The impact of the structuring of hydrotropes in water on the mesoscale solubilisation of a third hydrophobic component

In the present contribution, the pre-structuring of binary mixtures of hydrotropes and H 2 O is linked to the solubilisation of poorly water miscible compounds. We have chosen a series of short-chain alcohols as hydrotropes and benzyl alcohol, limonene and a hydrophobic azo-dye (Disperse Red 13) as organic compounds to be dissolved. A very weak pre-structuring is found for ethanol/H 2 O and 2-propanol/H 2 O mixtures. Pre-structuring is most developed for binary 1-propanol/H 2 O and tert -butanol/H 2 O mixtures and supports the bicontinuity model of alcohol-rich and water-rich domains as already postulated by Anisimov et al. Such a pre-structuring leads to a high solubilisation power for poorly water miscible components (limonene and Disperse Red, characterized by high octanol/water partition coeﬃcients, log( P ) values of 4.5 and 4.85), whereas a very weak pre-structuring leads to a high solubilisation power for slightly water miscible components (benzyl alcohol). This diﬀerence in solubilisation power can be linked to (i) the formation of mesoscale structures in the cases of ethanol and 2-propanol and (ii) the extension of pre-structures in the cases of 1-propanol and tert -butanol. Three diﬀerent solubilisation mechanisms could be identified: bulk solubilisation, interface solubilisation and a combination of both. These supramolecular structures in binary and ternary systems were investigated by small-and-wide-angle X-ray and neutron scattering, dynamic light scattering and conductivity measurements (in the presence of small amounts of salt).


Introduction
Ternary systems comprising a short chain amphiphilic molecule (hydrotrope) and two immiscible liquids, with both of them being fully miscible with the hydrotrope, are considered as powerful solubilisation media 1-3 and exhibit anomalies concerning enzymatic reactions 4,5 and vapour pressures. 6 The existence of well-defined mesoscale inhomogeneities in macroscopically transparent solutions was shown to be responsible for such unexpected behaviour. Such mesoscale inhomogeneities and compartmentation phenomena of oil-rich and water-rich domains are comparable to the micro-domains observed in water/oil/surfactant ternary systems (direct-, bicontinuous-and reverse-microemulsions) as shown using scattering techniques, molecular dynamics simulations (MD simulations) and conductivity measurements. [7][8][9] Only recently, Zemb et al. provided an extended Derjaguin-Landau-Verwey-Overbeek (DLVO) theory as a general explanation for the existence and thermodynamic stability of such surfactant-free microemulsions (SFME). This extended DLVO theory describes the subtle balance between entropy, i.e. homogenous mixing of three components, and enthalpy, i.e. hydrophobic effects between two immiscible fluids causing micellar-like aggregation. 10 Hydrotropes play a major role in the mesoscale solubilisation phenomenon of SFME. The concept of hydrotropy, defined by C. Neuberg in 1916, 11 outlines the capability of short chain amphiphilic molecules to solubilize hydrophobic compounds in a hydrophilic solvent. In SFME showing the compartmentation of hydrophilic and hydrophobic domains, the hydrotrope accumulates mostly at the interface between water-rich and oil-rich domains as deduced from contrast variation experiments with small-angleneutron-scattering (SANS) and MD simulations. The interface between the oil-and water-rich domains is usually considered as a kind of highly flexible film in dynamic exchange with the surrounding medium. 7,12 When using hydrotropes, as in the case of SFME, the solubilisation of hydrophobic compounds in water is only significant at higher hydrotrope concentrations, typically above c(hydrotrope) 4 0.2-0.5 M, which may be compared to surfactants for which solubilisation appears above the critical micellar concentration c(surfactant), which is typically 410 À5 -10 À2 M. As a rule of thumb, the solubilisation by hydrotropes starts in the concentration range (c 4 1 M), where the average distance between hydrotrope molecules becomes smaller or in the order of the molecular size (B1 nm), encouraging molecular contact between hydrotrope molecules (cluster formation) and between the hydrotrope and the hydrophobic component to be dissolved. 13 In contrast to surfactants, the amphiphilic character of hydrotropes is usually considered to be not enough pronounced to promote micellisation or self-aggregation of the hydrotrope itself in water. 13 Nevertheless, some hydrotropes, such as tertbutanol, are known to form clusters in water and thus produce heterogeneities in the sub-nanometer (molecular) or nanometer range. [14][15][16][17] Only recently, the group of Shimizu et al. developed an approach to describe hydrotropic solubilisation theoretically. [18][19][20][21] This approach derived from pure statistical thermodynamics uses the exact Kirkwood Buff theory to describe the cooperative phenomena in hydrotropic solubilisation such as (i) the sudden onset of solubilisation of hydrophobic compounds in H 2 O (commonly referred to as MHC) and (ii) solubility saturation of hydrophobic compounds at high hydrotrope concentrations. In a nutshell, they consider hydrotropic solubilisation to be the result of a subtle balance between solute-hydrotrope interaction and hydrotrope-hydrotrope interaction. In other studies the authors argued that strong hydrotrope-hydrotrope interactions resulting in a pre-structuring of the hydrotrope in H 2 O diminish the solubilisation efficiency of solutes. 22,23 As we will show here, things are even more complex.
