of entropy leads to the conclusion that the water molecules absorbed by the adsorbent are motionless, i.e., in a solid state. At values of entropy adsorption value 6.02 mmol/g, the value of entropy ∆S = -47.52 J/(mol*K was reduced to a high minimum. In the next view of entropy, it was observed that the value of entropy ranged from 6.75 mmol/g to 9.35 mmol/g at a negative value between ∆S= -7.0 J/(mol*K).
At the end of the adsorption entropy, a sharp maximum was observed, and when the adsorption amount reached 9.77 mmol/g, the positive value of entropy increased to S = 66.0 J/(mol*K). The motion of the water molecules then equals the motion of the molecules in the liquid state due to capillary condensation in the adsorbent mesocytes. The results of the dependence of the time of formation of the adsorption equilibrium in the PPAU-A adsorbent on the adsorption are shown in Figure 4. The setting time of the adsorption equilibrium in the areas of formation of the first p-complexes lasted up to 4 h. With an increase in adsorption, a decrease in adsorption time to 2 hours was observed in the wavy