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Physical and molecular changes during storage of gluten-free rice and oat bread Anna-Sophie Hager, Geertrui Bosmans, and Jan A. Delcour J. Agric. Food Chem., Just Accepted Manuscript • DOI: 10.1021/jf502036x • Publication Date (Web): 26 May 2014 Downloaded from http://pubs.acs.org on May 31, 2014
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Journal of Agricultural and Food Chemistry
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Physical and molecular changes during storage of
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gluten-free rice and oat bread
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Anna-Sophie Hager*, Geertrui Bosmans, Jan A. Delcour
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Laboratory of Food Chemistry and Biochemistry and Leuven Food Science and Nutrition Research
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Centre (LFoRCe), KU Leuven, Kasteelpark Arenberg 20, B-3001 Leuven, Belgium
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*Corresponding author. Phone: (+32)-16-379193. Fax: (+32)-16-321997.
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E-mail:
[email protected] 1 ACS Paragon Plus Environment
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Abstract
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Gluten-free bread crumb generally firms more rapidly than that of regular wheat bread. We here
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combined differential scanning calorimetry (DSC), texture analysis and time-domain proton nuclear
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magnetic resonance (TD 1H NMR) for investigating the mechanisms underlying firming of gluten-free
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rice and oat bread. Molecular mobility of water and biopolymers in flour-water model systems and
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changes thereof after heating and subsequent cooling to room temperature were investigated as a
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basis for underpinning the interpretation of TD 1H NMR profiles of fresh crumb. The proton
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distributions of wheat and rice flour - water model systems were comparable, while that of oat flour-
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water samples showed less resolved peaks and an additional population at higher T2 relaxation times
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representing lipid protons. No significant crumb moisture loss during storage was observed for the
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gluten-free bread loaves. Crumb firming was mainly caused by amylopectin retrogradation and water
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redistribution within bread crumb. DSC, texture, and TD 1H NMR data correlated well and showed
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that starch retrogradation and crumb firming are much more pronounced in rice-flour bread than in
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oat-flour bread.
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Key words
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Gluten-free, time-domain proton nuclear magnetic resonance, proton mobility, amylopectin
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retrogradation, crumb firming
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Introduction
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Coeliac disease is one of the most frequent genetically based food intolerances. It affects
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approximately 1% of the Western population.1 The only available therapy is lifelong avoidance of
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storage proteins from wheat, rye and barley, which, in the context of this disease, are referred to as
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gluten. While oat has been considered unsuitable for coeliac patients, recent scientific evidence has
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allowed concluding that most gluten-intolerant people can consume oat without adverse health
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effects.2 Nowadays, the gluten-free diet is also followed by an increasing number of individuals who
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do not have coeliac disease but appear to benefit from avoiding gluten. These include sufferers of
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non-coeliac gluten sensitivity3 and dermatitis herpetiformis.4,5 In addition, also the increasing number
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of individuals following a gluten-free diet as life style choice creates an increasing demand for
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tasteful gluten-free bakery products with a texture comparable to that of their wheat counterparts.
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Due to the lack of a viscoelastic gluten network, production of leavened baked goods from non-
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wheat sources is challenging and the resulting bread has low volume and a firm crumb.6 Due to its
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wide availability, bland taste and white color,7 rice is the most commonly used gluten-free raw
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material.8 However, rice flour contains lower levels of nutrients such as protein, fiber and minerals
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than wheat flour.9 Hence, rice-based gluten-free products are often nutritionally inferior to standard
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wheat products. Oat bread not only has a better nutritional quality than rice bread, it also results in
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bread of improved volume, texture and taste.10
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Crumb firming of wheat bread is mainly related to changes in the starch fraction that result in a
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continuous, rigid, crystalline starch network.11-15 On a molecular scale, amylose crystallizes already
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during cooling after baking, while amylopectin does so over a longer time span in a process referred
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to as retrogradation.12,16-18 The amylose and amylopectin crystallites create network junction zones.