Already a vast number of publications have focused on the microscopic inhomogeneities of short chain alcohols in H 2 O. [24][25][26][27][28][29][30][31][32][33][34][35][36][37][38][39] The microscopic structuring in these binary mixtures is mostly attributed to the hydrophobic hydration of non-polar aliphatic chains of alcohols and a highly dynamic network of hydrogen bonds between alcohols and H 2 O. 15 Anomalies concerning permittivity, surface tension, self-diffusion coefficients, structuring, etc. are most pronounced for tert-butanol-H 2 O mixtures as tert-butanol provides the largest aliphatic chain among fully water-miscible alcohols. [29][30][31][32][33][34][35][36][37][38]40,41 The goal of this work is to link such molecular inhomogeneities in binary alcohol/H 2 O mixtures to the mesoscale solubilisation of a third hydrophobic component, called ''third component'' hereafter. To establish this link, it is essential to understand the origin of the compartmentation of water-and oil-rich domains in the ternary systems. Three questions are essential in this context: (i) Do the pre-structuring and microscopic inhomogeneities of the hydrotrope in the binary system alcohol/H 2 O have an influence on the structuring of the ternary system? (ii) Is the structuring in SFME caused by the hydrotrope or by a third, (more) hydrophobic component?
(iii) Does the mesoscale solubilisation mechanism of the third, hydrophobic component depend on its hydrophobicity?
Hence, it is necessary to understand the structuring of short chain alcohols in water as a function of the increasing aliphatic moiety of the alcohol. We extend the pioneering studies by M. Anisimov and M. Sédlak on the mesoscale solubilisation of a third component in the pre-structured binary mixture tertbutanol/H 2 O 14,17,42 to the homologous series of alcohols and to other hydrophobic compounds. To this purpose, we investigate the structuring of ethanol (EtOH), 1-propanol (NPA), 2-propanol (IPA) and tert-butanol (TBA) in water using conductivity measurements and scattering techniques. The structuring in the binary alcohol/H 2 O mixtures is related to its impact on the mesoscale solubilisation of a third hydrophobic component, i.e. benzyl alcohol, limonene and an azo dye, Disperse Red 13 (DR-13). As we will show, the observed differences in solubility are the consequence of different solubilisation mechanisms.
All chemicals were used without further purification. Aqueous solutions were prepared using deionized water with a resistivity of 18 MO cm.

Methods and techniques
2.2.1 Ternary phase diagrams. Phase diagrams were recorded using dynamic and static processes according to Clausse et al. 43 For this purpose, binary mixtures (each 3 g) were prepared in screw tubes of borosilicate glass. The third component was added gradually until a visible change in the phase behaviour occurred. Measurements were carried out at room temperature and phase transition was determined by the naked eye. Weight fractions were calculated from the mass of the individual components derived from precise weight measurements.
