N. Sudheesh‡
,
Manu Vasudevan§
,
Haresh M. Mody,
Hari C. Bajaj and
Ram S. Shukla*
Discipline of Inorganic Materials and Catalysis, Council of Scientific and Industrial Research, Central Salt and Marine Chemicals Research Institute, G. B. Marg, Bhavnagar, Gujarat – 364 002, India. E-mail: rshukla@csmcri.org; sudhinarayanan@gmail.com; Fax: +91 278 2566970; Tel: +91 278 2567760
First published on 16th December 2014
Investigations on the time dependent analysis of the structural and textural properties of the mesoporous silica material MCM-41 were performed by analyzing the samples at regular intervals for one year by powder X-ray diffraction (PXRD) and nitrogen sorption techniques for samples stored (i) under a dry nitrogen atmosphere in a glove box and (ii) under dry ambient atmospheric conditions. The stability and durability of this high surface area material gave promising results under both storage conditions in terms of its structural and textural properties. Under the typical storage conditions employed, the values of various textural properties, including the surface area (SA, m2 g−1), pore volume (PV, cm3 g−1), pore diameter (PD, Å) and wall thickness (WT, Å) determined by nitrogen adsorption were found to be 1030 ± 49, 1.015 ± 0.066, 27.55 ± 0.60 and 17.04 ± 0.61 respectively for the glove box samples. Almost identical values (SA = 1022 ± 45 m2 g−1), (PV = 0.933 ± 0.065 cm3 g−1), (PD = 27.54 ± 0.14 Å), (WT = 16.58 ± 0.81 Å) were obtained for the samples under ambient atmospheric conditions. The experimental analysis indicated that this material has potential as a standard reference material for the analysis of the multi-textural characteristics of high surface area mesoporous materials.
Every instrument and apparatus has to be standardized and calibrated at appropriate intervals to ensure accurate and precise performance and data collection. Many of these instrument techniques need a reference material or standard for calibration. Surface area and pore size analyzers need standard reference materials for calibration. The Institute for Reference Materials and Measurements (IRMM), the Bundesanstalt für Materialforschung und-prüfung (BAM) and the National Institute of Standards and Technology (NIST) are major suppliers of surface area standards,12–14 and reference standards with surface areas ranging from 0.0686 to 258.0 m2 g−1 are available. The BAM is the major producer and supplier of reference standards for pore size analysis. CRM BAM-PM-103 and CRM BAM-PM-104 are the standards for pore size analysis. The high surface area standards are activated nanoporous carbon BAM-P108 with a BET surface area of 550 ± 5 m2 g−1 and BAM-P109 with a BET surface area of 1396 ± 24 m2 g−1.
Although different materials like alumina and silica are used as reference materials for surface area analysis, only alumina based materials have been developed as reference materials for pore size analysis. However, majority of the reference standards for surface area and pore size analysis are related to alumina. Studies have been conducted to develop more silica based reference standard materials. Gel-derived silica was investigated for its textural properties and was developed as a standard reference material.15–17 This gel-derived silica had a surface area of 165.5 m2 g−1 and a pore radius of 11.9 nm. So it is well understood that most of these standard reference materials are of lower surface area when compared with high surface area carbon, mesoporous silica and MOFs. Many of the recently developed porous materials are mesoporous materials of very large surface area. The prominent features of periodic mesoporous materials are: very high surface areas, well defined pore shapes, narrow distributions of pore sizes, very high degrees of pore order, the ability to tailor and fine tune the pore dimensions, large pore volumes, large amounts of internal hydroxyl groups, the ease of modification of surface properties, enhanced catalytic selectivity and excellent thermal and mechanical stabilities. The advantages associated with these properties include: (i) permitting free ingress of reactants and egress of product species that have cross-sections smaller than the diameter of the pores, (ii) offering a greater scope for the grafting of organometallic moieties onto the inner surface of the pores for the heterogenization of homogeneous catalysts and (iii) opening up new strategies for the production of novel materials like porous carbons and other composite materials. There is a pressing need to develop a standard from these high surface area materials. For a material to have the potential to be developed as a reference material, it is necessary to qualify the durability and stability. Durability refers to the performance over a period of time and stability refers to the performance on repeated usage.