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These serve as nucleation sites for an intermolecular and maybe even intergranular mesoscale
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network18 that includes unfreezable water. These changes can be monitored with differential
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scanning calorimetry (DSC) as an increase in melting enthalpy of retrograded amylopectin and a
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concomitant decrease in amount of freezable water (FW).15 The fast-forming amylose network and 3 ACS Paragon Plus Environment
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the thermoset gluten network are largely responsible for initial crumb firmness and resilience, while
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amylopectin retrogradation strengthens the network during bread storage.18 In wheat-bread crumb,
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part of the water included in the continuous starch network is withdrawn from the amorphous
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networks, which therefore lose plasticizing water. In addition, the thermodynamic incompatibility of
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starch and gluten causes water to diffuse from gluten to starch as shown for a model system.19 The
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changes, which occur in the biopolymers during wheat-bread baking as starch gelatinizes and gluten
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cross-links, and during storage as amylopectin retrogrades,20 probably cause the water diffusion
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process to proceed until (new) equilibria are reached. Not only does water redistribute within bread
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crumb during storage, it also migrates from crumb to crust, leading to further local reduction in
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moisture content of the biopolymer networks. As a result, the moisture content of the gluten
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network can drop below that needed for full plasticization during storage. The resulting increase in
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stiffness of the gluten network then also contributes to crumb firming, mostly after a couple of days
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of storage.15
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Molecular mobility of water and biopolymers in wheat model systems and wheat bread has already
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been studied with time-domain (TD) proton nuclear magnetic resonance (1H NMR).15,21-25 Six
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populations of different mobility, depending on the local environment of the water and biopolymer
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protons, were categorized for fresh wheat-bread crumb and interpreted by comparing the obtained
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NMR profiles to those of heated and cooled biopolymer model systems.21 The least mobile and hence
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most rigid fraction, contains non-exchanging CH protons of amylose crystals formed during cooling
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and of amorphous starch and gluten not in contact with water. Proton populations of higher mobility
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include CH protons of amorphous starch and gluten in little contact with water and exchanging
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protons of confined water, starch and gluten. The largest population consists of mobile exchanging
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protons of water, starch and gluten in the formed gel network. Finally, lipid protons represent a
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population with highest T2 relaxation time.15,26-28 Molecular and physical changes that occur during
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storage of starch-containing systems, result in changes in proton distributions. Amylopectin
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retrogradation can be observed as an increase in area of the population containing rigid CH protons 4 ACS Paragon Plus Environment
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and a decrease in areas of populations containing protons of amorphous starch due to a shift of
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protons to populations of lower mobility. In addition, the mobility of the exchanging protons is
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reduced, which can be attributed to strengthening of the starch network, loss of water from the
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gluten network and moisture migration from the crumb.15 Based on this, TD 1H NMR appears
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promising for also studying changes on molecular scale during storage of gluten-free bread. So far
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and to the best of our knowledge, only one publication has reported on the use of 1H NMR to
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investigate gluten-free bread. It stated, that the mobility of the most mobile proton population,
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representing movable water, decreases during storage. However, no population assignment was
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carried out.29
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Against this background, the present study investigates the mechanisms underlying firming of the
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crumb of gluten-free rice and oat bread. Storage-related changes are studied on a macroscopic (loaf
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volume, crumb texture) and on a molecular (proton mobility, amylopectin retrogradation, FW) level.
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Interpretation of complex NMR proton distributions in bread crumb is based on observations from
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simple oat and rice flour-water model systems.
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Materials and Methods
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Materials and analysis of their composition
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Rice flour [11.8% moisture, 7.1% wet basis (wb) protein, 70.1% wb total starch, 0.9% wb lipids, 0.46%
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wb ash] and commercial wheat flour (Crousti) (13.4% moisture, 11.4% wb protein, 65.5% wb total
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starch, 2.4% wb lipids, 0.61% wb ash) were obtained from BENEO-Remy (Wijgmaal, Belgium) and
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Dossche Mills (Deinze, Belgium), respectively. Oat flour was purchased from E. Flahavan & Son
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(Kilmacthomas, Ireland) and sifted to obtain flour particle sizes below 400 µm. The sifted flour
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consisted of 10.7% moisture, 11.1% wb protein, 60.2% wb total starch, 6.6% wb lipids and 1.39 % wb
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ash. Dry yeast was obtained from Puratos (Groot-Bijgaarden, Belgium). Sugar and salt were
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purchased at a local supermarket. All reagents, solvents and chemicals were purchased from Sigma–
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Aldrich (Bornem, Belgium) and were of analytical grade unless otherwise specified. 5 ACS Paragon Plus Environment
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Flour and crumb moisture contents (MC) were determined according to AACC Approved Method 44-
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15.02.30 Flour protein content was determined using an adaptation of the AOAC Official Method31
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with an automated Dumas protein analysis system (EAS VarioMax C/N, Elt, Gouda, The Netherlands).
