Agnieszka
Wlodarczyk
*abc,
Paul F.
McMillan
ab and
Susan A.
Greenfield
bc
aDepartment of Chemistry and Materials Chemistry Centre, Christopher Ingold Laboratories, University College London, 20 Gordon Street, London, UK WC1H 0AJ
bRoyal Institution of Great Britain, Davy-Faraday Research Laboratory, 21 Albemarle Street, London, UK W1X 4BS. E-mail: agnieszka@ri.ac.uk
cDepartment of Pharmacology and Oxford Centre for the Science of the Mind, Oxford University, Mansfield Road, Oxford, UK OX1 3QT. E-mail: agnieszka.wlodarczyk@pharm.ox.ac.uk
First published on 1st September 2006
There is growing interest in determining the effects of high pressure on biological functions. Studies of brain processes under hyperbaric conditions can give a unique insight into phenomena such as nitrogen narcosis, inert gas anaesthesia, and pressure reversal of the effects of anaesthetic and narcotic agents. Such research may shed light on the action of anaesthetics, which remains poorly understood, and on the nature of consciousness itself. Various studies have established the behavioural response of organisms to hyperbaric conditions, in the presence or absence of anaesthetic agents. At the molecular level, X-ray crystallography has been used to investigate the incorporation of species like Xe in hydrophobic pockets within model ion channels that may account for pressure effects on neuronal transmission. New magnetic resonance imaging techniques are providing tomographic three-dimensional images that detail brain structure and function, and that can be correlated with behavioural studies and psychological test results. Such whole organ techniques are linked to the molecular scale via voltage-sensitive dye (VSD) imaging studies on brain slices that provide time-resolved images of the dynamic formation and interconnection of inter-neuronal complexes. The VSD experiments are readily adapted to in situ studies under high pressure conditions. In this tutorial review we review the current state of knowledge of hyperbaric effects on brain processes: anaesthesia and narcosis, recent studies at the molecular level via protein crystallography at high pressure in a Xe atmosphere, and we also present some preliminary results of VSD imaging of brain slices under hyperbaric conditions.
![]() Agnieszka Wlodarczyk | Dr Agnieszka Wlodarczyk is a postdoctoral researcher in the Davy-Faraday Laboratory at the Royal Institution of Great Britain and also in the Chemistry Department at University College London. She is also a visiting researcher in the Pharmacology Department at Oxford University. She graduated with an MS in Theoretical Physics in 1998 and completed her PhD in Biophysics in 2003 at Adam Mickiewicz University, Poznan, Poland. Since moving to London in 2003 she has started an interdisciplinary project on hyperbaric effects in neuroscience. Her research interests include optical methods to study biomolecules in solution and the dynamics of neuronal assemblies. |
![]() Paul F. McMillan | Paul F. McMillan has an established career in physical/solid state chemistry and physics with special emphasis on high pressure science, including designing high pressure cells and carrying out optical spectroscopy/imaging experiments in situ under high P conditions. He holds a joint post as Professor of Chemistry at UCL and in the Davy-Faraday laboratory at the RI. He has worked across the entire pressure range, from "extreme" high pressure conditions into the megabar range, to pressures of a few hundreds of atmospheres important in deep ocean biochemistry. His current research involves synthesis and study of novel solid state materials, including solids and liquid-state transitions, under high pressure–high temperature conditions. He has built programmes for in situ experiments on solids and liquids under "extreme" P–T conditions, using laser-heated diamond anvil cells to investigate materials at up to ∼1 Mbar and 3000-5000 °C. Other synthesis studies use "large volume" devices (1–20 GPa; 500–1800 °C); he is now developing "soft chemistry" approaches to inorganic–organic materials syntheses in the "lower" pressure range, between 1–5 kbar and up to a few hundred °C. |
![]() Baroness Greenfield | Baroness Greenfield is Director of the Royal Institution of Great Britain (the first woman to hold that position) and Professor of Pharmacology at the University of Oxford, where she leads a multidisciplinary team investigating neurodegenerative disorders. In addition she is Director of the Oxford Centre for the Science of the Mind, exploring the physical basis of consciousness. Her books include The Human Brain: A Guided Tour (1997), The Private Life of the Brain (2000), and Tomorrow's People: How 21st Century Technology Is Changing the Way We Think and Feel (2003). She has spun off four companies from her research, made a diverse contribution to print and broadcast media, and led a Government report on “Women In Science”. She has received 28 Honorary Degrees, Honorary Fellowship of the Royal College of Physicians (2000), a non-political Life Peerage (2001) as well as the Ordre National de la Legion d'Honneur (2003). In 2006 she was installed as Chancellor of Heriot-Watt University and voted ‘Honorary Australian of the Year'. |