2.2.2 Dynamic light scattering. Dynamic light scattering (DLS) experiments were performed using a temperature controlled CGS-3 goniometer system from ALV (Langen, Germany) equipped with an ALV-7004/FAST Multiple Tau digital correlator and a vertically polarized 22 mW HeNe laser (wavelength l = 632.8 nm). Before starting the measurements, all samples were filtered into dust-free cylindrical light scattering cells (10 mm outer diameter) using a 0.2 mm PTFE membrane filter. The sealed measurement cells could be directly placed into the measurement apparatus. Measurements were performed at a scattering angle of 901 after thermostatting to 25 AE 0.1 1C. Data points were collected for 300 s. Aggregates in SFME are usually highly fluctuating and have no well-defined shape. Hence, we renounced the calculations of the exact hydrodynamic radii. Instead, the DLS spectra were evaluated qualitatively with regard to their correlation coefficient and their lag time, and an estimate of the size of the microscopic inhomogeneities is provided. (As a rule of thumb, it was assumed that a higher intercept of the correlation function for small lag times and larger lag times of the correlation function represent the more time-stable and more pronounced structuring in the solution.) 2.2.3 Small-and-wide-angle X-ray and neutron scattering. Small-and-wide-angle X-ray scattering (SWAXS) measurements were performed on a bench built by XENOCS using Mo radiation (l = 0.071 nm). The scattered beam was recorded using a large online scanner detector (diameter: 345 mm, from MAR Research). A large q-range (0.2 to 40 nm À1 ) was covered with an off-center detection. Collimation was applied using a 12:N multilayer Xenocs mirror (for Mo radiation) coupled to two sets of scatterless FORVIS slits providing a 0.8 Â 0.8 mm X-ray beam at the sample position. Preanalysis of data was performed using FIT2D software. The scattered intensities are recorded versus the magnitude of the scattering vector q = [(4p)/l]sin(y/2), where l is the wavelength of incident radiation and y the scattering angle. 2 mm quartz capillaries were used as sample containers for the solutions. The usual corrections for background (empty cell and detector noise) subtractions and intensity normalization using a high density polyethylene film as a standard were applied. Experimental resolution was Dq/q = 0.05. Silver behenate in a sealed capillary was used as the scattering vector calibration standard. Measurements were performed at room temperature.
Small-angle-neutron-scattering (SANS) experiments were performed using a D33 instrument at the ILL, Grenoble, France. 44 The wavelength was set at 6 Å and two sample-to-detector distances 2 m and 5 m with collimation at 5.3 m for both configurations were used to cover a q-range from 0.08 to 0.47 Å À1 . A 7 Â 10 mm 2 aperture was placed before the sample. The samples were filled in 1 mm thick Hellma cells and thermostatted at room temperature using a circulating water bath. The raw data were corrected for the electronic background and empty cells, and were normalized on the absolute scale using the attenuated direct beam to calculate the incident flux using the ILL Lamp software. 45 The scattering intensity was plotted against the magnitude of q, and the curves were fitted with an Ornstein-Zernike (OZ) function: 10 x is the correlation length in Å and I(0) is the intensity for q = 0 and takes into account the scattering length density of the different species and volume fraction of each phase. The full fitting of the spectra is beyond the scope of this paper.

Conductivity measurements.
Conductivity measurements were carried out in a thermostatted measurement cell (25 AE 0.2 1C) under permanent stirring using a low-frequency WTW inoLab Cond 730 conductivity meter connected with a WTW TetraCon 325 electrode (Weilheim, Germany). 20 g of each sample (pure hydrotrope or hydrotrope/benzyl alcohol mixtures of different mass fractions) were filled in the measurement cell and successively diluted with pure water. Each sample contained in addition 0.2 wt% sodium bromide to ensure a sufficient amount of charge carriers, which did not noticeably affect the microstructure or the miscibility gap present in the phase diagram. In cases where sodium bromide did not dissolve completely, a small amount of water was added to the pure hydrotrope or hydrotrope/benzyl alcohol mixture before the measurement was started. In addition, conductivity measurements of a classical SDS based microemulsion system were carried out for comparison. For this purpose, a mixture of SDS, 1-pentanol, dodecane and water was used as a starting solution with 9 wt% water, a R SDS/PenOH mass ratio of SDS to 1-pentanol of 1 : 2 and a R O/TS mass ratio of oil to total surfactant of 21 : 79. The conductivity curve was determined as described above.
