Accepted Manuscript Influence of non-fat particulate network on fat bloom development in a model chocolate Huanhuan Zhao, Gokhan Bingol, Bryony J. James PII:
S0260-8774(18)30012-8
DOI:
10.1016/j.jfoodeng.2018.01.006
Reference:
JFOE 9139
To appear in:
Journal of Food Engineering
Received Date: 6 November 2017 Revised Date:
8 January 2018
Accepted Date: 9 January 2018
Please cite this article as: Zhao, H., Bingol, G., James, B.J., Influence of non-fat particulate network on fat bloom development in a model chocolate, Journal of Food Engineering (2018), doi: 10.1016/ j.jfoodeng.2018.01.006. This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.
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Influence of non-fat particulate network on fat bloom development in a
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model chocolate
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Huanhuan Zhao a, Gokhan Bingol a, and Bryony J. James a
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Department of Chemical and Materials Engineering, University of Auckland, Auckland 1142, New Zealand
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6 Abstract: Particle size effect on fat bloom formation in chocolate was studied. Model chocolates with
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68% (w/w) sand particles of varying particle size distributions (D90 of 18.7, 29.3, 41.4 and 51.1µm)
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were produced and stored under cycling temperatures of 20°C (7 hours) and 29°C (17 hours). Fat
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bloom formation was evaluated by the change of surface whiteness during 60 days’ storage, whilst the
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associated changes of melting temperatures were determined using Differential Scanning Calorimetry.
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The melting temperatures increased significantly (P<0.05) from 31.5 to 35.7°C with storage time due
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to polymorphic transformation of fat; the increase in onset temperature indicated reduced liquid fat
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content which decreased the rate of bloom formation from 9 days of storage. Image analysis showed
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that smaller particle sizes had higher particle packing density, decreasing the radius of inter-particle
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channels for fat movement. Therefore, the samples with smaller particle size were more resistant to fat
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migration and had less changes of surface whiteness, thus bloom rate was slower.
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Keywords: Plain chocolate; Fat bloom; Particle size effect; Particle packing density
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1. Introduction
21 Plain (dark) chocolate is preferred by many consumers due to its flavour and, more recently, due to
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the perceived health benefits of antioxidants. It has a shelf-life of more than one year when stored at a
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temperature below 18°C (Cebula & Ziegleder, 1993). However, during storage fat bloom, a whitish
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haze on the surface, may render the chocolate unacceptable for consumption due to the unappealing
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appearance caused by the formation of flake- or needle-like fat crystals (≥5µm) (Lonchampt & Hartel,
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2004; Rousseau, 2007). The process of bloom formation can be accelerated when chocolate or
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chocolate products are stored under elevated and/or cycled temperatures (Ali, Selamat, Che Man, &
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Suria, 2001; Ghosh, Ziegler, & Anantheswaran, 2002; Rousseau, 2007).
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There are many factors influencing bloom formation in chocolate products: 1) tempering methods
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(De Graef et al., 2005; Lonchampt & Hartel, 2004; Svanberg, Ahrné, Lorén, & Windhab, 2011), 2)
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composition (Liang & Hartel, 2004; Sonwai & Rousseau, 2010), 3) storage temperature (Ali et al.,
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2001; Jin & Hartel, 2015) and 4) chocolate microstructure (Delbaere, Van de Walle, Depypere,
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Gellynck, & Dewettinck, 2016; Rousseau & Sonwai, 2008). However, during commercial production
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chocolate is normally properly tempered and is therefore relatively stable at optimum storage
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temperature of 12-18°C (Afoakwa, Paterson, Fowler & Vieira, 2008a; Stauffer, 2017). The first two
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factors can be well controlled during production and the third during storage. Particle size and
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packing, as revealed by for example the D90 value of non-fat particles coupled with particle volume
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ratio and morphology (Beckett, 2011; Delbaere et al., 2016), is harder to control and less well
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understood. Therefore, a better understanding of the microstructure of chocolate, which is affected by
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particle size distribution (PSD), plays a very significant role in control of fat bloom formation in plain
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chocolate (Aguilera, 2005; Rousseau & Smith, 2008).
