|
Integrated Approach to a Basic Understanding of
Chemical Reactivity and Reaction Order with Illustrated Applications to
Selected General Chemistry Problems
|
|
|
Kenneth M.
Maloney
Chemistry and Physics Division,
Baton Rouge Community College, 201 Community College Drive, LA 70806
|
|
The complete
formulations of three(3) new problems, in general chemistry, are
illustrated with the selective applications of the significant and basic
equation or learning tool{i.e., WF = tp•exp[p(1 -
t)]}
to three distinctly different experimental systems. For each one of the reaction systems,
formulation of the respective reduced dependent variable WF(proportion
reacted) and the corresponding reduced independent variable t(i.e.,
reduced time, etc.) are instructive.
Importantly, for a given reaction system, the geometry factor, p,
offers an expanded perspective from which a system, or integrated
comprehension of reaction order and the conservation laws, can be
visualized and appreciated by the student.
Significantly, a student’s three - part question, catalyzed a
substantial enrichment of an important basic general chemistry course. Additionally, presented, herein, are
enlightening aspects of what also transpired, as a result of questions
which were posed by students, in a series of various learning scenarios,
where listening vs hearing and critical thinking were integral components
of the learning environment.
|
|
Introduction
Two of the best methods to foster
and enhance critical thinking skills, in general chemistry, are open
inquiry experiments and the practice of solving challenging problems. Occasionally, the process of solving a
well formulated chemistry problem can clear up a great deal of misconceptions. This is especially true when simple
pictures, images, and analogies, familiar to the students, are
constructively used in the explanations.
It is also particularly effective when the learning occasion allows
a return to basic considerations which enable seemingly unrelated topics to
be seamlessly interwoven into clearly defined patterns (1 - 4). Stoichiometry and the law of the
conservation of mass present such an opportunity.
Generally,
the law of the conservation of mass is broadly familiar to most
individuals. Of course, it is only
one of the basic conservation laws considered to be the most fundamental
laws in nature. In general
chemistry, the area of study in which the mass quantities of reactants and
products are calculated, conserved, and balanced is broadly called
stoichiometry. An essential part of
a basic knowledge of general chemistry begins with a fundamental
understanding of stoichiometry.
Previously,
the results of an open inquiry experiment were reported (1). This article is an example of the
synergistic effects of solving a general chemistry problem where the
questions of a student required the thoughtful integration of stoichiometry
and some of the conventional perceptions with regards to the law of the
conservation of mass.
The Answers to a Curious
Student’s Questions
Part one. During the process of administering an
examination, in a first course of basic general chemistry, a student asked
a question about some apparent difficulties encountered when attempting to
balance the chemical reactions presented as integral parts of a particular
problem on the examination. Because
the stoichiometry, in the problem, was particularly uncomplicated, it was
even more important to carefully listen to the essence of the question
being asked rather than, at the moment, simply hearing the particular
vocabulary employed by the student.
The problem, in question, involved stoichiometry as
follows;
Problem Statement:
A sample containing only CaCO3 and MgCO3 is
ignited and the following reaction occurs:
|
|
CaCO3(s) ® CaO(s) + CO2(g)
|
|
|
|
MgCO3(s) ® MgO(s) +
CO2(g)
|
|
The ignited sample has half the mass of the
original. What percentage of the
original sample is CaCO3?
As it happened,
a typographical error, in one of the equations, caused the difficulty. After elimination of the error in
question, the examination proceeded uneventfully. Subsequently, in a post-exam review, the
solution to the problem was presented in the following typical manner:
Solution A: Let x
= original mass of CaCO3 and 100-x = the original mass of MgCO3,
then 100 grams = mass of the original mixture(CaCO3 + MgCO3)
and 50 grams = mass of the product mixture(CaO + MgO). Thus,
|
|

|
(1)
|
|
where Mm(CaO) is the molar mass of CaO, Mm(CaCO3)
is the molar mass of CaCO3, Mm(MgO) is the molar mass
of MgO, and Mm(MgCO3) is the molar mass of MgCO3. Substituting the appropriate values gives
|
|
[0.560×x] + [0.478×(100-x)] = 50 grams
|
|
which yields
|
|
x = grams of CaCO3
in a sample size of 100 grams = 26.8 grams
|
|
Thus, CaCO3 is, simply, 26.8% of the original
sample.
