Membrane distillation

Water desalination
Methods
A Microscopic image of a membrane.
REM-image of a PTFE membrane

Membrane distillation is a thermally driven separational program in which separation is enabled due to phase change. A hydrophobic membrane displays a barrier for the liquid phase, allowing the vapour phase (e.g. water vapour) pass through the membrane's pores. The driving force of the process is given by a partial vapour pressure difference commonly triggered by a temperature difference.

Principle of membrane distillation

Capillary depression
Capillary depression of water on a hydophobic membrane
Memdest
Schematic image of the membrane distillation process
Temperature and pressure profile
Temperature and pressure profile through the membrane considering temperature polarisation

State of the art processes that separate mass flows by a membrane, mostly use a static pressure difference as the driving force between the two bounding surfaces (e.g. RO), a difference in concentration (dialysis) or an electric field (ED). Selectivity of a membrane is produced by, either its pore size in relation to the size of the substance to be retained, its diffusion coefficient or electrical polarity. However, the selectivity of membranes used for membrane distillation (MD) is based on the retention of liquid water with-at the same time- permeability for free water molecules and thus, for water vapour. These membranes are made of hydrophobic synthetic material (e.g. PTFE, PVDF or PP) and offer pores with a standard diameter between 0.1 to 0.5 µm. As water has strong dipole characteristics, whilst the membrane fabric is non-polar, the membrane material is not wetted by the liquid. Even though the pores are considerably larger than the molecules, the liquid phase does not enter the pores because of the high water surface tension. A convex meniscus develops into the pore. This effect is named capillary action. Amongst other factors, the depth of impression can depend on the external pressure load on the liquid. A dimension for the infiltration of the pores by the liquid is the contact angle Θ=180 – Θ'. As long as Θ > 90° and accordingly Θ' > 0° no wetting of the pores will take place. If the external pressure rises above the so-called wetting pressure, then Θ = 90°resulting in a bypass of the pore. The driving force which delivers the vapour through the membrane, in order to collect it on the permeate side as product water, is the partial water vapour pressure difference between the two bounding surfaces. This partial pressure difference is the result of a temperature difference between the two bounding surfaces. As can be seen in the image, the membrane is charged with a hot feed flow on one side and a cooled permeate flow on the other side. The temperature difference through the membrane, usually between 5 and 20 K, conveys a partial pressure difference which ensures that the vapour developing at the membrane surface follows the pressure drop, permeating through the pores and condensing on the cooler side.[1]

Membrane distillation techniques

Schematic DCMD arrangement
Schematic AGMD arrangement

Many different membrane distillation techniques exist. The basic four techniques mainly differ by the arrangement of their distillate channel or the manner in which this channel is operated. The following technologies are most common:

Direct-contact MD

In DCMD, both sides of the membrane are charged with liquid- hot feed water on the evaporator side and cooled permeate on the permeate side. The condensation of the vapour passing through the membrane happens directly inside the liquid phase at the membrane boundary surface. Since the membrane is the only barrier blocking the mass transport, relatively high surface related permeate flows can be achieved with DCMD. A disadvantage is the high sensible heat loss, as the insulating properties of the single membrane layer are low. However, a high heat loss between evaporator and condenser is also the result of the single layer. This lost heat is not available to the distillation process whereby its efficiency is lowered.

Air-gap MD

In air-gap MD, the evaporator channel resembles that in DCMD, whereas the permeate gap lies between the membrane and a cooled walling and is filled with air. The vapour passing through the membrane must additionally overcome this air gap before condensing on the cooler surface. The advantage of this method is the high thermal insulation towards the condenser channel, thus minimizing heat conduction losses. However, the disadvantage is that the air gap represents an additional barrier for mass transport, reducing the surface- related permeate output compared to DCMD. A further advantage towards DCMD is the fact, that volatile substances with a low surface tension such as alcohol or other solvents can be separated from diluted solutions, due to the fact that there is no contact between the liquid permeate and the membrane with AGMD.

