Hydrogen storage Molecular hydrogen has the highest
specific energy of any fuel. However, unless the hydrogen gas is compressed, its volumetric energy density is very low, so the transportation and storage of hydrogen require energy-intensive compression and liquefaction processes. Therefore, development of new hydrogen storage methods which decrease the concomitant pressure required for practical volumetric energy density is an active area of research. Materials with high porosity and high surface area such as MOFs have been designed and synthesized in an effort to meet these targets. These adsorptive materials generally work via physical adsorption rather than chemisorption due to the large
HOMO–LUMO gap and low HOMO energy level of molecular hydrogen. A benchmark material to this end is MOF-177 which was found to store hydrogen at 7.5 wt % with a volumetric capacity of 32 g L−1 at 77 K and 70 bar. MOF-177 consists of [Zn4O]6+ clusters interconnected by 1,3,5-benzenetribenzoate organic linkers and has a measured
BET surface area of 4630 m2 g−1. Another exemplary material is PCN-61 which exhibits a hydrogen uptake of 6.24 wt % and 42.5 g L−1 at 35 bar and 77 K and 2.25 wt % at atmospheric pressure. PCN-61 consists of [Cu2]4+ paddle-wheel units connected through 5,5,5-benzene-1,3,5-triyltris(1-ethynyl-2-isophthalate) organic linkers and has a measured BET surface area of 3000 m2 g−1. Despite these promising MOF examples, the classes of synthetic porous materials with the highest performance for practical hydrogen storage are
activated carbon and
covalent organic frameworks (COFs).
Design principles Practical applications of MOFs for hydrogen storage are met with several challenges. For hydrogen adsorption near room temperature, the hydrogen
binding energy would need to be increased considerably. There is considerable effort being put forth in developing MOFs composed of other light main group metal ions, such as magnesium in Mg4(bdc)3.
Surface area The general trend in MOFs used for hydrogen storage is that the greater the surface area, the more hydrogen the MOF can store. High surface area materials tend to exhibit increased micropore volume and inherently low bulk density, allowing for more hydrogen adsorption to occur. The interaction between hydrogen and uncharged organic linkers is not this strong, and so a considerable amount of work has gone in synthesis of MOFs with exposed metal sites, to which hydrogen adsorbs with an enthalpy of 5–10 kJ/mol. Synthetically, this may be achieved by using
ligands whose geometries prevent the metal from being fully coordinated, by removing
volatile metal-bound solvent molecules over the course of synthesis, and by post-synthetic impregnation with additional metal cations. however, their high metal-hydrogen
bond dissociation energies result in a tremendous release of heat upon loading with hydrogen, which is not favorable for
fuel cells. To compensate for this, specially constructed storage containers are required, which can be costly. Strong metal-ligand bonds, such as in metal-imidazolate, -triazolate, and -pyrazolate frameworks, are known to decrease a MOF's sensitivity to air, reducing the expense of storage.
Pore size In a microporous material where
physisorption and weak
van der Waals forces dominate adsorption, the storage density is greatly dependent on the size of the pores. Calculations of idealized homogeneous materials, such as graphitic carbons and
carbon nanotubes, predict that a microporous material with 7 Å-wide pores will exhibit maximum hydrogen uptake at room temperature. At this width, exactly two layers of hydrogen molecules adsorb on opposing surfaces with no space left in between. 10 Å-wide pores are also of ideal size because at this width, exactly three layers of hydrogen can exist with no space in between.
Structural defects Structural defects also play an important role in the performance of MOFs. Room-temperature hydrogen uptake via bridged
spillover is mainly governed by structural defects, which can have two effects: :1) a partially collapsed framework can block access to pores; thereby reducing hydrogen uptake, and :2) lattice defects can create an intricate array of new pores and channels causing increased hydrogen uptake. Structural defects can also leave metal-containing nodes incompletely coordinated. This enhances the performance of MOFs used for hydrogen storage by increasing the number of accessible metal centers. Finally, structural defects can affect the transport of
phonons, which affects the
thermal conductivity of the MOF.
