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International Journal of
eISSN: 2475-5559

Petrochemical Science & Engineering

Short Communication Volume 4 Issue 2

Catalytic hydrogenation of carbon dioxide for the production of methanol in a catalytic membrane reactor of fixed bed

Kaio Cesar Gomes da Silva, Mario Rocha Cavalcanti, Jornandes Dias Silva

Polytechnic School - UPE, Laboratory of Environmental and Energetic Technology, Brazil

Correspondence: Jornandes Dias Silva, Polytechnic School - UPE, Laboratory of Environmental and Energetic Technology, Rua Benfica - 455, Madalena, Recife – PE, Brazil, Tel +50750-470

Received: January 27, 2017 | Published: April 4, 2019

Citation: Silva KCG, Cavalcanti MR, Silva JD. Catalytic hydrogenation of carbon dioxide for the production of methanol in a catalytic membrane reactor of fixed bed. Int J Petrochem Sci Eng. 2019;4(2):54-55. DOI: 10.15406/ipcse.2019.04.00103

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Introduction

It is known that fossil fuels pertain to hydrocarbons. Therefore, when they are burned for the purpose of getting heat and power, water and carbon dioxide (CO2) are generated and liberated to the atmosphere. Global warming is largely attributed to an increase in the atmospheric level of greenhouse gases. CO2 is considered as the most important greenhouse gas with the largest impact on climate change. Several preoccupations have been raised with respect to the impact in increasing concentrations of CO2 in the atmosphere to the environment.1 Catalytic hydrogenation of carbon dioxide (CHCD) in a catalytic membrane reactor of fixed bed is one of most important chemical processes for the production of methanol.2,3

Mathematical modelling

A schematic diagram of the membrane reactor (MR) is proposed in the present paper to carry out the CHCD. The MR consists of two concentric tubes, as shown in Figure 1. The proposed mathematical model was described by a partial differential equation system and it is restricted to the following assumptions:

  1. Isothermal system;
  2. All flow rates are constant throughout the reactor;
  3. The intraparticle diffusion resistance was not considered;
  4. Radial concentration gradient was considered. Based on the above assumptions, mass balance equations in the reaction zones could be written as follows.

Figure 1 Scheme of the MR for the production of methanol.

Model of the shell side zone

The mass balance of chemical species i in the shell side is given as follows.

4 Q g π d shell 2 C i z =ε D e,r 1 r r ( r C i r )+ ρ b i=1 5 j=1 3 η j σ ij R j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaSaaaeaaca aI0aGaaGPaVlaadgfadaWgaaWcbaGaam4zaaqabaaakeaacqaHapaC caaMc8UaamizamaaDaaaleaacaWGZbGaamiAaiaadwgacaWGSbGaam iBaaqaaiaaikdaaaaaaOWaaSaaaeaacqGHciITcaWGdbWaaSbaaSqa aiaadMgaaeqaaaGcbaGaeyOaIyRaamOEaaaacaaMc8Uaeyypa0JaaG PaVlabew7aLjaaykW7caWGebWaaSbaaSqaaiaadwgacaGGSaGaaGPa VlaadkhaaeqaaOWaaSaaaeaacaaIXaaabaGaamOCaaaacaaMc8+aaS aaaeaacqGHciITaeaacqGHciITcaWGYbaaamaabmaabaGaamOCamaa laaabaGaeyOaIyRaam4qamaaBaaaleaacaWGPbaabeaaaOqaaiabgk Gi2kaadkhaaaaacaGLOaGaayzkaaGaaGPaVlabgUcaRiabeg8aYnaa BaaaleaacaWGIbaabeaakmaaqahabaWaaabCaeaacqaH3oaAdaWgaa WcbaGaamOAaaqabaGccqaHdpWCdaWgaaWcbaGaamyAaiaadQgaaeqa aOGaaGPaVlaadkfadaWgaaWcbaGaamOAaaqabaaabaGaamOAaiaayk W7caaMc8Uaeyypa0JaaGPaVlaaykW7caaIXaaabaGaaG4maaqdcqGH ris5aaWcbaGaamyAaiaaykW7cqGH9aqpcaaMc8UaaGymaaqaaiaaiw daa0GaeyyeIuoaaaa@89AF@    (1)

Where, i = CH4, H2O, H2, CO, CO2

Model in the reaction zone of methanol

The mass balance of chemical species i in the reaction zone of methanol is given as follows.