Mobil Composition of Matter, MCM-41,18 has a large surface area and nanometer-sized pore sizes (from 20 to 100 Å) and finds application in adsorption,19 separation,20 catalysis21,22 and sensing.23 It also offers a special environment for the chemical separation of large molecules.24 It has a simple structure and an easy synthesis procedure. It is the most suitable model mesopore adsorbent available for studying some of the fundamental features of adsorption, such as the effects of pore size, hysteresis, etc., owing to its relatively uniform cylindrical/hexagonal pore channels. It is characterized by parallel and ideally shaped pore structures without the complications of a network. The cylindrical pore structure and high degree of pore symmetry associated with MCM-41 merit it as a representative mesoporous material for the testing of existing adsorption and diffusion models.25 Our intense research activities on mesoporous material based catalysis1–5,26–28 and these specific properties of MCM-41 led us to carry out investigations on its use as a standard. Therefore to the best of our knowledge, we herein report the first investigation into the development of the ordered mesoporous material MCM-41 (ref. 18), associated with a high surface area, as a reference material with the potential to analyze properties such as surface area, pore volume, pore diameter and wall thickness as a single standard.
In the present investigations the well-known material MCM-41 was hydrothermally synthesized and studied for its durability and stability at regular intervals for a period of one year. A nitrogen adsorption–desorption technique is used for the characterization of the textural properties of solid materials. Microporous and mesoporous materials can be studied using this technique to measure the surface area, pore volume, pore diameter and wall thickness etc. Additionally, powder X-ray diffraction (PXRD) of MCM-41 was performed over a period of one year to study the effect of storage on the structural properties of the material.
PXRD analysis was recorded using a Rigaku-MiniFlex instrument, Japan, with Ni filtered Cu Kα radiation (1.54056 Å) at 30 kV and 15 mA in the 2θ range of 1.0° to 8.0° at a scan speed of 0.25° min−1. The peak positions and peak intensity were obtained from the instrument’s software. The surface area, pore volume, pore diameter and wall thickness were determined by N2 adsorption at 77.3 K using an automated surface area and pore size analyzer (Quadrasorb SI, Model no: 3SI-9, Quantachrome Instruments, USA) with a pressure tolerance (ads/des) of 0.050/0.050, equilibrium time (ads/des) of 200/200 s, and equilibrium timeout (ads/des) of 400/400 s. The samples were degassed at 300 °C for 3 h prior to analysis. A multi-point BET plot was plotted between P/P0 of 0.08 to 0.234. The pore size distribution analysis was performed using a BJH method using the desorption branch of the isotherm, and the total pore volume was calculated from the adsorption data at ∼0.99 P/P0.
The data obtained from the PXRD analyses are given in Table 1. The values of 2θ for the (100) plane were calculated from the experimental values of 2θ for the 110, 200 and 210 planes by eqn (1)–(3).
2θ(d100) = 2θ(d110)/√3 | (1) |
2θ(d100) = 2θ(d200)/2 | (2) |
2θ(d100) = 2θ(d210)/√7 | (3) |
Sample | Parameter | d100 (Å) | d110 (Å) | d200 (Å) | d210 (Å) | Standard deviation | Unit cell a0, Å |
---|---|---|---|---|---|---|---|
a XRD conditions: 2θ = 1–10°, scan speed = 0.25, sampling width = 0.02, kV = 30, mA = 15. | |||||||
SN1 (as synthesized) | 2θ experimental | 2.018 | 3.580 | 4.110 | 5.376 | 49.38 | |
2θ(d100) calculated | 2.018 | 2.067 | 2.055 | 2.032 | 0.0221 | ||
d Spacing experimental | 43.70 | 24.69 | 21.48 | 16.43 | |||
d Spacing (d100) calculated | 43.70 | 42.76 | 42.96 | 43.47 | 0.4354 | ||
Intensity, cps | 1407 | 178 | 123 | 93 | |||
SN2 (freshly calcined) | 2θ experimental | 2.274 | 3.957 | 4.540 | 6.010 | 44.62 | |
2θ(d100) calculated | 2.274 | 2.284 | 2.270 | 2.271 | 0.0065 | ||
d Spacing experimental | 38.81 | 22.31 | 19.43 | 14.70 | |||
d Spacing (d100) calculated | 38.81 | 38.64 | 38.86 | 38.89 | 0.1113 | ||
Intensity, cps | 4460 | 538 | 328 | 120 |
Similarly the d spacing of 100 planes were calculated by eqn (4)–(6).
d100 = d110 × √3 | (4) |
d100 = d200 × 2 | (5) |
d100 = d210 × √7 | (6) |
There is an improvement in the regularity of the material after calcination as indicated by the decrease in values of standard deviation for 2θ and d100 spacing.
