# Phase Characterization of Cucumber Growth: A Chemical Gel Model

Authors: Bo Li; Xuejing Liu; Junshi Zhang
Journal: International Journal of Polymer Science
 (2016)

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## Abstract

Cucumber grows with complex phenomena by changing its volume and shape, which is not fully investigated and challenges agriculture and food safety industry. In order to understand the mechanism and to characterize the growth process, the cucumber is modeled as a hydrogel in swelling and its development is studied in both preharvest and postharvest stages. Based on thermodynamics, constitutive equations, incorporating biological quantities, are established. The growth behavior of cucumber follows the classic theory of continuous or discontinuous phase transition. The mechanism of bulged tail in cucumber is interpreted by phase coexistence and characterized by critical conditions. Conclusions are given for advances in food engineering and novel fabrication techniques in mechanical biology.


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## Body

## 1. Introduction

Development of fruit growth can be identified as a series of successive stages. Before harvest, it develops nonlinearly, then enlarges slowly at initial period, and then grows rapidly as it approaches its maturation. At the moment of harvesting, the fruit is not fully ripened but leaves space for growth that may continue during agricultural storage and transportation for sale. This explains why bananas are almost green and stiff on the shelves of a supermarket and then turn yellow and soft gradually in your kitchen. The growth of fruit after harvest is denoted as postharvest behavior. Ethylene is frequently used to accelerate the process of ripening [1].According to recent TV news, some cucumbers in the kitchen displayed inhomogeneous deformation in body and their tails bulged locally, as seen in Figure1. Concerns for the food safety were raised about this unusual phenomenon, since the underlying mechanism, relating multifields knowledge in chemistry, biology, and mechanics, was elusive. In cross-disciplines of plant study, enormous efforts have been devoted to the research of plant growth, including experts from botany to mathematics [2, 3]. In solid mechanics, the establishment of the nonlinear gel theory offers a new insight to the study of biomechanics. Using the gel theory, the quantities in physics, chemistry, and biology are coupled [4]. Since both gel and biological tissues are soft, flexible, and stretchable, the expansion of biological organs under the regulation of hormones is analogous to the swelling of gel. Large deformation and mass transportation of gel are capable of characterizing the biological system, that is, the morphology of esophagi in growth [5], pattern formation of pumpkin shell [6], wrinkle profile of a finger immersed in water [7], dehydrated green pea in a dry environment [8], and so forth. Through these researches, the capability of gel theory has been reproduced and verified by modeling in biology. In the current presentation, we also adopt the gel theory to analyze the growth process in a specific fruit category: the cucumber. The phenomenon in growth resembles the phase transition in classic thermodynamic systems, while the biochemistry is involved.Figure 1
Growth of cucumber is complex. After harvest, the cucumbers are immature and ripen gradually during storage. This phenomenon is defined as postharvest ripening. During postharvest, as a result of biological nature, some cucumber species select to ripen part of the whole body, with limited nutrition. Therefore, they show a local inhomogeneous growth at the tail of a cucumber body. Report by Phoenix TV:http://v.ifeng.com/news/society/201205/05a4eed1-dc0b-4936-b3be-fb70681691f9.shtml.


