ACS Publications
[Journal Home Page] [Search the Journals] [Table of Contents] [PDF version of this article] [Download to Citation Manager]

J. Proteome Res., 4 (1), 180 -184, 2005. 10.1021/pr0498382 S1535-3893(04)09838-0
Web Release Date: January 26, 2005

Copyright © 2005 American Chemical Society

Functions and Possible Provenance of Primordial Proteins-Part II: Microorganism Aggregation in Clouds Triggered by Climate Change

Andrei P. Sommer* and N. Chandra Wickramasinghe

Central Institute of Biomedical Engineering, University of Ulm, 89081 Ulm, Germany and Cardiff Centre for Astrobiology, Cardiff University, Cardiff, CF10 3DY, United Kingdom

Received September 5, 2004

Abstract:

Current models predict that the elevation of the Earth's surface temperature due to global warming is accompanied by a warming of the troposphere, and a thickening cloud cover associated with longer-lasting clouds, in particular over land. These effects can have an instant impact on the vitality level of microorganisms in clouds and the spreading of airborne diseases. Microorganisms could originate from locations on the Earth, or even arrive from space. Primordial proteins in nanobacteria, only recently identified in the atmosphere, could play a significant role in clouds-accelerating the formation of cloud droplets and interconnecting nanobacteria (and possibly nanobacteria and other microorganisms), thus enhancing their chances to eventually reach the Earth.

Keywords: global warming primordial proteins slime light living nanovesicles nanobacteria microorganisms atmosphere


I. Sealing and Adhesion-Complementary Functions of Primordial Proteins

A prominent function of primordial proteins is adhesion, as described in our previous work.1 Adhesion is a prerequisite for establishing nonspecific contacts to the surface of various materials, hence providing favorable conditions for the realization of the evolutionary potential of primitive life-forming units, e.g., nanobacteria (NB).2 A second and less evident function of primordial proteins is surface sealing, recognized by us as vital for NB.3 Interestingly, there seems to exist a functional complementarity between adhesion and sealing. The primary role of sealing is to secure the survival of individual NB in a dry environment, as practically realized in the atmosphere external to clouds. The primary role of adhesion becomes clear from the biological advantage of colony formation. NB arriving from space, as might be indicated by their capture at an altitude of 41 km over sea level, have their first chance to meet in the wet environment of the clouds.1 Here, the slime enveloping NB is likely to soften and to become gradually more and more adhesive, depending on residence time, humidity, and the ambient cloud temperature. The slime consists of proteins (probably glycoproteins)1 and some minerals. An adhesive slime layer is certainly instrumental in promoting the formation of colonies on Earth, and ensures that whenever NB suspended in the clouds encounter each other, they will stick together. In this way, aggregates of NB can find a realistic chance to reach the Earth by the action of gravity. NB are presumably uniquely effective as cloud condensation nuclei (CCN). Due to their strongly hydrophilic shells (apatite), possibly carrying a glycoprotein film (probably extremely hydrophilic because of the sugars), NB are expected to form cloud droplets before the CCN coexisting with them. Under the action of gravity, accelerated droplet growth may result in the coalescence of some NB-nucleated droplets, preferentially at the base of the cloud-thus fostering the creation of larger rain drops, which may eventually reach the Earth.

Water is essential for microorganisms and is stored by them in various ways. Desiccation can inactivate bacteria and viruses, and most probably also living nanovesicles (NB) possessing internal compartments (nanocavities) suitable for the storage of aqueous fluids. Microorganisms passing through the terrestrial atmosphere can, in principle, be partially or completely desiccated via thermal effects involving the heating of the entire particle by solar radiation. Instantaneous water loss can result from absorption of light intensities of the order of 1000 Wm-2, where the photons interact selectively with the water content of microorganisms. Both effects, in particular their synergistic interplay, can perform important physical and biological functions in the terrestrial atmosphere. On the basis of the prevalence of nanoscopic water layers on ice, found by Döppenschmidt and Butt,4 the aforementioned effects have been predicted by us to affect thundercloud electrification.5-7 Similar effects would be expected to control cloud albedos and indeed, most importantly, the vitality level of aerosolic biosystems. While the desiccation caused by absorption of solar radiation is clear, the direct effect of intensive sunlight on nanoscopic quantities of water contained in microorganisms has not yet been explored. In this paper, we establish a connection between results of experiments that could serve as a model for the latter effect, and their possible implication in mechanisms controlling the level of vitality of atmospheric NB. Previously, we have identified possibly still living nanovesicles at stratospheric altitudes in concentrations suggesting their massive presence in the clouds.1 We now proceed to introduce a model for the interaction of light with water contained in porous nanoscale cavities, allowing us to analyze processes of dehydration and rehydration that can modulate the vitality level of airborne microorganisms in general, and NB in particular.

