Physical Chemistry

2012;  2(4): 43-47

doi: 10.5923/j.pc.20120204.01

C = C’ – r, A Silver Bullet for Evaluation of Components in Simple Equilibrium Reactions: The Relation Revisited

R. Sanjeev 1, V. Jagannadham 2, R. Veda Vrath 3

1Department of Chemistry, Mizan-Teppi University, Teppi Campus, Teppi, Ethiopia

2Department of Chemistry, Osmania University, Hyderabad-500007, India

3Department of Chemistry, L N Gupta Evening College, Hyderabad-500002, India

Correspondence to: R. Sanjeev , Department of Chemistry, Mizan-Teppi University, Teppi Campus, Teppi, Ethiopia.

Email:

Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.

Abstract

Phase rule is an integral part of the undergraduate curriculum in many universities across the globe. In an appreciable number of universities, it is dealt with in the freshman year. The students find it extremely confusing to find the number of components even in simple equilibrium reactions. Normally they end up giving wrong answers, or if at all they give correct answers, they are just conjectures. To overcome this overwhelming confusion we have first considered different simple and relatively uncomplicated equilibriums from standard physical chemistry books and research journals. In these different equilibriums first we evaluated the number of components as illustrated in the books. In each of the book, dissimilar methods were employed to evaluate the number of components which is not a straightforward task for the freshmen students. Then we presented an easy generic method which involved the use of the less involving relation C = C’ – r. Our endeavour in this article is to present a terse and lucid method, by means of which the number of components can be evaluated. Finally, one feels, after going through this article, that this convenient and handy relation C = C’ – r is undeniably a silver bullet for the evaluation of components in simple and relatively less complicated equilibriums.

Keywords: Phase, Components, Restrictions, Constituents, Phase Rule

1. Introduction

It has been found that one of the most difficult areas in physical chemistry at freshmen level is the phase rule, which requires large amount of imagination on the part of the students when it comes to evaluation of the number of components, one of the vital terms in phase rule. Even though there are easy formulae to overcome this requirement, the students are not made aware of. One such formula is C = C’ – r for the evaluation of number of components C. Here C’ is the total number of number of chemical constituents in the system, and r is the number of restrictions imposed on the independent variation of these constituents. In this article, we have shown how the use of the relation C = C’ – r is far more superior to the other methods when it comes to the ease of evaluation of number of components.

2. Objective

As described in the title the very purpose of writing this article is to revisit the relation C = C’ – r. This generic andhandy relation enables easy evaluation of components in various equilibriums, especially for freshmen students. Even in the case where large amount of imagination is required to evaluate the components, the relation C = C’ – r comes to aid.

3. Method

Since this article involves the use of the handy relation C = C’ - r, the method is less involving. The evaluation of components of various equilibriums from standard physical chemistry text books and research journals are examined. Finally the easy evaluation of the components using the handy relation is presented and verified.