Hydrogen adsorption Adsorption is the process of trapping atoms or molecules that are incident on a surface; therefore the adsorption capacity of a material increases with its surface area. In three dimensions, the maximum surface area will be obtained by a structure which is highly porous, such that atoms and molecules can access internal surfaces. This simple qualitative argument suggests that the highly porous metal-organic frameworks (MOFs) should be excellent candidates for hydrogen storage devices. Adsorption can be broadly classified as being one of two types:
physisorption or
chemisorption. Physisorption is characterized by weak
van der Waals interactions, and bond enthalpies typically less than 20 kJ/mol. Chemisorption, alternatively, is defined by stronger
covalent and
ionic bonds, with bond enthalpies between 250 and 500 kJ/mol. In both cases, the
adsorbate atoms or molecules (i.e. the particles which adhere to the surface) are attracted to the adsorbent (solid) surface because of the surface energy that results from unoccupied bonding locations at the surface. The degree of
orbital overlap then determines if the interactions will be physisorptive or chemisorptive. Adsorption of molecular hydrogen in MOFs is physisorptive. Since molecular hydrogen only has two electrons, dispersion forces are weak, typically 4–7 kJ/mol, and are only sufficient for adsorption at temperatures below 298 K.
Determining hydrogen storage capacity Two hydrogen-uptake measurement methods are used for the characterization of MOFs as hydrogen storage materials:
gravimetric and
volumetric. To obtain the total amount of hydrogen in the MOF, both the amount of hydrogen absorbed on its surface and the amount of hydrogen residing in its pores should be considered. To calculate the absolute absorbed amount (
Nabs), the surface excess amount (
Nex) is added to the product of the bulk density of hydrogen (ρbulk) and the pore volume of the MOF (
Vpore), as shown in the following equation: N_{\rm abs}=N_{\rm ex} + \rho_{\rm bulk} V_{\rm pore}
Gravimetric method The increased mass of the MOF due to the stored hydrogen is directly calculated by a highly sensitive microbalance.
Volumetric method The changing of amount of hydrogen stored in the MOF is measured by detecting the varied pressure of hydrogen at constant volume.
Other methods of hydrogen storage There are six possible methods that can be used for the reversible storage of hydrogen with a high volumetric and gravimetric density, which are summarized in the following table, (where is the gravimetric density, is the volumetric density,
T is the working temperature, and
P is the working pressure): Of these, high-pressure gas cylinders and liquid hydrogen in cryogenic tanks are the least practical ways to store hydrogen for the purpose of fuel due to the extremely
high pressure required for storing hydrogen gas or the extremely
low temperature required for storing hydrogen liquid. The other methods are all being studied and developed extensively. Currently there are two routes: 1. Using MOFs as precursors to prepare electrocatalysts with carbon support. 2. Using MOFs directly as electrocatalysts. However, some results have shown that some MOFs are not stable under electrochemical environment. The electrochemical conversion of MOFs during electrocatalysis may produce the real catalyst materials, and the MOFs are precatalysts under such conditions. Therefore, claiming MOFs as the electrocatalysts requires
in situ techniques coupled with electrocatalysis.
Biological imaging and sensing A potential application for MOFs is biological imaging and sensing via
photoluminescence. A large subset of luminescent MOFs use lanthanides in the metal clusters.