a0 = (2 × d100)/√3 | (7) |
The first analysis was carried out in quadruplicate for the freshly calcined material and the rest of the analyses were done at regular intervals of two months in triplicate and their mean and standard deviation are given in Tables 1S and 2S (ESI†). The observed surface area, pore diameter, pore volume and wall thickness at different months are given in Fig. 5–8. The mean values of the surface area for the samples in the glove box (Table 1S†) were in the range 975–1099 m2 g−1 with a standard deviation range of 2.2–70.6. Under atmospheric conditions in closed vials (Table 2S†), the mean values of the surface area were in the range 977–1082 m2 g−1 with a standard deviation range of 2.2–71.6. The standard deviations for the surface area analyses carried out at 4 months were the highest for both the glove box sample and atmospheric conditions sample. The variation in the results may be attributed to experimental error. This variation is prominent only in the case of 4 month samples, which is indicative of a problem associated with the analytical handling of the sample, either from human or instrumental error. The surface area was calculated from a 5 point BET plot. Therefore any variations in these points can lead to higher percentage error in the surface area. Even a small change in the degassing or even the analytical conditions can affect the result. From the PXRD results (Fig. 9 and 10) it is clear that there is no change in its structural feature.
Analytical results of textural properties of the material stored under glove box and atmospheric conditions for different time intervals revealed that there is good reproducibility in the values of the surface area, pore volume, pore diameter and wall thickness under the employed time of analysis over a period of one year. To assign a single value for all these textural properties for both the samples stored in glove box and atmospheric conditions, overall means of all the values and standard deviations were taken corresponding to all the four properties and are given in Table 2. Almost identical values were found for all the four parameters for the MCM-41 stored under glove box and atmospheric conditions.
Storing system | Value | BET SA, m2 g−1 | Total PV, cm3 g−1 | BJH adsorption PD, Å | Wall thickness, Å |
---|---|---|---|---|---|
Glove box conditions | Mean value | 1030 | 1.015 | 27.55 | 17.04 |
Standard deviation | 49.0 | 0.066 | 0.60 | 0.61 | |
% Standard deviation | 4.8 | 6.5 | 2.2 | 3.6 | |
Atmospheric conditions | Mean value | 1022 | 0.933 | 27.54 | 16.58 |
Standard deviation | 45.0 | 0.065 | 0.14 | 0.81 | |
% Standard deviation | 4.4 | 6.9 | 0.5 | 4.9 |
The wall thickness of the material is amorphous in nature. Therefore it can vary with changes in the synthetic procedure. The rate of addition of reagents and the hydrothermal temperature can contribute to the wall thickness. The wall thickness for each batch can vary if the synthesis is not performed according to a uniform procedure. However, by calculating the wall thickness of the standard materials, one can prove whether the structure has collapsed during storage. The collapse of the structure results in a variation of the wall thickness and thus a stable wall thickness means a stable porous material.
It is of interest to compare MCM-41 with existing high surface area standards BAM-P108 and BAM-P109. They are nanoporous carbon based systems with a high surface area. The lower surface area standard BAM-P108 has a surface area of 550 ± 5 m2 g−1. The high surface area standard BAM-P109 has a surface area of 1396 ± 24 m2 g−1. It has to be noted that these standards are microporous materials and hence the BET surface area analysis is conducted between the relative pressure ranges of 0.001 and 0.1. There are many surface area instrumental systems which do not go to such low relative pressures. These instruments are intended to be used for the analysis of mesoporous materials. Therefore standards based on microporous materials are not suitable for the standardization of such surface area analyzers. In the present study, a BET plot was plotted between P/P0 values of 0.08 to 0.25 and the surface area was found. Therefore MCM-41 like materials are better suited to study surface areas in this range.
I(d100) × 2θ(d100) = A | (8) |
I(d100) × 2θ(d100 calculated by eqn 1) = B | (9) |
I(d200) × 2θ(d100 calculated by eqn 2) = C | (10) |
I(d210) × 2θ(d100 calculated by eqn 3) = D | (11) |
2θ(d100)WA = (A + B + C + D)/(I(d100) + I(d210) + I(d200) + I(d210)) | (12) |
Similarly the WA of the d spacing was calculated by replacing the 2θ values with d spacing in eqn (8)–(12).
In both cases, for the samples stored in the glove box and under ambient conditions, there was not much change in the 2θ values, and hence d spacing, with time. Considering the results of the PXRD analyses of samples aged for 2 months and 4 months (Fig. 10), a decrease in the peak intensity is observed for the samples stored under atmospheric conditions. However, there is not much change in the intensity upon further aging. Furthermore, there were no regular trends of decrease or increase in the values of the peak intensities with time. However, they vary randomly and that may be attributed to the experimental errors of analysis. Qualitatively it can be concluded from the results of PXRD analyses of the samples stored in a glove box and under atmospheric conditions that the structure of MCM-41 remained the same during the period of analysis.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra11509k |
‡ Present address: Department of Chemistry, N. S. S. College, Pandalam, Pathanamthitta, Kerala – 689501, India. |
§ Present address: Department of Chemistry, St. Gregorious College, Kottarakkara, Kollam, Kerala – 691531, India. |
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