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In the last two decades, many studies (Afoakwa, Paterson, Fowler & Vieira, 2009a; Aguilera, 2005;
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Aguilera, Michel, & Mayor, 2004) have emphasised the importance of relating fat bloom
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development with the particulate network of chocolate. However, almost all of these studies have
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been carried out on the effect of PSD on bloom formation in filled chocolates, in which the plain or
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model chocolate is in direct contact with fat-based substances, e.g. peanut butter (Choi, McCarthy,
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McCarthy, & Kim, 2007; Dahlenborg, Millqvist-Fureby, & Bergenståhl, 2015a, 2015b); it has been
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shown that the PSD of non-fat solids in chocolate significantly affects the migration rate of
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triglycerides from the fat-based substances into the chocolate (Choi et al., 2007; Dahlenborg et al.,
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2015a). However, for plain chocolate in isolation from fillings, thus far and to the best of our
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knowledge, only two studies have been carried out to reveal the relationship between PSD and fat
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bloom. Altimiras et al. (2007) showed that for sand-based chocolate, bloom formation rate was
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inversely correlated to the mean particle size (D50) ranging from 5 to 120µm, and the authors reasoned
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that when chocolate was partially melted Brownian displacement of small sand particles promoted
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cocoa butter movement. However, on the other hand, for under-tempered dark chocolate with D90
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value between 18 and 50µm, Afoakwa et al. (2009b) reported contrary findings regarding the effect of
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particle size on fat bloom rate and they attributed the higher bloom rate in chocolate with larger
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particle size to the larger inter-particle pathways for capillary migration. Although for filled chocolate products there is ample evidence from literature that the PSD affects
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fat bloom formation, for plain chocolate, the number of studies in literature is scarce and furthermore
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results are contradictory. Therefore, for the particle size range mainly used in the confectionery
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industry a clear understanding of the particle size effect on bloom formation is crucial to develop
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more bloom-resistant plain chocolates. The objective of this study was thus to investigate the
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resistance offered by different particulate networks to bloom formation using a well-controlled model
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system.
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2. Materials and Methods
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Model chocolate was made of 32% (w/w) black sand particles (Bethells Beach, New Zealand) and
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68% (w/w) refined cocoa butter (PureNature, Pure Ingredients Ltd, New Zealand). The black sand
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was used to model the non-fat solid particles in real chocolate since it offered high visual contrast
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with the fat phase, therefore enabling accurate image analysis. Black sand was firstly washed and
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dried in a convection oven at 120°C for 24 hours, and then was ground in a ball mill at different
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milling speeds and times to obtain sand particles of varying size distributions. In our preliminary
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experiments, when using sand particles with D90 (90% smaller than the size) of 107.8µm for sample
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preparation significant phase separation was observed prior to solidification, such that a cocoa butter
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layer was separated from the mixture and migrated to the top surface, whereas sand particles settled at
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the bottom. As a result, particles with smaller D90 values of 18.7, 29.3, 41.4 and 51.1µm were
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prepared to minimise phase separation. The D90 was used to represent the size of sand particles in this
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study since it is a key parameter to describe non-fat particles in chocolate industry (Afoakwa, 2010;
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Beckett, 2011).
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2.2 Sample preparation
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The sample (sand-based chocolate) making method was adapted from Altimiras et al.’s (2007) with
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some minor modifications. Cocoa butter was held at 60°C in a water bath (WB-11, WiseBath, South
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Korea) for 1 hour to completely melt it. Sand particles with the above-mentioned D90 values were
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added and premixed by a mechanical stirrer (RW 20 digital, IKA-works Inc. NC, USA) for 30 min.
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The mixture was then continuously mixed in a temper machine (Revolation 2, ChocoVision, USA) at
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42.2°C for 30 min to ensure sufficient coating of sand particles with the cocoa butter. The mixture
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was then cooled down in approximately 10 min to 24°C in a water bath at 21°C with continuous 3
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mixing, using a mechanical stirrer, to achieve a high viscosity prior to moulding. The mixture was
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cast and solidified in shallow cylindrical moulds (Diameter = 45mm, Height = 12mm) in a fridge at
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2°C for 15 hours; quick solidification at 2°C was used to avoid sedimentation of sand particles. After
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solidification, all disc-shaped samples were stabilised at ambient temperature (20±0.5°C, relative
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humidity <50%) for 6 hours. Each sample was then demoulded and placed mould side up since bloom
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formation on the mould-side surface was used for DSC, VP-SEM and whiteness index measurements. Several discs of each type of model chocolates were run in parallel for different measurements.