II. Impact of Global Warming on Primordial Proteins

The motivation for this investigation is derived from a model scenario based on calculations done by Liepert et al., suggesting that global warming will increase the liquid water content of clouds, but with relatively less precipitation.8 Less precipitation is equivalent here to extended cloud lifetimes. Microorganisms lofted into the atmosphere through a variety of processes would tend to become rapidly desiccated under the known conditions of low humidity levels and sustained temperature elevation due to radiative heating. Inactive, transiently desiccated microorganisms, transported back from the dry atmosphere to the Earth by gravity, are likely to cause little harm, compared to those returning in rain drops, after having been incorporated for some time in long-lived clouds, where they would encounter better conditions for revitalization. Rain suppression by aerosols has been already confirmed by Rosenfeld.9 When cloud nucleation occurs by small aerosols, e.g., stemming from biomass burning, urban or industrial air pollution, or desert dust, cloud droplets tend to evaporate before they reach the threshold-sizes that are required for precipitation. Notably, in warm clouds over urban areas, polluted with high concentrations of biomass particles, microorganisms might find an ideal environment (a wet and nutrient-rich milieu), facilitating the uptake of water, and water-mediated incorporation of nutrients, prerequisites for replication and growth. Replication of microorganisms in clouds has been reported by Sattler et al.10 The biological impact of the scenario may be accentuated by a continuous long-term warming of the troposphere, as has been found by Vinnikov and Grody.11 The environmental circumstances indicate the prevalence of distinct variations in the biological activity of airborne microorganisms, depending on whether the source clouds are warmer or colder, contain more or less biomass particles, and have longer or shorter lifetimes (Figure 1). Due to the dual action of the surface proteins, the situation is different for the return of NB (and possibly other microorganisms) to the Earth, contingent on whether they come down dry or in rain drops.


Figure 1 For airborne microorganisms, it is not the same if they are within the protective, wet and nutrient-rich envelope of a cloud, or outside of it. (Courtesy: Katlin Sommer)

III. Desiccation of Living Nanovesicles: Laboratory Analogues

In previous laboratory experiments, we have provided evidence that the thickness of nanoscopic water layers, deposited at room temperature and normal humidity conditions from the air onto translucent polymer films, decreased in response to the exposure of such films to 670 nm laser light applied at a moderate intensity of 1000 Wm-2, practically as low as the solar constant.12 The result clearly demonstrated (a) the existence of water layers in the air, and (b) that photons of 670 nm, which are only minimally absorbed by water, interact with the nanoscopic water layers attached to surfaces. A similar effect was predicted by us to play a role in the transfer of charge at the sun-exposed side of thunderclouds, where the intensive sunlight could instantly deplete the nanoscopic water layers coating ice crystals.7,12 The interplay between the sunlight and atmospheric humidity would thus have a major impact in defining the state of vitality of airborne NB. From an experimental model, we concluded that NB, whose nanocrystalline mineral shells are optimized to serve as tiny light collectors,13 would respond to variations in solar irradiation and atmospheric humidity. For example, on leaving a cloud during periods of high solar intensity, they would react to an increase in irradiation intensity coupled with a drop in humidity by sealing the pores of their shells with slime-a programmed process, whose reversibility will presumably depend on the ambient conditions,3 and on the proper time-scale of the two competing processes: sealing and evaporation.

