Introduction

Epoxy resins based on materials are thermosetting polymers widely used for structural applications, adhesives, organic coatings, electrical engineering and aeronautics due to their superior thermal, mechanical, and corrosion-resistance properties [1, 2]. Moreover, they are the most extensively used advanced composite materials in aerospace and advanced automotive applications because of their excellent combination of mechanical properties and corrosion resistance, good adhesion, wetting properties, and dimensional stability with respect to their cost [3, 4].

When composites are considered for long applications, it is necessary to know how the materials will behave during the estimated service life [5]. Many researches have investigated the effects of absorbed water on the mechanical behavior of organic matrix composites under humid conditions or during immersion [6, 7]. It is well known that absorbed water can affect the physico-chemical and mechanical properties, and reduction of the Tg of the material resulting from plasticization and degradation of chemical structure [8, 9].

Like all polymeric materials, epoxy resin systems undergo physical ageing phenomena in which the free volume decreases during a period of time because of the tendency of the material to reach the equilibrium condition. The last effect is responsible for increasing the brittleness of the material as a consequence of increasing the density. Physical aging is accelerated and emphasized by plasticization as a result of the water absorption by the resin which increases the mobility of the molecular chain [3].

Water aging was performed to investigate the effect of absorption of seawater in epoxy composites; it can affect the mechanical and chemical properties of the epoxy matrix by plasticization and hydrolysis [10, 11]. Molecular weight is varied by structural changes such as hydrolysis [12].

One of the interesting aspects of epoxy system is water sorption and water transport which have been considered by various categorization techniques including IR, NIR, UV, NMR, dielectric and dynamic mechanical spectroscopy [13].

Polymer nanocomposites are at the center of attention as a new class of materials which may enhance stiffness, strength, as well as fracture toughness and ductility [14, 15]. Fine particle size and high specific surface area make the fumed silica the most popular reinforced filler for composites [16]; in spite of their low cost, they have various applications, but the viscosity will be increased by formation of hydrogen bonds between the particles leading to the formation of a three-dimensional network in the matrix [17]. Increasing the affinity of the particle surface to the matrix polymer leads to reduced conglomeration behavior [18]. The surface treatment of the particles with organic molecules enhances compatibility and adhesion between the components [19]. Organosilanes in the treated silica surfaces can form chemical bonds between inorganic and organic composite. Recently, these materials which can couple filler to an organic media have attracted lot of attention. Thus, an amino silane can act as a bridge between silica and polymer; thereby those interactions will increase. For silica treatment, amino silane is used regularly [19].

Photo and thermal aging of polymer can be influenced by various aspects such as time of aging, temperature, different environment, and presence of various materials, therefore a suitable experimental design and well-developed models can be unique approaches to analyze the aging behavior and to attain the best composites. One convenient and remarkable method is using the statistical models developed by response surface methodology (RSM). RSM is a statistical and mathematical method that was developed by Box et al. [20]. This is fitted to the mathematical model, and its use has been widely adopted to tests on chemometrics. Statistically based design of experiments (DOE) help to increase the speed of the development cycle time, improve reliability, reduce process variability, and increase overall product quality. Using the RSM, one is able to develop the statistical models to evaluate the effect of particular parameters of any process as well as to optimize the conditions for desirable responses. Therefore, in the present study, RSM based on central composite design (CCD) was used to design the experiments and develop new models to determine the optimum mixture for aging process. RSM can be very helpful in designing the experiments and to figure out the aging parameters and their interactions. This technique can be used to investigate the responses of any industrial process and to determine the relation between the response and independent variables by developing a statistical model [21]. This is followed by analyzing the experimental results using the analysis of variance (ANOVA) to determine as to which parameters show the strongest interactions and/or which ones exhibit significant influence on the outputs of the process. The process responses are then represented as statistical developed models. The developed models are then validated by testing at the optimum conditions predicted by RSM [22].

In this paper, in order to design the experiments by a statistical method, firstly the parameters that exhibit significant influence on an aging process such as presence of fumed silica or amino silane should be estimated.

The effect of accelerated hydrothermal ageing on the thermal and mechanical properties was investigated through DMTA and SEM techniques. Accelerated ageing was performed in natural sea water (Persian Gulf) at 60 °C at different times and the results were compared with neat epoxy composite.