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2.3 Quantification of particle size distribution
A laser diffractometer with a Hydro SM dispersion unit (Mastersizer 2000, Malvern Instruments
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Ltd., Malvern, U.K.) was used. Approximately 0.1g of sand particles was dispersed in water until
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achieving an obscuration of 20%. The refractive index of sand particles was 2.42. The mixing speed
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was set to 2500 rpm and the dispersion was exposed to ultrasound treatment for 2 min before each
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measurement. Particle volume diameter distribution and D90 values were obtained using the built-in
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software (Mastersizer 2000, version 5.54).
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2.4 Bloom induction
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An elevated storage temperature within the temperature range of 18 to 30oC was recommended by
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Lonchampt and Hartel (2004) to accelerate the bloom process without overheating the samples.
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Therefore, after the initial measurements of DSC and surface whiteness, all disc samples were stored
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in a dry incubator (Lab Armor Bead Bath 20L, Shel Lab, Australia) at 29±0.5°C for approximately 17
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hours. Each day, the discs were transferred from the incubator to ambient temperature (20±0.5°C) for
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7 hours to cycle the temperature (Jin & Hartel, 2015). Therefore, each day the discs experienced a
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temperature cycle of 20°C for 7 hours and 29°C for 17 hours.
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2.5 Quantification of microstructure
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2.5.1 Image acquisition
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A piece of sample with a flat surface was cut from the mould side of sample disc using a scalpel.
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Images were obtained using a variable pressure scanning electron microscope (VP-SEM) (Quanta 200
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FEG SEM, FEI Company, Eindhoven, Holland). To avoid thermal damage, the sample was mounted
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on a peltier-cooled stage with the temperature set to -5°C (James & Smith, 2009), and nitrous oxide
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was used as an imaging gas with a pressure of 50.7 Pa. The distribution of sand particles in each
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chocolate was imaged using a solid state backscatter detector and an accelerating voltage of 20 kV.
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2.5.2 Image processing
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ImageJ software (Schneider, Rasband, & Eliceiri, 2012) was employed to separate sand particles
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from the VP-SEM images. Sand particles with areas smaller than 0.02µm2 were eliminated to remove 4
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particles and the total number of particles were obtained. Thus, in a measured image area (A), the
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total cross-sectional area of particles (Atotal), particle area fraction (AA) which is the ratio of Atotal to A,
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the total cross-sectional perimeter of particles (Ptotal) and the number of particles per unit image area
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(NA) were calculated to be able to accurately define the microstructure of the model chocolate.
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Moreover, since a porous medium could be considered as an assembly of many tiny capillaries
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(Chikao, 2006), the void space in between the sand particles, i.e. the space of fat matrix, could be
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assumed as equal-sized capillaries, whose hydraulic radius (RH) was calculated using Eq.1 (Masoodi
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& Pillai, 2012).
RH = 2
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A − Atotal Ptotal
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(1)
2.6 Colour analysis
To determine the colour changes on the surface of the chocolate a machine vision system,
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developed by Luzuriaga et al. (1997), and the “two image” method, developed by Alçiçek and
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Balaban (2012), were used. Two images were taken using the front- and back-lighting methods for
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each measurement. The mould side surface of each disc was measured three times by horizontally
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rotating around 30º between measurements as suggested by Lonchampt and Hartel (2006) to minimise
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errors caused by diffraction of light due to uneven surface. The images were analysed using image
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analysis software (LensEye, Gainesville, FL, USA). L* a* b* values were determined, and WI values
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and the normalised values of WI were calculated using Eqs. 2 and 3, respectively.
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2 W I = 100 − (100 − L * ) + a * 2 + b * 2
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WI t − WI 0 × 100 WI 0
Percentage normalised WI =
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where subscripts 0 and t denotes the initial and the WI value at time t, respectively.
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(3)
2.7 DSC measurements
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(2)
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The melting behaviour of model chocolate discs was analysed using Differential Scanning
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Calorimetry (Shimadzu DSC-60, Columbia, MD, USA). Three samples, each about 5 mg, were cut
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from the mould side surface of each disc, which was kept for a total of 50 days for measurements at
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different time intervals. The sample was put in an aluminium pan and then was heated from 10 to
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40°C at a rate of 2°C/min in a helium stream. The melting curve and the peak (Tpeak), onset (Tonset) and
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final melting temperature (Tendset) values were obtained (TA-60WS Thermal Analyser).