For a better understanding of the underlying process controlling the capacity of nanocavities to store water, it could be instructive to summarize phenomena related to the arrangement of water molecules at surfaces. Exceptional orientational effects were first reported for water in interfacial contact with hydrophobic liquids by Scatena et al.14 According to Fawcett et al., interfacial order can also be imposed to molecules by normal gravity.15 The concept of interfacial water layers, acting as an interlayer between a solid body immersed in water, and the bulk water surrounding it, has been introduced on the basis of an intuitive model,16 in which we predicted that the mobility of water molecules at solid surfaces is restricted, compared to bulk water. This concept was applied by us in the design hydrophobic biosensors for uses in an aqueous milieu, and developed further to exploit the advantages of near-field optical analysis, promising to image, e.g., proteins in living cells.17

The physical relevance of a layer of water molecules with unilaterally constrained mobility, existing between the bulk water and a hydrophobic surface, has been recently revealed in our lab. In a representative number of experiments performed with four to six 15 L drops of pure water, successively placed on translucent hydrophobic substrates, where they evaporated under equal temperature and humidity conditions, one drop was continuously irradiated with a 670 nm laser, applied at an intensity of ~1000 Wm-2.7 The light-exposed drop was placed always first on the substrate. Importantly, the light did not accelerate evaporation, as possibly might be anticipated, but clearly delayed it in comparison to the nonirradiated drops, illustrating implicitly the subaquatic persistence of ordered water layers at the liquid-solid interface. The difference has been correlated with a perturbation of the integrity of the ordered interlayer located at the interface between bulk water and substrate. In analogy to the modulation of the nanoscopic water layers masking substrates in air, achieved with virtually nondestructive light intensities,12 the subaquatic modulation was interpreted in terms of resonant fluctuations induced by the light into the layer of interfacial water molecules, changing their actual state transiently from "low mobility" to "bulk mobility".16 From the fact that 670 nm laser light is minimally absorbed by water, a simple picture suggests itself: due to the presence of a number of less mobile interfacial water molecules, the probability that more than one photon can transfer identical momentum to a given water molecule is higher when this target molecule is in a quasi stationary state, than it would be in the case of more mobile target molecules. This concept receives justification from the observation that the evaporation of water drops irradiated with a laser (intensity 1000 Wm-2) operating at 650 nm, a wavelength which is even less absorbed than 670 nm, resulted in a similar delay. Considering the moderate light intensity employed, the delay-effect could not be traced back to the interaction of the light with "nanobubbles"-gas bubbles with a mean radius around 35 nm, and 20-30 nm in height, identified by Tyrrell and Attard via atomic force microscopy (AFM) on hydrophobic substrates immersed in water, using a closed fluid cell.18 Calculations predict inner pressures for such small bubbles far above atmospheric pressure,18 signifying stability. Therefore, even if present at the interface between evaporating drop and substrate, the applied laser light intensity is not likely to affect the state of the bubbles. Nanobubbles with a mean radius of 70 nm and a height of about 7 nm were imaged at the interface between polystyrene and water via AFM by Simonsen et al.19 In contrast to the stationary situation in imaging the nanobubbles, the interior of the water drops evaporating on hydrophobic substrates is constantly dynamic, with a powerful convective flow. The flow has been shown by us to transport 60-200 nm nanospheres suspended in water drops to the periphery of the drops, producing on both hydrophilic and hydrophobic substrates crystalline rings.7,20 We have demonstrated that in cases where the initial drop size coincided with the final ring size, the rings were formed prior to the complete evaporation of the drops, thus visualizing the action of the convective flow on nanoparticles deposited onto substrates.7 This flow may prevent the formation of nanobubbles in water drops. Nanosuspension drops, when irradiated with laser light intensities observed to delay the evaporation of drops of pure water, exhibited a significant retardation in evaporation, compared to nonirradiated drops.7 The similarity in the reaction of a representative number of drops of pure water and aqueous nanosuspensions to their irradiation with low level laser light indicates, however, that the light did not affect nanobubbles that might have been present, or such bubbles were completely absent.