Part two. On a separate occasion, this same student
inquired about a generalized approach to similar problems. Interestingly, a generalized approach
surfaced as the course transitioned into discussions of formal aspects of
the quantitative treatment of chemical transport, that is, the conversion
of reactants into new chemical species.
Suppose one has the general reaction
|
|
a×A
+ b×B
+ ... ® Products
|
(2)
|
|
where the coefficients a, b,.. are the numbers of moles
of the respective reactants A, B,.. and A is the limiting reactant. If m represents the total mass of the
original reactants and x is the mass of A remaining unreacted after a
reaction time of t > 0, then
|
|
WF = 1 - W
|
(3)
|
|
where WF is the proportion reacted and the unreacted fraction
is W = x/m. From algebraic division,
we introduce the following expression
|
|
|
1
―—— = 1 – x + x2 – x3
+…. @
1 – x
1 + x
|
for x << 1
|
(4)
|
|
For x = W, eq 4 becomes
|
|
|
1
WF = 1 - W @
―――
1 + W
|
for W << 1
|
(5)
|
|
Since the number of moles of A = x/molar weight(A), eq 5
takes the form
|
|
|
A w1×t
WF = a×
――― = ―――
A0 + A 1 + w2×t
|
for 0 £
W £
1
|
(6)
|
|
where the coefficient of proportionality, a,
restores equality over the complete range of W(= x/m = A/A0)[since
A0 = m/molar weight(A)]. If
an effective reaction rate that also incorporates the reaction rate at
initiation (i.e., at t = 0) is defined as R*, then the initial
concentration A0 = R*×tL where tL
denotes the time required for the reaction to go to completion and t
= t/tL. An overall
reaction rate of R results in A = R×t which defines the
coefficients as w1
= a(R/R*)
and w2
= (R/R*).
Notably, the
Peleg equation(3, 4) for osmotic hydration, is a specialized form of eq
6. It is defined as
|
|
|
t w1×t
WF = a× ———― = ———
btL
+ kwt 1 + w2×t
|
for 0 £
W £
1
|
(7)
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
where tL corresponds to the terminal value of
the time. Thus, the
interrelationship, between the regression correlation coefficients, b
and kw
is simply
|
|
|
a
b
= ——— - kw
WFL
|
|
(8)
|
|
where WFL is the terminal value of the
proportion reacted, w1 = a/b,
and w2
= kw/b. The limits of eq 7 are readily apparent when
the data, for a given reaction, are normalized to the terminal values of WFL
and tL (see Problem 1 below).
Clearly, from eq 6, the coefficients defined by the specialized
application of the Peleg equation are k1 = tL/w1
and k2 = w2×(k1/tL).
|
|
WF = ¡×tp×
exp(- k*×t
)
|
(9)
|
|
where ¡ is the scaling factor, p is the
geometry factor, k*(= p/tL) is the reaction sequence time
constant, tL (= b×tf) is the
value of the characteristic time length for the reaction sequence. Hence, the correlation coefficient, b,
is defined by the differences in the terminal values that result from the
nonlinear regressions of eqs 7 and 9 with identical data sets (i.e., b
= tf /tL).
