ISSN: 2689-7636
Annals of Mathematics and Physics
Review Article       Open Access      Peer-Reviewed

Theoretical calculation of self-propagating high-temperature synthesis (SHS) preparation of AlB12

Chao Wang1*, Xiaoming Cao2, Mengge Dong3, Lu Zhang4, Jianxing Liu3, Xiaozhou Cao3* and Xiangxin Xue3*

1Department of Mechanical Engineering, the University of Texas at Dallas, Richardson, TX, 75080, USA
2Institute of Metal Research, Chinese Academy of Science, Shenyang, Liaoning, 110016, China
3School of Metallurgy, Northeastern University, Shenyang, Liaoning, 110819, China
4School of Energy and Environment, Anhui University of Technology, Ma’anshan, 243002, China
*Corresponding author: Chao Wang, Department of Mechanical Engineering, the University of Texas at Dallas, Richardson, TX, 75080, USA, E-mail: wang.chao@utdallas.edu Xiaozhou Cao, School of Metallurgy, Northeastern University, Shenyang, Liaoning, 110819, China, , E-mail: caoxz@smm.neu.edu.cn Xiangxin Xue, School of Metallurgy, Northeastern University, Shenyang, Liaoning, 110819, China, E-mail: xuexx@mail.neu.edu.cn
Received: 17 Febraury, 2021 | Accepted: 22 March, 2021 | Published: 23 March, 2021
Keywords: AlB12; SHS; Theoretical calculations; Adiabatic temperature; Standard gibbs free energy

Cite this as

: Wang C, Cao X, Dong M, Cao X, Xue X, et al. (2021) Theoretical calculation of self-propagating high-temperature synthesis (SHS) preparation of AlB12. Ann Math Phys 4(1): 009-012 DOI: 10.17352/amp.000019

Although experimental results of preparing AlB12 by self-propagating high-temperature synthesis using Mg-B2O3-Al2O3 as raw material has been studied, the theoretical calculations for the preparation of AlB12 have not been examined as thoroughly. In this article, for the first time, we report on the study of theoretical calculation and the adiabatic temperature, calculated, and compared with the actual reaction temperature. The Gibbs free energy for each level of reaction is also calculated. The calculation results show that the adiabatic temperature is 2789.5 K, the standard Gibbs free energy of each reaction is less than 0, and the reaction can proceed spontaneously, which is consistent with the results of the experiment.

Introduction

In the process of SHS synthesis reaction research, the reaction system must meet certain thermodynamic conditions so that the reaction can self-sustain the combustion reaction process [1-3]. Among them, the most basic thermodynamic parameter is the Adiabatic Temperature of the reaction [4-7]. Self-propagating high-temperature synthesis (or SHS) is a chemical reaction under special conditions [8-11]. Thermodynamic analysis mainly discusses the feasibility of the reaction, such as how to judge whether a chemical reaction can proceed under given conditions, to what extent, and what effect the reaction will have after changing the conditions [12-14].

Thermodynamic analysis of the combustion system is the basis for studying the SHS process [15-17]. The main task of thermodynamic analysis is to calculate the combustion temperature and product balance under adiabatic conditions, that is, when all the heat released by the reaction is used to heat the product synthesized during the reaction [18,19]. The calculation is based on the minimum principles of conservation of mass and energy and chemical potential (Gibbs free energy) [20,21]. Thermodynamic calculation is a very effective method for studying the SHS process, as it helps to control the temperature and composition of the process products [22-25].

Previous studies have shown that AlB12 can be prepared by the self-propagating method [26-28] and the reaction temperature is higher than 2300°C. However, the self-propagating reaction has not been calculated theoretically. In this article, the basic principle of self-propagating reaction is explained, the theoretical calculation of self-propagating preparation of AlB12 is studied, and the calculated results are compared with the actual test results.

Principle of self-propagating reaction

Adiabatic temperature is an important thermodynamic parameter describing the characteristics of combustion synthesis (SHS) reaction. Merzhanov et al. put forward the following empirical criterion, that is, only when>1800K, the SHS response can be self-sustained [25]. Munir found that the ratio of the heat of formation of some compounds below their melting point to the heat capacity at 298K has a linear relationship with and [29,30]. It can be concluded that the reaction can maintain itself only when (corresponding to). Otherwise, only the outside world can supplement energy into the system, such as by using a “preheating”, “chemical furnace” or the use of “thermal explosion” methods to maintain self-reaction.