We note that in experiments conducted with evaporating sessile drops (aqueous suspensions containing nano- or microspheres), the suspended particles tended to reach the initial solid-liquid-air contact line, irrespective of size, even in millimeter-scale drops.21,22 This exposed the range of the evaporation-driven convective flow mentioned above. Within this picture, the difference in evaporation time between irradiated and nonirradiated water drops indicates that, due to a restricted molecular mobility in the interfacial layer at the bottom of nonirradiated drops, the convective flow, driving material toward the edge of the drops, will be less effective for the molecules belonging to this interlayer than for those isotropically surrounded by partners with identical degrees of freedom. Remarkably, a light-induced retardation of the evaporation could not be observed for water drops placed on substrates with a pronounced hydrophilic nature. This may signify differences in the molecular arrangement of the water molecules, or is simply explained by the larger area covered by the water drops on hydrophilic surfaces, relative to hydrophobic surfaces. We have recently shown that the mechanisms by which drops of aqueous suspensions containing nanospheres evaporate and form extremely symmetrical ring patterns on substrates (e.g., on mirror-polished titanium) can be exploited in proteomics to design a test platform for the systematic evaluation and adjustment of protein-protein binding preferences in a liquid environment.23

It is useful to examine the entropic transition between the ordered interfacial water layers and the less-ordered bulk phase within a drop, and to realize its expression as a discontinuity in viscosity, ensuring that during evaporation, the bulk material can reach the periphery of the drop without contacting the substrate directly. Direct contact is energetically a costly solution because of dissipative shear-force effects. It becomes plausible that fluctuations induced in the partially immobilized interlayer by the laser light will affect both its rheological properties and its density profile.7 Obviously, a minimal change in density can have a major effect on the space required by an aqueous phase contained in a nanocavity-a relationship of an enormous potential importance in proteomics as well as in pharmaceutics. Immediate pharmaceutical applications include light-triggered pumping processes-providing production principles for porous nanovesicles for drug release, and methods to force microorganisms to uptake antiinfectives dissolved in their environment.24 Thus, the previously proposed desiccation model3 receives manifest justification from the experimental side, with evidence for a new photobiological effect which probably controls the capacity of nanocavities to store water.

IV. Application to Cloud Microorganisms

Applying the foregoing observations to nanoscale cavities in microorganisms containing water or aqueous liquids, it seems reasonable to expect, that to some extent, solar irradiation will affect the viscosity and density profiles of the fluid phase within such cavities. In combination with heating caused by the sun, such effects could desiccate microorganisms outside clouds. However, for desiccated microorganisms entering the clouds, the coupled, reciprocal change in irradiation intensity and humidity, could induce a rapid uptake of water, including dissolved nutrients, leading to their subsequent revitalization. The difference between the protective cloud cover (wet, nutrient-rich, and low irradiation) and the surrounding atmosphere could be responsible for important differences in the level of vitality of microorganisms reaching the Earth. In addition, it is expected that the manner in which they reach the Earth, e.g., by sedimentation from the dry atmosphere, or from a cloud dissolved by its evaporation, or incorporated in rain drops, will make a difference.

Discussion

The mechanism we have explored may be crucial in controlling the viability of NB returning from space to the Earth. Due to their size, predominantly ranging between 80 and 300 nm,25 a biologically vital aqueous content stored in internal nanocavities, is likely to respond instantaneously to alternations between the light-shielded wet environment of clouds and the luminous dry conditions that prevail outside. NB have been isolated from various terrestrial sources, including animals, humans, and apparently wastewater.26-29 Except the fossil structures identified by McKay et al. on Meteorite ALH84001,30 which could be ancient witnesses for a presence of NB on Earth and maybe on Mars, there has been, so far, no clear evidence for their presence in the atmosphere.

Recently, we presented environmental scanning electron microscope (ESEM) images showing a very large number of nanoparticles (nanovesicles) collected in the stratosphere over Hyderabad, India, via balloon.1 They were virtually indistinguishable from NB isolated from mammalian sources: The complete set of seven morphological parameters (size, shape, size distribution, interconnection, chain arrangement, conglomeration, and cracking in apparently mineral shells) was identical to the corresponding structures regarded as characteristic of NB, both in vitro,25 and in vivo.31-33 One ESEM image showed not only more than 1000 nanovesicles on a substrate, but also larger clumps formed by their aggregation.1 The presence of this aggregation supports the hypothesis that under favorable conditions, e.g., in clouds, NB can use their slime (Figure 2) to form larger clumps. Such giant hydrophilic nuclei would serve as ideal CCN, with a potential to finally form larger rain drops, thus allowing NB to reach the surface of the Earth in a viable state.