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2.8 Statistical analysis
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The effect of storage time and sand particle size (D90) on melting temperatures were analysed by
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two-way ANOVA at a significance level of 95% using SPSS (IBM SPSS Statistics for Windows, 5
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version 21.0, IBM Corp., Armonk, NY, USA). One-way ANOVA with a Tukey post-hoc test (α=0.05)
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was used to examine the effect of particle size (D90) on AA, NA and RH values using the SPSS software.
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3. Results and Discussion
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3.1 Particle size distribution The D90 values of the four batches of sand particles used in this study, 18.7, 29.3, 41.4 and 51.1µm,
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are in line with Afoakwa et al. (2009b) who used a particle size range of around 18 to 50µm (D90) for
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non-fat particles in dark chocolate. As expected, and shown in Fig. 1, as the D90 value increased the
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ratio of large particles and the range of the distribution increased. It is also seen that the PSD curves
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of all sand particles were generally unimodal. However, Afoakwa et al. (2009b) not only observed
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unimodal distributions but also bimodal and multimodal distributions. The modality of the distribution
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gives a significant insight into the microstructure of chocolate, because the proportions of different
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particle sizes could have a significant effect on fat bloom, since the percolation of fat through the
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inter-particle channels, which are correlated with particle size, will be different. Therefore, when
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making comparisons between different D90 values, working with unimodal curves could yield more
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accurate results in terms of bloom formation.
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PSD of non-fat particles in the range of 0.3 to 100µm is commonly found in conventional
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chocolates (Afoakwa, Paterson, Fowler, & Vieira, 2008b; Ziegler & Hogg, 2017). In our preliminary
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experiment, the PSD of 107.8µm (D90) sand particles, wherein the percentage of particles larger than
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100µm was 21.7%, caused significant phase separation. However, in this study the PSD of the
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51.1µm (D90) sand particles contained 3.8% particles larger than 100µm (Fig. 1). Therefore, due to
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the considerably smaller percentage of particles larger than 100µm, it is reasonable to assume that
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phase separation caused by large particles will be negligible. Furthermore, it is clearly seen from Fig.
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2 that the two histograms of sand particles on mould and non-mould sides of the 51.1µm samples
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almost overlapped, which therefore indicates that a similar PSD existed on both sides of the chocolate
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surface. As a result, it could be safely assumed that sand particles were homogenously distributed
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within the samples, with no gravity driven separation, and the quantification of microstructure
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represented all locations in the samples accurately.
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3.2 Effect of microstructure on bloom formation
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Particle packing ability has been found to affect the resistance against liquid movement in a
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particulate network (Chikao, 2006; Masoodi & Pillai, 2012) and is also an important factor
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influencing fat migration in chocolate (Aguilera et al., 2004). Thus, using image processing, we have
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characterised particle packing density (PPD) using parameters such as NA, AA and RH, which are
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presented in Table 1. It is seen from Table 1 that as the D90 values increased, RH values increased
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significantly (p<0.05) whereas the NA and AA values decreased significantly (p<0.05), except the 6
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in PPD can also be visually observed from processed VP-SEM images, which illustrates sand particle
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spatial distributions, as shown in Fig. 3 (B2, C2 and D2). This finding is consistent with Afoakwa et
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al.’s (2009b) observations of the sugar network in molten dark chocolate, where chocolate containing
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larger-sized sugar particles had a lower PPD. A lower PPD could increase the possibility of fat bloom
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formation since there will be significantly larger void spaces, the significant (p<0.05) increase in RH,
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between sand particles for the flow of liquid fat which will eventually result in a higher bloom rate.
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It should be noted that since the shape of sand particles was irregular, similar to that of sugar
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crystals (grains of crystal-like shapes) in conventional chocolates, but different from cocoa particles
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or milk powders which are porous and have more complex surface structures, the projected areas of
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sand particles varied considerably based on orientation. However, since more than 13000 randomly
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orientated sand particles were taken into account for the calculations, it can be expected that the
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results presented in Table 1 are reliably representative.
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3.3 The changes of melting temperatures during bloom formation
The Tonset, Tpeak and Tendset values, which represent different points of melting of the fat in model
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chocolates, significantly (p<0.05) increased with the storage time, but did not significantly (p>0.05)
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change with the particle size (D90); in addition, the effect of interaction of storage time and particle
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size on the melting temperatures was not significant (p>0.05). This suggests that the melting
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temperatures were primarily storage time-dependent, and thus Fig. 4 only presents DSC thermograms
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of the 18.7µm (D90) samples during 50 days of storage.