|
|
WF = 0, t
= 0 at initiation
|
|
and
|
|
WF = 1, t
= 1 at termination
|
|
which gives
|
|
¡
= exp(p)
|
|
Thus, for a fully normalized single reaction sequence,
the proportion reacted is
|
|
WF = exp(p)×tp×exp(-
k×t
)
|
|
or
|
|
WF = tp×exp{p(1
- k×t/p)}
|
|
In essence, the relative magnitudes of k∙t versus
p result in the following limiting conditions for chemical reactivity
|
|
WF @ tp×
exp(p) = ¡∙tp for
k∙t << p
|
(10a)
|
|
|
|
WF = tp for k∙t = p
|
(10b)
|
|
|
|
WF @ tp×
exp(- k×t
) for k∙t >> p
|
(10c)
|
|
Since k* = p/tL, eq 9 becomes
|
|
WF = tp×
exp[p(1 - t)]
|
(11)
|
|
where eqs 7 and 9 combine to yield
|
|
|
w1×t
WF = tp×
exp[p(1 - t)]
= ———
1 + w2×t
|
|
(12)
|
|
Based on the
conventional definition of reaction order(represented as n), the proportion
reacted (1) is
|
|
WF = 1 – {1 - [(1 - n)×t/tC]
}1/(1-n)
|
(13)
|
|
where tC = k-1∙[A]0 (1
- n) and W = {1 - [(1 - n)×t/tC]
}1/(1-n). Of course, the
first order case of n = 1 defines the singularity and eq 13 becomes
|
|
WF = 1 – exp(-k×t)
|
(14)
|
|
where W = exp(-k×t). Significantly, eqs 11 and 13 are distinctly
different analytical relationships which equivalently assess the progress
of chemical reaction sequences.
Nonlinear regression analysis of the continuous functional
relationship between the conventional reaction order, n, and the geometry
factor, p, yields the following quantitative expression
|
|
p = 0.487 ×
tanh(4.316 – [3.550 ×ïnï0.493]) +
0.510
|
(15)
|
|
A graphical representation of eq 15 is illustrated by
Figure 1.
|
|

|
|
Figure 1. A graphical representation of the
p-geometry factor vs n, the conventional order parameter, quantitatively
expressed by eq 15.
|
|
Thus, the singularity, defined by the first order case
for the conventional rate equation, is algebraically reformulated and,
simply, restated as a point in a continuum; namely, the boundary condition
where tL = finite for p = 1(see Appendix).
New Problems with
Solutions
Significantly, the relationships for the proportion reacted, WF,
which followed directly from conservation of mass considerations, provide
an additional analytical approach to the analysis of a given set of
reaction rate data. To illustrate
these properties of WF, two additional general chemistry problems which
necessarily involve sets of reaction rate data that exhibit zero, first,
and second order behavior are systematically examined. The analyses that follow are presented in
the form of problem statements that may be easily incorporated into texts,
homework assignments, or tests in general chemistry.
Problem 1
During an
examination of the sample repository of a space probe recently returned
from the unmanned exploration of a distant asteroid, an unknown compound, AxBy,
composed of the two unknown elements A and B, was recovered. After a series of tests, it was found
that the compound reacted with hydrochloric acid as follows
|
|
AxBy(s) +
z HCl(aq) ® AxByClZ(aq) +
(z/2) H2(g)
|
(I)
|
|
In a statistically representative test, a 327 mg sample
of AxBy was added to a solution of 0.0622 M HCl. The reaction was investigated at
atmospheric pressure (i.e., under constant pressure conditions) and 50.4 °C. The data were collected and are reported
in the following table as
|
|
Table 1. Symbolic Kinetic
Data for the
Hypothetical Chemical
Reaction(II)
|
|
|
Time
(s)
|
[HCl]
(mol/L)
|
H2-Volume
(cc)
|
|
|
0
|
0.0622
|
0.00
|
|
|
50
|
0.0514
|
2.66
|
|
|
100
|