2.2.5 UV-Vis measurements. The solubilisation of DR-13 in different hydrotrope/water mixtures was determined by optical density (OD) measurements via UV-Vis measurements. Saturated solutions of DR-13 in hydrotrope/water mixtures of different mass fractions were prepared. For this purpose, an excess of DR-13 was added to the mixtures. After equilibrating the solutions under intense stirring for 7 days, excess dye was removed by filtration using a 0.2 mm PTFE membrane filter. OD measurements were carried out at l = 525 nm in 10 mm path length cells using a Lambda 18 UV-Vis spectrometer from Perkin Elmer (Waltham, USA). Samples with absorbance higher than 1 were diluted with an appropriate amount of acetone before the measurement. The initial absorbance was calculated by using the respective dilution factor. In addition, a standard curve of DR-13 in acetone was measured to further calculate the amount of DR-13 dissolved by a given amount of hydrotrope.  [24][25][26][27] However, this type of structuring appearing at the small molecular scale would produce too fast fluctuations, i.e. with high diffusion coefficients, in EtOH/H 2 O and IPA/H 2 O systems to be detectable by DLS.

Results and discussion
As the DLS auto-correlation functions are most pronounced for TBA/water mixtures, additional SWAXS and one particular SANS measurement were performed for this system, see Fig. 2 and Fig. S1 in the ESI. † Four features can be observed in SWAXS spectra, assigned to i-iv. A correlation peak (i) is observed at 20 nm À1 , originating mainly from the O-O pair correlations in the H-bonding network of H 2 O. This peak does not significantly shift in position and decreases in intensity as the amount of water decreases.
Another correlation peak (ii) is found at 10.5 nm À1 , corresponding to the pair correlations between aliphatic chains. This peak also does not undergo any shift in position and its intensity depends on the TBA concentration.
For TBA concentrations above 70 wt%, a correlation peak (iii) emerges at 5-7 nm À1 , which corresponds to average distances between 0.9 and 1.3 nm. This peak can be attributed to the pair-correlations between hydroxyl groups of TBA as its intensity increases with the TBA content. The peak (iii) shifts to lower q-values with increasing water concentrations indicating a swelling of the H-bond network, formed by the TBA hydroxyl groups, by the addition of water. Furthermore (iv), a significant excess of scattering is observed in the low-q range (q o5 nm À1 ) for 40, 50 and 60 wt% of TBA with a maximum I(0) intensity for 40 wt%. It has been noticed that the low-q scattering is only observed in the absence of a correlation peak of the alcohol (-OH) groups (iii). The existence of low q-scattering in smallangle-X-ray-scattering experiments indicates the existence of a meso-structured system. 10,12 Curves exhibiting low q-scattering were fitted with an Ornstein-Zernike formalism to determine    Fig. S1 (ESI †). The existence of low scattering again indicates the presence of a structured system. Fitting the curve with an OZ fit yields a correlation length of 0.7 nm, which is approximately the same as that obtained for SWAXS for this composition (0.8 nm). The slight difference in the correlation lengths obtained from SWAXS and SANS can be ascribed to the different scattering contrasts of SWAXS and SANS.
Therefore, SWAXS and SANS experiments support the results obtained by DLS: the existence of a structured system in the binary mixture TBA/H 2 O with microscopic inhomogeneities in the order of 4-6 nanometers. The structuring is most pronounced between 30 and 50 wt% of TBA.