Experimental

Material

The epoxy resin, diglycidyl ether of bisphenol F (DGEBF, Epoxy equivalent weight equal to 320), and the Tri Ethylene Tetra Amine (TETA) as hardener (stoichiometric ratio amino hydrogen-to-epoxy 100:15) both is supplied by local compony, Mokarar engineering material (Iran).

Inorganic fillers containing Fe2O3 (good anticorrosive behavior) and mica (to improve mechanical strength) were also used. Fe2O3 was provided by Merk C and mica was provided by Borna Company (Iran). Nanoscale silica particle was AEROSIL® 200, fumed silica (specific surface area = 200 m2/g, Degussa Co.) (http://www.degussa.com, 2011). Aminopropyltrimethoxysilane (APTMS), C9H3NO3Si, 0.98 % in ethanol, was purchased from Merck Co. All other chemical reagents, including ethanol, hydrochloric acid and caustic soda were purchased from Merck Co. All materials were used as received.

Sample preparation

The amounts of silica and silane were calculated according to a stoichiometric value and hydrolysis ratio as follows:

$$ M = { 3} \times {\text{SsSi}} \times {\text{mSi}} \times {\text{M Silane}} \times {\text{OH}} . {\text{No}} \times 1 ,0 1 9/{\text{NA }} $$
(1)

where M is the amount of silane (in g), SsSi is the surface area of silica, mSi is the weight of silica, and M Silane is the molecular weight of silane. OH.No is the number of hydroxyl groups per nm2 on silica surface, NA is the Avogadro number and 1,019 is a conversion factor. Silane is poured drop wise. The amounts of materials in the reaction vessel are used from Ref. [18].

An ultrasonic homogenizer is used for all samples at 19,000 rpm for 15 min to disperse nanoparticles in the solvent. Total reactions last for 3 h. The resulting slurries are centrifuged at 5,000 rpm to remove the untreated particles. Then, in order to increase pH up to 4, 2 cc sodium hydroxide is added to the solution.

Preparation of composites with treated and untreated fumed silica

Silica particles are ultrasonically dispersed in epoxy resin for 5 min at amplitude of 20 %. A pulser cycle (turning on and off-time ratio of 5:1) is used to control the temperature of the mixture (temperature of the mixture at around 30–40 °C).

The resin was mixed with the additives and inorganic fillers (Fe2O3, mica and calcium carbonate) via stirring at room temperature until a homogeneous mixture was formed. Afterwards, a vacuum of 1–5 mbar is applied for 3 min to degas the compounds. The resulted mixture was mixed with the hardener by stirring [the ratio of epoxy and amine groups is kept constant (100:15)]. Eight composites are formulated, containing three different amounts of fumed silica (0, 1, and 2 wt %) and amino silane (as is shown in Table 1).

Table 1 Selected levels of variables for central composite design (coded value)

Thermal analysis was performed using a Mettler Toledo (TGNSDTA851) model under nitrogen flow at a heating rate of 10 °C/min.

Weathering experiment conditions

The fully cured (at 60 °C for 24 h) composites were immersed in natural sea water (Persian Gulf) at 60 °C at different time intervals. The sea water was filtered to remove sedimented particles. To do so, the film thickness of composites for hydrothermal aging was 2 mm. Gravimetric analysis was conducted by weighing with a resolution of 0.0001 g to evaluate moisture content, which was expressed as a percentage of the composite’s initial dry mass. Samples were wiped with paper towels and placed in the oven for 12 h (at 40°) before weighing to dry the surfaces. The mass M of each sample at time is expressed as (2).

$$ {\text{Moisture content}}\,\% = \frac{{M_{{{\text{t}} }} - M_{\text{dry}} }}{{M_{\text{dry}} }} \times 100 $$
(2)

where M t is the measured mass at equilibrium moisture content (g) and M dry is the dry mass (g):

Dynamic mechanical thermal analysis (DMTA) and scanning electron microscopy (SEM)

The formulated composites are casted in silicon molds and cured in the oven for DMTA test (60 °C, 24 h); then, the tests are conducted after 7 days. DMTA has been performed by a Perkin Elmer DMTA instrument. Experiments are carried out in a temperature range between 25 and 150 °C, as well as at a heating rate of 2 °C/min under a flow of nitrogen. The frequency is set to 1 Hz (isochronal measurement) and maximum strain amplitude 0.02 %. All experiments are performed on a 25 × 10 mm silicon rectangular sheet. Visco-elastic properties such as modulus and mechanical loss tangent (tan δ) are reported as a function of temperature [22]. The degree of dispersion of the filler within the matrix was analyzed by SEM investigations. The SEM analysis was carried out with VEGA, TESCAN, Czech Republic.