Lanthanide photoluminescence has many unique properties that make them ideal for imaging applications, such as characteristically sharp and generally non-overlapping emission bands in the visible and near-infrared (NIR) regions of the spectrum, resistance to photobleaching or "blinking", and long luminescence lifetimes. However, lanthanide emissions are difficult to sensitize directly because they must undergo
LaPorte forbidden f-f transitions. Indirect sensitization of lanthanide emission can be accomplished by employing the "antenna effect", where the organic linkers act as antennae and absorb the excitation energy, transfer the energy to the excited state of the lanthanide, and yield lanthanide luminescence upon relaxation. A prime example of the antenna effect is demonstrated by MOF-76, which combines trivalent lanthanide ions and
1,3,5-benzenetricarboxylate (btc) linkers to form infinite rod SBUs coordinated into a three dimensional lattice. As demonstrated by multiple research groups, the BTC linker can effectively sensitize the lanthanide emission, resulting in a MOF with variable emission wavelengths depending on the lanthanide identity. Additionally, the Yan group has shown that Eu3+- and Tb3+- MOF-76 can be used for selective detection of acetophenone from other volatile monoaromatic hydrocarbons. Upon acetophenone uptake, the MOF shows a very sharp decrease, or
quenching, of the luminescence intensity. For use in biological imaging, however, two main obstacles must be overcome: • MOFs must be synthesized on the nanoscale so as not to affect the target's normal interactions or behavior • The absorbance and emission wavelengths must occur in regions with minimal overlap from sample autofluorescence, other absorbing species, and maximum tissue penetration. Regarding the first point, nanoscale MOF (NMOF) synthesis has been mentioned in an earlier section. The latter obstacle addresses the limitation of the antenna effect. Smaller linkers tend to improve MOF stability, but have higher energy absorptions, predominantly in the ultraviolet (UV) and high-energy visible regions. A design strategy for MOFs with
redshifted absorption properties has been accomplished by using large, chromophoric linkers. These linkers are often composed of polyaromatic species, leading to large pore sizes and thus decreased stability. To circumvent the use of large linkers, other methods are required to redshift the absorbance of the MOF so lower energy excitation sources can be used. Post-synthetic modification (PSM) is one promising strategy. Luo et al. introduced a new family of lanthanide MOFs with functionalized organic linkers. The MOFs, deemed MOF-1114, MOF-1115, MOF-1130, and MOF-1131, are composed of octahedral SBUs bridged by amino functionalized dicarboxylate linkers. The amino groups on the linkers served as sites for covalent PSM reactions with either salicylaldehyde or 3-hydroxynaphthalene-2-carboxaldehyde. Both of these reactions extend the π-conjugation of the linker, causing a redshift in the absorbance wavelength from 450 nm to 650 nm. The authors also propose that this technique could be adapted to similar MOF systems and, by increasing pore volumes with increasing linker lengths, larger pi-conjugated reactants can be used to further redshift the absorption wavelengths. Biological imaging using MOFs has been realized by several groups, namely Foucault-Collet and co-workers. In 2013, they synthesized a NIR-emitting Yb3+-NMOF using phenylenevinylene dicarboxylate (PVDC) linkers. They observed cellular uptake in both HeLa cells and NIH-3T3 cells using confocal, visible, and NIR spectroscopy. Although low quantum yields persist in water and Hepes buffer solution, the luminescence intensity is still strong enough to image cellular uptake in both the visible and NIR regimes.
Nuclear wasteform materials With an increased public awareness and concern regarding
radioactive contamination, there has been an increased interest in the development of new pathways for the capture, containment, and disposal of nuclear waste, which has largely been generated through the operation of nuclear power plants and continued decommissioning of nuclear weapons. One of the largest challenges currently recognized within the nuclear waste sector is the development and synthesis of novel materials capable of long-term containment and selective capture of actinides. Thus, metal-organic frameworks have emerged as a promising material towards this application; their remarkable modularity, high surface area, selective binding affinities, and customizable topology/crystallinity allow for a material with tunable, on-demand properties and high structural stability. These properties allow for the design of a framework that connects material properties with changes in structure at the atomic level, providing insight into the processes that these materials rely upon. For