3.1.2 Conductivity measurements. To further investigate the structuring of the binary mixture alcohol/H 2 O, conductivity measurements were performed. Conductivity measurements provide detailed information on the mobility of charge carriers and yield insight into the structuring of a system, for example, for surfactant-stabilised microemulsions. 43,46,47 Conductivity measurements in surfactant-stabilised microemulsions are a well-known and common method to distinguish between regions of o/w, w/o and bicontinuous microemulsions. 9,43 The results of conductivity measurements as a function of the alcohol/H 2 O mass and mole fractions, respectively, are depicted in Fig. 3a and b. All curves show a more or less pronounced increase for low water content. With increasing water content, a maximum is reached before the conductivity decreases again due to excessive dilution of the present charge carriers. The slope of increase in conductivity and sharpness of the maximum increases in the following order: TBA 4 NPA E IPA 4 EtOH.
Conductivity was also measured for a classical SDS-based microemulsion, see Fig. 3c. 43 Such systems show a flat rise at  low water content, followed by a change in the slope passing over into a strong linear increase of conductivity (point T1 in Fig. 3c) with the increasing water content. After this linear increase, the slope of the curve starts to decrease again (point T2) and passes a maximum (point T3). For structured solutions -as is the case for microemulsions -these changes in conductivity are explained by transitions between o/w, bicontinuous, and w/o microemulsions. A w/o microemulsion is present for low water content and causes low conductivity. With the increasing water content, percolation of water droplets is observed, causing the formation of conducting water channels by merging water droplets, which leads to a significant change in the slope (point T1). Further, point T2 marks the transition to an oil-rich bicontinuous microemulsion. A subsequent transition to a water-rich bicontinuous microemulsion is observed upon addition of H 2 O. The maximum conductivity represents the presence of an extended water-rich bicontinuous phase (point T3). For very high water contents (x 4 0.9), an o/w microemulsion is formed and dilution effects prevail, causing conductivities to decrease. A comparison of the conductivity curve of this SDS system with the curves of TBA and NPA (Fig. 3b and c) shows many similarities regarding the range of increase, the percolation behaviour and the decrease in conductivity for high water contents. The maximum conductivity for NPA/H 2 O lies in a range of approximately 75-90 mol% water content and for TBA in a range of approximately 85-95 mol% water content. This maximum conductivity coincides with the highest correlation coefficients in DLS and the strongest signal in low q of SWAXS. It is also well known for TBA/H 2 O that the binary mixture displays two eutectics, one of them being located at 94 mol% H 2 O, which also coincides with the range of maximum conductivity. 48 It was found that thermodynamic anomalies and inhomogeneous mixing are most pronounced for this composition even at temperatures above the deep eutectic temperature. The presence of a percolation point around 40 mol% H 2 O in the case of TBA and a conductivity behaviour, see points T1-T3 in Fig. 3b, similar to the SDS system lead to the conclusion that the structuring of TBA/H 2 O is similar to the structuring of H 2 O/SDS/1-pentanol/dodecane. Therefore, we propose the presence of a bicontinuity of water-rich and TBArich domains, as already suggested by the research group of Anisimov et al. for the ternary system H 2 O/TBA/propylene oxide, based on MD simulations and the observation of mesoscale inhomogeneities. 42 However, conductivity measurements here suggest the formation of a bicontinuous phase already in the binary mixture TBA/H 2 O. Apparently, this bicontinuous structuring behaviour is not only restricted to TBA, but is also observable for aqueous NPA mixtures, as suggested by DLS measurements, although to a much smaller extent.
The conductivity curve of EtOH differs strongly from the conductivity curves of IPA, NPA, TBA and SDS regarding the ranges of increase, decrease and the position of the maximum. The small conductivity increase for low water contents might be explained by an enhanced ion dissociation as well as a higher electrophoretic mobility in aqueous media. For the increasing water content, the conductivity decrease can be explained by the excessive dilution of charge carriers. Therefore, it is assumed that microscopic inhomogeneities in the case of EtOH are very weak and cannot be detected in detail by conductivity measurements.