Modeling by response surface methodology (RSM)

The aim of modeling of aging properties by RSM was to find the optimal combination to attain the maximum water aging resistant trace. The parameters for modeling was selected as aging-time, untreated and treated nano silica. For each parameter, five values were considered in the model. The investigated parameters and their levels are given in Table 1. In this table, α refers to the position of the axial point of the cubic in central composite design (CCD). Functional relationships between the independent variables (aging-time, fumed silica and aminosilane amount) and dependent variables (Tg, damping and modulus) were determined using the multiple regression technique having the following format:

$$ Y = \varepsilon 0 + \mathop \sum \limits_{i = 1}^{n} \varepsilon iXi + \mathop \sum \limits_{i = 1}^{n - 1} \mathop \sum \limits_{j = i + 1}^{n} \varepsilon_{ij} X_{i} X_{j} + \mathop \sum \limits_{i = 1}^{n} \varepsilon_{ii} X_{i}^{2} $$
(3)
$$ Y = \varepsilon_{0} + \mathop \sum \limits_{i = 1}^{n} \varepsilon_{i} X_{i} + \mathop \sum \limits_{i = 1}^{n - 1} \mathop \sum \limits_{j = i + 1}^{n} \varepsilon_{ij} X_{i} X_{j} + \mathop \sum \limits_{i = 1}^{n} \varepsilon_{ii} X_{i}^{2} $$
(4)

where ε 0, ε i , ε ij and ε ii are coefficients, X i and X j are the independent variables, Y (as a dependant variable) is the response and n is the number of independent variables. The regression equations are then developed and used to describe the effects of controlling parameters on the responses, determine the relationships between variables, and to represent the total effect of all variables. To develop a regression model, the experimental variables were coded according to Eq. 5

$$ x_{i} = \frac{{X_{i} - X_{0} }}{{{{\Updelta}}X_{i} }} $$
(5)

where x i and X i are, respectively, the coded and actual values of the experimental variable; X 0 is the actual value of the experimental variable at the central point; and \( {{\Updelta}} \) X i is the step change value. In the present study, we selected central composite design for three of the variables; in this way, 17 DMTA tests were carried out for different composites. The most important factors which were controlled in this study were:

  • amount of fumed silica (A),

  • amount of aminopropyltrimethoxysilane (APTMS) (B),

  • time of aging (C).

In this work, experimental design was performed using Design-Expert 7 computer software (trial version, Stat-Ease Inc., USA) to study the aging behavior of epoxy nanocomposites and determine the most significant variables that can affect the ageing.

Results and discussion

Treated fumed silica

TGA analysis (Fig. 1) was conducted on the product to indicate that the treatment of silica surface has taken place. The TG thermogram for treated silica shows three stages of weight loss steps with total weight loss. In the first step, weight loss occurs at 64.6 °C. In the second step, weight loss of approximately 6.44 % at temperature of 101.96 °C was attributed to the release of adsorbed water and volatiles such as alcohol, while the weight loss in the temperature range 200–400 °C results from the silanol condensate groups and the decomposition of the grafted APTMS molecule. The decomposition of aminopropyl groups occurs slowly at 200–400 °C, followed by a rapid degradation above 4,008 °C. The decomposition of amino silane leads to the formation of ammonia, ethylene, hydrazine and methane which is in good agreement with the literature [19].

Fig. 1
figure 1

TGA of treated fumed silica

Dynamic mechanical analysis

Dynamic mechanical properties are the mechanical properties of materials as they are deformed under periodic or varying forces. In the linear region, the applied force and the resulting deformation both vary sinusoidally with time. The importance of determining the dynamic mechanical properties of polymers and composites can be illustrated by outlining the various aspects of material structure or behavior to which the dynamic properties are related and the range of applications for which dynamic data are directly relevant. In the present study, the tan δ curve as a function of temperature (obtained from a temperature sweep test) was chosen for Tg determination because the Tg is found most accurately at the peak of the tan δ curve. In addition, the tan δ curve is more sensitive to property changes at the molecular level of the material [23]. Properties such as glass transition, damping, and modulus of these samples were investigated before and after the samples were soaked in sea water at an aging condition.