## 2. A Chemomechanical Model

Figure2 sketches an illustration of a thermodynamic system for gel. We first model the growth of a cucumber before harvest as a process of swelling in a cylinder gel. The dry polymer network imbibes solvent molecules (individual volume of v) and enlarges itself from volume π
R
2
×
L at initial state to volume π
r
2
×
l at harvested state. In fruit development, the hormones stimulate the expansion of cells, tissues, and organs, which is similar to the swelling mechanism of gel under its chemical potential μ.Figure 2
The growth of a cucumber is analogous to the process of swelling in a tubular gel. Subjected to the chemical potential, the dry polymer network imbibes solvent molecules, forming a swollen gel. The sketched model characterizes the shape change of cucumber during growth, with the dimension enlarging from (a)π
R
2
×
L at the initial state to (b) π
r
2
×
l at the harvested state.W
λ
1
,
λ
2
,
λ
3
,
μ, the free energy per unit initial volume of the gel, is the combination of W
s, the strain energy in polymer network due to stretching, and W
m, the chemical energy due to mixing network with solvent [4, 9]. Consider(1)
W
λ
1
,
λ
2
,
λ
3
,
μ
=
W
s
+
W
m
.Here, λ
i
,
i
=
1,2
,
3 are the principle stretches to be determined by coordinates. The free energy expression is then specified by Gent model [10] and Flory-Rehner function [11] as(2)
W
s
=
-
N
K
T
2
J
m
log
⁡
1
-
λ
1
2
+
λ
2
2
+
λ
3
2
-
3
J
m
+
N
K
T
2
J
2
-
1
2
-
log
⁡
J
4
,
W
m
=
-
K
T
v
J
-
1
log
⁡
J
J
-
1
+
χ
J
-
μ
v
J
-
1
,where N is the number of crosslinks in unit initial volume, K is the Boltzmann constant, T is the temperature, J
m is the maximum extension limit, χ is a dimensionless constant, C is the concentration of solvent molecule in initial volume, and J
=
1
+
v
C
=
λ
1
λ
2