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The shift of Tpeak values to higher temperatures suggests the formation of relatively more stable fat
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crystals. Cocoa butter has six polymorphic forms, I to VI, where I has the lowest and VI has the
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highest melting point (Wille & Lutton, 1966). It was reported by Huyghebaert et al. (1971) that the
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polymorphic form V and VI of cocoa butter have Tpeak values in the ranges of 31.3-33.2°C and 33.8-
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36.0°C, respectively, and in our samples, the increase of Tpeak from 31.5 to 35.7oC indicates the
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transformation of cocoa butter from form V to VI during the storage period. This type of
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transformation along with the formation of storage bloom on well-tempered chocolates was also
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reported by Lonchampt & Hartel (2004).
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The Tonset value gives information on amount of cocoa butter in the liquid state when the samples
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were stored at 29°C. Hence, as the Tonset values increased during storage, the samples became more
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heat resistant in terms of melting of the cocoa butter and consequently the ratio of liquid-solid fat
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reduced. Since fat migration occurs in the liquid fat portion, a reduction in liquid-solid fat ratio can
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considerably retard bloom formation, which can be seen in Fig. 5, after approximately 9 days of
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storage the rate of increase in surface whiteness noticeably decreased.
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3.4 The changes of surface whiteness during bloom formation
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Prior to storage, the samples had surface whiteness values (WI0) of approximately 14.5, 15.5, 15.9
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and 17.0 for D90 of 18.7 28.3, 41.1 and 51.1µm, respectively, which is in line with the findings of
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Afoakwa et al. (2009b). Therefore, in order to make concrete comparison of the changes of WI values
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between different D90 values, we have used percentage normalised values of WI to eliminate the
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initial minor differences of surface whiteness among the samples. The surface whiteness of all samples increased with time during storage as seen in Fig. 5, which
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indicates the formation of fat bloom when liquid fat migrated and recrystallised onto surface. As we
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have shown in Fig. 3 (A2-D2) and quantified using image processing, the existence of numerous
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micro-channels filled with fat can be assumed where this assumption is in line with literature
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(Aguilera & Mayor, 2004; Loisel, Lecq, Ponchel, Keller, & Ollivon, 1997). Since in our experiments
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the samples were exposed to a temperature cycle of 20 to 29°C, above the Tonset temperature the cocoa
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butter partially melted, and therefore the volume expanded; however, below the Tonset temperature it
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recrystallised, and hence the volume contracted. Due to above-mentioned expansion and contraction
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cycles a pressure gradient is formed which drives liquid fat from the internal volume to the surface
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(Bricknell & Hartel, 1998). Therefore, the retardation of the change of surface whiteness after
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approximately 9 days of cycling, shown in Fig. 5, could be explained by the shift of Tonset values to
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higher temperatures during the whole period of storage since a higher Tonset value indicates the
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presence of a lower liquid-solid fat ratio, which consequently lowers the rate of fat bloom formation.
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It can also be observed from Fig. 5 that during the first 9 days of storage, when the fat phase was
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rich in the liquid state, as the D90 values increased the values for normalised surface WI also increased,
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which indicated a faster rate of bloom formation. It is also seen from Fig 5 that after 9 days of storage
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the slope of the curves for all D90 values significantly decreased and became almost flat after 21 days
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of storage, which revealed that no further bloom was occurring. At the end of 21 days of storage the
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samples with larger D90 values had higher normalised WI values, which could be due to the fact that
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as the D90 values increased, the micro-channels, wherein liquid fat moved, had larger RH values as
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presented in Table 1. This is in line with findings of Altimiras et al. (2007) who, by using Lucas-
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Washburn equation, showed that under capillary effect, which could promote liquid fat movement in
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plain chocolates (Aguilera & Mayor, 2004), migration of liquid cocoa butter was quicker in pathways
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with larger diameter. Furthermore, it is also worth emphasising that the samples with larger D90 had
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lower PPD (as shown in Table 1); therefore, the length of the tortuous pathways were shorter for fat
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migration and thus offered less resistance to fat movement. As a result, a combination effect of larger
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radius and lower tortuosity of fat migration pathways led to more rapid and more pronounced bloom
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formation on the samples with larger D90 values.
