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Thermophysical and rheological properties of dulce de leche with and without coconut flakes as a function of temperature

Propriedades termofísicas e reológicas de doces de leite puro e adicionado de flocos de coco em função da temperatura

Abstracts

Dulce de leche (DL), a dairy dessert highly appreciated in Brazil, is a concentrated product containing about 70% m/m of total solids. Thermophysical and rheological properties of two industrial Brazilian Dulce de leche formulations (classic Dulce de leche and Dulce de leche added with coconut flakes 1.5% m/m) were determined at temperatures comprised between 28.4 and 76.4 °C. In general, no significant differences (p < 0.05) were observed in the presence of coconut flakes in the two formulations. Heat capacity varied from 2633.2 to 3101.8 J/kg.°C; thermal conductivity from 0.383 to 0.452 W/m.°C; specific mass from 1350.7 to 1310.7 kg/m³; and, thermal diffusivity from (1.082 × 10-7 to 1.130 × 10-7) m²/s. The Bingham model was used to properly describe the non-Newtonian behavior of both formulations, with yielding stress values varying from 27.3 to 17.6 Pa and plastic viscosity from 19.9 to 5.9 Pa.s.

Bingham model; dulce de leche; heat capacity; thermal conductivity; specific mass; thermal diffusivity


Doce de leite é uma sobremesa láctea concentrada (cerca de 70% de sólidos) muito apreciada no Brasil. Propriedades termofísicas e reológicas de duas formulações de doce de leite brasileiro (puro e adicionado de coco ralado a 1,5% em massa) foram determinadas a temperaturas compreendidas entre 28,4 e 76,4 °C. No geral, a presença de flocos de coco não acarretou diferenças significativas (p < 0,05) nestas propriedades das duas formulações. A capacidade calorífica variou entre (2633,2 e 3101,8) J/kg.°C; a condutividade térmica entre (0,383 e 0,452) W/m°C; a massa específica entre (1350,7 e 1310,7) kg/m³; e enfim, a difusividade térmica entre (1,082 × 10-7 e 1,130 × 10-7) m²/s. O modelo de Bingham descreveu adequadamente o comportamento não Newtoniano dos dois produtos, com tensão crítica de escoamento variando entre (27,3 e 17,6) Pa e a viscosidade plástica de (19,9 a 5,9) Pa.s.

modelo de Bingham; doce de leite; capacidade calorífica; condutividade térmica; densidade; difusividade térmica


Thermophysical and rheological properties of dulce de leche with and without coconut flakes as a function of temperature

Propriedades termofísicas e reológicas de doces de leite puro e adicionado de flocos de coco em função da temperatura

Vanessa Camarinha BarbosaI; Edwin Elard Garcia-RojasI, II; Jane Sélia dos Reis CoimbraIII; Paula de Aguiar CiprianoIII; Eduardo Basílio de OliveiraIII; Javier Telis-RomeroIV, * * Corresponding author

IUniversidade Federal Rural do Rio de Janeiro - UFRRJ, Rod. BR 465, Km 7, CEP 23890-000, Seropédica, RJ, Brasil

IIDepartamento de Engenharia do Agronegocio, Universidade Federal Fluminense - UFF, CEP 27255-125, Volta Redonda, RJ, Brasil

IIIDepartamento de Tecnologia de Alimentos, Universidade Federal de Viçosa - UFV, CEP 36571-000, Viçosa, MG, Brasil

IVDepartamento de Engenharia e Tecnologia de Alimentos, Universidade Estadual Paulista "Júlio de Mesquita Filho" - UNESP, CEP 15054-000, São José do Rio Preto, SP, Brasil, e-mail: javier@ibilce.unesp.br

ABSTRACT

Dulce de leche (DL), a dairy dessert highly appreciated in Brazil, is a concentrated product containing about 70% m/m of total solids. Thermophysical and rheological properties of two industrial Brazilian Dulce de leche formulations (classic Dulce de leche and Dulce de leche added with coconut flakes 1.5% m/m) were determined at temperatures comprised between 28.4 and 76.4 °C. In general, no significant differences (p < 0.05) were observed in the presence of coconut flakes in the two formulations. Heat capacity varied from 2633.2 to 3101.8 J/kg.°C; thermal conductivity from 0.383 to 0.452 W/m.°C; specific mass from 1350.7 to 1310.7 kg/m3; and, thermal diffusivity from (1.082 × 10-7 to 1.130 × 10-7) m2/s. The Bingham model was used to properly describe the non-Newtonian behavior of both formulations, with yielding stress values varying from 27.3 to 17.6 Pa and plastic viscosity from 19.9 to 5.9 Pa.s.