4. Discussion

Most of the textbooks give the example of decomposition of calcium carbonate reaction to illustrate the evaluation of number of components in an equilibrium reaction (and so does Glasstone1).
(1)
It might appear, at the first sight, that there are three components, viz., CaCO3, CaO and CO2, but it is evident that these substances are not independent, as required by the definition of the component; thus CaCO3 is really equivalent to CaO + CO2. The two components may consequently be taken as CaO and CO2, so that the composition of calcium carbonate can be represented as xCaO + xCO2, that of the calcium oxide as yCaO + 0CO2, while that of carbon dioxide gas phase is 0CaO + zCO2. The two components might equally have been chosen as CaCO3 and CaO, when the composition of the gas phase would be given by zCaCO3 - zCaO. The actual nature of the components is not important; it is their number that is significant, and this should always be the same for a given system if the components are chosen properly.
We shall now consider other examples. Let us take the example when ethanol2 and acetic acid are mixed. At the first sight, we might predict two components because there are two constituents viz. HOAc and EtOH. However these constituents react to give ethyl acetate and water. Therefore ethyl acetate and water are also present at equilibrium together with the reactants. This raises the number of components from 2 to 4.
(2)
But because of equilibrium condition and since at equilibrium [EtOAc] = [HOH], the number of components is reduced back to 2.
If we consider the example of decomposition of pure PCl5 ref.2,
(3)
Three chemical species are apparent but the number of components is reduced to one. This is because ofequilibrium condition and the relation [PCl3] = [Cl2].
The solution of acetic acid3 in water is also a case in point
(4)
There are many chemical species; clearly, however, the presence of two species can imply the presence of other species determined by the equilibrium relations that exist.
Avoiding the strict attention to the possible equilibriums among the species of the system, the consideration of the example, (gaseous system of water vapor, hydrogen and oxygen) will yield meaningful inference. In the presence of electric arc or suitable catalyst, the equilibrium can be described as
(5)
This system has two components. It can be seen that if the concentration of any two species is arbitrarily set, the concentration of third is fixed and can be calculated from equilibrium constant.
In the thermal decomposition of ammonium chloride, there are three chemical species. NH3 and HCl are formed in fixed stoichiometric proportions by the reaction.
(6)
And therefore, the composition of both phases can be expressed in terms of a single species NH4Cl suggesting that there is only one component in the system.
The decomposition of magnesium carbonate can be described by equation 7.
(7)
There are three constituents but the number ofcomponents is two. The explanation for this is same as that for decomposition of calcium carbonate (as already explained).
The solvolysis of benzyl-gem-dichloride4,5 is depicted in scheme 1 (for X – Cl).
Scheme 1. Depicting the solvolysis of benzyl-gem-dichloride
In our earlier study5,6,7,8 wherein we had sought insight into the mechanism of this reaction by testing the conformity of the data to the Hammett’s equation, the first equilibrium step and the subsequent step, were considered separately. It would be instructive to treat the equilibrium separately. In this simple solvolysis reaction, the solvolysis step involves a simple equilibrium. The equilibrium constant can be written as Keq =[α-chloro-carbocaton]/[benzyl-gem-dichloride]. From the knowledge of Keq and the concentration of any one of the speciesα-chloro-carbocation or benzyl-gem-dichloride the concentration of other can be obtained. Thus the number of components is one. In a similar manner, in the equilibrium of solvolysis of benzyl-gem-dibromide6 and benzyl-gem-diazide7, the number of components obtained would be one.
In the above simple ten equilibriums, the manner in which the components are evaluated is not the same for all the systems. This places a heavy toll on the grey cells of the freshman teenagers.