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For conversion of nitrogen content to protein content, the following factors were used: 5.7 for
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wheat, 5.8 for oat and 6.0 for rice flour.32 Starch content was calculated as 0.9 times the
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monosaccharide glucose content, determined by gas-liquid chromatography as by Van Craeyveld et
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al.33 Total lipid content was measured gravimetrically following extraction with water-saturated
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butanol (WSB). Ash content was determined according to AACC Approved Method 08-01.01.34 All
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analyses were performed in triplicate.
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Defatting of oat flour and lipid extraction
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Oat flour was defatted with WSB. In practice, 1.0 g of oat flour was shaken in 10 mL WSB for 60 min
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and the solvent was removed from the residue with a rotational vacuum concentrator (RVC, Q-Lab,
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Vilvoorde, Belgium) (60°C, 1 mbar). This cycle was repeated twice before the resulting defatted flour
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was air dried overnight, used to prepare flour-water model systems and analyzed with TD 1H NMR
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(see below).
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Total lipid extract was obtained by WSB extraction of oat flour with an ASE200 (Dionex, Amsterdam,
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The Netherlands) as described previously by Gerits et al.35 The obtained total lipid extract was then
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further purified to remove protein and other non-lipid material by discarding the upper phase
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obtained following addition of chloroform, methanol, and water [ratio of 1:1:0.9 (v/v/v)] to the total
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lipid extract and vigorous shaking as described by Bligh and Dyer.36 Upon evaporation of the solvent
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with a RVC (40°C, 1 mbar), the total lipid extract was transferred into NMR tubes and subjected to
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analysis (see below).
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Flour-water model systems
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Flour-water model systems with a MC of 47% (representing a typical wheat dough MC) were
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prepared by gently stirring flour and water to obtain homogeneous mixtures. After a rest of 30 to 6 ACS Paragon Plus Environment
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120 min, all model systems were analyzed with DSC and TD 1H NMR before and after heating and
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subsequent cooling to room temperature. Heating of the flour-water model systems was carried out
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in sealed NMR tubes placed in an oil bath (10 min at 110 °C).
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Bread making
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Gluten-free formulations usually consist of complex mixtures of ingredients. To reduce complexity
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and to allow comparison with wheat-bread recipes, simple formulations based solely on flour, water,
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sugar, salt and yeast described earlier by Hager et al.10 were used here. Batters were prepared by
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using 1.5% salt, 6.0% sugar, 3.0% yeast and a water addition level of 95.0% for oat and rice
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(percentages based on flour weight). Optimal water addition levels were determined by preliminary
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baking tests. To control mold growth during storage 0.1% calcium propionate and 1.6% potassium
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sorbate were added to oat and rice batter, respectively (percentages based on flour weight). Yeast
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was suspended in the water (30 °C) and rested for 10 min in a fermentation chamber (National
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Manufacturing, Lincoln, NE, USA) at 30 °C and a relative humidity of 90%. The suspension was then
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added to the premixed dry ingredients. Mixing was carried out for 60 s at speed 1 with a KitchenAid
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KPM5 (KitchenAid, St. Joseph, MI, USA) equipped with a batter blade. The bowl content was scraped
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down, followed by further mixing for 90 s at speed 4. Greased baking tins [internal dimension (width
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× length × height), 8.0 cm × 14.5 cm × 5.5 cm] were filled with batter (350 g) and placed in the
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fermentation chamber for 30 min. Bread was then baked in a Condilux deck oven (Hein, Strasse,
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Luxemburg) for 45 min at 195 °C top and bottom heat. Prior to analyses, bread loaves were cooled
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for 2 h.
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Bread storage and crumb sampling
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Cooled fresh bread loaves were wrapped in plastic foil and stored in sealed plastic bags for up to
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120 h at 23 °C. Three bread loaves each were analyzed by crumb texture analysis and DSC at 2, 48
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and 120 h after removal from the oven. Additionally, center-crumb samples were withdrawn at these
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time points and transferred into NMR tubes, which were then sealed and analyzed (see below).