Keywords: Bingham model; dulce de leche; heat capacity; thermal conductivity; specific mass; thermal diffusivity.

RESUMO

Doce de leite é uma sobremesa láctea concentrada (cerca de 70% de sólidos) muito apreciada no Brasil. Propriedades termofísicas e reológicas de duas formulações de doce de leite brasileiro (puro e adicionado de coco ralado a 1,5% em massa) foram determinadas a temperaturas compreendidas entre 28,4 e 76,4 °C. No geral, a presença de flocos de coco não acarretou diferenças significativas (p < 0,05) nestas propriedades das duas formulações. A capacidade calorífica variou entre (2633,2 e 3101,8) J/kg.°C; a condutividade térmica entre (0,383 e 0,452) W/m°C; a massa específica entre (1350,7 e 1310,7) kg/m3; e enfim, a difusividade térmica entre (1,082 × 10-7 e 1,130 × 10-7) m2/s. O modelo de Bingham descreveu adequadamente o comportamento não Newtoniano dos dois produtos, com tensão crítica de escoamento variando entre (27,3 e 17,6) Pa e a viscosidade plástica de (19,9 a 5,9) Pa.s.

Palavras-chave: modelo de Bingham; doce de leite; capacidade calorífica; condutividade térmica; densidade; difusividade térmica.

Introduction

Dulce de leche is a kind of milk jam obtained by concentrating the mixture of milk and sucrose (approximately 20 mass % of the total milk volume) under heat and normal or reduced pressure until nearly 70 mass % of total solids is reached (TAMIME, 2009). From a physicochemical point of view, it is a mixed aqueous dispersion composed mainly of carbohydrates (sucrose and lactose) and milk proteins, in which the continuous phase contains different types of dispersed particles. The typical mass composition of this product is: 30% of water (maximum); 6% of proteins (minimum); 2% of lipids (minimum); 2% of ashes (minimum); and 70% of sugars (maximum), of which 30% of sucrose (maximum) and the remaining corresponds to the milk lactose. Glucose and fructose syrup, sorbitol, corn starch, maltodextrin, chocolate, fruits puree, coconut powder, sodium bicarbonate, run, coffee, and vanilla extracts are also ingredients that can be used to create variations of the "traditional" dulce de leche (RANALLI; ANDRÉS; CALIFANO, 2011; TOLSTOGUZOV, 2000; NAVARRO; FERRERO; ZARITZKY, 1999; PAULETTI et al., 1990; HOUGH et al., 1988). The higher the solids content, the more consistent is the dulce.

The modern food industry requires products that are simultaneously low cost, safe, and attractive from both nutritional and sensorial point of view, thus needing constant technological upgrades. Accordingly, the knowledge of physical properties is essential for the design and periodic improvement in the machinery used in the food product processing, especially that involved in unit operations such as pumping and evaporation. Accurate thermophysical data of products (e.g., thermal conductivity, thermal diffusivity, heat capacity, and specific mass) are necessary, as well as determining their variation as a function of temperature during the processes. Also, the knowledge of rheological properties of processed products is required because these properties are very useful in quality control, design of flow processes, and definition of transport and storage conditions. The flow characteristics determine the texture of products, which affects the perception and, thus, the acceptance by consumers. Rheological variables such as yielding stress, consistency index, and apparent viscosity are affected by the composition and the processing conditions of food products (GABAS et al., 2012; ASTOLFI-FILHO et al., 2012, 2011; MILANI; KOOCHEKI, 2011; REZAEI et al., 2011; CABRAL et al., 2007; GARITTA; HOUGH; SÁNCHEZ, 2004). In a few words, thermophysical and rheological data, and how they behave with temperature variations, are essential to a proper processing of the dulce de leche (DL) in order to avoid losses and to assure a good final quality.

Some studies dealing with the determination of physical properties of formulations of DL can be found in the literature. In such studies, the analyzed DL products had rheological behavior intermediate rheological behavior between that of the concentrated solution and that of the gel. Such differences are often attributed to the differences in the composition and type of ingredients used in the products' formulation. For instance, in some studies, DL sucrose was partially replaced by glucose syrup and sodium bicarbonate in order to avoid crystallization and protein coagulation; in others, coffee and vanilla extract were sometimes used for flavoring; and, in other cases, polyols and/or hydrocolloids were used to improve the texture (RANALLI; ANDRÉS; CALIFANO, 2011; ZIMMERMANN et al., 2007; CORRADINI; PELEG, 2000; NAVARRO; FERRERO; ZARITZKY, 1999; HEIMLICH; BÓRQUEZ; CÉSPEDES, 1994; ROVEDO; VIOLLAZ; SUAREZ, 1991; PAULETTI et al., 1990). Even though these studies reported physical characterization of some DL formulations, to the best of our knowledge, specific studies dealing with the characterization of thermophysical and rheological properties of DL containing coconut flakes, which is very common in Brazil, are not yet available in the literature.