0.0448
|
5.33
|
|
|
150
|
0.0402
|
8.00
|
|
|
200
|
0.0368
|
10.7
|
|
|
250
|
0.0341
|
13.3
|
|
|
300
|
0.0319
|
16.0
|
|
|
350
|
0.0301
|
18.6
|
|
|
400
|
0.0286
|
21.3
|
|
|
450
|
0.0273
|
23.9
|
|
|
500
|
0.0261
|
26.6
|
|
|
550
|
0.0251
|
29.2
|
|
|
600
|
0.0242
|
31.9
|
|
|
650
|
0.0234
|
34.5
|
|
|
700
|
0.0227
|
37.2
|
|
|
750
|
0.0220
|
40.0
|
|
|
|
Based on additional tests and analyses,
it was found that z = 3. From the
data collected in the table, AxBy is the limiting
reactant. Use the data table to
obtain the following: (a) determine
the molar mass of the unknown compound AxBy and the
initial volume of the HCl reactant; (b) determine the order of the reaction
with respect to the individual reactants as well as the overall order of
the reaction; (c) determine the specific rate constant; (d) plot graphs of
the WF vs t
relationships for HCl consumption and H2 production
respectively; (e) plot a graph which illustrates the summary relationships
between the geometry factors kw(eq 7) and p(eq
11) versus n(eq 13). [Density of H2
(15 °C)
= 0.085 kg/m3 = 0.04217 mol/L]
Solution
(a)
The combined gas law, at constant pressure(i.e.,
Charles’ law), is
|
|
V1/T1 = V2/T2
|
(16)
|
|
where
V1 is the gas volume at temperature(in degrees Kelvin) T1
and V2 is the volume at temperature T2. Since density = r = mass/volume = m/V,
eq 16 can also be expressed as
|
|
(r1×T1)
= (r2×T2)
|
(16a)
|
|
(b)
Thus, from eq 16a, the density of H2 gas
produced, in the reaction for constant pressure conditions, is
|
|
r2 = r1×(T1/T2)
|
|
where substitution of the appropriate values yields,
|
|
r2
= (0.04217 mol/L)×(15.0 °C + 273.15 K)/(50.4 °C
+ 273.15 K) = 0.03756 mol/L
|
|
The molar quantity of H2 is
|
|
(0.03756 mol/L)×(40
cc)×(10-3
L/cc) = 0.00150 mol
|
|
Therefore, the molar mass of AxBy is
|
|
(327 mg)×(10-3
g/mg)/(2/3)×(0.00150
mol) = 327 g/mol
|
|
The initial volume of the HCl reactant is determined as follows:
|
|
(initial
concentration)×(initial
volume) = moles reacted + moles unreacted
|
|
The data table and the reaction stoichiometry yield
|
|
(0.0622 M)×V
= 2(0.00150 mol) + (0.0220)×V
|
|
Therefore,
|
|
V = 0.00300
mol/(0.0622 – 0.0220)M = 0.0746 L = 74.6 mL
|
|
(c)
The reciprocal of the square of the HCl
concentration (i.e. [HCl]-2) plotted vs time yields a linear
relationship (Figure 2- Part
A). The volume of H2 plotted
vs time yields a linear relationship (Figure 2-Part B).
|
|
 
|
|
A.
B.
|
|
Figure 2. Part A. Plot of [HCl]-2
against time. Part B. Plot of the
volume of H2 against time.
|
|
The simple third – order rate law, for the disappearance
of HCl, has the form,
|
|
d[HCl/dt = -
k[HCl]3
|
|
which, according to calculus, gives the integrated form
|
|
½ ×
{(1/[HCl]2) – (1/[HCl]0 2)} = kt
|
|
Therefore, the reaction is pseudo - third order in
HCl. Since the reactant AxBy(s)
is a solid, the reaction order is zero with respect to AxBy(s). Hence, overall, the order of the reaction
is third order.
(d)
The specific rate constant k = 1.21 L2
mol-2 sec-1.
(e)
The Figure 3 (Part A) is a graphical illustration
of the proportion reacted(WF) vs reduced time(t) for p = 0.0495
(i.e.,
n = 3) which represents the progress of the reaction system in terms
of the consumption of the acid reactant HCl. Part B, which represents the parallel
production of H2 gas{i.e., corresponds to the consumption …. of
AxBy(s)}, is an illustration of p = 1 (i.e., n =
0). Hence,
|
|
 
|
|
A.