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Loaf volume and crumb texture analysis
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After cooling for 2 h, loaf volume was determined using a VolScan Profiler (Stable Micro Systems,
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Surrey, UK). Firmness and springiness of crumbs were measured at 2, 48 and 120 h after removal
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from the oven using an Instron 3342 (Norwood, MA, USA) equipped with a cylindrical probe
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(diameter 25 mm). From the center of each of three fresh and stored bread loaves, three slices were
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cut (25 mm thickness), from which cylindrical samples were obtained with a cookie cutter (diameter
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35 mm). In a first test (test speed of 100 mm/min), one indentation was carried out. The force
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required to cause an indentation of 30% in the center of the samples is referred to as firmness. In the
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second test (same test speed), two indentations of 30% in the center of the samples were carried out
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with a resting period of 60 s in between. The maximum force in the second indentation cycle divided
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by the maximum force in the first indentation cycle is the springiness, which is a measure for the
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reversibility of the imposed bread-crumb deformation.
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Differential scanning calorimetry
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DSC was carried out using a Q1000 DSC (TA Instruments, New Castle, DE, USA) previously calibrated
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with indium. To determine the temperatures and enthalpies corresponding to melting of natively
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present amylopectin crystals or such crystals formed as a result of retrogradation, 2.5-4.0 mg of
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sample were accurately weighed in triplicate in aluminum pans (Perkin-Elmer, Waltham, MA, USA).
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Deionized water was added in a ratio of 1:3 w/w (sample dry matter : water). Flour-water model
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systems were analyzed as such, while bread crumb was freeze-dried and ground prior to analysis.
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Pans were hermetically sealed and equilibrated at 0 °C together with an empty reference pan before
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heating to 120 °C at a heating rate of 4 °C/min. Samples were measured after 2, 48 and 120 h of
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storage. The resulting endotherms were evaluated using the TA Instruments Universal Analysis
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software. Enthalpies were expressed in J/g sample dry base (db).
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For determination of the portion of FW, i.e. the water that transforms into ice during cooling to -40
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°C, fresh bread crumb (10-15 mg) was accurately weighed in quadruplicate in aluminum pans. The
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samples were equilibrated at 15 °C and cooled to -40 °C at a rate of 4 °C/min. The portion of FW
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(Equation 1) was calculated from the melting enthalpy of the sample (ΔHmelting, in J/g sample
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measured between -6 and 0 °C), the MC of the sample (g water/g sample), and the melting enthalpy
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of ice (ΔHice = 334 J/g ice).
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% = × × 100
(Equation 1)
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The FW content of fresh bread crumb was analyzed using samples withdrawn within 12 h after
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baking. Pans with fresh crumb withdrawn after baking and stored at 23 °C were also analyzed after
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48 and 120 h of storage.
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Time-domain proton nuclear magnetic resonance
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Measurements of proton distributions in model systems and bread were performed as described by
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Bosmans et al.21 with a Minispec mq 20 TD NMR spectrometer (Bruker, Rheinstetten, Germany) at an
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operating resonance frequency of 20 MHz for 1H (magnetic field strength of 0.47 T). An external
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water bath maintained the temperature of the probe head at 25 ± 1 °C. Relaxation curves were
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acquired using a single 90° pulse (free induction decay, FID) and a Carr-Purcell-Meiboom-Gill (CPMG)
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pulse sequence with 90° and 180° pulse lengths of 2.86 μs and 5.42 μs, respectively. For the FID, an
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acquisition period of 0.5 ms was used and 500 data points were collected. For the CPMG sequence,
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the 90° and 180° pulses were separated by 0.1 ms and 2500 data points were acquired. For both
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measurements, a recycle delay of 3.0 s was used and 32 scans were accumulated to increase the
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signal-to-noise ratio. Three samples (approximately 0.3 g, accurately weighed) of a model system or
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bread crumb were placed in three different NMR tubes (10 mm external diameter). All samples were
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tightly compressed to a height of about 8 mm to remove air bubbles. Each tube was analyzed in
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triplicate and the exact sample weight in each tube was taken into account during the computations.
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The CONTIN algorithm of Provencher37 (software provided by Bruker) was applied to transform the
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transverse relaxation curves with an inverse Laplace transformation to a continuous distribution of
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transverse or spin-spin (T2) relaxation times, which are related to proton mobility. The area under the
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curve of a population with a certain T2 relaxation time is proportional to the number of protons in
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that population. The calculations were performed on 500 data points logarithmically spread between
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T2 relaxation times of 0.007 and 0.5 ms and of 0.2 and 500 ms for the FID and CPMG measurements,
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respectively. Because the inhomogeneity of the static magnetic field affected the output for the most
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mobile FID population found around 0.5 ms,38,39 this fraction was not taken into account in the
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following discussion.