4 Q g π d reac.Zone 2 C i z =ε D e,r 1 r r ( r C i r )+ ρ b i=1 5 j=1 3 η j σ ij R j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbdfwBIj xAHbstHrhAaeXatLxBI9gBaerbd9wDYLwzYbItLDharuavP1wzZbIt LDhis9wBH5garqqtubsr4rNCHbGeaGqkY=Mj0xXdbba91rFfpec8Ee eu0xXdbba9frFj0=OqFfea0dXdd9vqaq=JfrVkFHe9pgea0dXdar=J b9hs0dXdbPYxe9vr0=vr0=vqpWqaaeaabiGaciaacaqabeaadaabau aaaOqaamaalaaabaGaaGinaiaaykW7caWGrbWaaSbaaSqaaiaadEga aeqaaaGcbaGaeqiWdaNaaGPaVlaadsgadaqhaaWcbaGaamOCaiaadw gacaWGHbGaam4yaiaac6cacaWGAbGaam4Baiaad6gacaWGLbaabaGa aGOmaaaaaaGcdaWcaaqaaiabgkGi2kaadoeadaWgaaWcbaGaamyAaa qabaaakeaacqGHciITcaWG6baaaiaaykW7cqGH9aqpcaaMc8UaeqyT duMaaGPaVlaadseadaWgaaWcbaGaamyzaiaacYcacaaMc8UaamOCaa qabaGcdaWcaaqaaiaaigdaaeaacaWGYbaaaiaaykW7daWcaaqaaiab gkGi2cqaaiabgkGi2kaadkhaaaWaaeWaaeaacaWGYbWaaSaaaeaacq GHciITcaWGdbWaaSbaaSqaaiaadMgaaeqaaaGcbaGaeyOaIyRaamOC aaaaaiaawIcacaGLPaaacaaMc8Uaey4kaSIaeqyWdi3aaSbaaSqaai aadkgaaeqaaOWaaabCaeaadaaeWbqaaiabeE7aOnaaBaaaleaacaWG Qbaabeaakiabeo8aZnaaBaaaleaacaWGPbGaamOAaaqabaGccaaMc8 UaamOuamaaBaaaleaacaWGQbaabeaaaeaacaWGQbGaaGPaVlaaykW7 cqGH9aqpcaaMc8UaaGPaVlaaigdaaeaacaaIZaaaniabggHiLdaale aacaWGPbGaaGPaVlabg2da9iaaykW7caaIXaaabaGaaGynaaqdcqGH ris5aaaa@929B@    (2)

Where, i = H2, CO, CO2, CH3OH, H2O

Results and discussion

The mathematical model was developed to analyze the behaviour of chemical species i (i = CH4, H2O, H2, CO, CO2) in the shell side of MR. Numerical experiments were performed using a computational code which was developed for catalytic hydrogenation of carbon dioxide. Figure 2 shows the predicted product distribution (concentrations i components) in wet basis (water vapour included in the product). It is noted that as the operation proceeds, methane is consumed by steam reforming reaction with water available in inlet gas mixture. Based on results from the mathematical modelling after that all curves describing the concentrations reach to stable levels, the following definition of the yield of methanol is used for describing the MR performance as follows:

Y MeOH = C MeOH C C H 4 in MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbdfwBIj xAHbstHrhAaeXatLxBI9gBaerbd9wDYLwzYbItLDharuavP1wzZbIt LDhis9wBH5garqqtubsr4rNCHbGeaGqkY=Mj0xXdbba91rFfpec8Ee eu0xXdbba9frFj0=OqFfea0dXdd9vqaq=JfrVkFHe9pgea0dXdar=J b9hs0dXdbPYxe9vr0=vr0=vqpWqaaeaabiGaciaacaqabeaadaabau aaaOqaaiaadMfadaWgaaWcbaGaamytaiaadwgacaWGpbGaamisaaqa baGccqGH9aqpcaaMc8UaaGPaVpaalaaabaGaam4qamaaBaaaleaaca WGnbGaamyzaiaad+eacaWGibaabeaaaOqaaiaadoeadaqhaaWcbaGa am4qaiaadIeadaWgaaadbaGaaGinaaqabaaaleaacaWGPbGaamOBaa aaaaaaaa@4DDB@    (3)

Figure 2 The concentrations profiles of i chemical species in the MR.

Figure 3 reports the effect of the operating temperature on the conversion of methane at reaction pressure (950kPa). As can be seen, the yield of methanol reaches to stable levels at operating temperatures from 200°C to 300°C, respectively.

Figure 3 Yield of methanol versus reactor length.

Conclusion

A two-dimensional mathematical model along with a kinetic model was used to report predictions in the MR reactor. It can seen that the yield of methanol increase with increasing reaction temperature on the catalytic performance of Cu/ZrO2 catalysts.

Acknowledgements

None.

Conflicts of interest

The author declares that there are no conflicts of interest.

References

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©2019 Silva, et al. This is an open access article distributed under the terms of the, which permits unrestricted use, distribution, and build upon your work non-commercially.