The conductivity of IPA is in between the conductivities of EtOH and NPA indicating a progressive structuring with the increasing aliphatic chain length. Therefore, EtOH/H 2 O is a good example of a weakly structured system and TBA/H 2 O is a representative binary mixture of a system with pronounced structuring. In the next step, three different hydrophobic compounds were dissolved in alcohol/H 2 O binary mixtures, i.e. benzyl alcohol, limonene and DR-13. The difference between these compounds is their miscibility with water. Benzyl alcohol is slightly miscible with H 2 O. Limonene, as well as DR-13, are poorly water miscible compounds. The realms of solubility in the cases of benzyl alcohol and limonene are shown in the ternary phase diagrams in Fig. 4a and b and the OD as a measure of the solubility of DR-13 in Fig. 4c. 49,50 The solubilisation power of the alcohols in the case of benzyl alcohol decreases in the following order: EtOH 4 IPA 4 NPA E TBA, while phase diagrams with NPA and TBA are very similar.
The solubilisation power of the alcohols in the case of limonene gradually increases in the following order: EtOH o IPA o NPA o TBA. Its miscibility with H 2 O is very poor (less than in the case of benzyl alcohol) and therefore the two-phase region is larger than in the case of benzyl alcohol. The solubility of limonene in TBA/H 2 O starts to increase significantly at x(TBA) = 10 mol% (see point T3 in Fig. 4) and at x(TBA) 4 40 mol% and the miscibility gap is closed. Furthermore, and most importantly, the hydrotrope efficiency for the solubilisation of limonene is reversed compared to the solubilisation efficiency of the alcohols considered for benzyl alcohol.
In For EtOH and IPA, no or very weak structuring is observed for their binary mixtures with H 2 O. The addition of benzyl alcohol and limonene, respectively, induces the formation of a well-ordered system. 2,6 Hydrophobic hydration and agglomeration cause the hydrophobic compound to form clusters with accumulation of the hydrotrope mostly at the interface between the benzyl alcohol clusters and the water-rich domain. Consequently, the solubility of the hydrophobic compound is enhanced with increasing hydrotrope concentration. This is in perfect agreement with the ideas forwarded recently. 22,23,51 However, in contrast to weakly structured EtOH/H 2 O and IPA/H 2 O, the situation is completely different for binary prestructured TBA/H 2 O and NPA/H 2 O systems. As a bicontinuous structure is already given, the structure is not induced by the third component, but by the hydrotrope itself. Due to the formation of a bicontinuous system, an aliphatic-rich domain as well as a waterrich domain and a large area of interface are created. In such a case of a pre-structured binary hydrotrope-water system, three possible solubilisation pathways are possible: (i) solubilisation in the water-rich bulk phase (appears only for highly polar solutes which are not considered here), (ii) solubilisation in the aliphatic-rich bulk phase and (iii) solubilisation within the interfacial film between the aliphatic and water-rich pseudo-bulk phases, see Fig. 6.
The aliphatic-rich bulk-like pseudo-phase permits the incorporation of large amounts of hydrophobic components. This is confirmed by the solubilisation power of the hydrotropes in the case of limonene, where TBA shows the highest solubilisation power and EtOH the lowest solubilisation power. Further indications are conductivity measurements for ternary systems H 2 O/alcohol/benzyl alcohol, where the absolute conductivity of NPA and TBA is maintained, indicating the retention of the pre-structures.
The SANS spectrum of one exemplary composition of a ternary mixture D 2 O/TBA/benzyl alcohol (60/32/8 wt%) was compared to a SANS measurement of a binary TBA/H 2 O mixture (40/60 wt%) to further support this fact, see Fig. S1 (ESI †). The substitution of TBA by benzyl alcohol leads to a large increase of the scattered intensity. Analysis of the correlation length of these curves (0.8 nm for the binary mixture and 2.1 nm for the ternary mixture) indicates an enlargement of the correlation length of the TBA/benzyl alcohol aliphatic rich phase. This implies that benzyl alcohol and certainly also TBA are ''driven'' towards the aliphatic rich continuum which is ''blown up'' and causes an increase of the correlation length. Therefore, the structure is reinforced by the addition of benzyl alcohol.