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The findings of this study confirm and further clarify those of Afoakwa et al. (2009b) where
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increasing particle size increased the rate of bloom formation. The apparent contradiction between the
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results observed in this study and that of Altimiras et al (2007) is owing to the considerably large sand 8
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particles (e.g. D50: 120µm) those authors used. As significant phase separation was observed in our
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preliminary experiment using sand particles with D90 of 107.8µm, sand particles with D50 of 120µm
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could have led to gravity driven separation, which might have caused a non-homogeneous chocolate
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system and therefore interfered with the particle size effect.
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The sand-based chocolate system was chosen to simplify the microstructure of multicomponent
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real chocolate since the sand-based network was easy to be identified. Sand particles with D90 smaller
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than 51.1µm were recommended to create relatively homogeneous chocolate systems. During storage,
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the polymorphic transformation of cocoa butter increased the melting temperatures and thus led to the
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reduction in liquid fat ratio which retarded bloom formation after 9 days of storage. The particle size
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effect influenced the changes of surface whiteness but had limited impacts on cocoa butter melting
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temperatures. Variations in particle size distributions affected the PPD of model chocolates and more
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flocculated particulate networks were found in samples with smaller D90 values. It was also shown
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that model chocolates with larger D90 values had more pronounced bloom formation because of lower
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PPD. As the PPD reduced, the inter-particle channels became larger and less torturous, and as a result,
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more liquid fat migrated to surface showing higher rate and extent of bloom.
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Overall it is clear that microstructure of the non-fat solid particulate network contributes to bloom rate by altering the ease with which fat can migrate through inter-paticle channels.
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microstructure of the solid network has no direct effect on the melting behaviour of the fat phase.
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The
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Rousseau, D., & Sonwai, S. (2008). Influence of the dispersed particulate in chocolate on cocoa butter microstructure and fat crystal growth during storage. Food Biophysics, 3(2), 273–278. Schneider, C. A., Rasband, W. S., & Eliceiri, K. W. (2012). NIH Image to ImageJ: 25 years of image analysis. Nat Meth, 9(7), 671-675. Sonwai, S., & Rousseau, D. (2010). Controlling fat bloom formation in chocolate – Impact of milk fat on microstructure and fat phase crystallisation. Food Chem, 119(1), 286-297. Stauffer, M. B. (2017). Quality control and shelf life Beckett's Industrial Chocolate Manufacture and Use (pp. 532-554): John Wiley & Sons, Ltd. Svanberg, L., Ahrné, L., Lorén, N., & Windhab, E. (2011). Effect of sugar, cocoa particles and lecithin on cocoa butter crystallisation in seeded and non-seeded chocolate model systems. Journal of Food Engineering, 104(1), 70-80. . Wille, R. L., & Lutton, E. S. (1966). Polymorphism of cocoa butter. Journal of the American Oil Chemists Society, 43(8), 491-496. Ziegler, G. R., & Hogg, R. (2017). Particle size reduction Beckett's Industrial Chocolate Manufacture and Use (pp. 216-240): John Wiley & Sons, Ltd.
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ACCEPTED MANUSCRIPT Fig. 1: Particle size distributions of sand particles with D90 of (a) 18.7µm, (b) 29.3µm, (c) 41.4µm and (d) 51.1µm. Fig. 2: Histograms of particle area distributions for individual sand particles on the mould- and nonmould-side surfaces of the sample with a D90 value of 51.1µm.
18.7µm, (B) 29.3µm, (C) 41.4µm and (D) 51.1µm.
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Fig. 3: Original (VP-SEM) and processed images of mould-side surfaces for samples with D90 of (A)
Fig. 4: DSC transitional thermograms of samples (D90: 18.7µm) during 50 days of storage. The Tpeak
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Fig. 5: The percentage normalised values of Whiteness Index (WI) for samples with varying D90
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Hydraulic radius
NA (/1000µm2)
AA (-)
RH (µm)
18.7
199േ3 a
25.7േ0.5% a
1.21േ0.01 a
29.3
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26.0േ0.4% a
1.35േ0.03 b
41.4
142േ1 b
24.1േ0.3% b
51.1
116േ3 c
21.6േ0.5% c
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Particle number count
D90 (µm)
1.46േ0.01 c
1.86േ0.05 d
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1. Smaller non-fat particle size resulted in higher particle packing density (PPD). 2. Higher PPD led to a lower rate and extent of bloom. 3. Chocolate with smaller particle size had less extensive bloom formation. 4. The increase of melting temperatures also resulted in a decreased rate of bloom.