Background

Physical properties of the crystals can be altered by varying the crystal lattice. Size alteration mainly includes agglomeration where small crystals adhere to form bigger particles. Various physical properties such as flow properties can be modified during the crystallization process. Crystal habit can be modified by optimizing the process parameters, like stirring rate, selection of solvent, pH, temperature, etc., which affect the physico-chemical properties (solubility, dissolution rate, bioavailability, and stability) and micrometric properties (bulk density, flow property, compressibility) of the crystals [1, 2].

In crystallization, the solute separates out from the solution as solid. Thus, there is a phase change involved. This change depends on the solubility of solute in the system, which is related to temperature. Crystallization of active pharmaceutical ingredients is carried out in pharmaceutical industries to increase the dissolution rate and reach sufficient bioavailability. It can also enhance the flow properties and drug dosage control. The complex behavior of industrial crystallizers remains elusive. One of the reasons for this is the lack of appropriate tools for measurement and monitoring of crystallization processes. On the other hand, demands for consistent product quality, purity, and crystal size are ever increasing and are therefore creating a large interest in crystallization research. The aim of all crystallization processes is to create a supersaturated solution or melt. The supersaturation becomes the driving force under which new crystals are formed and existing crystals grow. For majority of the substances, solubility increases with temperature. Any solute added in the soluble region dissolves. On the other hand, in the metastable stage, existing crystals will grow but new crystals are not formed. On cooling further, we enter the labile region where spontaneous formation of new crystals; that is nucleation occurs [3, 4].

The crystal growth rate is the rate at which the size of the crystal increases. The nucleation rate is defined as the number of new crystals formed per unit time and volume of suspension. Secondary nucleation can take place at low supersaturation when crystals are already present. Small parts of the existing crystals are washed off and form new nuclei that can grow. Several methods are available for crystallization. The methods that are used for the purpose of this report are solvent evaporation method and cooling crystallization. In solvent evaporation, the solute is dissolved at a constant temperature and pressure, in one solvent in which it is moderately soluble, or in a mixture of two solvents—one of which is a good solvent or co-solvent, and the other which is an anti-solvent, until saturation is achieved. The solvent system is then allowed to evaporate at room temperature, leaving behind the crystals. In cooling crystallization, a saturated solution of the solute is formed in a solvent system, at an elevated temperature just below the boiling point of the solvent system, then allowed to cool, forming crystals [5].

Sulphanilamide has a myriad of uses in the pharmaceutical industry and thus was used as a model drug in this study. It has a chemical formula of C6H8N2O2S (IUPAC name 4-aminobenzenesulfonamide) with a molecular weight of 172.202 g/mol. It is white in color and has a melting point of 165.5 °C. It has a pH range of 5.8–6.1, density of 1.08 at 25 °C. It is an antibacterial agent and often used in pharmaceutics and cosmetics.

In 2019, Rasmuson et al. investigated the growth of single salicylamide crystals in non-stirred experiments. In their study, it was discovered that the solvent system influenced the growth rate and supersaturation. The growth kinetics was also strongly affected by temperature. We expected to see a similar relationship between temperature, solvent system, and crystal structure in this study [6,7,8].

Methods

Chemicals

Sulphanilamide extra pure (99% pure), ethanol (purity 99.7%), heptane (purity 99%), toluene (purity 99 to 99.4%), acetone (purity 99%), and methanol (purity 99.6%) were purchased from Molychem and used with no further purification. The solvent evaporation apparatus consists of a hot plate with temperature probe, a magnetic stirrer, 100 ml beakers, and magnetic beads. Aluminum foil with equal sized holes is used to cover the beakers to allow for uniform slow evaporation. Every foil cap had 18–20 holes of diameter 1 mm with an inter hole distance of 5 mm. All the beakers used were of uniform size. The cooling method apparatus consist of a cooling bath, 100 ml beakers covered with aluminum foil to prevent solvent from evaporating when heated, a heating plate and a mechanical stirrer.

Solvent evaporation

Twenty milliliters of solvent was taken in a 100 ml beaker and kept for stirring at 700 rpm, at 25 °C on a hot plate. Once the system is stable, sulphanilamide was weighed and added. Once a clear solution was formed, the beaker was removed and covered with aluminum foil with holes, and left to evaporate for a given time at room temperature at the desired stirring speed. After the time was elapsed, the foil was removed and any crystals that were formed were collected and sent for analysis. The process was repeated for different time periods, different concentrations of solute and different solvent systems.

Cooling method

Required concentration of clear solution at 50 °C was taken in a beaker and placed in a cooling bath. The temperature was brought down to 5 °C. The solution was then allowed to cool at this temperature for either 4 h or 6 h with the desired stirring speed. After the time elapsed, the sample was removed. Any crystals formed were collected by filtration and sent for analysis. The previous steps were repeated for different concentrations of solutes and different solvents. The samples collected were sent for SEM, XRD, and DSC analysis.