Sweeping-gas MD

Schematic SWGMD arrangement
Schematic VCMD arrangement

Sweeping-gas MD, also known as air stripping, uses a channel configuration with an empty gap on the permeate side. This configuration is the same as in AGMD. Condensation of the vapour takes place outside the MD module in an external condenser. As with AGMD, volatile substances with a low surface tension can be distilled with this process. The advantage of SWGMD over AGMD is the significant reduction of the barrier to the mass transport through forced flow. Hereby higher surface-related productwater mass flows can be achieved than with AGMD. A disadvantage of SWGMD caused by the gas component and therefore the higher total mass flow, is the necessity of a higher condenser capacity. When using smaller gas mass flows there is a risk of the gas heating itself at the hot membrane surface, thus reducing the vapour pressure difference and therefore the driving force. One solution of this problem for SWGMD and for AGMD is the use of a cooled walling for the permeate channel, and maintaining temperature by flushing it with gas.

Vacuum MD

Vacuum MD contains an air gap channel configuration. Once it has passed through the membrane, the vapour is sucked out of the permeate channel and condenses outside the module as with SWGMD. VCMD and DWGMD can be applied for the separation of volatile substances from a watery solution or for the generation of pure water from concentrated salt water. One advantage of this method is that undissolved inert gasses blocking the membrane pores are sucked out by the vacuum, leaving a larger effective membrane surface active. Furthermore, a reduction of the boiling point results in a comparable amount of product at lower overall temperatures and lower temperature differences through the membrane. A lower required temperature difference leaves a lower total- and specific thermal energy demand. However, the generation of a vacuum, which must be adjusted to the salt water temperature, requires complex technical equipment and is therefore a disadvantage to this method. The electrical energy demand is a lot higher as with DCMD and AGMD. An additional problem is the increase of the pH value due to the removal of CO2 from the feed water.

Permeate-gap MD

Schematic image of a DCMD channel configuration
Schematic image of a PGMD channel configuration

In the following, the principle channel configuration and operating method of a standard DCMD module as well as a DCMD module with separate permeate gap shall be explained. The design in the image to the right depicts a flat channel configuration, but can also be understood as a schema for flat-, hollow fibre - or spiral wound modules.

The complete channel configuration consists of a condenser channel with inlet and outlet and an evaporator channel with inlet and outlet. These two channels are separated by the hydrophobic, micro porous membrane. For cooling, the condenser channel is flooded with fresh water and the evaporator e.g. with salty feed water. The coolant enters the condenser channel at a temperature of 20 °C. After passing through the membrane, the vapour condenses in the cooling water, releasing its latent heat and leading to a temperature increase in the coolant. Sensible heat conduction also heats the cooling water through the surface of the membrane. Due to the mass transport through the membrane the mass flow in the evaporator decreases whilst the condenser channel increases by the same amount. The mass flow of pre-heated coolant leaves the condenser channel at a temperature of about 72 °C and enters a heat exchanger, thus pre-heating the feed water. This feed water is then delivered to a further heat source and finally enters the evaporator channel of the MD module at a temperature of 80 °C. The evaporation process extracts latent heat from the feed flow, which cools down the feed increasingly in flow direction. Additional heat reduction occurs due to sensible heat passing through the membrane. The cooled feed water leaves the evaporator channel at approximately 28 °C. Total temperature differences between condenser inlet and evaporator outlet and condenser inlet and evaporator outlet are about equal. In a PGMD module, the permeate channel is separated from the condenser channel by a condensation surface. This enables the direct use of a salt water feed as coolant, since it does not come into contact with the permeate. Considering this, the cooling-or feed water entering the condenser channel at a temperature T1 can now also be used to cool the permeate. Condensation of vapour takes place inside the liquid permeate. Pre-heated feed water that was used to cool the condenser can be conducted directly to a heat source for final heating, after leaving the condenser at a temperature T2. After it has reached temperature T3 it is guided into the evaporator. Permeate is extracted at temperature T5 and the cooled brine is discharged at temperature T4.