The glass transition temperature of the neat epoxy composite was 76.2 °C (Fig. 3). In the presence of the untreated fumed silica, the Tg decreases by increasing the percentage of nanoparticle. At 1 % wt, the glass transition decreased by nearly 4.8 °C. Water molecules adsorbed on the surface of the nanoparticles may cause decrease in composite’s Tg containing untreated fumed silica. The untreated nano silica particles used in this study show a remarkably hydrophilic behavior; they carried a significant amount of water into the epoxy matrix, which can decrease the glass transition temperature significantly. The surface of the untreated fumed silica contains a lot of hydroxyl groups, causing extremely hydrophilic behavior. So it could absorb water easily, linked to the particles via hydrogen bonds [24].

The silane-treated particles significantly affect the glass transition temperature, the Tg will increase 8.2 °C (±0.5) for 1 % wt fumed silica treated with 1 % silane; also for 2 % wt fumed silica the Tg will increase 12.7 °C (±0.5) (for 1 % wt amino silane) and 18.1 °C (±0.5) (for 2 % wt silane). It could be related to the formation of covalent bond between silica surface and the matrix to form chemical bonds [13]. Increasing of Tg and decreasing of the free volume may be related to crosslinking of polymer. It required more rotation energy because of more specific volume and mobility of the molecular motion. It is evidence of the successful treatment of the silica surface [25].

SEM analysis was performed on the surfaces of the nanocomposites (Fig. 2). It could be seen in Fig. 2a, c, the fumed silica was partially agglomerated which indicates the poor dispersion and weak interfacial bonding between fumed silica and the epoxy matrix. However, in the case of the treated-fumed silica/epoxy nanocomposites (Fig. 2d), the particles were dispersed better and the amount of wetted nano silica increased compared to the untreated particles. These results indicate that the surface treatment could help dispersion and interfacial bonding between the nano silica and the epoxy matrix. A strong agglomeration phenomenon was observed for the 4 % wt untreated fumed silica (Fig. 2c).

Fig. 2
figure 2

SEM micrographs of not aged surfaces. a 0 % wt fumed silica; b 2 % wt; c 4 % wt; d treated 2 % wt

SEM micrograph (Fig. 2b) shows that silica nanoparticles were well dispersed, however, Fig. 2c shows that silica particles are spherical in shape and agglomerates. It may show that the silica particles are well bonded in the epoxy matrix but the particles have a strong tendency to agglomerate due to weak interaction between the two phases. It shows that the particles dispersion into the epoxy matrix is not homogeneous. The agglomerate is a result of the formation of a silica–silica aggregated structure due to hydrogen bonding.

The influence of hydrothermal ageing on dynamic mechanical and morphology properties of nanocomposites

Sea water can change the physical and mechanical properties of the nanocomposite because of absorbing and diffusing through the film. Besides, the existence of hydrogen-bonding sites is a main factor in the polymer–water affinity along the polymer chains, which produces attractive forces between the polymer and the water molecules [13].

As could be seen in Fig. 3a, b, Tg decreases from 76.2 to 68.5° C for neat epoxy composite. Decreasing of the glass transition temperature and modulus, and increasing of damping could be related to plasticization by water and wider distributions of molecular weights of composite during environmental exposure especially at the elevated temperature [3, 9, 26]. As the temperature increases, water penetrated into the cross-linked domain (less plasticized phase) where water hardly penetrated at room temperature aging.

Fig. 3
figure 3figure 3

A comparison of plots of tan delta, loss factor, and storage modulus vs. temperature for different percentages of fumed silica and amino silane (fumed silica:amino silane) aged in sea water at 60° at different times a 0:0/unaged, b 0:0 aged for 500 h, c 1:0/unaged, d 1:0 aged for 250 h, e 1:1/unaged, f 1:1, aged for 250 h, g 2:1/unaged, h 2:1 aged for 250 h

In treated nanocomposite, silane molecule could relieve strained flexible Si–O–Si bonds and might increase the resistance of the interfacial Si–O–Si bonds to water attack [27]. It could lessen the amount of absorbed water, furthermore, the treated silica particles interface had considerably more resistance to crack growth than the untreated fumed silica.