The phenomenon of general anaesthesia is, by definition, a loss of consciousness and a reduced perception of and response to external stimuli, among mammals and other organisms, as a result of exposure to chemical agents. It is systematically applied in clinical practice, to suppress patient sensation and movement during highly traumatic and invasive surgery. Narcotics cause related physiological effects that involve altered states of consciousness, which are achieved voluntarily or involuntarily, by medical application or self-administration of drugs. Various anaesthetics have been identified and are administered with precision, according to empirical principles that have been developed through decades (and in some cases centuries) of medical experimentation. However, there is as yet no explanation for anaesthetic action.1–4
Major advances in neuroscience are now being made at a molecular level, through a combination of biochemistry and biophysics methods including electrophysiology, protein crystallography and sequencing, and recombinant DNA techniques and cell-expression studies of transmembrane ion channels, to gain a detailed understanding of the structure and properties of the ion channels involved in neuronal cell signalling and neurotransmitter receptor sites. The neurotransmitters themselves and the regions of the CNS in which they are active are identified by biochemical assays, combined with neurophysiology experiments. A large gap must be filled between those observations that link neurological chemistry to the electrophysiological responses at a molecular scale, and the large-scale properties of the dynamically evolving neuronal networks that are imaged by MRI and fMRI scanning, however. A link between the two can be provided by the use of voltage-sensitive dye (VSD) imaging techniques that are applied to brain slices during in vitro or in vivo experiments. These studies permit visualisation of the flow of electrochemical information though specified pathways in brain slices, via difference fluorescence spectroscopy with a time resolution appropriate to neuronal information transfer (e.g., 1–10 ms).5,6
Hyperbaric effects in neuroscience are well known. The physiological consequences of breathing compressed air and various gas mixtures have been documented since the advent of deep diving and as a result of studies of workmen exposed to sub-surface conditions in mines and other excavation sites. The unusual anaesthetic effects of chemically inert gases such as xenon, and nitrogen narcosis under hyperbaric conditions, have long provided an unresolved problem for neuroscience.7–10 Even more intriguing is the observation that the action of various narcotic and anaesthetic species can be reversed by application of high pressure conditions.11–13
This paper begins with a review of the pioneering experiments, which first demonstrated the link between high pressure and anaesthesia/narcosis. The next section is devoted to nitrogen narcosis and xenon anaesthesia, and these two phenomena are discussed together because the active species, namely N2 and Xe, gain their narcotic and anaesthetic properties respectively under increased pressure. There follows a review of recent experiments which have revealed that noble gases can occupy hydrophobic pockets buried within protein molecules; these findings may shed new light on the understanding of anaesthesia and narcosis. Next, we introduce the theories of anaesthesia and give possible explanations, as discussed in the literature, as to how pressure can reverse anaesthesia. The next section gives an introduction to a relatively new method in neuroscience in which optical imaging of neuronal voltage wave propagation in real time is studied using voltage-sensitive dyes. This technique has been used within a newly developed high pressure chamber for the in situ VSD imaging of rat hippocampal slices under hyperbaric conditions. The last section gives a summary and future directions. An introduction to basic concepts and techniques in neuroscience can be found in standard texts.14
Following early observations of extinction of the luminescence from firefly luciferase and luminescent bacteria under hyperbaric conditions,21 the first direct evidence for pressure reversal of anaesthesia/narcosis was obtained from studies of tadpoles treated with ethanol.11 In a now-classic study, young larvae of Rana sylvatica were placed in a 3–6% ethanol solution in water (i.e., similar to beer) where they became narcotised, in that they ceased moving spontaneously and they no longer responded to external stimuli. They were then transferred to a hyperbaric chamber equipped with observation windows. As the pressure was raised to 2000–5000 psi (130–330 atm) the animals resumed their normal swimming behaviour, indicating that the effects of alcohol had been antagonised by the application of high hydrostatic pressure. A similar pressure reversal effect was observed for tadpoles narcotised using urethane (0.08 M), but not for n-amyl carbamate (0.001 M), showing that the effect is not completely general for all anaesthetic or narcotic species. Johnson and Flagler made an interesting observation on unnarcotised tadpoles under hyperbaric conditions. With increasing pressurisation, the animals became more active, indicating that pressure alone has an influence on neuronal excitability. The maximum hyperactivity occurred at around 2000 psi (1 atm = 14.7 psi), and thereafter it decreased. By 5000 psi, all motion had ceased. As noted by Johnson and Flagler, similar behaviour had been observed previously for other aquatic species under hyperbaric conditions.