An advantage of PGMD towards DCMD is the direct use of feed water as cooling liquid inside the module and therefore the necessity of only one heat exchanger to heat the feed before entering the evaporator. Hereby heat conduction losses are reduced and expensive components can be cut. A further advantage is the separation of permeate from coolant. Therefore, the permeate does not have to be extracted later in the process and the coolant's mass flow in the condenser channel remains constant. The low flow velocity of the permeate in the permeate gap is a disadvantage of this configuration, as it leads to a poor heat conduction from the membrane surface to the condenser walling. High temperatures on the permeate side's membrane bounding surface are the result of this effect (temperature polarisation), which lowers the vapour pressure difference and therefore the driving force of the process. However, it is beneficial, that the heat conduction losses through the membrane are also lowered by this effect. Compared to AGMD a higher surface related permeate output is achieved, as the mass flow is not additionally inhibited by the diffusion resistance of an air layer.[1]

Vacuum multi-effect membrane distillation

The hydrophobic membranes (or PP foils) are welded at both sides of the memsys frame. This frame are designed to combine and distribute vapor, feed, non condensable gas and distillate flows.
Different numbers of memsys frame are friction welded as memsys module (e.g. steam raiser, membrane stage and condenser). GOR and capacity of memsys module can be easily modified deponding on the application or customer's needs.
Diagram of memsys V-MEMD process

The typical vacuum multi-effect membrane distillation (e.g. the memsys brand V-MEMD) module consists of a steam raiser, evaporation–condensation stages, and a condenser. Each stage recovers the heat of condensation, providing a multiple-effect design. Distillate is produced in each evaporation–condensation stage and in the condenser.

Steam raiser: The heat produced by the external heat source (e.g. solar thermal or waste heat) is exchanged in the steam raiser. The water in the steam raiser is at lower pressure (e.g. 400 mbar), compared to the ambient. The hot steam flows to the first evaporation–condensation stage (stage 1).

Evaporation–condensation stages: Stages are composed of alternative hydrophobic membrane and foil (Polypropylene, PP) frames. Feed (e.g. seawater) is introduced into stage 1 of the module. Feed flows serially through the evaporation–condensation stages. At the end of last stage, it is ejected as brine.

Stage 1: Steam from the evaporator condenses on a PP foil at pressure level P1 and corresponding temperature T1. The combination of a foil and a hydrophobic membrane creates a channel for the feed, where the feed is heated by the heat of condensation of the vapour from the steam raiser. Feed evaporates under the negative pressure P2. The vacuum is always applied to the permeate side of the membranes.

Stage [2, 3, 4, x]: This process is replicated in further stages and each stage is at a lower pressure and temperature.

Condenser: The vapour produced in the final evaporation–condensation stage is condensed in the condenser, using the coolant flow (e.g. seawater).

Distillate production: Condensed distillate is transported via the bottom of each stage by pressure difference between stages.

Design of memsys module: Inside each memsys frame, and between frames, channels are created. Foil frames are the ‘distillate channels’. Membrane frames are the ‘vapour channels’. Between foil and membrane frames, ‘feed channels’ are created. Vapour enters the stage and flows into parallel foil frames. The only option of for the vapour entering the foil frames is to condense, i.e. vapour enters a ‘dead-end’ foil frame. Although it is called a ‘dead-end’ frame, it does contain a small channel to remove the non-condensable gases and to apply the vacuum.

The condensed vapour flows into a distillate channel. The heat of condensation is transported through the foil and is immediately converted into evaporation energy, generating new vapour in the seawater feed channel. The feed channel is limited by one condensing foil and a membrane.The vapour leaves the membrane channels and is collected in a main vapour channel. The vapour leaves the stage via this channel and enters the next stage. memsys has developed a highly automated production line for the modules and could be easily extended. As the memsys process works at modest low temperatures (<90 °C) and moderate negative pressure, all module components are made of polypropylene (PP). This eliminates corrosion and scaling and allows large-scale cost efficient production.