Water is a present compound that can be absorbed into and diffused through epoxy-based composite. The primary mechanism for moisture absorption in epoxy composite is surface absorption which can diffuse through the resin phase [5]. In this work, the moisture absorption of fumed silica/epoxy composites was calculated using the weights of the specimens before and after moisture absorption by Eq. (1). Table 2 shows the seawater contents for all samples of epoxy nanocomposite and time of immersion in water. The results showed water diffusion increased significantly for untreated samples, since treated nanocomposites showed lower water uptake due to hydrogen bonds between the particles leading to the formation of a three-dimensional network.

Table 2 Moisture content of different composites

One relaxation peak can be observed for treated composite (tan δ/T curves) (Fig. 3), but a shoulder can be observed (in 190–200 °C) for untreated composite (especially for 1 % fumed silica). It may be related to treatment, which can decline water diffusion, and indicates a more uniform network.

Optimization by RSM and CCD

Aging of fumed silica/epoxy composites in sea water at different time or in different combination with sustained load is detrimental to their thermal, physical, and mechanical properties. In the present study, an aging condition was applied to fumed silica/epoxy composite. Their changes of epoxy composites were followed by DMA measurements. The following models, i.e. Eqs. (6) and (7), were then developed, respectively, for Tg, modulus (M), and damping (D) using the regression coefficient summarized in Table 3. Where A, B and C are, respectively, the coded values for, amount of fumed silica (% wt), amino silane (% wt) and aging-time (h), also R 1 is Tg from tan δ, R2 is modulus at 140 °C (M), and R3 is damping (length of half height) (Tables 4, 5, 6, 7).

Table 3 Central composite design and experimental results
Table 4 ANOVA of RSM regression analysis for modulus and Tg
Table 5 ANOVA of RSM regression analysis for Tg
Table 6 Analyses of the results of central composite design for Tg and modulus
Table 7 Analyses of the results of central composite design for damping

Final equation in terms of coded factors Tg:

$$ \begin{aligned} {\text{Tg}} = & + 75.75 + 4.50A - 2.99B - 1.91C + 8.94AB + 2.89AC \\ & \quad - 1.44BC - 6.97A^{2} - 3.50B^{2} + 0.18C^{2} \\ \end{aligned} $$
(6)

Final equation in terms of actual factors Tg:

$$ \begin{aligned} \text{Tg} &= 76.699 + 13.57A - 6.487 - 0.02C + 25.279AB + 0.02AC \\ &\quad - 0.013BC - 19.72A^{2} - 9.88B^{2} + (5.5342E - 006)C^{2} \\ \end{aligned} $$
(7)

Final equation in terms of coded factors for modulus:

$$ \begin{aligned} M & = 8.40 + 0.82A - 0.43B + 0.1C + 0.51AB + 0.11AC + 0.79BC \\ & \quad - 2.81A^{2} - 1.03B^{2} + 0.33C^{2} \\ \end{aligned} $$
(8)

Final equation in terms of actual factors for modulus:

$$ \begin{aligned} M & = 1.597 + 15.56A + 1.46B - 0.014C + 1.44AB + \left( {1.08E - 003} \right)AC \\ & \quad + (7.45E - 003BC) - 7.977A^{2} - 2.927B^{2} + 1.025E - 005C^{2} \\ \end{aligned} $$
(9)

Final equation in terms of coded factors damping:

$$ \begin{aligned} D & = 36.35 - 5.31A + 0.11B + 6.34C - 3.49AB - 3.61AC - 2.31BC \\ & \quad + 1.13A^{2} - 1.03B^{2} - 6.12C^{2} \\ \end{aligned} $$
(10)

There are so-called f values and P values. The higher amounts of the f value and lower amounts of the P value can imply more significant coefficient values of “Prob > F” less than 0.0500 indicate model terms are significant. For Tg, A, B, AC, AB, A 2, B 2 are significant model terms. Therefore, they are considered as significant variables for each response of Tg. Besides, it is necessary to test the accuracy of the model using analysis of variance (ANOVA) method. ANOVA is applied to statistically analyze the performance of the developed models by the Fisher’s F test (overall model significance). One way to do this is determining the value of R 2. With respect to the models developed for Tg, the R 2 was 0.9648. This indicates that the model can explain 96 % variation in the response for Tg. As already mentioned, the regression models can be used to predict the effects of processing parameters as well as to optimize them. As it is observed, there is a very good agreement between the experimental and predicted amounts.

