Journal of Agricultural Chemistry and Environment, 2015, 4, 1-7
Published Online April 2015 in SciRes. http://www.scirp.org/journal/jacen
http://dx.doi.org/10.4236/jacen.2015.42B001
How to cite this paper: Lien, C.-C. and Ting, C.-H. (2015) Characterising the Progress of Gelation in Tofu Making with Ohmic
Heating. Journal of Agricultural Chemistry and Environment, 4, 1-7. http://dx. doi.org/10. 4236/ja cen.2015. 42B 001
Characterising the Progress of Gelation in
Tofu Making with Ohmic Heating
Cheng-Chang Lien1, Ching-Hua Ting2,3*
1Department of Biomechatronic Engineering, National Chiayi University, Chiayi, Taiwan
2Department of Mechanical and Energy Engineering, National Chiayi University, Chiayi, Taiwan
3Center of Energy and Sensor Technology, National Chiayi University, Chiayi, Taiwan
Email: *cting @mail.ncyu.edu.tw
Received December 2014
Abstract
In tofu making by heat treatment, the addition of coagulant ionizes the proteins as a result of heat
dissolution and the ionized proteins aggregate with the coagulant to form protein clusters. The
electrical conductivity (EC) of the soya milk emulsion varies in response to the progress of gela-
tion. By ohmic heating, the applied current and voltage directly indicate the electrical conductivity
of the soya milk emulsion and then indirectly the progress of tofu gelation. In this paper, ultrason-
ic measurement is adopted to explore the feasibility of using EC as an indicator of tofu gelation.
Experiments showed a strong correlation between EC and ultrasonic measurement in characteri-
sation of tofu gelation.
Keywords
Ohmic He a tin g, Electrical Condu ctivi ty, Ultrasound, Gelation
1. Introduction
Tofu is a salt- or acid-coagulated water-based gel, with soya lipids and proteins as well as other constituents
trapped in gel networks [1]. It is rich in proteins and isoflavones and has a notable name “meat from the soil”. It
is made by coagulating soya milk-followed by either pressure or heat treatment after the addition of a coagulant.
The taste of tofu is s ignificantly affected by its final texture [2], i.e., by the firmness of the tofu gel’s structure.
The textural property is determined by the concentration of soya milk, the type and concentration of coagulant,
the gelating pressure and temperature, and the gelation time [3].
The quality of a tofu can be examined using destructive testing. A textural analyzer is suitable for characte-
rizing the mechanical property; while microscope analysis explores the chemical composition and the micro-
structure [4] [5]. The above tw o methods are of a destructive nature and require laboratory practice. They are not
suitable for on-line applicatio n as a quality indicator. Ultrasound which can give a big amount of information in
a short time [6] has been shown to be effective in detecting the gelation process and the final product in an effi-
cient way [3] [5]. While ultrasound is a means feasible for on-line quality detection, its setup is expensive.
*Corresponding a uthor.
C.-C. Lien, C.-H. Ting
2
The formation of a tofu gel requires soya milk mixed with a coagulant to be heated to a reaction temperature.
In gelation, protein clusters are formed as a mechanism of ion exchanging between soya milk and the added
coagulant. The concentration of the exchanging ions, anions orcations, is a result of the ongoing gelation process.
The ion concentration can be easily characterized as electrical conductivity, an easy, economic, and efficient
measurement [7]. Adequate temperature rising rates of soya milk is controllable by application of different vol-
tages onto the soya milk. The temperature profile can be used in tofu making with heat treatment and the elec-
trical conductivity response can be for monitoring of gelation [8].
The objective of this study is to explore the feasibility of using EC in ohmic heating as a gelation indicator of
tofu making. Ultrasonic measurements are used as a reference for calibrating EC measurements.