5. Conclusions and Results

The system is discussed and concluded as correct when the result obtained from C = C’ – r is the same as we imagined.
In the forgoing examples for the illustration of evaluation of components, uniformity in the explanation is not maintained. Therefore a general expression for evaluation of components would be of much benefit, both to the teacher and taught. The number of components in a system can be determined in the following general manner1.
Let C’ be the number of chemical constituents in the system, and let r be the number of restrictions imposed on the independent variation of these constituents. The number of components C is given by the equation:
(8)
For instance, let us apply the relation 8 to reaction 1. Here C’ = 3 and r = 1 i.e. the equilibrium condition restricts the independent variation of the constituents. Hence C = 2.
In reaction 2, C’ = 4 and r = 2 i.e. equilibrium and the relation [EtOAc] = [HOH] restrict the independent variation of the constituents. Hence C i.e. number of components is 2.
In reaction 3, C’ = 3 and r =2 i.e. the equilibrium condition and the relation [PCl3] = [Cl2] restrict the independent variation of the constituents. Therefore C = 1.
In reaction 4, C’ = 4 and r =2 i.e. the equilibrium condition and the relation [CH3COO-] = [H3O+] restrict the independent variation of the constituents. Hence C = 2.
In reaction 5, C’ = 3 and r =1 i.e. the equilibrium condition restricts the independent variation of the constituents. Hence C = 2.
In reaction 6, C’ = 3 and r = 2 i.e. the equilibrium condition and the relation [NH3] = [HCl] restrict the independent variation of the constituents. Hence C = 1.
In reaction 7, C’ = 3 and r =1 i.e. the equilibrium condition restricts the independent variation of theconstituents. Hence C = 2.
In the equilibrium of solvolysis of benzyl-gem-dichloride, C’ is 2 but the equilibrium restricts their independent variation i.e. r = 1. Hence C = 2 – 1 =1. Analogously in the solvolysis of benzyl-gem-dibromide andbenzyl-gem-diazide the components can be obtained as 1 by applying our simple relation C = C’ – r.
Let us see a system that is a little more complex where in AlCl3 is dissolved in water9, noting that hydrolysis and precipitation of Al(OH)3 occur, giving various ions. Al3+, H+, AlCl3, Al(OH)3, OH-, Cl-, H2O are the seven species present in this system. There are also three equilibriums:
And one condition of electrical neutrality
Hence for this system, C’ = 7 and r = 4 i.e. the three equilibriums and the condition of electrical neutrality restrict the independent variation of the constituents. Hence C = 7 – (3+1) = 3.
Let us take a similar but a little more complex example9 where in one finds the number the components of (a) Na2HPO4 in water at equilibrium with water vapour but disregarding the fact the salt is ionized. (b) The same but taking into account the ionization of the salt (disregarding the water vapour). In the former case (a) total numbers of constituents (C’) are three, namely, salt, water and water vapour, there is an equilibrium condition (restriction) between liquid water and its vapour. Hence the total number of components are C = 3 – 1 = 2; In the latter case (b) there are seven (C’) species: Na+, H+, H2PO4-, HPO42-, PO43-, H2O and OH-. There also exist three equilibriums (disregarding the water vapour), namely
Further there are also two conditions of neutrality, namely
[Na+] = [phosphates] and [H+] = [OH-] + [phosphates] where [phosphates] = [H2PO4-] + 2[HPO42-] + 3[PO43-]
Hence the total numbers of restrictions are the three equilibriums, and the two conditions of neutrality i.e., they restrict the independent variation. Thus the total number of components (C) are C = 7 – (3 + 2) = 2.
The comprehension of the important term restriction is better understood if one studies the derivations of phase rule. The derivation of phase rule10 was first put forth by J. Willard Gibbs in 1878. Unfortunately it was published in a rather obscure journal Transactions of the Connecticut Academy of Arts and Sciences11 and was overlooked for 20 years. The derivation of phase rule like any other derivations has essential concepts and assumptions embedded in it. It is here the teaching acumen of the instructor is wanting, and it is for the teacher to discern and accentuate the number of intensive variables fixed by free energy equilibrium relations. Let us recapitulate the phase rule obtained by J. Willard Gibbs.
Consider the C components to be distributed throughout each of the P phases of a system as schematically indicated in Figure 1.
To get the total number degrees of freedom one has to first add the total number of intensive variables required to describe separately each phase and then subtracting the number of intensive variables, whose values are fixed by free-energy equilibrium relations between different phases. To begin, each component is assumed to be present in every phase.
Figure 1. Depicting ‘C’ components distributed throughout each of the ‘P’ phases
In each phase (C -1) quantities will be required to define the composition of the phase quantitatively. Thus, if mole fractions are used to measure the concentrations, one needs to specify the mole fraction of all but one of the components, the remaining one being determined because the sum of the mole fractions must be unity. Since there are P phases, there will be total of P (C – 1) such composition variables. In addition, the pressure and the temperature must be specified, giving a total of P (C -1) + 2 intensive variables if the system is considered phase by phase.
The number of these variables, which are fixed by the equilibrium conditions of the system, must now be determined. Component 1, for example, is distributed between phases P1 and P2. When equilibrium is established for any one component distributed between any two phases, a distribution relation12 can be written. Thus, if the concentration of a component in phase P1 is specified, its concentration in phase P2 is automatically fixed. Similar equilibriums are set up for each component between the various pairs of phases. For each component there are (P -1) such relations. Thus, for C components a total of C (P -1) intensive variables are fixed by equilibrium conditions.
The number of degrees of freedom, i.e., net adjustable intensive variables, is therefore
In this derivation of phase rule C (P – 1) as already described, is the number of intensive variables, whose values are fixed by free energy equilibrium relations. Teachers should try to emphasize this aspect and try to be as lucid as possible. This would enable the students to comprehend the extremely important term ‘r’ that is the restriction13 imposed on the independent variation of the constituents. Once the students comprehend this, the evaluation of components would be a blithesome experience.
One million dollar perplexing query, the students raise, is that in the decomposition of CaCO3, why isn’t [CaO] = [CO2] although it is analogous to [CH3COO-] = [H3O+] for reaction 4 or [EtOAc] = [HOH] for reaction 2 or [PCl3] = [Cl2] for reaction 3. The thermodynamic property, intensive variable, answers this query. The “concentration” of a solid, like its density, is an intensive property and therefore does not depend on how much of the substance is present. For example, the “molar concentration” of copper14 (density: 8.96g/cm3) at 20oC is the same, whether we have 1 gram or 1 ton of the metal:
[Cu] = 8.96g/1 cm3 x 1 mol/63.55g = 0.141 mol/cm3 = 141 mol/L
For this reason, the concentration of solid [CaO] is constant, and thus has nothing to do with concentration of [CO2]. And since [CaO] is not equal to [CO2], the number of restrictions is reduced to one in this case. The same reasoning can be extrapolated for decomposition of MgCO3, where [MgO] is not equal to [CO2].
Atkins15 has a self-test problem, which is, “How many components does autoprotolysis of water has?” and the answer given is one. Let us solve this problem as follows:
Pure liquid water has concentration of 55.5M (density = 1g/cc and calculations analogous to concentration of solids, as already explained in the foregoing paragraph), and since negligible concentrations of products are formed, the concentration of water can be taken as constant. The equilibrium expression for this process is Kw = [H3O+][OH-]. Therefore if concentration of H3O+ is known, the concentration of OH- is set. Analogously, if the concentration of OH- is known, the concentration of H3O+ is set. Hence auto-protolysis is one component system. Thus this example is underpinning the reasoning; put forth in the foregoing paragraph regarding concentration of solids (it is equally applicable for pure liquids).
If we apply our generic formula, then C’ is 4 and r is 3 i.e. the equilibrium condition, the relation [H3O+] = [OH-] and the relation [H2O] = [H2O]. Therefore C = 4 - 3 i.e. 1.
Thus this simple relation of C = C’ - r is a silver-bullet for freshman students to evaluate the number of components (for simple equilibrium reactions) when learning the phase rule.