B.
|
|
Figure 3. Part A. represents the proportion
reacted(WF) vs. the reduced time(t) for the consumption of the acid reactant,
HCl.
Part B. represents the corresponding relationship for the
simultaneous production of H2 as indicated by reaction eq(II).
|
|
(f)
Illustrated in figure 4 are the summary
results of a comparative evaluation of the geometry factors kw(eq
7) and p(eq 11) vs n(eq
13).
|
|

|
|
Figure 4. A graphical
illustration of the quantitative relationship between the geometry factors,
kw( )
and p(o), vs n (conventional order parameter) where the
proportion reacted(WF) vs the reduced time(t) relationship is constrained to the normalized
form(i.e., WFL = 1, tL = 1)[see
eq 7].
|
|
Clearly,
the point of intersection at kw = p = n @
0.9 is unique.
|
|
Problem 2
A student
decided to investigate the characteristics of the solid-liquid magnesium hydrochloric
acid single replacement reaction
|
|
Mg(s) + 2
HCl(aq) ® MgCl2(aq) + H2(g)
|
(II)
|
|
The student performed the experiments in a simple
reaction-controlled flow unstirred reactor (RCFUR) (1) (i.e., constant pressure). The system was maintained at a constant
temperature of 32.7 °C and pressure of 1.00
atm. The data are tabulated below.
|
|
Table 2. Data for the Mg(s) + 2 HCl(aq) ®
MgCl2(aq) +
H2(g) … Reaction
|
|
Time
(min)
|
[HCl]
(mol/L)
|
H2-Volume
(cm3)
|
|
0
|
0.0368
|
0.0
|
|
1
|
0.0106
|
1.54
|
|
2
|
0.00618
|
3.09
|
|
3
|
0.00436
|
4.63
|
|
4
|
0.00337
|
6.17
|
|
5
|
0.00275
|
7.72
|
|
6
|
0.00232
|
9.26
|
|
7
|
0.00200
|
10.8
|
|
8
|
0.00178
|
12.3
|
|
9
|
0.00158
|
13.8
|
|
10
|
0.00143
|
15.4
|
|
11
|
0.00130
|
16.9
|
|
12
|
0.00120
|
18.5
|
|
13
|
0.00111
|
20.0
|
|
|
Use the data table to obtain the following: (a) determine the initial volume of the
HCl reactant; (b) calculate the grams of Mg metal initially present; (c)
express the rate law and determine the specific rate constant for this
reaction; (d) calculate the p – geometry factor and construct a graph of
the WF vs t
relationship for the HCl reactant consumption sequence.
Solution
(a)
The density of H2 gas produced, in the
reaction for constant pressure conditions(see eq 16 and problem 1), is
|
|
r2
= r1×(T1/T2)
|
|
where substitution of the
appropriate values yields,
|
|
r2
= (0.04217 mol/L)×(15.0 °C + 273.15 K)/(32.7 °C
+ 273.15 K) = 0.03929 mol/L
|
|
The molar quantity of H2
is
|
|
(0.03929 mol/L)×(20
cc)×(10-3
L/cc) = 0.000786 mol
|
|
The initial volume of the HCl
reactant is determined as follows:
|
|
(initial
concentration)×(initial
volume) = moles reacted + moles unreacted
|
|
The data table and the reaction
stoichiometry yield
|
|
(0.0368 M)×V
= 2(0.000786 mol) + (0.00111)×V
|
|
Therefore,
|
|
V = 0.00157
mol/(0.0368 – 0.00111)M = 0.0440 L = 44.0 mL
|
|
(b)
The quantity of Mg metal initially present is
|
|
(0.000786
mol)(24.3 g/mol) = 0.0191 g = 19.1 mg
|
|
(c)
As illustrated in Figure 5, a plot of the
reciprocal of [HCl] vs time yields a straight line relationship
|
|

|
|
Figure 5. Plot of [HCl]-1 against time.
|
|
The second – order rate law,
for the disappearance of HCl, has the form,
|
|
R = -d[HCl]/dt =
k[HCl]2
|
|
Inasmuch as Mg(s) is a solid(i.e.,
zero order-see Problem 1) and the reaction is second order with respect to
[HCl] consumption, the overall order for the reaction is second order. Therefore, the integrated form of the
rate law, gives
|
|
1/[HCl] = k×t
+ 1/[HCl]o
|
|
Regression of the data (Table
2, Figure 5) yields the specific rate constant k = 67.4 L mol-1
min-1.