In studies by Lever et al., narcosis induced in Italian crested newts by 34 atm of N2 (see next section) was found to be antagonised by increasing the pressure to 140 atm using He gas. Newts were also submerged in liquids and anaesthetised with solutions of sodium pentobarbitone, ether, halothane or butanol, and the pressure was applied mechanically in the absence of a gas phase. In both series of hyperbaric experiments, increasing the total pressure over a range up to 140 atm was found to antagonise the anaesthetic effects.13 Observations of pressure reversal effects were then extended to mammals. Mice were first narcotised by exposure to 45 atm of N2, and then subjected to hyperbaric compression with He. Analogous results were obtained with sodium pentobarbitone.13
In more recent work, specialised hyperbaric chambers were developed to carry out not only behavioural studies of whole animals, but to enable detailed neuronal electrophysiology measurements at high pressure. Using the new chambers, continuous intracellular recording signals (ICRs) could be obtained from, e.g., mammalian neurons within brain slices at high pressure.12,22–24 The methods are readily extended to studies of individual receptor sites and transmembrane ion channels, that are conveniently expressed via recombinant DNA techniques within the large eggs (i.e., oocytes) of the frog Xenopus. Patch-clamp techniques that enable a direct measurement of an ion current passing through ion channel proteins are implemented in the high pressure chamber.12
Within the hyperbaric chambers designed for electrophysiology experiments, gas pressures up to approximately 12 atm absolute (i.e., 12 ata, rather than pressures relative to ambient conditions) are applied using various pure or mixed gases (e.g., compressed air, He, He–O2 ‘heliox’ mixtures) that can be pumped into the chamber or derived from high pressure gas cylinders. Important external parameters, such as the bath and tissue slice temperature, the O2 partial pressure (pO2), and the pH, are all constantly monitored during the hyperbaric voltage recording experiments. Such studies give detailed information on features of the neuronal electrochemical activity, including membrane conductance, synaptic potentials, and firing rate that can be correlated with the presence or absence of anaesthetic or narcotic species under hyperbaric conditions.