example, metal-organic frameworks tend to have high structural stability, as evidenced by their crystallinity. This has been applied towards nuclear waste by demonstrating that metal-organic frameworks, specifically a zirconium-based framework, resist prolonged exposure to gamma-rays, a deeply penetrating, highly hazardous form of radiation known to be emitted by highly radioactive substances such as 241Am, while retaining crystallinity. There are several known methods by which metal-organic frameworks have been used to sequester radionuclides. Foremost is the incorporation of radionuclides into the metal-organic framework as the metal nodes. This effectively captures the actinides by incorporating them into the rigid crystal structure itself, locking it in place. The incoperation of actinides as metal nodes can be achieved through a variety of methods, including synthesis, metal-node extension, and cation exchange. Actinide-containing metal-organic frameworks can be synthesized directly from actinide salts, allowing for direct incorporation without further or previous modification required. Additionally, the metal-node can be extended, allowing for a combination of actinides and transition metals to serve as the nodes simultaneously. Finally, actinides can be incorporated into the metal node through cation exchange; a previously-synthesized metal-organic framework is exposed to actinide cations, where the radionuclides are allowed to slowly replace the transition metal as the metal nodes, incorporating themselves into the crystal itself. Another reported method of radionuclide capture by metal-organic frameworks is through the incorporation of guest molecules. In this method, radionuclides are locked in the crystalline pores through first introducing the actinide cations into these pores and subsequent installation of additional or capping linkers. The central concept is that once the actinides are in the crystalline structure, additional linkers hinder the actinide cations and slow the leaching process from the crystal structure. Leeching from these capped frameworks has been reported to be on a similar order of magnitude as other materials used in radionuclide containment, such as perovskites, zeolites, and phosphate ceramics. In 2010 Smaldone et al., an international research group, synthesized a biocompatible MOF termed CD-MOF-1 from cheap edible natural products. CD-MOF-1 consists of repeating base units of 6 γ-cyclodextrin rings bound together by potassium ions. γ-cyclodextrin (γ-CD) is a symmetrical cyclic oligosaccharide that is mass-produced enzymatically from starch and consists of eight asymmetric α-1,4-linked D-glucopyranosyl residues. The molecular structure of these glucose derivatives, which approximates a truncated cone, bucket, or torus, generates a hydrophilic exterior surface and a nonpolar interior cavity. Cyclodextrins can interact with appropriately sized drug molecules to yield an inclusion complex. Smaldone's group proposed a cheap and simple synthesis of the CD-MOF-1 from natural products. They dissolved sugar (γ-cyclodextrin) and an alkali salt (KOH, KCl, potassium benzoate) in distilled bottled water and allowed 190 proof grain alcohol (Everclear) to vapor diffuse into the solution for a week. The synthesis resulted in a cubic (γ-CD)6 repeating motif with a pore size of approximately 1 nm. Subsequently, in 2017 Hartlieb et al. at Northwestern did further research with CD-MOF-1 involving the encapsulation of ibuprofen. The group studied different methods of loading the MOF with ibuprofen as well as performing related bioavailability studies on the ibuprofen-loaded MOF. They investigated two different methods of loading CD-MOF-1 with ibuprofen; crystallization using the potassium salt of ibuprofen as the alkali cation source for production of the MOF, and absorption and deprotonation of the free-acid of ibuprofen into the MOF. From there the group performed in vitro and in vivo studies to determine the applicability of CD-MOF-1 as a viable delivery method for ibuprofen and other NSAIDs. In vitro studies showed no toxicity or effect on cell viability up to 100 μM. In vivo studies in mice showed the same rapid uptake of ibuprofen as the ibuprofen potassium salt control sample with a peak plasma concentration observed within 20 minutes, and the cocrystal has the added benefit of double the half-life in blood plasma samples. The increase in half-life is due to CD-MOF-1 increasing the solubility of ibuprofen compared to the pure salt form. Since these developments many groups have done further research into drug delivery with water-soluble, biocompatible MOFs involving common over-the-counter drugs. In March 2018 Sara Rojas and her team published their research on drug incorporation and delivery with various biocompatible MOFs other than CD-MOF-1 through simulated cutaneous administration. The group studied the loading and release of ibuprofen (hydrophobic) and aspirin (hydrophilic) in three biocompatible MOFs (MIL-100(Fe), UiO-66(Zr), and MIL-127(Fe)). Under simulated cutaneous conditions (aqueous media at 37 °C) the six different combinations of drug-loaded MOFs fulfilled "the requirements to be used as