(d)
Based on eq 15, p = 0.221 for a second order
reaction. Figure 6 is a graph of the
WF vs t
relationship for the HCl
reactant consumption
sequence.
|
|

|
|
Figure 6. A graphical representation of the
proportion reacted(WF) vs. the reduced time(t) for the consumption of the acid reactant,
HCl(see
Figure 5).
|
|
Problem 3
The copious amounts of acid oxides
(i.e., SO2, NO2) released into the atmosphere, by
industrialized countries, results in acid rain. Subsequently, this acid rain does serious
environmental and property damage by reacting with the calcium carbonate
content of Earth, limestone, marble, buildings, monuments, etc. A method for the determination of calcium
carbonate in eggshells was developed by means of a systematic investigation
of the corrosive reaction of CaCO3 with HCl(5):
|
|
CaCO3(s)
+ 2 H+(aq) ® Ca2+(aq) + CO2(g) +
H2O(l)
|
(III)
|
|
The mass of the sample sizes were 0.01 g for sample 1,
0.03 g for sample 2, and 0.05 g for sample 2. All experiments were performed with the
acid in large excess. The reaction vessel
had a gas containment volume of 43.2 mL and the temperature was maintained
at 298.15 K. The data for three
representative experiments are tabulated below.
|
|
Table 3. Data for the …
CaCO3(s) + 2 H+(aq) ®
Ca2+(aq) +
CO2(g) + H2O(l) … Reaction
|
|
|
Time
(min)
|
1.) 0.01 g
CaCO3(s)
|
2.) 0.03 g
CaCO3(s)
|
3.) 0.05 g
CaCO3(s)
|
|
|
CO2
(kPa)
|
CO2
(kPa)
|
CO2
(kPa)
|
|
|
0
|
0.00
|
0.00
|
0.00
|
|
|
1
|
1.68
|
5.05
|
8.42
|
|
|
2
|
2.87
|
8.60
|
14.3
|
|
|
3
|
3.70
|
11.1
|
18.5
|
|
|
4
|
4.29
|
12.9
|
21.4
|
|
|
5
|
|
14.1
|
23.5
|
|
|
6
|
|
15.0
|
25.0
|
|
|
7
|
|
15.6
|
26.0
|
|
|
8
|
|
|
26.7
|
|
|
|
Use the data table to obtain the following: (a) for each reaction sequence(i.e., 1,
2, and 3), calculate the expected final pressure from the mass of CaCO3
initially present; (b) determine the reaction order and express the rate
law for this reaction; (c) determine the specific rate constant for this
reaction; (d) calculate the p – geometry factor of the reaction and
construct a graph of the WF vs t relationship for the
reaction; (e) compare the first order case as a singularity with a single
quadrant of a circle and the golden ratio.