Figure 2 Transmission electron microscopy image showing NB isolated from human serum by culturing in mammalian cell culture conditions for three weeks. Reprinted from ref 35 with permission. Image clearly shows how several NB are kept together by slime. Bar 100 nm.

In the dry terrestrial atmosphere, NB presumably survive over extended periods-analogous to desiccated mollusks surviving in deserts-by sealing the surface of their nanoporous shells with a self-synthesized slime film. Solar effects seem plausible because of the susceptibility of the living nanovesicles to exposure to light intensities of the order of the solar constant, as has been amply demonstrated by us in vitro.34,35 As a basic system, the nanovesicle model may inspire the discovery of similar interaction modalities between sunlight and more advanced microorganisms in clouds. At atmospheric altitudes, outside the wet and sun-blocking environment of protective clouds, exposure to the sun is likely to quickly inactivate microorganisms by desiccation via a combination of heating (produced by absorption of solar radiation) and selective interaction of the light with their water content. The experiments thus indicate that there is a higher probability for microorganisms to reach the Earth in an activated state when they have previously spent some time in the wet environment of warm clouds.

Conclusions

Our results indicate that NB, falling solitarily or as clumps through a dry atmospheric column, are likely to reach the surface of the Earth in an inactive state. Those transiting long-lived clouds of high humidity, on the other hand, would reach the ground in rain drops and mist in a revitalized form. Their prolonged stay in the wet environment of clouds is likely to soften the dried slime layer protecting them from desiccation. After revitalization, NB are potential pathogens for both animals and humans-who after contamination, may become sources of release of NB.36 Infectivity could be reduced, however, if anthropogenic emissions predicted to cause long-lived clouds could be checked. Political and social intervention will be needed to encourage the development and use of cleaner sources of energy. We note, that the scientific community is at long last waking up to the asteroid-impact threat to our planet, with a large body of contingency measures already well under discussion. Averting an impending impactor is considerably more difficult, of course, than the consensual measures that can be taken to reverse the effects of global warming. Additional motivation for the urgent search for strategies to combat global warming would emerge from the activation of microorganisms in clouds, a process which is likely to constitute a significant biohazard in the era of the anthropocene.

* To whom correspondence should be addressed. E-mail: samoan@ gmx.net.

Central Institute of Biomedical Engineering, University of Ulm.

Cardiff Centre for Astrobiology, Cardiff University.

1. Sommer, A. P.; Miyake, N.; Wickramasinghe, N. C.; Narlikar, J. V.; Al-Mufti, S. J. Proteome Res. 2004, 3, 1296.[Full text - ACS] [ChemPort] [Medline]

2. Sommer, A. P.; McKay, D. S.; Ciftcioglu, N.; Oron, U.; Mester, A. R.; Kajander E. O. J. Proteome Res. 2003, 2, 441.[Full text - ACS] [Medline]

3. Sommer, A. P.; Pavláth, A. E. J. Proteome Res. 2003, 2, 558.[Full text - ACS] [ChemPort] [Medline]

4. Döppenschmidt, A.; Butt, H. J. Langmuir 2000, 16, 6709.[Full text - ACS]

5. Sommer, A. P.; Levin, Z. Atmos. Res. 2001, 58, 129. [ChemPort] [CrossRef]

6. Sommer, A. P.; Franke, R. P. Nano Lett. 2003, 3, 573.[Full text - ACS] [ChemPort]

7. Sommer, A. P. Crystal Growth. Des., in print.

8. Liepert, B. G.; Feichter, J.; Lohmann, U.; Roeckner, E. Geophys. Res. Lett. 2004, 31, L06207.

9. Rosenfeld, D. Science 2000, 287, 1793 [ChemPort] [Medline] [CrossRef]

10. Sattler, B.; Puxbaum, H.; Psenner, R. Geophys. Res. Lett. 2001, 28, 239.

11. Vinnikov, K. Y.; Grody, N. C. Science 2003, 302, 269. [ChemPort] [Medline] [CrossRef]

12. Sommer, A. P.; Franke, R. P. NanoLett. 2003, 3, 19. [ChemPort] [CrossRef]

13. Sommer, A. P. Proceedings of the 2nd International Conference on Near-field Optical Analysis: Photodynamic Therapy & Photobiology Effects. Johnson Space Center, May 2001, Houston, TX, NASA Conference Publication, 2002, CP-2002-210786, 78.