Application

Typical applications of membrane distillation are:

Solar-powered membrane distillation

Plant design of a compact system
Plant design of a two loop system

Membrane distillation is very suitable for compact, solar powered desalination units providing small and medium range output <10000 l/day. Especially the spiral wound design patented by GORE in the year 1985 suits this application. Within the MEMDIS project, which kicked off in 2003, the Fraunhofer Institute for Solar Energy Systems ISE began developing MD modules as well as installing and analysing two different solar powered operating systems, together with other project parters. The first system type is a so-called compact system, designed to produce a drinking water output of 100-120 l/day from sea-or brackish water. The main aim of the system design is a simple, self-sufficient, low maintenance and robust plant for target markets in arid and semi-arid areas of low infrastructure. The second system type is a so-called two-loop plant with a capacity of around 2000 l/day. Here, the collector circuit is separated from the desalination circuit by a saltwater resistant heat exchanger.[1] Based on these two system types, a various number of prototypes were developed, installed and observed.

The standard configuration of today's (2011) compact system is able to produce a distillate output of up to 150 l/day. The required thermal energy is supplied by a 6,5 m² solar thermal collector field. Electrical energy is supplied by a 75 W PV-module. This system type is currently being developed further and marketed by the Solar Spring GmbH,[2] a Spin -Off of the Fraunhofer Institute for Solar Energy Systems. Within the MEDIRAS project- a further EU-project, an enhanced two-loop system was installed on the Island of Gran Canary. Built inside a 20 ft container and equipped with a collector aray size of 225 m², a heat storage tank makes a distillate output of up to 3000 l/day possible. Further applications with up to 5000 l/day have also been implemented, either 100% solar powered or as hybrid projects in combination with waste heat.

Exemplary systems
Membrane distillation plant, installed inside a 20ft ship container with integrated heat storage (Location: Namibia)
Collector array connected to a two-loop plant
Solar powered two-loop plant with 12 MD modules and a capacity of ~3000 L/day (Location: Gran Canary)
Compact system Oryx150 with a capacity of ~150 L/Tag (Location: Mexico)

Activities

There are various companies and research institutes working with and investigating membrane distillation. Here are some of the most relevant ones (in alphabetic order):

References

  1. 1 2 3 Joachim Koschikowski: Entwicklung von energieautark arbeitenden Wasserentsalzungsanlagen auf Basis der Membrandestillation Fraunhofer Verlag, 2011, 3839602602
  2. ↑ "SolarSpring GmbH"
  3. ↑ "Aquaver"
  4. ↑ "Ecover"
  5. ↑ "ISE"
  6. ↑
  7. ↑ "Instituto Tecnológico de Canarias"
  8. ↑ "Istituto per la Tecnologia delle Membrane"
  9. ↑ "Keppel Seghers"
  10. ↑ "memsys"
  11. ↑ "Plataforma Solar Almeria"
  12. ↑ "Scarab"
  13. ↑ [solarspring.de/ "SolarSpring"]
  14. ↑ "Università della Calabria - Dipartimento di Ingegneria Chimica e dei Materiali"
  15. ↑ "Università Degli Studi Di Palermo"
  16. ↑ "AEE INTEC Institute for Sustainable Technologies"
  17. ↑ "Génie des Procédés et Environnement - Laboratoire d'Ingénierie des Systèmes Biologiques et des Procédés"

15. Evaluation of commercial PTFE membranes in desalination by direct contact membrane distillation, MMA Shirazi, A Kargari, M Tabatabaei, Chemical Engineering and Processing: Process Intensification, 2014, in press. 16. Sweeping gas membrane distillation (SGMD) as an alternative for integration of bioethanol processing: study on a commercial membrane and operating parameters, MMA Shirazi, A Kargari, M Tabatabaei, Chemical Engineering Communications, 2014, in press. 17. Production of drinking water from seawater using membrane distillation (MD) alternative: direct contact MD and sweeping gas MD approaches, MMA Shirazi, A Kargari, D Bastani, L Fatehi, Desalination and Water Treatment, 2013, in press. 18. Characterization of polymeric membranes for membrane distillation using atomic force microscopy MMA Shirazi, D Bastani, A Kargari, M Tabatabaei, Desalination and Water Treatment, 2013, in press. 19. Direct contact membrane distillation for seawater desalination, MMA Shirazi, A Kargari, MJA Shirazi, Desalination and Water Treatment 49 (1-3), 368-375

Literature

External links

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