λ
3.According to the thermodynamics, we define the nominal stresses ass
1
=
∂
W
λ
1
,
λ
2
,
λ
3
,
μ
/
∂
λ
1, s
2
=
∂
W
λ
1
,
λ
2
,
λ
3
,
μ
/
∂
λ
2, and s
3
=
∂
W
λ
1
,
λ
2
,
λ
3
,
μ
/
∂
λ
3. Then we have(3a)
s
1
K
T
/
v
=
N
v
λ
1
1
-
λ
1
2
+
λ
2
2
+
λ
3
2
-
3
/
J
m
+
2
λ
1
λ
1
λ
2
λ
3
2
-
1
λ
1
λ
2
λ
3
2
-
1
2
-
log
⁡
λ
1
λ
2
λ
3
3
+
1
λ
1
1
+
λ
1
λ
2
λ
3
log
⁡
1
-
1
λ
1
λ
2
λ
3
+
χ
λ
1
λ
2
λ
3
-
μ
K
T
λ
1
λ
2
λ
3
,
(3b)
s
2
K
T
/
v
=
N
v
λ
2
1
-
λ
1
2
+
λ
2
2
+
λ
3
2
-
3
/
J
m
+
2
λ
2
λ
1
λ
2
λ
3
2
-
1
λ
1
λ
2
λ
3
2
-
1
2
-
log
⁡
λ
1
λ
2
λ
3
3
+
1
λ
2
1
+
λ
1
λ
2
λ
3
log
⁡
1
-
1
λ
1
λ
2
λ
3
+
χ
λ
1
λ
2
λ
3
-
μ
K
T
λ
1
λ
2
λ
3
,
(3c)
s
3
K
T
/
v
=
N
v
λ
3
1
-
λ
1
2
+
λ
2
2
+
λ
3
2
-
3
/
J
m
+
2
λ
3
λ
1
λ
2
λ
3
2
-
1
λ
1
λ
2
λ
3
2
-
1
2
-
log
⁡
λ
1
λ
2
λ
3
3
+
1
λ
3
1
+
λ
1
λ
2
λ
3
log
⁡
1
-
1
λ
1
λ
2
λ
3
+
χ
λ
1
λ
2
λ
3
-
μ
K
T
λ
1
λ
2
λ
3
.Consider the shape of cucumber is cylindrical, so the stretches are represented by(4)
λ
1
=
l
L
=
λ
L
,
λ
2
=
λ
3
=
r
R
=
λ
R
.Thus, the constitutive equations are expressed as(5a)
s
L
K
T
/
v
=
N
v
λ
L
1
-
λ
L
2
+
2
λ
R
2
-
3
/
J
m
+
2
λ
L
λ
L
2
λ
R
4
-
1
λ
L
2
λ
R
4
-
1
2
-
log
⁡
λ
L
λ
R
2
3
+
1
λ
L
1
+
λ
L
λ
R
2
log
⁡
1
-
1
λ
L
λ
R
2
+
λ
L
λ
R
2
-
μ
K
T
λ
L
λ
R
2
,
(5b)
s
R
K
T
/
v
=
N
v
λ
R
1
-
λ
L
2
+
2
λ
R
2
-
3
/
J
m
+
2
λ
2
λ
L
2
λ
R
4
-
1
λ
L
2
λ
R
4
-
1
2
-
log
⁡
λ
L
λ
R
2
3
+
1
λ
R
1
+
λ
L
λ
R
2
log
⁡
1
-
1
λ
L
λ
R
2
+
χ
λ
L
λ
R
2
-
μ
K
T
λ
L
λ
R
2
.In cucumber growth, no external forces are applied to the biological entity, so that we model the growth of the cucumber as an isotropic free swelling process of the gel. Therefore, we haves
L
=
s
R
=
0 and λ
L
=
λ
R
=
λ. Equations (5a) and (5b) are reduced to (6)
N
v
λ
1
-
3
λ
2
-
1
/
J
m
+
2
λ
λ
6
-
1
λ
3
-
1
2
-
log
⁡
λ
3
3
+
1
λ
1
+
λ
3
log
⁡
1
-
λ
-
3
+
χ
λ
3
-
μ
K
T
λ
3
=
0
.