14. Scatena, L. F.; Brown, M. G.; Richmond, G. L. Science 2001, 292, 908. [ChemPort] [Medline] [CrossRef]

15. Fawcett, N. C.; Craven, R. D.; Zhang, P.; Evans, J. A. Langmuir 2004, 20, 6651.[Full text - ACS] [ChemPort] [Medline]

16. Sommer, A. P.; Franke, R. P. Micron 2002, 33, 227. [ChemPort] [Medline] [CrossRef]

17. Sommer, A. P.; Franke, R. P. J. Proteome Res. 2002, 1, 111.[Full text - ACS] [ChemPort] [Medline]

18. Tyrrell, J. W. G.; Attard, P. Phys. Rev. Lett. 2001, 87, 176104. [ChemPort] [Medline] [CrossRef]

19. Simonsen, A. C.; Hansen, P. L.; Klösgen, B. J. Colloid Interface Sci. 2004, 273, 291. [ChemPort] [Medline] [CrossRef]

20. Sommer, A. P.; Ben-Moshe, M.; Magdassi, S. J. Phys. Chem. B 2004, 108, 8.[Full text - ACS] [ChemPort]

21. Deegan, R. D.; Bakajin, O.; Dupont, T. F.; Huber, G.; Nagel, S. R.; Witten, T. A. Nature 1997, 389, 827. [ChemPort] [CrossRef]

22. Sommer, A. P. J. Phys. Chem. B 2004, 108, 8096.[Full text - ACS] [ChemPort]

23. Sommer, A. P. J. Proteome Res. 2004, 3, 1086.[Full text - ACS] [ChemPort] [Medline]

24. Sommer, A. P. World Conference on Dosing of Antiinfectives (Magic Bullets), 2004, Sept. 9-11, Nürnberg, Germany.

25. Kajander, E. O.; Ciftcioglu, N. Proc. Natl. Acad. Sci. U.S.A. 1998, 95, 8274. [ChemPort] [Medline] [CrossRef]

26. Breitschwerdt, E. B.; Sontakke, S.; Cannedy, A.; Hancock, S. I.; Bradley, J. M. J Clin. Microbiol. 2001, 39, 879. [ChemPort] [Medline] [CrossRef]

27. Wang, X. J.; Liu, W.; Yang, Z. L.; Wie, H.; Wen, Y.; Li, Y. G. Zhonghua Liu Xing Bing Xue Za Zhi 2004, 25, 492. [ChemPort] [Medline]

28. Maniscalco, B. S.; Taylor, K. A. Pathophysiology 2004, 11, 95. [ChemPort] [Medline] [CrossRef]

29. Kim, B. H.; et al. Appl. Microbiol. Biotechnol. 2004, 63, 672. [ChemPort] [Medline] [CrossRef]

30. McKay, D. S.; et al. Science 1996, 273, 924. [ChemPort] [Medline]

31. Jelic, T. M.; et al. South. Med. J. 2004, 97, 194. [Medline]

32. Khullar, M.; et al. Urol. Res. 2004, 32,190. [ChemPort] [Medline]

33. Miller, V. M.; et al. Am. J. Physiol. Heart. Circ. Physiol. 2004, 287, H1115. [ChemPort] [Medline] [CrossRef]

34. Sommer, A. P.; Hassinen, H. I.; Kajander, E. O. J. Clin. Laser Med. Surg. 2002, 20, 241. [Medline] [CrossRef]

35. Sommer, A. P.; et al. Clin. Laser Med. Surg. 2003, 21, 231.

36. Sommer, A. P. J. Proteome Res. 2003, 2, 665.[Full text - ACS] [ChemPort] [Medline]