topical drug delivery systems, such as released payload between 1 and 7 days" and delivering a therapeutic concentration of the drug of choice without causing unwanted side effects. The group discovered that the drug uptake is "governed by the hydrophilic/hydrophobic balance between cargo and matrix" and "the accessibility of the drug through the framework". The "controlled release under cutaneous conditions follows different kinetics profiles depending on: (i) the structure of the framework, with either a fast delivery from the very open structure MIL-100 or a slower drug release from the narrow 1D pore system of MIL-127 or (ii) the hydrophobic/hydrophilic nature of the cargo, with a fast (Aspirin) and slow (Ibuprofen) release from the UiO-66 matrix." Moreover, a simple ball milling technique is used to efficiently encapsulate the model drugs 5-fluorouracil, caffeine, para-aminobenzoic acid, and benzocaine. Both computational and experimental studies confirm the suitability of [Zn4O(dmcapz)3] to incorporate high loadings of the studied bioactive molecules. Recent research involving MOFs as a drug delivery method includes more than just the encapsulation of everyday drugs like ibuprofen and aspirin. In early 2018 Chen et al., published detailing their work on the use of MOF, ZIF-8 (zeolitic imidazolate framework-8) in antitumor research "to control the release of an autophagy inhibitor, 3-methyladenine (3-MA), and prevent it from dissipating in a large quantity before reaching the target." The group performed in vitro studies and determined that "the autophagy-related proteins and autophagy flux in HeLa cells treated with 3-MA@ZIF-8 NPs show that the autophagosome formation is significantly blocked, which reveals that the pH-sensitive dissociation increases the efficiency of autophagy inhibition at the equivalent concentration of 3-MA." This shows promise for future research and applicability with MOFs as drug delivery methods in the fight against cancer.
Semiconductors In 2014 researchers proved that they can create electrically conductive thin films of MOFs (Cu3(btc)2 (also known as
HKUST-1; BTC, benzene-1,3,5-tricarboxylic acid) infiltrated with the molecule 7,7,8,8-tetracyanoquinododimethane) that could be used in applications including photovoltaics, sensors, and electronic materials and a path toward creating semiconductors. The team demonstrated tunable, air-stable electrical conductivity with values as high as 7 siemens per meter, comparable to bronze. (2,3,6,7,10,11-hexaiminotriphenylene)2 was shown to be a metal-organic
graphene analogue that has a natural
band gap, making it a semiconductor, and is able to self-assemble. It is an example of
conductive metal-organic framework. It represents a family of similar compounds. Because of the symmetry and geometry in 2,3,6,7,10,11-hexaiminotriphenylene (hitp), the overall organometallic complex has an almost
fractal nature that allows it to perfectly self-organize. By contrast, graphene must be doped to give it the properties of a semiconductor. Ni3(hitp)2 pellets had a conductivity of 2 S/cm, a record for a metal-organic compound. In 2018 researchers synthesized a two-dimensional semiconducting MOF (Fe3(THT)2(NH4)3, also known as THT, 2,3,6,7,10,11-triphenylenehexathiol) and showed high electric mobility at room temperature. In 2020 the same material was integrated in a photo-detecting device, detecting a broad wavelength range from UV to NIR (400–1575 nm). This was the first time a two-dimensional semiconducting MOF was demonstrated to be used in opto-electronic devices. is a 2D MOF structure, and there are limited examples of materials which are intrinsically conductive, porous, and crystalline. Layered 2D MOFs have porous crystalline structure showing electrical conductivity. These materials are constructed from trigonal linker molecules (phenylene or
triphenylene) and six functional groups of –OH, -NH2, or –SH. The trigonal linker molecules and square-planarly coordinated metal ions such as {{chem2|Cu^{2+} }}, {{chem2|Ni^{2+} }}, {{chem2|Co^{2+} }}, and {{chem2|Pt^{2+} }} form layers with hexagonal structures which look like graphene in larger scale. Stacking of these layers can build one-dimensional pore systems. Graphene-like 2D MOFs have shown decent conductivities. This makes them a good choice to be tested as electrode material for evolution of hydrogen from water, oxygen reduction reactions, supercapacitors, and sensing of
volatile organic compounds (VOCs). Among these MOFs, has exhibited the lowest conductivity, but also the strongest reaction in sensing of VOCs.