The self-propagating reaction can be expressed as equation (1):

A(s)+B(s)AB(s)+ΔH MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqaiaacIcacaWGZbGaaiykaiabgUcaRiaadkeacaGGOaGaam4CaiaacMcacqGHsgIRcaWGbbGaamOqaiaacIcacaWGZbGaaiykaiabgUcaRiabfs5aejaadIeaaaa@45E3@ (1)

(1) Taking the enthalpy of the system as the state function, the heat released during the reaction is:

ΔH=Δ H 298 θ = 298 Tad ΔCpdT MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeuiLdqKaamisaiabg2da9iabfs5aejaadIeadaqhaaWcbaGaaGOmaiaaiMdacaaI4aaabaGaeqiUdehaaOGaeyypa0Zaa8qmaeaacqqHuoarcaWGdbGaamiCaiaadsgacaWGubaaleaacaaIYaGaaGyoaiaaiIdaaeaacaWGubGaamyyaiaadsgaa0Gaey4kIipaaaa@4C89@ (2)

in which is the standard enthalpy for formation of the product at a temperature of 298K, and is the heat capacity of the product.

When adiabatic, the thermal effect of the system is , and the adiabatic temperature can be calculated in the following situations:When <:

T ad MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBaaaleaacaWGHbGaamizaaqabaaaaa@38C6@ T mp MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBaaaleaacaWGTbGaamiCaaqabaaaaa@38DE@ (3)

when : Δ H 298 θ = 298 Tad ΔCpdT MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeyOeI0IaeuiLdqKaamisamaaDaaaleaacaaIYaGaaGyoaiaaiIdaaeaacqaH4oqCaaGccqGH9aqpdaWdXaqaaiabfs5aejaadoeacaWGWbGaamizaiaadsfaaSqaaiaaikdacaaI5aGaaGioaaqaaiaadsfacaWGHbGaamizaaqdcqGHRiI8aaaa@4A3D@

T ad = T mp MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBaaaleaacaWGHbGaamizaaqabaGccqGH9aqpcaWGubWaaSbaaSqaaiaad2gacaWGWbaabeaaaaa@3CC2@ (4)

in which is the enthalpy of the product in the molten state, and is the heat of fusion of the product.

when >: Δ H 298 θ = 298 Tad ΔCpdT +γΔ H m MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeyOeI0IaeuiLdqKaamisamaaDaaaleaacaaIYaGaaGyoaiaaiIdaaeaacqaH4oqCaaGccqGH9aqpdaWdXaqaaiabfs5aejaadoeacaWGWbGaamizaiaadsfaaSqaaiaaikdacaaI5aGaaGioaaqaaiaadsfacaWGHbGaamizaaqdcqGHRiI8aOGaey4kaSIaeq4SdCMaeuiLdqKaamisamaaBaaaleaacaWGTbaabeaaaaa@5021@

Δ H 298 θ = 298 Tad ΔCpdT MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeyOeI0IaeuiLdqKaamisamaaDaaaleaacaaIYaGaaGyoaiaaiIdaaeaacqaH4oqCaaGccqGH9aqpdaWdXaqaaiabfs5aejaadoeacaWGWbGaamizaiaadsfaaSqaaiaaikdacaaI5aGaaGioaaqaaiaadsfacaWGHbGaamizaaqdcqGHRiI8aaaa@4A3D@ (5)

It can be calculated approximately with the following equation:

Cp=a+b× 10 3 ×T+c× 10 5 T 2 +d× 10 6 T 2 MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4qaiaadchacqGH9aqpcaWGHbGaey4kaSIaamOyaiabgEna0kaaigdacaaIWaWaaWbaaSqabeaacqGHsislcaaIZaaaaOGaey41aqRaamivaiabgUcaRiaadogacqGHxdaTcaaIXaGaaGimamaaCaaaleqabaGaaGynaaaakiaadsfadaahaaWcbeqaaiabgkHiTiaaikdaaaGccqGHRaWkcaWGKbGaey41aqRaaGymaiaaicdadaahaaWcbeqaaiabgkHiTiaaiAdaaaGccaWGubWaaWbaaSqabeaacaaIYaaaaaaa@55C3@ (6)

Calculation of gibbs free energy

The Gibbs free energy change ∆G is a criterion for determining whether a chemical can proceed spontaneously under constant temperature and pressure conditions [31]. The Gibbs free energy in the standard state can roughly reflect the possibility of a reaction or reaction trend. If ∆Gθ<0 in the system, the reaction process is irreversible and proceeds spontaneously. If it is ∆Gθ=0, the reaction process is reversible and spontaneous. And if it is ∆Gθ>0, the reaction cannot proceed spontaneously.