Therefore, the aim of the present study was to evaluate the thermophysical properties and the rheological behavior of typically Brazilian DL formulations, with and without coconut flakes. These properties were evaluated at temperatures ranging from 28.4 to 76.4 °C, comprising the temperatures reached during preparation and storage.

Materials and methods

Materials

The Brazilian dulce de leche used for the measurements were manufactured by FUNARBE S.A. (Viçosa, MG, Brazil) and acquired from a commercial supermarket. Both products are commercialized as a food paste in 800 g packages. The DL without coconut flakes has the following mass composition: water ≈17.5%, total sugars ≈65%, proteins ≈10% , and lipids ≈7.5%. The composition of the DL with coconut flakes is: water ≈17%, total sugars ≈64%, proteins ≈10%; lipids ≈7.5%, and coconut flakes (mean diameter < 1 mm) ≈1.5%. Both formulations contain traces of Na (≈100 mg/100 g).

Determination of thermophysical properties

The thermophysical properties measurements (thermal conductivity, thermal diffusivity and specific mass) were performed in triplicate at each temperature [(28.4, 37.8, 48.2, 59.2, 68.8 and 76.4) °C] by taking samples from the top, center, and bottom of a same can. Prior to each experiment, the sample was kept at the working temperature using a thermostatic bath water (Marconi, MA-184, Brazil).

Thermal conductivity was measured according to the method described by Bellet, Sengelin and Thirriot (1975). This technique uses a cylindrical cell, composed of two coaxial cylinders with an annular space, which is filled with the liquid whose properties are to be determined. In order to keep the temperature constant, the cell was immersed in a thermostatic bath (Marconi, MA-184, Brazil) with an accuracy of ± 0.05 °C. The power input to the heater resistance inserted inside the inner cylinder was controlled using a microprocessor stabilizer source (Entelbra, ETB-252, Brazil), which allowed the adjustment of the electrical current with a stability of 0.05%. The temperature was monitored using a data logger (HP, 75.000-B, USA) with an accuracy of 0.6 °C. The calibration of the cell was performed with distilled water and glycerin, according to Telis-Romero et al. (1998).

Thermal diffusivity was determined using the method proposed by Dickerson (1965). The experimental apparatus consisted of a cylindrical cell (internal radius = 0.025 m and length = 0.25 m) made of chromium plated brass with two nylon covers with thermal diffusivity of 1.09 × 10-7 m2/s in order to prevent axial heat diffusion. A type T thermocouple was fixed along the central axis of the cylinder and another one tangential to the external surface of the cylinder. The system (cylinder filled with dulce de leche + thermocouples) was immersed in a thermostatic bath (MLW, MK70, Germany) and heated at a constant rate. Temperatures were controlled using the same data acquisition system used in the thermal conductivity measurements. The changes in temperature were monitored both at the cell wall and the center of the cell.

Heat capacity was calculated from the thermal diffusivity definition using its formal definition:

where Cp is the heat capacity, λ is the thermal conductivity, ρ is the specific mass, and α is the thermal diffusivity.

Specific mass (density) was evaluated by the gravimetric method using an analytical balance (Mettler, AB204, USA; uncertainty of ± 0.0001 g) and a standard volumetric pycnometer. The pycnometer of 25 mL was previously calibrated with distilled water at each temperature.

Rheological measurements

Rheological measurements were carried out using an AR2000 rheometer (TA Instruments, USA) with a cone and plate geometry (disk radius = 0.06 m; angle = 4°) under controlled shear stress and temperature. Shear rate varied between (25 and 300) 1/s, and both upward and downward tests were performed in duplicate in the temperature range of (28.4 and 76.4) °C. The experiments were performed as described in details by Astolfi-Filho et al. (2011).

Data analysis

All the regression model adjustments and statistical analyses (analyses of variance and Duncan test for comparison of means) were carried out using the SAS® software package (STATISTICAL..., 2009) licensed for the Federal University of Viçosa (Viçosa, MG, Brazil).

As for the thermophysical properties, 3th order polynomial models (Equation 2) were adjusted to the obtained data.

where ψ is the thermophysical property, T is the temperature, and β0, β1, β2, β3 are the adjusted coefficients of Equation 2.

