1 Introduction

Diatomites are inorganic materials originating from rock sedimentation and formed by an accumulation of seaweed skeletons [1, 2]. These materials contain a large amount of silicon and some aluminum. They are usually applied as adsorbents and catalysts, for example, in the removal of Zn(II) from aqueous solutions [3] or as supports in the dry reforming of methane [4]. Another possible application is their use as alternative raw materials for green synthesis [5], in the same way that kaolin is used for zeolite synthesis [6]. Diatomites are inexpensive and available natural materials, but as their origins are diverse, it is interesting to perform a complete characterization and comparison for possible applications.

Removal of dyes from effluents is extremely important as they are toxic compounds, particularly under prolonged exposure and can cause various symptoms such as vomiting, diarrhea, increased heart rate and even necrosis of human tissues [7]. Examples of dyes are methylene blue, C13H18N3ClS, and rhodamine B, C28H13N2O3Cl, which are both used in industry. Their chemical structures are shown in Fig. 1, and their difference in size is demonstrated. Several studies have proposed natural materials for adsorption [8,9,10,11]. However, due to the characteristics of natural products varying from one origin to another, the elimination of dyes from residual water is still a problem to solve. Some dye adsorption studies with diatomites have already been reported [12, 13], which shows the importance of continued testing to normalize their application with the origin of the natural material.

Fig. 1
figure 1

Representation of rhodamine B (a) and methylene blue (b) using a free version of ChemSketch [14]

Due to the reported ability of diatomites as adsorbents in the literature, the aim of this work is to fully characterize and compare diatomites from different Brazilian locations and to study their application in the adsorption of methylene blue and rhodamine B.

2 Materials and methods

The diatomites studied in this article are from two Brazilian states: Rio Grande do Norte (denoted as D1 and D2, depending on the deposit in which they were obtained) and Bahia (denoted as D3).

These materials were characterized by X-ray fluorescence (XRF) on a Bruker S2 Ranger (Billerica, MA, USA) with Pd radiation, a Ag anode and an XFlash® SiliconDrift detector. X-ray diffraction (XRD) measurements were obtained on a Bruker D2 Phaser (Billerica, MA, USA) with a LynxEye detector and Cu radiation. The samples were also studied by scanning electron microscopy (SEM) on a Hitachi TM3000 (Chiyoda, Tokyo, Japan). Thermogravimetric (TG/DTG) analysis was performed on a TA Instruments SDTQ600 equipment (New Castle, Delaware, USA) by weighing 10 mg in a platinum crucible and using a N2 purge gas at 50 mL/min with a heating rate of 10 °C/min. Measurements of mercury intrusion–extrusion porosimetry for the materials under study were carried out using a porosimeter Autopore III 9410 (Micromeritics, Norcross, GA, USA) from 0.002 up to 240 MPa.

The experiments adsorbing the dyes rhodamine B (Sigma-Aldrich, ≥ 95%) or methylene blue (Sigma-Aldrich, ≥ 95%) were performed in triplicate. The three diatomites were separately used as adsorbents (one diatomite per adsorption experiment). First, a 7 ppm solution of a chosen dye was prepared in deionized water. Second, 50-mL aliquots of the previous solution were transferred to several Erlenmeyer flasks containing 100 mg of the chosen diatomite. The suspensions were stirred for different times (2, 5, 10 and 20 min). Subsequently, 4 mL of the resulting solution was filtered through 0.2-μm nylon filters, and the solution was read in a spectrophotometer (HachDR500), recording the absorbances at a 553 nm wavelength for rhodamine B or at a 665 nm wavelength for methylene blue. The concentration of the measured solutions was obtained after applying the Lambert–Beer equation [15]: Abs = a·b·c, where Abs is the absorbance, c is the concentration in ppm, b is the optical path (1 cm), and a is the absorptivity coefficient in mL μg−1 cm−1. The efficiency was calculated by having previously measured the exact concentration of the starting solution in the spectrophotometer. The formula used was [16]: efficiency (%) = 100·(c0 − c)/c0, where c0 is the initial concentration and c is the concentration measured at the time of adsorption.

3 Results and discussion

The three diatomite samples, D1, D2 and D3, were analyzed by X-ray fluorescence (XRF). Table 1 collects the results, showing that their composition was essentially Si and Al, with D3 having a higher aluminum content than D1 and D2. The Si/Al ratios of the diatomites resulted in 23.6, 11.9 and 6.0 for D1, D2 and D3, respectively. Comparing our Si/Al results to those obtained by Yuan et al. [17] on the chemical composition of diatomites from China (Si/Al = 8.4), Australia (Si/Al = 20.6) and the USA (Si/Al = 12.6), we found a wider Si/Al range in just one country, so it is necessary to choose the diatomite with the needed composition.

Table 1 Composition of diatomites

X-ray diffraction (XRD) results of the diatomite samples are shown in Fig. 2. All the diffractograms were characteristic of amorphous materials, which is the representative phase of diatomites accompanied by a quartz impurity (2θ = 21° and 27°). Sample D2 contained the highest quartz content, as the intensity of the Bragg reflection corresponding to quartz was the highest among all the samples.

Fig. 2
figure 2

X-ray diffractograms of the diatomite samples

The micrographs from scanning electron microscopy (SEM) (Fig. 3) presented the samples as inhomogeneous objects with different particle sizes and shapes, such as navicular morphology or fishbones. Some of these structures were also coincident with those reported by Liu et al. [18] for Chinese diatomites.