2. Materials and Methods
2.1. Materials
Washed soya beans (800 g) were soaked for 8 - 12 hr s at a constant temperature (30˚C) in reverse osmosis (RO)
water. On e time by weight of RO water was added to the equivalent dry weight of the soya beans. The mixtures
were ground and centrifugally filtered for 2 min to remove the residue. The soya milk produce was adjusted to a
concentra tion of 10˚ Brix. The procedure of preparing soya milk is summarized as Figure 1.
2.2. Ohmic Heating in Tofu Making
The performance of ohmic heating in food processing depends on the electrical conductivity of the foodstuff. An
electrical current flowing through the foodstuff has power conduction by the moving ions in the foodstuff fluid.
The viscosity of the fluid decreases in response to a hotter fluid. This speeds up the ionic motion and hence the
electrical conductivity. The food fluid consists of conductive and resistive components which in turn, convert
the electric current into heat [9] [10].
Addition of a coagulant into heated soya milk triggers the formation of tofu gels. The formation is a two -step
mechanism [1]: soya pro teins are denatured and then aggregated by the coagulant. Soya beans contain 35% - 40%
of stor ag e and whey proteins by weight. The 7S protein, conglycinin, and 11S protein, glycinin, are the two ma-
jor protei ns that construct the property of a tofu produce [11].
Figure 2 depicts the mechanism of soya milk transforming to tofu gels. When soya milk is heated to 65˚C and
beyond, the oil body is released. This is the first step of transformation. The 7S and 11S proteins will escape
from the subunits at 75˚C and 80˚C, respectively. Subunits are surrounded by protein particles with a size of 100
nm [11]-[13]. The transformation completes.
Figure 1. Procedure of soya milk preparation.
C.-C. Lien, C.-H. Ting
3
Figure 2. Process of protein separation in heated soya milk [11].
The process of tofu coagulation by ohmic heating is graphically illustrated in Figure 3. The ions become a
good conductor to the impinging current in ohmic heating and the milk is therefore heated up by the current.
Ions dissolve in the milk uniformly. Hence the milk will have a homogeneous temperature distribution in the
whole vol ume.
2.3. Circuitry Model of Ohmic Heating
Figure 4 presents ohmic heating in soya milk as a circuitry model. The resistance R characterizes the intrinsic
electrical conductivity of the soya milk and the capacitance C describes the capacitive effect built by the two
electrode plates with the soya milk as the electrolyte in between. The circuit has the following first-order dy-
namics:
V dv
IC
R dt
= +
(1)
The capacitive effect is transient. In theory, it becomes a barrier to DC (direct current) power and energy sto-
rage to alternate current (AC).
While the temperature of the soya milk increases, the electrical conductivity of the soya milk increases in a
positive trend as a result of more ionized subunits [1] [11]-[12]:
( )
1
T refref
mTT
σσ
⋅⋅

= +−

(2)
where
T
σ
is the electrical conductivity at current temperature T and
ref
σ
is the electrical conductivity at the
reference temperature Tref. Ions in an electrolyte are easily to escape from the substance molecules at a hot at-
mosphere. Different substances will have different properties and hence the
T
σ
is substance-specific [10] [14].
2.4. Experimental Rigs and Procedures
The setup for ohmic heating experiments and ultrasonic measurement is shown in Figure 5 . Readers are referred
to [3] for details of ultrasonic measurements. Soya milk is placed in a steel container (L × W: 11 × 7 cm2) with
ceramic coating. The two titanium electrodes are powered with an AC/DC power supply (APS-1102, Instek,
Taiwan) which is remotely controlled by a computer using the LabVIEW software (V8.3, National Instrument,
USA). The temperature of the soya milk is detected using a TM-925 temperature transducer (Prosperous, Tai-
wan).
A 1 MHz ultrasonic transducer (WesternNDE, Canada) is mounted onto the sample chamber. A computer-
controlled ultrasonic instrument (WT-UT-001A, Western NDE, Canada) excites the transducer to emit a chirp of
ultrasound waves into the chamber, amplifies the received ultrasound waves at a gain of 60 dB, and acquires
responsive waveforms at a sampling frequency of 100 MHz. Ultrasonic responses and inferred data are dis-
played on-line for visual inspection and recorded for subsequent off-line analysis. The transducer was calibrated
C.-C. Lien, C.-H. Ting
4
Figure 3. Soya milk under ohmic heating [13].