The following concentrations of solutions were taken g/ml where g denotes weight of the solute sulphanilamide and ml represents the volume of solvent:

Acetone : 0.218, 0.1826, 0.1383, 0.1016

Methanol : 0.065, 0.058, 0.05, 0.04

Ethanol : 0.041, 0.032, 0.024, 0.019

Time for solvent evaporation : 12 h, 24 h, 48 h (only in the case of ethanol and methanol systems) and 72 h (only in case of methanol systems)

Time for cooling method : 4 h and 6 h

Stirring speeds : 0 rpm and 100 rpm.

DSC

To notice how the crystals have melted as well as to check whether any reaction has occurred between the solute and the solvent, differential scanning calorimetry scans of the crystals obtained were taken and compared. Here, the samples were heated in an inert environment containing Nitrogen with a gas flow of 50 ml/min on an aluminum crucible. The temperature was increasing at the rate of 10 °C per minute within a range of 26 °C to 200 °C.

X-ray diffraction

The X-ray diffraction was carried out in a copper tube (Cu-K1) with X-rays having a wavelength of 1.506 Å, at a voltage of 40 mV and a current of 30 mA.

SEM analysis

The surface morphology was compared using scanning electron microscopy (Table 1).

Table 1 Summary of the results obtained

Results

In solvent evaporation method, all crystals obtained were of uniform size. It was found that no crystals were formed for ethanol systems with any concentration of solute when the solutions were left to evaporate for time periods of 12 h and 24 h. However, at lower concentrations (0.019 g/ml and 0.024 g/ml), very small needles were formed after evaporation for 48 h when left without stirring and very small crystals were formed only at the highest concentration of 0.041 g/ml in the ethanol system. Similarly for methanol systems no crystals were formed in the first 12 h but when left for 24 h, at lower concentrations (0.04 g/ml and 0.05 g/ml) needles were formed, and at higher concentrations (0.058 g/ml and 0.065 g/ml) small crystals were formed as shown in Fig. 1. When the cubical crystals in the methanol system were left for 48 h and 72 h, crystal growth was observed as shown in Fig. 2. Even when a smaller amount of solute was used in the methanol system with no stir, well defined crystals were observed. The largest crystals formed in methanol systems after 72 h had dimensions 4 × 5 × 2 mm3. For acetone systems, small needles were formed at low concentrations (0.1016 g/ml and 0.1383 g/ml) when left for 24 h for the solvent to evaporate, and small cuboidal crystals were observed at higher concentrations (0.1826 g/ml and 0.218 g/ml). When acetone systems were placed for evaporation with stirring at 100 rpm for 24 h very small needles were formed only at the concentration of 0.218 g/ml as shown in Fig. 3. The largest crystals formed in acetone systems had dimensions 2mmx1mmx1mm. The crystals formed in ethanol systems were irregular in shape and were very small.

Fig. 1
figure 1

SEM image of 0.065 g/ml of solute in methanol obtained by solvent evaporation method carried out for 48 h with no stir (× 100)

Fig. 2
figure 2

SEM image of 0.65 g/ml of solute in methanol obtained by solvent evaporation method carried out for 72 h with no stir (× 60)

Fig. 3
figure 3

SEM image of 0.218 g/ml of solute in acetone obtained by solvent evaporation method carried out for 24 h with 100 rpm stir (× 60)

In Cooling method no crystallization was observed for acetone and ethanol systems. In methanol systems when 0.65g/ml of sulphanilamide was allowed to cool for 4 hrs and 6 hrs, very small irregularly shape crystals were formed with and without stirring. At the low concentrations of 0.04 g/ml and 0.05 g/ml, no crystals were formed.

From the DSC scans shown in Figs. 4 and 5, it can be concluded that the crystals obtained were pure and free of any contamination. The crystal behavior under changing temperature is also seen in these scans.

Fig. 4
figure 4

DSC scan of pure Sulphanilamide. It matches with the DSC scan of commercially available pure sulphanilamide

Fig. 5
figure 5

DSC scan of crystals formed from 0.218 g/ml of solute in acetone obtained from solvent evaporation method carried out for 24 h with stir. The peak at 108 oC shows the crystal losing intrinsic solvent

In order to find the crystallite size, the XRD graphs of the crystals were obtained and the Debye-Scherrer formula was used:

$$ \tau =\frac{k\lambda}{\beta cos\varTheta} $$
$$ \mathrm{Where}\ \tau \mathrm{size}\ \mathrm{of}\ \mathrm{crystal}\ \mathrm{grain},k=\mathrm{shape}\ \mathrm{factor}\ \mathrm{taken}\ \mathrm{as}\ 0.9,\kern0.5em \lambda =\mathrm{X}-\mathrm{ray}\ \mathrm{wavelength}\ \mathrm{taken}\ \mathrm{as}\ 1.5406\ {\AA},\varTheta =\mathrm{Braggs}\ \mathrm{angle} $$

It can be observed that the width of the peaks vary in different samples due to the way the crystal lattice shape and structure changes (Figs. 6 and 7). In some cases, a zero error exists due to rotation of crystal plane, thus the peaks shift more toward a higher two-theta angle value (Figs. 8 and 9). Calculating grain size for the given compounds using Debye-Scherrer formula for the samples taken in Table 2, we found the sizes of crystallites as shown in Table 3. In Table 2, few of the crystal samples obtained by solvent evaporation method that were used to compare crystallite size are shown.