Fig. 3
figure 3

Micrographs of the D1 (a), D2 (b) and D3 (c) diatomites

The thermogravimetric analyses of the three diatomites (Fig. 4) presented a single event: a mass loss of 1–2% until approximately 250 °C, which is related to the adsorbed water and unidentified small organic molecules possibly adsorbed on the surface or inside the pores. Different porosity probably caused the small variations observed between the diatomites, as we will explain later.

Fig. 4
figure 4

Thermogravimetric curves of the diatomites (TG/DTG)

The three diatomites were studied by mercury intrusion–extrusion porosimetry because macropores appeared in the SEM micrographs. The resulting curves are shown in Fig. 5. The results presented an abrupt mercury intrusion (in the pressure range of 0.01–10 MPa), indicating that the samples presented a well-defined porosity in the macropore range, as shown in a pore size distribution (PSD). The PSD profile of the samples has a unimodal distribution with modal pore sizes of 1.8 μm, 2.2 μm and 4.8 μm for D1, D2 and D3, respectively. The macropore sizes of these Brazilian diatomites were larger than those reported by Liu et al. [18] describing a modal macropore size of 0.7 μm.

Fig. 5
figure 5

Mercury intrusion–extrusion curves (a) and pore size distribution of the diatomite samples (b). Three different symbols show the different data for the D1 (spheres), D2 (triangles) and D3 (squares) diatomites

The textural properties of the samples are shown in Table 2. Sample D1 had the highest density (bulk and skeletal) and consequently the lowest total pore volume. Sample D3 presented the lowest specific surface area, porosity and skeletal density. These differences between the samples seemed to be the cause of the different losses found in the thermogravimetric analysis, as different quantities of small molecules could be adsorbed on the pores or the surface depending on how porous a material is. This fact justified our interest in testing dye adsorption as a less expensive and natural alternative for decontamination.

Table 2 Textural properties of the diatomite samples

The dye adsorption experiments were started by obtaining two calibration curves, one per dye that allowed us to experimentally calculate the absorptivity coefficients according to the Lambert–Beer law by linear adjustment. The values of these coefficients were 0.12 mL μg−1 cm−1 for methylene blue (R2 = 0.9995) and 0.20 mL μg−1 cm−1 for rhodamine B (R2 = 0.9999).

Then, the adsorption experiments were continued by testing rhodamine B as a contaminant. The results are shown in Fig. 6a. The three diatomites reached equilibrium after 10 min, with an adsorption efficiency of approximately 65% for all the materials. This maximum value is due to the larger size of the rhodamine B molecule, which probably did not differentiate between the pores and the external surface as adsorption sites.

Fig. 6
figure 6

Experimental data from the adsorption experiments: rhodamine B (a) and methylene blue (b). The efficiency was calculated from the measurements performed after 2, 5 10 and 20 min of adsorption. Each diatomite is represented by a color and a pattern (D1: light gray—forward slash; D2: dark gray—backslash; D3: white—zigzag)

Methylene blue adsorption results (Fig. 6b) were more interesting for these materials. The maximum adsorption (96%) and equilibrium was rapidly reached after 2 min of adsorption when testing the D2 diatomite. This result was directly related to D2 having the highest porosity and pore volume. The other two diatomites achieved their maximum adsorptions and equilibrium after 5 min, adsorbing 90% and 77% in D3 and D1, respectively. Again, these results were in accordance with the order of pore volume observed with the mercury intrusion–extrusion porosimetry analysis.

In agreement with the results from both dye adsorption experiments, the porous structure of the diatomites proved to be an important characteristic directly related to the efficiency of the application. Another characteristic important for the dye–diatomite interaction is the hydroxyl species and acid sites present on the diatomite surface. This type of research was already performed by Yuan et al. [19] studying several Chinese diatomites. As a proposal for further study, it will be interesting to continue with a comparative study between Brazilian and Chinese diatomites.

4 Conclusions

The complete characterization of the diatomite samples shows that they are amorphous heterogeneous materials, and their differences in composition and porosity are the main interests for possible applications. In this article, we tested two different contaminant dyes for adsorption in Brazilian diatomites. Our results showed a direct relationship between the adsorption efficiency and the pore structure and volume. For instance, our analysis of the mercury porosimetry data presented the D3 diatomite as the material with the smallest specific area, porosity and apparent density. Moreover, the D1 diatomite had the highest bulk and apparent densities but the lowest total pore volume. When these materials were tested in adsorption, the D2 diatomite showed a better removal efficiency of methylene blue; the dye removal efficiency of the other diatomites followed the same order as their pore volume. However, testing rhodamine B resulted in equal efficiencies for all the samples due to the larger size of the dye molecule.

In conclusion, even though the different intrinsic characteristics of the diatomites proved to influence their performance under a certain application, these materials were good dye adsorbents. Thus, better knowledge of the diatomite structures from different origins will help tailor their use for more efficient results. This research work focused on Brazilian diatomites to be able to transfer the knowledge to industry in a way that it would be possible to apply them directly. The application chosen was directly related to one of the most concerning problems, which is existing contamination, and the characterization results indicated which of the diatomite sources would be best for particular cases. Other contaminants may be chosen for future work and tested following the description presented in this article.