Solution
(a) Based
on the stoichiometry of reaction(III) and assuming ideal gas behavior and
the initial mass CaCO3sample,
of each CaCO3 sample, the
expected final CO2 pressure, from the decomposition of each
original sample, is
|
|
P = [(Grams of CaCO3)/Mm(CaCO3)]×(RT/V)
|
|
where Mm(CaCO3)
is the molar mass of CaCO3, P is the final pressure, V is the
volume, R is the gas constant and T is
the absolute temperature. Hence, the expected final CO2 pressures,
for the reaction sequences, are respectively:
1)
Pressure of CO2 = [0.01 g/(100.01g/mol)]×[(0.08206
L atm K-1mol-1)×(298.15 K)/(0.0432 L)]×(101.3
kPa/atm) =
5.74 kPa
2)
Grams of CaCO3 = [0.03 g/(100.01g/mol)]×[(0.08206
L atm K-1mol-1)×(298.15 K)/(0.0432 L)]×(101.3
kPa/atm) =
17.2 kPa
3)
Grams of CaCO3 = [0.05 g/(100.01g/mol)]×[(0.08206
L atm K-1mol-1)× (298.15 K)/(0.0432
L)]×(101.3
kPa/atm) =
28.7 kPa
(b)
Since the
progress and stoichiometry of reaction(III) requires
|
|
|
d[HCl] dP(CO2)
- ¾¾¾¾
= + ¾¾¾¾
dt dt
|
|
|
Thus, for a given sequence, the
difference between the final CO2 pressure (Pf) and
the CO2 pressure, at any other time (i.e., t ¹
tf) during the progress of the reaction (Pt), defines
the quantity P(DCO2)
= (Pf - Pt). In
essence, each change in P(DCO2) directly
reflects the corresponding change in [HCl].
Plots of the logarithm of the CO2 pressure changes, in
terms of P(DCO2)
against time (Table 3), are shown in Figure 7.
|
|

|
|
Figure 7. The natural logarithm of CO2
pressure changes [i.e., Ln{P(DCO2)}] plotted against time. The CaCO3 masses are
represented as (¨) = 0.01 g,
(·)
= 0.03 g, and () = 0.05 g.
|
|
The straight line relationships
confirm first order dependence. Thus,
reaction(III) is pseudo-first order with respect to the concentration of
[HCl]. Hence, the rate law
|
|
R = -d[HCl]/dt = k[HCl]
|
|
which, from calculus,
integrates to
|
|
kt = ln[HCl]0
- ln[HCl]t = lnPf – ln{P(DCO2)}
|
|
[HCl]0 represents
the initial concentration of HCl and [HCl]t represents the
HCl concentration at time t.
(c) From
(b) and figure 7, the specific rate constant is found to be k = 0.0059 sec-1.
(d) From
eq 15, p = 0.824 for the first order case(i.e., n = 1) and the following
figure(i.e., fig 8) is a graphical illustration of the WF vs t
relationship.
|
|

|
|
Figure 8. A graphical representation of the proportion
reacted(WF) vs. the reduced time(t) for the first order case [see Reaction(III)].
|
|
(e) The
first order case defines a singularity.
For a complete discussion, see Appendix.
Conclusions
In the present
article, it has been demonstrated that conservation of mass considerations,
fundamental to balancing chemical reactions, can be seamlessly extended to
directly incorporate reaction rate and order. Expressed in terms of the proportion
reacted versus an appropriate independent variable, such as time, results in
an analytical relationship defined by a geometry/curvature factor, p, and
the length of the reaction sequence, tL. Application of this relationship to three
different problems in general chemistry, demonstrate the utility of this
relationship as a diagnostic as well as a learning tool. In fact, it is suggested that important
aspects of basic stoichiometric and reaction rate considerations can be
naturally integrated much earlier in the general chemistry curriculum.
Importantly,
it is seen that the removal of the singularity, inherent to the first order
case for the conventional rate equation, is an algebraic reformulation in
which the singular point is simply redefined as the boundary condition tL
= finite for p = 1. In effect, the
first order singularity is restated as a point in a continuum. The fact that the progress of many other
chemical reactions can be expressed in terms of a single dimensionless
variable enhances the utility of this approach as an additional tool in the
analysis of reaction rate data.
Finally, it
is shown how a student’s three - part question resulted in the significant
enrichment of a general chemistry course.
It is yet another example of what can happen when enlightening
questions are strategically interjected at appropriate moments in the
learning process. Occasionally, it
is important to be reminded of the significant difference between listening
and hearing; because, questions are the windows to understanding. To listen well, becomes even more
critical when exchanging information with students during the formative
stages of learning and understanding basic science.