Biomimetic mineralization Biomolecules can be incorporated during the MOF crystallization process. Biomolecules including proteins, DNA, and antibodies could be encapsulated within ZIF-8. Enzymes encapsulated in this way were stable and active even after being exposed to harsh conditions (e.g. aggressive solvents and high temperature). ZIF-8, MIL-88A, HKUST-1, and several luminescent MOFs containing lanthanide metals were used for the biomimetic mineralization process. In addition, individual living cells were encapsulated within MOF shells via
single-cell nanoencapsulation (SCNE).
Carbon capture Adsorbent MOF's small, tunable pore sizes and high void fractions are promising as an adsorbent to capture CO2. MOFs could provide a more efficient alternative to traditional
amine solvent-based methods in CO2 capture from coal-fired power plants. MOFs could be employed in each of the main three carbon capture configurations for coal-fired power plants: pre-combustion, post-combustion, and oxy-combustion. The post-combustion configuration is the only one that can be retrofitted to existing plants, drawing the most interest and research. The
flue gas would be fed through a MOF in a packed-bed reactor setup. Flue gas is generally 40 to 60 °C with a partial pressure of CO2 at 0.13 – 0.16 bar. CO2 can bind to the MOF surface through either
physisorption (via
Van der Waals interactions) or
chemisorption (via
covalent bond formation). Once the MOF is saturated, the CO2 is extracted from the MOF through either a temperature swing or a pressure swing. This process is known as regeneration. In a temperature swing regeneration, the MOF would be heated until CO2 desorbs. To achieve working capacities comparable to the amine process, the MOF must be heated to around 200 °C. In a pressure swing, the pressure would be decreased until CO2 desorbs. Another relevant MOF property is their low heat capacities.
Monoethanolamine (MEA) solutions, the leading capture method, have a heat capacity between 3-4 J/(g⋅K) since they are mostly water. This high heat capacity contributes to the energy penalty in the solvent regeneration step, i.e. when the adsorbed CO2 is removed from the MEA solution. MOF-177, a MOF designed for CO2 capture, has a heat capacity of 0.5 J/(g⋅K) at ambient temperature.
Catalyst A MOF loaded with
propylene oxide can act as a
catalyst, converting into
cyclic carbonates (ring-shaped molecules with many applications). They can also remove carbon from
biogas. This MOF is based on
lanthanides, which provide chemical stability. This is especially important because the gases the MOF will be exposed to are hot, high in humidity, and acidic. Triaminoguanidinium-based POFs and Zn/POFs are new multifunctional materials for
environmental remediation and biomedical applications.
Water treatment Metal–organic frameworks (MOFs) have attracted increasing attention as functional materials for water treatment due to their high surface area, tunable pore structures, and chemical versatility. These properties enable MOFs to act as efficient platforms for the removal of a wide range of contaminants from aqueous systems. In particular, MOFs have been extensively investigated for the adsorption of heavy metal ions such as lead, chromium, arsenic, and cadmium , as well as for the removal of organic pollutants including dyes, pesticides, and pharmaceutical residues. In water treatment applications, adsorption is one of the primary mechanisms by which MOFs operate. The porous structure of MOFs provides abundant active sites for interaction with pollutants, while the ability to tailor the chemical functionality of the framework allows for selective binding through coordination interactions, electrostatic attraction, and hydrogen bonding. This tunability has enabled the design of MOFs with enhanced selectivity toward specific contaminants, making them promising candidates for targeted water purification. Beyond adsorption, MOFs have also been explored in membrane-based separation processes and as catalytic materials for the degradation of pollutants. For example, MOF-based membranes have demonstrated potential for selective ion separation and removal of dissolved contaminants, while photocatalytic and advanced oxidation processes involving MOFs have been used to degrade persistent organic pollutants into less harmful species. In addition, composite materials incorporating MOFs with polymers, carbon materials, or magnetic nanoparticles have been developed to improve mechanical stability, facilitate recovery, and enhance overall treatment efficiency. Despite these promising applications, several challenges remain for the large-scale implementation of MOFs in water treatment systems. These include limited stability in aqueous environments for certain frameworks, the cost and scalability of synthesis, and the need for improved durability under realistic operating conditions . Ongoing research efforts are therefore focused on developing more robust MOF structures and scalable production methods to enable their practical deployment in water purification technologies.