References

[1]  S. Glasstone and D. Lewis, Elements of Physical Chemistry, Second Edition, Published in India by Macmillan Company of India Limited. ISBN 0 333 90291 2, pp 349, Indian edition, 2002.
[2]  Keith J. Laidler and John H. Meiser, Physical Chemistry, Second Edition CBS Publishers and distributers, New Delhi, this edition has been published in India by arrangement with Houghton Miffin Company USA CBS ISBN 81-239-0645-5 Houghton ISBN 0-395-64153-5, pp 222, Indian edition, Reprint 2006..
[3]  Gordon M. Barrrow, Physical Chemistry by 5th Edition, Tata Mc Graw Hill edition 1992, , ISBN 0-07-462031-2, pp394, Indian edition, 6th reprint 2005.
[4]  Sanjeev R and Jagannadham V, Lifetimes of α-halo and α-azidobenzyl carbocations in aqueous solution, Proc. Indian Acad. Sci (Chem Sci.), Vol.114, No. 1, pp-47-54, February 2002;.
[5]  Sanjeev R and Jagannadham V, Substituent effects on the spontaneous cleavage of benzyl-gem-dichloride in aqueous solution, Indian Journal of Chemistry; Vol. 41B, pp-2145-2149, October 2002.
[6]  Sanjeev R and Jagannadham V, Substituent effect on the spontaneous cleavage of benzyl-gem-dibromide in aqueous solution, Indian Journal of Chemistry; Vol 41A, pp 1841 -1844 September 2002.
[7]  Richard, J. P., Tina, L. Amyes, Jaganndham. V., Yong-Gu Lee and Doughlas J. Rice, Spontaneous cleavage of gem-diazides: A comparison of Effects of α-aido and other electron-donating groups on Kinetic and Thermodynamic stability of benzyl and alkyl carbocations in aqueous solution, J. Am. Chem. Soc., 117, pp-5198-5205. 1995.
[8]  Sanjeev, R and Jaganndham V, A simple explanation from the sign of rho value for the kind of charge that develops in the intermediate or the transition state of the reactions series: A one hour physical-organic chemistry graduate classroom lecture, Khimaya, pp-71-77, Vol. 21, No:1, 2012.
[9]  Peter Atkins and Julio de Paula, Physical Chemistry 7th edition, Oxford University Press, ISBN 0-19-879285-9; 0-19-925579-2 (EPZ), pp 216, U.K.,2002.
[10]  Gordon M. Barrrow, Physical Chemistry 5th Edition, Tata McGraw Hill edition 1992, ISBN 0-07-462031-2, pp 397, Indian edition, sixth reprint 2005.
[11]  J. W. Gibbs, "On the Equilibrium of Heterogeneous Substances," Transactions of the Connecticut Academy of Arts and Sciences, 3, 108-248, 343-524, USA, 1878.
[12]  Patrick. J. Sinko, Martin's, Physical Pharmacy & Pharmaceutical Sciences, 5th edition, Lippincot Williams & Wilkins, Wolters Kluwer Business, , ISBN 0-7817-6426-2, USA, 2005
[13]  Sanjeev, R., Jagannadham, V, & Veda Vrath R, The term, “Restriction” in phase rule rendered more intelligible: One hour lecture for freshman students. Paper submitted to Resonance journal of Science Education, India, 2012.
[14]  Raymond Chang, Chemistry, Ninth Edition, Tata Mc Graw Hill ISBN -13: 978-0-07-064819-7, ISBN – 10: 0-07-064819-0, pp 610, Special Indian Edition, 2008.
[15]  Peter Atkins and Julio de Paula, Physical Chemistry,7th edition, Oxford University Press; ISBN 0-19-879285-9; 0-19-925579-2 (EPZ), pp 195,U.K.,2002.