In addition to determination of pressure reversal effects, the electrophysiology experiments allow us to determine the tissue and cellular responses to hyperbaric conditions elicited by different pressurising gases, to identify various types of barosensitivity, and also to study the phenomenon of inert gas narcosis and O2 sensitivity in the same neuron.12,22–24
The new apparatus and experimental strategies have been applied to study the binding of alcohols, especially ethanol, to receptor sites within the CNS.12,23,24 Exposure to 12 ata heliox was found to antagonise ethanol potentiation of GABAA-activated Cl− uptake in brain membranes from three strains of genetically modified mice. At the range of alcohol concentrations used in the study (25–200 mM), the gas-applied high pressure conditions caused the behavioural and anaesthetic effects of ethanol to be reversed.23 These results provided new evidence that ethanol potentiation of the GABAA receptor (i.e., GABAAR) site is a key function of ethanol that leads to its behavioural and psychological consequences.23 Two years later the same authors extended their study to the biochemical level using glycine receptors (GlyR) expressed in Xenopus oocytes.12 Those pioneering results indicated that pressure directly and selectively antagonises ethanol potentiation of the α1GlyR function in a reversible and concentration- and pressure-dependent manner,12 and that alcohols may act by a common mechanism on ligand-gated ion channels.12,23
Although alcohol (ethanol) clearly exhibits pressure reversal effects, it is perhaps not an ideal test case to develop detailed models for hyperbaric effects on anaesthesia and narcosis, because of the biochemical and neurophysiological complexity of the drug action.25 For many years, it has been debated whether the primary mode of action of alcohol occurred within the lipid cell membrane, by disrupting the fatty acid structural arrangement or changing the membrane volume or its curvature, or more specifically at protein sites associated with receptors or transmembrane ion channel complexes.25 During the past two decades, there has been growing evidence that the most important sites for ethanol potentiation lie within neurotransmitter receptors or ion channels.12,23,25 Specific alcohol binding sites within protein complexes that provide useful models of the transmembrane ion channels and receptor sites are now being identified, by a combination of biochemical studies combined with X-ray crystallography and NMR structure determination techniques.23,26–28 The primary binding site for alcohols, including ethanol, is thought to occur deep within the GABAA receptor, thus modifying the inhibitory GABA-gated entry of Cl− ions into the cell29,30 (Fig. 1). However, glutamate (NMDA) receptors are also thought to form important targets for alcohol binding within the CNS, for example those for AMPA (α-amino-3-hydroxy-5-methylisoxazole-4-propionic acid) and/or kainate that mediate fast excitatory transmission within the CNS. Ethanol binding likely occurs at several different sites within various ion channels and neuroreceptor sites to result in the neurological and physiological consequences, and membrane lipid solubility likely also plays a role, under variable concentration- and pressure-dependent regimes.
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Fig. 1 A general structural model for the GABAA receptor redrawn from Cooper et al.29 The GABAA complex is a pentamer of two α, two β and one γ subunits, formed by α-helical portions of a single transmembrane protein that loops back and forth throughout the cell membrane. It is a ligand-gated Cl− channel that has an inhibitory action on neurotransmission. The receptor binds the agonist GABA and neuroactive species such as muscimol, and also the antagonist bicuculline on the α and β subunits. Also there are binding sites on the receptor for barbiturates, ethanol, and on the α subunit for the benzodiazepine family of narcotics. The primary binding site for alcohols including ethanol is thought to occur deep within the GABAA receptor.29,30 All these substances potentiate the channel-opening action of GABA on the GABAA receptor. |
The surprising general anaesthetic effect of the noble gases Xe and Kr has long proved a highly puzzling biochemical/physiological phenomenon.10,31–33 Xenon is now well known to produce anaesthesia in humans and other mammals, with apparently minimal side effects, and it has significant potential for clinical applications, despite the high cost of the gas.34 It was recently determined that anaesthetic use of Xe results in remarkable cardiovascular stability, rapid onset and offset of its action resulting from its extremely low blood–gas partition coefficient, neuroprotection and profound analgesia. No evidence of toxicity and no mutagenic or carcinogenic properties were found in several studies.34 The minimum alveolar concentration in humans (MAC†) of Xe is 0.6–0.7 atm. The MAC for Xe in other organisms is higher: for monkeys and dogs it ranges between 0.9–1.2 atm, and in rats it is ∼1.6 atm.10 Kr shows anaesthetic effects at higher pressures than Xe; He and Ne do not show any anaesthetic action before the onset of convulsions (followed by death) at ∼85 atm (He) and 90–130 atm (Ne) in rats and mice. The sites occupied by the noble gas atoms (and N2) are not well known at present. However, biochemical studies combined with crystallography and molecular dynamics simulations indicate that Xe, Kr and N2 could occupy hydrophobic sites or pockets within ion channels such as those associated with the excitatory glutamate (NMDA) neurotransmitter receptor complex.9