With regard to the rheological behavior, after examining the rheograms, the Bingham model (Equation 3) was adjusted to the experimental data for both DL formulations.

This model was chosen because the analyzed fluids have yield stress (τ0) > 0 and linear variations of the shear stress (τ) as a function of shear rate ().

Results and discussion

Experimental data of heat capacity (Cp), thermal conductivity (λ), specific mass (ρ), and thermal diffusivity (α) of the dulce de leche (DL) with and without the addition of coconut, at (28.4, 37.8, 48.2, 59.2, 68.8, and 76.4) °C, are shown in Table 1. The variations in the values of these properties showed different trends with the increasing temperature. Heat capacity increased from 2633.2 to 3101.8 J/kg·°C; thermal conductivity increased from 0.383 to 0.452 W/m°C; and thermal diffusivity increased from 1.082×10-7 to 1.130×10-7 m2/s. Conversely, the specific mass values decreased with the temperature, varying from 1350.7 to 1310.7 kg/m3. The same trend has been observed in the literature for other similar food products (MURAMATSU et al., 2010; TANSAKUL; CHAISAWANY, 2006). No statistically significant differences (p < 0.05) were found between the values determined for the formulations with and without coconut flakes, except for the specific mass at 59.2 °C, However, it is important to note that, in this case, the standard deviations values were higher than those observed for specific mass at other temperatures. This suggests that such difference may be simply due to variations in experiments.

With regard to the rheological behavior between 25 and 300 1/s, and yielding stress ≠ 0, a linear relationship between shear stress (τ) and shear rate () was found at each temperature. The Bingham mathematical model (Equation 3) was appropriate to describe the behavior of both DL formulations in all cases (R2 > 0.98). The values of yield stress (τ0) and plastic viscosity (ηB) are shown in Table 2. As can be seen, an increase in temperature led to a decrease of both parameters: the yield stress decreased from 27.3 to 17.6 Pa and plastic viscosity (ηB) from 19.9 to 5.9 Pa·s. These results mean that the product becomes less viscous (more fluid) as its temperature rises (RAO, 1999). A similar rheological behavior was previously reported by Rovedo, Viollaz and Suarez (1991) for Argentinian dulce de leche market samples. No significant difference (p < 0.05) was observed in the rheological parameters of the DLs studied, except for the yield stress at 48.2 °C and 76 °C. Nevertheless, as suggested by the values of standard deviations, such difference is again likely to be due to experimental variations.

A polynomial mathematical model of the third order (Equation 2) was fitted to experimental data for thermophysical and rheological properties as a function (ψ) of the temperature. The found regression coefficients of Equation 2 for Cp, λ, ρ, α, and ηB are shown in Table 3. Figure 1 (thermophysical properties) and Figure 2 (rheological properties) present the fractional deviations between the experimentally obtained data and the relative errors for these parameters. These data, along with the determination coefficients (R2> 0.7 in all cases), indicate that the polynomial models can be considered satisfactory to mathematically represent these variations as a function of temperature within the considered interval (MONTGOMERY; RUNGER; HUBELE, 2004).



In general, the evaluation of thermophysical and rheological data for the dulce de leche with coconut flakes (amount added = 1.5% m/m) indicated no significant differences in the comparison of means (p < 0.05) as compared with classic dulce de leche at the same temperature However, the physical properties values were affected by the temperature increase.

Conclusions

Thermophysical properties (thermal conductivity, thermal diffusivity, heat capacity, and specific mass) and the rheological behavior of Brazilian dulce de leche (DL) with and without coconut flakes were evaluated at temperatures comprised between 28.4 and 76.4 °C. The Bingham model was proven adequate to mathematically represent the rheology of these two products at each different temperature considered. In general, statistically significant differences were not found when comparing these physical properties of the DL formulations with and without coconut flakes at a given temperature. Third order polynomial models were satisfactorily adjusted to the experimental data in order to represent the variations of Cp, λ, ρ, α, and ηB as a function of temperature. All these findings can help guide the industrial processing of these two kinds of DL suggesting that no changes are needed in terms of machinery and process parameters when coconut flakes are included in the formulations up to 1.5% m/m.

Acknowledgements

The authors are grateful to CNPq, CAPES, FAPEMIG, FAPESP, FAPERJ, and FUNARBE for the financial support and grants.

Received 3/4/2012

Accepted 31/10/2012 (005654)

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  • Publication Dates

    • Publication in this collection
      25 Feb 2013
    • Date of issue
      Mar 2013

    History

    • Received
      03 Apr 2012
    • Accepted
      31 Oct 2012
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