Fig. 6
figure 6

XRD scan of pure sulphanilamide

Fig. 7
figure 7

XRD scan of crystals formed from 0.058 g/ml of solute in methanol obtained by solvent evaporation method carried out for 48 h with no stir

Fig. 8
figure 8

XRD scan of crystals formed from 0.065 g/ml of solute in ethanol obtained by solvent evaporation method carried out for 48 h with no stir

Fig. 9
figure 9

XRD scan of crystals formed by 0.218 g/ml of solute in acetone obtained by solvent evaporation method for 24 h with 100 rpm stir

Table 2 Few of the crystal samples obtained by Solvent Evaporation method
Table 3 Size of crystallite obtained by solvent evaporation method from Table 2

Table 3 shows the size of crystallite in the various crystal samples obtained by solvent evaporation method from Table 2. The 2θ value of some peaks for each sample was taken and the grain size was calculated per Debye-Scherrer formula. Table 4 shows the average size of the crystallites obtained from solvent evaporation method by using values gathered from Table 3. Tables 5 and 6 show the crystallite size and average crystallite size respectively. All the samples shown in this table were obtained by using the cooling method.

Table 4 Average size of the crystallites from solvent evaporation method
Table 5 Crystallite size obtained using the cooling method
Table 6 Average crystallite size of samples obtained using cooling method

Tables 4 and 6 show that there is no apparent trend in increasing concentration of solute and crystallite size.

Discussion

The crystals obtained in methanol and acetone by solvent evaporation method are very different. In pure sulphanilamide, the powder exists in irregular shapes and the surface is fairly rough as it is seen in Fig. 10. Crystals formed in ethanol, which are much smaller, demonstrate a similar irregularity as shown in Fig. 11. However, the crystals formed in acetone and methanol are smoother, have well defined edges and are more uniform in size. It can also be seen by comparing Fig. 12 and Fig. 3 that the crystals formed in acetone, under conditions with stir, are not as well defined and are much smaller than those obtained without stirring. They are also irregular in shape and size, and have rough surfaces. In this work, the crystals formed by the cooling method are very small, irregular, and not well defined as shown in Figs. 13 and 14. The cooling method albeit being faster is more difficult to control and is more cumbersome. For observing crystal growth, the solvent evaporation method is most ideal. The selection of solvents for the crystallization process has a major impact on the results and is a crucial step in the crystallization process.

Fig. 10
figure 10

SEM image of pure sulphanilamide (× 200)

Fig. 11
figure 11

SEM image of 0.041 g/ml ethanol obtained by solvent evaporation method. Process conditions: 48 h without stir (× 200)

Fig. 12
figure 12

SEM image of 0.218 g/ml of solute in acetone obtained by solvent evaporation method carried out for 24 h with no stir (× 60)

Fig. 13
figure 13

SEM image of 0.058 g/ml methanol obtained from cooling method. Process conditions: 4 h with no stir (× 500)

Fig. 14
figure 14

SEM image of 0.065 g/ml methanol obtained from cooling method. Process conditions: 6 h with no stir (× 85)

The knowledge of the influence of process conditions on the crystal growth of sulphanilamide allows one to create more efficient batch modes of purification of the solute by means of crystallization. It also allows one to carry out further work leading to spherical crystallization of the solute, as well as understanding how crystallization occurs in solvent systems having binary mixtures of solvents. As this is the initial study on the crystal growth of sulphanilamide, it gives us knowledge and guides to do further studies.

Conclusion

The crystals obtained from using methanol with high concentration of solute gave the most uniform and large-sized cubic crystals under solvent evaporation method. The surface of the crystal was also seen to be smooth with well-defined edges as shown in the SEM images. Methanol systems need to be left for evaporation for longer periods of time to obtain larger crystals. The solvent evaporation method used with continuous stirring did not give favorable results. With acetone, the solute formed cuboidal crystals. It is preferred to use higher concentrations of solutes to get saturated solutions for this method. Acetone systems can be left for shorter time than methanol systems. Crystal formation is not favorable in ethanol systems. The cooling method is not suitable to get uniform crystals. The XRD analysis of crystals was carried out along with DSC of the crystals. Data on the melting characteristics was obtained from DSC and crystallite size was obtained using Debye-Scherrer formula. The parameters were compared for both the methods—cooling method and solvent evaporation method.