Appendix
Reference Standard. The singularity
or first order case, defined by n = 1 for conventional reaction order (eq
13), is redefined, by the conservation of mass approach (eq 11), to the
non-zero equivalent of p = 0.824 (eq 15). Inasmuch as the curvature of a
given circle is always defined by the reciprocal of the radius of the
circle in question, the circle is designated as the appropriate internal
reference standard for the p-geometry factor. A single quadrant of a circle
(Figure 9) yields a characteristic value of p = 0.628(i.e., n = 1.32).
|
|

|
|
Figure 9.
An illustration of p = 0.628(■), for one quadrant of a circle, versus
the conventional first order case of n = 1[p = 0.824](o) where red. dep. var. = reduced dependent variable(WF)
and red. indep. var. = reduced independent variable(t).
|
|
In
essence, since 2p
radians @
6.28 for one revolution, the value of p = 0.628(@ 2p/10)
is consistence with that of a circle (Figure 10).
|
|

|
|
Figure 10.
An illustration of p = 0.628(■), for one quadrant of a circle, versus
the conventional first order case of n = 1[p = 0.824](o) where red. dep. var. represents the reduced
dependent variable (WF) and red. indep. var. represents the reduced
independent variable (t).
|
|
It is somewhat instructive to note
that the value of p = 0.628 is positioned as follows
|
|
p
= 0.824 < 0.628 < p = 1/j = 0.618
|
|
where
j
= golden ratio. Furthermore, the absolute value of the ratio of the
differences between values of p and n for the singularity relates to j
as follows
|
|
[p(singularity)
– p(j)]/[n(singularity)
– (j)]
= (0.824 – 0.618)/(1 – 0.333) = 0.618
|
|
Additionally,
the value of p = 0.628 is only 1.6% greater than p = 0.618(i.e., n = 1.333)
@
1 - j
@
1/j
which is exactly the value obtained for one quadrant of the logarithmic
spiral (Figure 11).
|
|

|
|
Figure 11.
Right-handed logarithmic spiral(, i.e., r = e-bq ) where the radial distance(r) = red. dep. var.,
the angle of rotation(q) = red. indep. var., and b is a constant.
|
|
The ratio of the respective values of p for the singularity
(i.e., n = 1) to that of the reference standard (i.e., a quadrant of a
circle) is 1.312(= 0.824/0.628). The ratio of p for the singularity to p =
0.618 is 1.333(= 0.824/0.618). In essence, based on eq 10, the ratio of the
value of the p - geometry factor for the singularity (i.e., n = 1) to the p
- geometry factor value for the reference standard (i.e., a quadrant of a
circle) is 1.31( = 0.825/0.628). The value of the corresponding ratio is
1.33 (= 0.825/0.618) for the golden ratio.
Finally, based on eq 13, the singularity as uniquely
defined in terms of conventional order (i.e., n = 1), yields
|
|
tC
= k-1∙[A]0 (1 - n) = k-1
|
|
Since
k = k* = p/tL, one has
|
|
tC
= tL/p
|
(17)
|
|
which
is a disarmingly simple and significant result that follows directly from
the boundary constraints of the consistency requirements (1,2).
Also,
presented elsewhere (3), application of eqs 11 and 12 to the analysis of
first order osmosis kinetics of hydration data result in additional
considerations and implications relative to the Peleg equation (4).
|
References
1.
Maloney, K. M.; Frye, A. C. http://kennethmaloney.com/Publications/ArticleBasic2Eqn.htm.
2.
Maloney, K. M. http://kennethmaloney.com/Publications/Article1BasicEqn2002July16.htm,
2003.
3.
Maloney, K. M.
http://kennethmaloney.com/Publications/AspectsOsmosis1.htm.
4.
Pinto, G.; Esin, A. J. Chem. Educ. 2004, 81, 532-536.
5.
Choi, M. M. F.; Wong, P. S. J. Chem. Educ. 2004, 81, 859-861.
|
|
Copyright © • Kenneth M. Maloney, Ph.D.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|