But in the case of benzyl alcohol, the situation is somehow different from the case of limonene, as it contains an alcohol functional group in addition to the aliphatic moiety. This leads us to the assumption that benzyl alcohol is not only dissolved within the aliphatic-rich continuum, due to its low water miscibility, but may also accumulate at the interfacial film, similar to a co-surfactant. Another indicator is the fact that TBA provides the lowest solubilisation power for benzyl alcohol in the series EtOH, IPA and NPA. In EtOH/H 2 O mixtures, benzyl alcohol induces the formation of mesoscale structures, whereas in the case of TBA/H 2 O mixtures, it intercalates into the given pre-structure. As soon as the given pre-structure is completely ''swollen up'' and the interfacial film is saturated, further  addition of benzyl alcohol causes the system to collapse and form two phases.
In the case of the solubilisation of DR-13, the situation is again different from both the limonene and benzyl alcohol solubilisation processes, since DR-13 bears polar functional groups and an aromatic backbone much larger than that of benzyl alcohol. The solubilisation power of the hydrotropes in the case of DR-13 follows the same series as for limonene. However, a closer look at the amount of dissolved DR-13 per amount of the hydrotrope reveals a huge difference of the order of several orders of magnitude. Furthermore, DR-13 is assumed to be not capable of inducing micro-structuring, as the overall solubility in H 2 O and H 2 O/hydrotrope is too low. Therefore, the solubility in EtOH/H 2 O is very low. However, as the solubility increases with progressive structuring of the H 2 O/hydrotrope, we assume that the difference in solubility is based on a completely different solubilisation mechanism as compared to limonene. Instead of a bulk solubilisation within a hydrophobic mesoscale pseudo-phase, we suppose DR-13 to be mostly dissolved within the interfacial film of the two pseudo-bulk phases. This assumption is in good accordance with all results, because an interfacial film provides much less space than a bulky pseudo-phase for the solubilisation of DR-13. The solubility of DR-13 in TBA/H 2 O mixtures starts to increase at point T3 representing the maximum of the water-rich bicontinuous phase, see Fig. 3b and 4c. Beginning from T1 (representing the percolation threshold) the solubilisation power of TBA/H 2 O diminishes compared to the region T3-T1. It is assumed that the interface of pre-structured binary alcohol/H 2 O mixtures is rapidly saturated for low concentrations of DR-13. The further increase of the solubilisation of DR-13 for a higher TBA content (x(TBA) 4 0.4) may be ascribed to bulk solubilisation due to saturation of the interface. Hence, DR-13 may preferentially solubilise at the interface in highly structured regimes of TBA 0.1 o x(TBA) o 0.4, passing over to a more bulk-like solubilisation mechanism for a higher TBA content. A more detailed analysis of the curve shapes clarifies these findings even better. A second-order differentiation of the fitted curves reveals huge differences in the solvent character of the hydrotrope (see Fig. S2, ESI †). In the case of EtOH the curvature of the curve stays always positive over the whole miscibility range whereas there is a negative curvature in the case of TBA in the range of approximately 0.23 o x(TBA) o 0.6. This second order differentiation shows that EtOH possesses a more co-solvent character, whereas TBA shows a hydrotropic behaviour when DR-13 is dissolved. The proposed interfacial solubilisation mechanism is further supported by the fact that DR-13 has a very poor solubility both in pure dodecane and pure water, for which both do not provide an interface at all. As a consequence, DR-13 is also scarcely soluble in poorly structured mixtures, such as EtOH/H 2 O.

Conclusion
We investigated the structuring of alcohol/H 2 O binary mixtures, where the alcohol is miscible with H 2 O in any proportion, i.e. EtOH, IPA, NPA and TBA. DLS, SWAXS, SANS and conductivity measurements revealed microscopic inhomogeneities in the cases of NPA/H 2 O and TBA/H 2 O. As in the case of micellar systems, we infer from conductivity measurements that these microscopic inhomogeneities are similar to direct or reverse micellar solutions (meaning organic aggregates in water or water aggregates in an organic pseudo-phase, respectively) and also, at some concentration ratios, to bicontinuous structuring with rapidly fluctuating water-rich and alcohol-rich domains in equilibrium. In the case of EtOH, no significant structuring could be detected by our methods. IPA marks the transition from a weakly structured system in the case of EtOH to structured systems in the cases of NPA and TBA.