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Fig. 2 The crystal structure of unligated maltose binding protein with xenon, deduced using 129Xe NMR spectroscopy.41 This type of Xe binding site within hydrophobic pockets developed in the transmembrane protein complexes is confirmed and established by X-ray crystallography, using the heavy-atom method. |
VSDs take their name from their ability to undergo changes in their electronic structure and consequently their fluorescence spectra in response to changes in the surrounding electric field. One of the most widely used VSDs for brain slice studies is di-4-ANEPPS (D-1199, Molecular Probes Inc.) which is sensitive to submillisecond membrane potential changes and ±0.1 mV changes in fluorescence intensity (Fig. 3). VSDs are generally lipophilic molecules, which stain the neural cell membranes. Other important properties include photostability and non-toxicity to the neuronal tissue. Their optical response is sufficiently fast to detect transient potential changes in neuronal cells. During passage of the electrical signal within the neurons the change in the intensity of fluorescence (ΔF) is measured in each pixel of the CCD image, relative to the initial intensity of fluorescence (F). The optical response recorded by VSD fluorescence thus tracks effectively, in real time, the passage of a voltage wave throughout the neuronal system. VSD imaging provides a useful way of observing the formation and flow of large-scale dynamic neuronal complexes in real time, at a distance scale that is intermediate between that of the molecular interactions at the membrane and synapse, and those at the whole-organ or whole-animal level probed by magnetic resonance imaging or physiological/psychology studies. A typical VSD imaging system consists of a stage with a chamber to mount the brain slice, an excitation light source, and a CCD camera for data collection.6 The sample stage is equipped with electrodes for stimulation of the neuronal signal that can also be used for electrophysiological recording. The excitation light is provided by a halogen lamp (150 W), introduced into the microscope system by a light-guide with an appropriate condenser lens. The fluorescence signal is collected by and captured on the CCD sensor of the optical imaging system (Fig. 4).
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Fig. 3 The structure of di-4-ANEPPS dye molecule used in VSD imaging. |
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Fig. 4 A schematic illustration of the CCD camera system, optics and set-up used in VSD imaging studies,6 including under hyperbaric conditions. |
We recently developed an experimental pressure chamber to conduct in vitro VSD imaging experiments of the flow of voltage-regulated information in neuronal complexes under hyperbaric conditions (Fig. 5). Preliminary results indicate that under hyperbaric conditions (P = 32 atm) the neuronal voltage response is much stronger, and the signal propagation along the CA3–CA1 Schaeffer collateral is considerably extended (Fig. 6).
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Fig. 5 Top and bottom: images of the hyperbaric cell for VSD imaging studies of neuronal signal propagation. Top: the specially designed carriage for x-, y-, z-manipulation of the electrode assembly is seen, with the electrode poking down into the circular brain slice mounting area. Bottom: the cell assembly is shown with the viewing windows in place. Pumping of artificial cerebrospinal fluid (aCSF) to achieve hyperbaric conditions is achieved through the inlet and outlet connections on the right, and electrode manipulation occurs by turning the knurled brass knobs. The cell fits underneath the VSD fluorescence microscopy imaging instrument. |
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Fig. 6 A fluorescent image of a rat hippocampal slice obtained using the VSD method at ambient pressure and 32 atm respectively in the high pressure cell. Still images of neuronal transient assembly formation on a Schaeffer collateral pathway of a rat hippocampal slice stained with VSD are shown. The overall image is 2 × 3 mm and each pixel provides an optical trace of differential fluorescence dF/F over time. The maximum dF/F signals are superimposed on the hippocampus image with the excitation electrode, The Schaeffer collateral and dentate gyrus are easily recognised on the slice. The amplitude of the optical signal represented in pseudo-colours indicates the degree of membrane depolarisation. Two electrical pulses of amplitude 60 V lasting 0.1 ms each, separated from each other by 60 ms, triggered spreading of the neuronal signal within the brain slice. The depolarisation started at the stimulating electrode, with the first excitation pulse occurring 100 ms after starting the measurement, and spread along the CA3–CA1 Schaeffer collateral pathway. Under hyperbaric conditions (P = 32 atm), the neuronal voltage response is much stronger, and the signal propagation along the CA3–CA1 Schaeffer collateral is considerably extended. |
Footnote |
† MAC is defined as the minimum alveolar concentration of an inhalation anaesthetic, at one atmosphere pressure, that produces immobility in 50% of the subjects exposed to a noxious stimulus. Thus, MAC corresponds to the effective dose that anaesthetised half of the subjects (i.e. ED50). |
This journal is © The Royal Society of Chemistry 2006 |