## 3. Results and Discussion

Figure3 plots the swelling of four types of gel, differing in the material density of crosslink, N
v, to characterize the growth of cucumbers. J
m
=
100 and χ
=
0.5 as selected for representative values [6]. Gel, which is heavily cross-linked, is stiffer, behaved in mechanical strain responding. So N
v characterizes the stiffness of material, which, in terms of biological interpretation, is the species of cucumber featuring in strength, elasticity, and firmness. The growth stretch shows a nonlinear trend which is in good coincidence of observation of real cucumber growth; during the early stage, the cucumber enlarges slowly, which corresponds to the small stretch. When the chemical potential reaches a critical value, cucumber expands abruptly and then reaches a plateau for harvest. Some fruit is able to increase its volume by 100 times which resembles the performance of hydrogel in solvents absorbent. Figure 3 shows a continuous phase transition in material volume which recalls classic phase transformation in physics. For example, PbZrO3 ceramic transits from antiferroelectric state to ferroelectric state when the electric field exceeds the critical magnitudes. In ferroelectric material, the transition is tunable by mechanical confinements such as stress or strain [12]. Here, we also investigate how the stiffness affects the cucumber growth. Figure 4 illustrates the swelling associated with crosslink density at selected chemical potentials. In Figures 4(c) and 4(d), the stretch curve is nonmonotonic that follows “Z” shape as crosslink density increases. At a specific N
v condition, two stretches coexist, which means that a special type of cucumber might grow with two shapes in the same body, at a prescribed hormone degree. Within a whole cucumber body, one part enables a fast and accelerated growth while the other grows normally. Figure 4(d) explains the news report in Figure 1 when the cucumber bulged locally in the tail. This verifies the first-order phase transition in thermodynamics. For example, at 0 degrees of temperature, H2O can coexist in both solid ice phase and liquid water phase.Figure 3
Stretch versus chemical potential during the gel swelling to model the growth of cucumber, showing an analogue to continuous phase transition.
(a)
(b)
(c)
(d)Figure 4
The growth processes by the model of gel swelling are influenced by chemical potential and density of crosslink, which are analogous to the concentration of plant hormone and cucumber stiffness in species. (a)–(d) show the effect of crosslink density, which denotes the firmness of cucumber species.
(a)
(b)
(c)
(d)We next investigate the phenomenon in Figure1 in detail to extend the model to the study of postharvest process. After harvest, the cucumber is close to maturation but not fully ripened. To regulate the ripening speed, ethylene is spayed to form an artificial hormones environment. Denote the concentrate of ethylene as Ω and reexpress the free energy as(7)
W
N
K
T
=
-
J
m
2
log
⁡
1
-
3
λ
2
-
3
J
m
+
1
2
λ
6
-
1
2
-
log
⁡
λ
3
4
-
1
N
v
λ
3
-
1
log
⁡
λ
3
λ
3
-
1
+
χ
λ
3
-
1
N
v
Ω
K
T
λ
3
-
1
.Figure 5 plots the free energy landscapes, normalized by N
K
T. Three magnitudes of crosslink density are prescribed with variation less than 10%, but the associated energy curves distinguish greatly in landscape. At N
v
=
11.2, the thermodynamics system stabilizes at a lower stretch phase, since the energy minimizes. The higher stretch phase, corresponding to the second-minimized energy, is the metastable state that the gel might stabilize here temporally; but under a small perturbation, it could transit to the lower stretch state for global stabilization. Similar case is also presented in N
v
=
11.4 since two minima are presented. The small stretch phase is metastable and large stretch phase is globally stable. Equation (7) offers to determine a level of density, N
v
=
11.317, when the two stretches, λ
′ and λ
′
′, share the same level of minimum free energy that both are globally stable. The two stretches in the growth of cucumber during postharvest process are possibly coexisting, only subject to a specific level of ethylene concentration.Figure 5
Coexistence of two stretch phases ofλ
′
=
1.15 and λ
′
′
=
1.04 subject to the conditions of Ω
/
K
T
=
10 and N
v
=
11.317.Not all the cucumbers ripen with coexistence. The phenomenon is determined by the critical conditions of both the density of crosslinkN
v and the chemical potential Ω
/
K
T. Here, Figure 6(a) shows the mechanism. At the onset of phase coexistence of λ
′ and λ
′
′, the critical density N
v
∗ separates the curve, resulting in two grey regions which are the same in area. In thermodynamics, this line is defined as Maxwell line [13]. Following the classic theory in physics, we denote the critical value as Maxwell density to study the phase behavior in the current biochemical system.Figure 6
(a) The Maxwell density determines the coexistence of stretch states where the two states have the equal grey area. (b) Above the critical value, the small growth stretch state is stable; below the value, the large stretch state is stable.
(a)
(b)The critical Maxwell density is a function of chemical potential that determines the occurrence for transition. By solving equations in Appendix, we plot in Figure6(b) the relations. Under a prescribed chemical ethylene concentrate, cucumbers with density above the critical line are stable in the rod phase (phase B) with a small growth stretch; for cucumbers with density below the critical line, they bulge (phase A) for stabilization. For cucumbers holding the density that exactly falls in the critical line, their tails bulge but bodies are left in rod state. The local bulging instability has been documented in the research of tissue engineering, that is, aneurysm angiogenesis [14–16], with extensive solution of the inhomogeneous deformation. Here, we explain the mechanism for the first time from the perspective of botany in biology and characterize it using chemical thermodynamics. Using this model, an engineer is able to regulate the growth of plant and to achieve a prescribed shape in fruits and vegetables [17]. This offers a new insight into on-demand manufacturing. The element in mechanical structure is fabricated in a biological way to form its profile naturally.


## 4. Conclusion

In summary, the growth of cucumber is analogous to the swelling of gel. We characterize the phenomena of cucumber growth, covering the processes of both preharvest and postharvest, by establishing a thermodynamic gel model. The phase behavior in plant growth resembles the transition in ferroelectric ceramic and other biological tissue growth. The model offers solutions to regulate fruit development and can be extended to other plant candidates for potential technique in biological and food engineering.



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*Source: 8283245-2016-04-05.xml*