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Statistical analysis
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Statistical analysis was performed using R version 3.0.2 "Frisbee Sailing" (The R Foundation for
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Statistical Computing, Vienna, Austria) and the package “Agricolae”. Analysis of variance was carried
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out, followed by Shapiro Wilk normality test and Tukey’s honest significant difference test.
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Results and Discussion
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Flour-water model systems
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Molecular mobility of water and biopolymers in wheat, oat and rice flour-water model systems and
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changes thereof after heating and subsequent cooling to room temperature were investigated first.
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The obtained proton distribution patterns of unheated and heated gluten-free flour-water models
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were comparable to those of wheat flour-water models21 and population assignment, therefore, was
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performed in a similar way. Figure 1 shows the FID and CPMG proton distributions of unheated and
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heated wheat, oat, and rice flour-water model systems. The unheated samples showed one
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predominant FID population (population A) (Figure 1, left pane). Based on previous studies, this
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population contains rigid CH protons of crystalline and amorphous starch21,40 and proteins not in
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contact with water.21,28
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Regarding the CPMG proton distributions, population E was most abundant in all samples (Figure 1,
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right pane). This population contains mobile OH protons of water in the extragranular space, which
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are in exchange with starch OH protons on the granule surface and with exchangeable protons of
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proteins21. Population C of the wheat flour-water model system contains CH protons of amorphous
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starch and gluten in contact with water21. Population D then contains OH protons of intragranular
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water and starch, but also some CH protons of gluten and exchanging protons of confined water and
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gluten.21,41 It can reasonably be assumed, that also CH protons of rice or oat protein are part of
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populations C and D.
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For unheated rice and wheat samples three distinct CPMG populations (C, D, E) were observed, even
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if these were not fully resolved for wheat. The difference with the oat samples is that in the latter
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population E was much broader and peaks C and D were not resolved. The total lipid extract from oat
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flour showed CPMG populations with T2 relaxation times corresponding to populations C, E and F of
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oat flour (results not shown). The lipid T2 relaxation times apparently are too similar to those of the
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mobile and exchangeable protons of starch and protein, to permit clean separation of peaks. In the 11 ACS Paragon Plus Environment
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case of unheated oat flour, an additional proton population F was observed with a T2 relaxation time
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of approximately 100 ms (Figure 1b, right pane). Prior removal of lipids from oat flour by WSB
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extraction, reduced the area of population F (Figure 2, right pane). Thus, this peak probably
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represents protons of the lipid fraction. That such peak was present in the oat flour-water model
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system, is in line with the higher endogenous lipid content of oat than of either wheat or rice.
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For heated flour-water model systems, DSC did not detect endothermic peaks (results not shown),
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confirming that heating model systems for 10 min at 110 °C fully gelatinized the starch in each flour
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model system.
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Heat treatment and subsequent cooling of the flour-water model system resulted in similar changes
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in proton distributions. The area of population A decreased, while those of populations B and C
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increased (Figure 1). These changes were related to starch gelatinization, resulting in a decrease in
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protons in a rigid environment due to melting of the starch crystals and swelling of the previously
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densely packed amorphous starch not in contact with water (present in population A), and an
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increase in protons of amorphous starch in contact with water (present in populations B and C).21 The
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area of population E, representing mobile protons in strong interaction with water, increased upon
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heating. The mobility of this population decreased during heat treatment. The reduced mobility was
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also observed for a starch-water model system and attributed to starch gelatinization and gelation.21
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After heating and subsequent cooling, this population consisted of mobile exchanging protons of
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water, starch and proteins present in the formed gel network. The reduced mobility was possibly
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caused by more intense contact between the biopolymers and water.21 The CPMG populations of
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heated wheat and rice flour-water model systems were well resolved, while this was not the case for
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the heated oat flour-water model system. The broadness of the oat peaks can possibly be attributed
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to the presence of endogenous lipids, as clearly resolved peaks were observed after heating and
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subsequent cooling of the oat flour model system prepared with defatted flour (Figure 2). Heated
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model systems prepared with oat or rice flour, contained an additional small population G with a T2
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relaxation time of 300 ms. The population was not influenced by defatting, hence does not contain
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protons of the lipid fraction, but possibly results from expulsion of water from the flour proteins
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during heating. This small proton population with very high mobility was also observed for heated
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and cooled egg28,42 and gluten.21
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Oat and rice bread
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Loaf specific volume was significantly higher (p