The self-propagating reaction system can be expressed as equation 7 as:

V 1 B 1 + V 2 B 2 +... V j B j +... MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOvamaaBaaaleaacaaIXaaabeaakiaadkeadaWgaaWcbaGaaGymaaqabaGccqGHRaWkcaWGwbWaaSbaaSqaaiaaikdaaeqaaOGaamOqamaaBaaaleaacaaIYaaabeaakiabgUcaRiaac6cacaGGUaGaaiOlaiabgkziUkaadAfadaWgaaWcbaGaamOAaaqabaGccaWGcbWaaSbaaSqaaiaadQgaaeqaaOGaey4kaSIaaiOlaiaac6cacaGGUaaaaa@49A7@ (7)

In equation (7), is the measurement coefficient of the element or compound.

The calculation equation for the change of its standard free energy is:

Δ G θ = v i G i T MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeuiLdqKaam4ramaaCaaaleqabaGaeqiUdehaaOGaeyypa0ZaaabqaeaacaWG2bWaaSbaaSqaaiaadMgaaeqaaOGaam4ramaaBaaaleaacaWGPbaabeaakiaadsfaaSqabeqaniabggHiLdaaaa@4213@ (8)

In the equation (8), , is the free energy of the element or compound B at temperature .

In the Al2O3-B2O3-Mg system, the following chemical reactions generally occur:

Al 2 O 3 +3Mg2Al+3MgO MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeyqaiaabYgadaWgaaWcbaGaaeOmaaqabaGccaqGpbWaaSbaaSqaaiaabodaaeqaaOGaae4kaiaabodacaqGnbGaae4zaiabgkziUkaabkdacaqGbbGaaeiBaiaabUcacaqGZaGaaeytaiaabEgacaqGpbaaaa@45B1@ (9)

B 2 O 3 +3Mg2B+3MgO MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeOqamaaBaaaleaacaqGYaaabeaakiaab+eadaWgaaWcbaGaae4maaqabaGccaqGRaGaae4maiaab2eacaqGNbGaeyOKH4QaaeOmaiaabkeacaqGRaGaae4maiaab2eacaqGNbGaae4taaaa@43D5@ (10)

Al+12B AlB 12 MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeyqaiaabYgacaqGRaGaaeymaiaabkdacaqGcbGaeyOKH4QaaeyqaiaabYgacaqGcbWaaSbaaSqaaiaabgdacaqGYaaabeaaaaa@407B@ (11)

Al 2 O 3 +12B 2 O 3 +39Mg 2AlB 12 +39MgO MathType@MTEF@5@5@+=feaaguart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeyqaiaabYgadaWgaaWcbaGaaeOmaaqabaGccaqGpbWaaSbaaSqaaiaabodaaeqaaOGaae4kaiaabgdacaqGYaGaaeOqamaaBaaaleaacaqGYaaabeaakiaab+eadaWgaaWcbaGaae4maaqabaGccaqGRaGaae4maiaabMdacaqGnbGaae4zaiabgkziUkaabkdacaqGbbGaaeiBaiaabkeadaWgaaWcbaGaaeymaiaabkdaaeqaaOGaae4kaiaabodacaqG5aGaaeytaiaabEgacaqGpbaaaa@4F12@ (12)

Table 1 shows the free energy changes. A more systematic study of the thermodynamics of related reaction systems, prediction of the phases that may exist and appear in the reactants and products from the perspective of thermodynamics, provides a theoretical basis for the regulation of the self-propagating high-temperature synthesis process.

Result of calculation

The adiabatic temperature was calculated using HSC6.0 software, and the adiabatic temperature of the reactions is 2789.5 K. Previous studies have shown that the reaction temperature of self-propagating preparation of AlB12 exceeds 2300°C (2573 K). This tested result matches the calculation result. Since=2789.5 K>1800K, self-propagation can proceed smoothly. Note that the reaction always has ∆Gθ<0 in Table 1, so the reaction can proceed spontaneously. Such calculation results can indicate that it is possible to prepare AlB12 by self-propagating reaction with Al2O3, B2O3, and Mg as raw materials, and the reaction temperature can support the completion of the propagation reaction.

Summary

The calculation results of preparing AlB12 using Mg, Al2O3 and B2O3 as the raw materials shows that the adiabatic temperature of the system is 2789.5K, which meets the self-propagating reaction conditions. The calculated results are consistent with the actual test results. The Standard Gibbs free energy of the reaction formula is less than zero, which also proves the possibility of self-propagating reactions.

This work was supported by Fundamental scientific research business expenses of central universities (award # N10060200).

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© 2020 Wang C, et al. This is an open-ampcess article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
 

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