Figure 4. Equivalent circuit model of ohmic heating.
Figure 5. The experimental setup.
C.-C. Lien, C.-H. Ting
5
with RO water as the reference medium.
3. Results and Discussion
3.1. Ultrasonic Characteristics of Ohmic Heating
In theory, the velocity of an ultrasound wave travelling in a medium is determined by:
(3)
where E is the elastic modulus and ρ the density of th e milk. The modulus of elasticity increasing as a function
of time in coagulating tofu gels and should, according to the above equation, increase the velocity.
Figure 6 shows ultrasonic measurements of ultrasound waves travel in coagulating tofu gels under traditional
heat treatment [3]. Its velocity profile is contradicto ry to the above statement. This is because, in tradition al heat
treatment, the formation of tofu gels (clusters and air bubbles) alters the molecular structure and intermolecular
interactions [4 ] and hence the elasticity changes in a dramatic degree because of the presence of airbubbles.
Figure 7 show ultrasonic velocity measurements under ohmic heating, which have totally contradictory pro-
files to Figure 6. There is no doubt that the soya tofu gels are in a liquid state at the beginning of coagulation.
But in the course of ohmic heating more protein clusters aggregate probably in a homogeneous way and hence
the elastic modulus of tofu gels strengthens. The homogeneous coagulation comes from that the electrical cur-
rent of ohmic heating can penetrate every protein in the soya milk and hence all proteins could have the same
intense of ionisation. This homogeneity of protein ionisation is unlikely to occur in traditional heat treatment
that heats the soya milk through non-uniform heat convection.
3.2. Characterisation by Electrical Conductivity
Figure 8 shows electrical co nductivities of 4 tofu gels with different concentr ations of coagulant. The EC mea-
surement has first-order dynamics. Th is behaviour is identical to that of ultrasonic velocity and attenuation. The
denser the coagulant is the higher the electrical conductivity. The EC is low in the beginning of ohmic heating
and nearly saturates in steady state.
4. Conclusion
In this paper, we have presented the potential application of combing ohmic heating and associated electrical
conductivity measurement in tofu making by heat treatment. In theory, the soya milk can be uniformly cooked
Figure 6. Ultrasonic measurements of coagulating tofu gelsunder traditional heat treat-
ment [3]: calcium sulphate, 1.0% w/w; induction temperature, 75˚C.
C.-C. Lien, C.-H. Ting
6
Figure 7. Ultrasonic measurements of coagulating tofu gels under ohmic heating:
calcium sulphate; soya milk, 10˚ Brix; induction temperature, 90˚C.
Figure 8. EC measurements of coagulating tofu gels under ohmic heating: cal-
cium sulphate; soya milk , 1 0˚ Brix; induction temperature, 90˚C.
By ohmic heating and leads to tofu gels with a homogeneous structure. The homogeneity is unveiled by ultra-
sonic velocity measurement. Ultrasonic measurement gives reliable, on-line indica tion of tofu gelation dynamics.
However, the instalment of an ultrasonic measurement system is costly. EC measurement from ohmic heating
can be an affordable gelation indicator. Hence the electrical conductivity measurement could be a fast, conve-
nient, and non-destructive testing method for on-line indication of tofu quality.
1400
1420
1440
1460
1480
1500
1520
1540
0100200 300400 500600 700
1.5%
1.0%
0.75%
0.5%
Time(sec)
2
2.5
3
3.5
4
4.5
0100 200 300400 500600 700
0.5%
0.75%
1.0%
1.5%
Time(sec)
C.-C. Lien, C.-H. Ting
7
Acknowledgements
This work was financially supported by the National Science Council of Taiwan under the Grant No. 102-2221-
E-415-010.
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