In damping model A, C, AB, AC, BC and C 2 are significant model terms, AB (interaction of fumed silica and amino silane) has minus coefficient, it is shown that damping and molecular distribution will decrease with treatment; also time (C) has the biggest coefficient (Eq. 10) that confirms aging behavior by lasting time and this effect will reduce in the presence of nanoparticles or silane.

This can be interpreted in terms of more mobility restriction, means of forming a so-named rigid amorphous phase, which is not able or less able to perform the glass transition. The evolution of the loss factor has not only one reason but during the radical-based oxidative ageing two competitive processes take place: chain scission and intermolecular chain radical combination thereby forming crosslinking. A decrease of tan (δ) causes formation of more cross links and therefore resulting in more rigid three-dimensional network. An increase of tan (δ) characterizes an increase of the macromolecular mobility, which can be caused by chain scission [28] and/or by dewetting [29].

Consequently, the developed models for Tg, damping, and modulus can be used successfully to optimize the aging process and its variables. The effects of three factors as well as their interactive effects on the responses are shown in Figs. 4 and 5. From these figures, the effect of each variable and their interactive effects can be studied. The shapes of the contour plots are then used to interpret the interactions between the variables. If the contour plots are circular, it means that the interactions between the variables are not significant, i.e. having no notable interaction. By contrast, elliptical plots imply that the interactions between variables are important, i.e. exhibiting strong interaction [30].

Fig. 4
figure 4

Contour plots of the Tg, for the interaction between a time (C) and fumed silica (C), b fumed silica (A) and amino silane (B), and c time (C) and amino silane (B)

Fig. 5
figure 5

Contour plots of the damping, for the interaction between a time (C) and fumed silica (C), b fumed silica (A) and amino-silane (B), and c time (C) and amino silane (B)

The aim of response surface optimization is to find a desirable composite. This position could be a maximum, a minimum, or an area where the response is stable over a range of factors. The main goal of this study was to develop a model process for optimizing the experimental parameters through preparing to obtain a nanocomposite with the best wet aging behavior. The importance of the factors and their effects (either positive or negative) can be explained by the magnitude and sign of the coefficients of coded equation (Eq. 6, 8, and 10). The Tg’s model coefficient of factor A × B (8.94) is the biggest coefficient which shows the importance of treating fumed silica rather than untreated nanocomposites or silane alone.

Therefore, using these plots one can determine the optimal combination of Tg variables. Each response plot offers an infinite number of combinations of two variables when the third one is kept at its respective zero level. For example, referring to three-dimensional surface plots in Fig. 4b, when the time (C) is kept at its zero level, i.e. 300 h, the Tg is increased with increasing amino silane and fumed silica (A) up to 1 % wt fumed silica that is treated with 1 % wt amino silane. This happens when the Tg increases from 49 to 79 °C and fumed silica increases from 0 to 1 %, corresponding to the values of B (1 % wt).

Conclusions

In this work a nanocomposite was treated with different concentrations of amino silane and thermally cured. The characterization was performed by DMTA, DSC and gravimetric measurements.

DMTA of cured treated samples showed an increase of the glass transition temperature of about 8.2 °C and an increase of the systems compared to the neat resin.

Different combinations of composites were immersed in seawater from the Persian Gulf for up to 600 h at 60 °C. Samples were tested in tension at durations up to 600 h. Absorption of seawater increased gradually with immersion time and decreased the Tg of the nanocomposites as water acts as plasticizer. Decreasing of the Tg of epoxy composites treated with amino silane is less than other samples due to the increase in cross-link density. The higher crosslink density means more epoxy ring open and so more −OH groups formed. Also sea water aging influences the lowering of Tg as well as the phase separation in fumed epoxy composite samples due to the plasticization effect. The effect of plasticization was greater in untreated epoxy composites than in treated composites.

The tan δ peak of the more plasticized phase of epoxy composites aged in sea water at an elevated temperature is wide. This shows that a broad molecular weight chain network had built up in the epoxy structure when the degradation occurred. At room temperature, sustained load had no significance effect on the Tg of the samples for all aging conditions.