Desalination/ion separation MOF membranes can achieve substantial ion selectivity due to their small repeating structures. This offers the potential for use in
desalination and water treatment. As of 2020,
reverse osmosis supplied more than two-thirds of global desalination capacity, and the last stage of most water treatment processes. Osmosis does not use
dehydration of ions, or selective
ion transport in biological channels and it is not energy efficient. The mining industry uses membrane-based processes to reduce water pollution, and to recover metals. MOFs could be used to extract metals such as lithium from seawater and waste streams. MOF membranes such as ZIF-8 and UiO-66 membranes with uniform subnanometer pores consisting of angstrom-scale windows and nanometer-scale cavities displayed ultrafast selective transport of alkali metal ions. The windows acted as ion selectivity filters for alkali metal ions, while the cavities functioned as pores for transport. The ZIF-8 and UiO-66 membranes showed a
LiCl/
RbCl selectivity of ~4.6 and ~1.8, respectively, much higher than the 0.6 to 0.8 selectivity in traditional membranes. A 2020 study suggested that a new MOF called PSP-MIL-53 could be used along with
sunlight to purify water in just half an hour.
Gas separation MOFs are also predicted to be very effective media to separate gases with low energy cost using computational high throughput screening from their adsorption or gas breakthrough/diffusion properties. One example is NbOFFIVE-1-Ni, also referred to as KAUST-7 which can separate propane and propylene via diffusion at nearly 100% selectivity. The specific molecule selectivity properties provided by Cu-BDC surface mounted metal organic framework (SURMOF-2) growth on alumina layer on top of back gated Graphene Field Effect Transistor (GFET) can provide a sensor that is only sensitive to ethanol but not to methanol or isopropanol.
Water vapor capture and dehumidification MOFs have been demonstrated that capture water vapor from the air. In 2021 under humid conditions, a polymer-MOF lab prototype yielded 17 liters (4.5 gal) of water per kg per day without added energy. MOFs could also be used to increase energy efficiency in room temperature space cooling applications. When cooling outdoor air, a cooling unit must deal with both the air's
sensible heat and
latent heat. Typical
vapor-compression air-conditioning (VCAC) units manage the latent heat in air through cooling fins held below the
dew point temperature of the moist air at the intake. These fins condense the water, dehydrating the air and thus substantially reducing the air's heat content. The cooler's energy usage is highly dependent on the cooling coil's temperature and would be improved greatly if the temperature of this coil could be raised above the
dew point. This makes it desirable to handle dehumidification through means other than condensation. One such means is by adsorbing the water from the air into a
desiccant coated onto the heat exchangers, using the waste heat exhausted from the unit to desorb the water from the
sorbent and thus regenerate the desiccant for repeated usage. This is accomplished by having two condenser/evaporator units through which the flow of refrigerant can be reversed once the desiccant on the condenser is saturated, thus making the condenser the evaporator and vice versa. Chemistry can help tune the optimal relative humidity for adsorption/desorption, and the sharpness of the water uptake.
Ferroelectrics and multiferroics Some MOFs also exhibit spontaneous electric polarization, which occurs due to the ordering of electric dipoles (polar linkers or guest molecules) below a certain phase transition temperature. If this long-range dipolar order can be controlled by the external electric field, a MOF is called ferroelectric. Some ferroelectric MOFs also exhibit magnetic ordering making them single structural phase multiferroics. This material property is highly interesting for construction of memory devices with high information density. The coupling mechanism of
type-I [(CH3)2NH2][Ni(HCOO)3] molecular multiferroic is spontaneous elastic strain mediated indirect coupling.
Future direction Over the last three decades, MOFs have been greatly refined and utilized in a wide range of applications. It has been speculated that the integration of artificial intelligence tools into MOF research could lead to the discovery of applications with the potential to solve modern energy and environmental challenges, though currently no public research exists to back this speculation. ==See also==