chloride homeostasis in central neuronsumu.diva-portal.org/smash/get/diva2:1047042/summary01.pdfthe...
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Chloride Homeostasis in Central Neurons
Tushar Yelhekar
The Department of Integrative Medical Biology
Umeå 2016
Responsible publisher under swedish law: the Dean of the Medical Faculty
This work is protected by the Swedish Copyright Legislation (Act 1960:729)
ISBN: 978-91-7601-602-2
ISSN: 0346-6612
New Series No: 1861
Cover illustrations: Membrane current traces from preoptic neurons
Elektronisk version tillgänglig på http://umu.diva-portal.org/
Printed by: Print & Media, Umeå University
Umeå, Sweden 2016
i
Dedicated to my teachers
ii
iii
Table of Contents
List of papers v
Abbreviations vi
Abstract vii
Introduction 1
GABA- and glycine-receptor mediated neurotransmission 2
Receptor structure 2
Currents 3
Desensitization 4
Neurosteroids 4
Thermodynamics of Cl– movement 5
Cation chloride cotransporters (CCCs) 7
KCC2 7
NKCC1 9
Thermodynamics of KCC2 and NKCC1 10
Role of impermeant anions in setting [Cl–]i 11
Specific aims of the thesis 12
Methodological considerations 13
Cell and tissue preparation 13
Electrophysiological recording 14
Electrophysiological measuring of [Cl–]i 15
Cl– transporter activity and [Cl–]i homeostasis 16
Estimating relative Cl– leak by a novel method 16
Immunoblotting 17
Computational modeling 17
Results and Discussion 19
Project 1: Estimating [Cl–]i by electrophysiological methods 19
Project 2: Role of Cl– transporters and extracellular matrix in [Cl–]i
homeostasis 22
Project 3: Influence of Cl– leak conductance on [Cl–]i homeostasis 26
Project 4: Role of KCC2 under conditions with different
inhibitory or excitatory conductances 30
Overall summary 31
Acknowledgements 32
References 33
Paper I-IV
iv
v
List of papers
This doctorate dissertation is based on the following four papers which will be referred
to by their roman numbers:
I. Yelhekar TD, Druzin M, Karlsson U, Blomqvist E and Johansson S
(2016) How to Properly Measure a Current-Voltage Relation?—
Interpolation vs. Ramp Methods Applied to Studies of
GABAA Receptors. Frontiers in Cellular Neuroscience 10:10. doi:
10.3389/fncel.2016.00010
II. Yelhekar TD, Kuznetsova T, Malinina E, Ponimaskin E, Dityatev A,
Druzin M and Johansson S (2016) Extracellular Matrix Regulates
Neuronal Chloride Concentration via K+-Cl–-cotransporter 2.
Manuscript.
III. Yelhekar TD, Druzin M and Johansson S (2016) Contribution of Resting Conductance, GABAA-Receptor Mediated Miniature Synaptic
Currents and Neurosteroid to Chloride Homeostasis in Central
Neurons. Manuscript.
IV. Johansson S, Yelhekar TD and Druzin M (2016) Commentary:
Chloride Regulation: A Dynamic Equilibrium Crucial for Synaptic
Inhibition. Frontiers in Cellular Neuroscience 10:182. doi:
10.3389/fncel.2016.00182
vi
Abbreviations
CCC cation chloride cotransporter
ChABC chondroitinase ABC
[Cl–]i intracellular chloride concentration
[Cl–]o extracellular chloride concentration
CNS central nervous system
CSPG chondroitin sulphate proteoglycan
DFCl driving force for Cl– current
DFGABA driving force for current mediated by GABAARs
ECl Cl– equilibrium potential
ECM extracellular matrix
EGABA reversal potential of current mediated by GABAARs
eIPSC evoked inhibitory postsynaptic current
EK K+ equilibrium potential
F Faraday constant
GABA γ-aminobutyric acid
GABAAR γ -aminobutyric acid type A receptor
GABABR γ -aminobutyric acid type B receptor
GABACR γ -aminobutyric acid type C receptor
gCl Cl– conductance
GlyR glycine receptor
IGABA current mediated by GABAARs
ICl Cl– current
IPSC inhibitory postsynaptic current
I-V current-voltage
KCC2 K+-Cl–-cotransporter 2
mIPSC miniature inhibitory postsynaptic current
MPN medial preoptic nucleus
NKCC1 Na+-K+-Cl–-cotransporter 1
P permeability
R gas constant
sIPSC spontaneous inhibitory postsynaptic current
T temperature
Vm membrane potential
vii
Abstract
The overall aim of the present thesis is to clarify the control of intracellular chloride
homeostasis in central neurons, because of the critical role of chloride ions (Cl–) for
neuronal function. Normal function of the central nervous system (CNS) depends on
a delicate balance between neuronal excitation and inhibition. Inhibition is, in the
adult brain, most often mediated by the neurotransmitter γ-aminobutyric acid
(GABA). GABA may, however, in some cases cause excitation. GABA acts by
activating GABA type A receptors (GABAARs), which are ion channels largely
permeable to Cl–. The effect of GABAAR-mediated neuronal signaling - inhibitory or
excitatory - is therefore mainly determined by the Cl– gradient across the membrane.
This gradient varies with neuronal activity and may be altered in pathological
conditions. Thus, understanding Cl– regulation is important to comprehend neuronal
function. This thesis is an attempt to clarify several unknown aspects of neuronal Cl–
regulation. For such clarification, a sufficiently sensitive method for measuring the
intracellular Cl– concentration, [Cl–]i, is necessary. In the first study of this thesis, we
examined two electrophysiological methods commonly used to estimate [Cl–]i. Both
methods, here called the interpolation and the voltage-ramp method, depend on an
estimate of the Cl– equilibrium potential from the current-voltage relation of GABA-
or glycine-evoked Cl– currents. Both methods also provide an estimate of the
membrane Cl– conductance, gCl. With a combination of computational and
electrophysiological techniques, we showed that the most common (interpolation)
method failed to detect changes in [Cl–]i and gCl during prolonged GABA application,
whereas the voltage-ramp method accurately detected such changes. Our analysis also
provided an explanation as to why the two methods differ. In a second study, we
clarified the role of the extracellular matrix (ECM) for the distribution of Cl– across
the cell membrane of neurons from rat brain. It was recently proposed that immobile
charges located within the ECM, rather than as previously thought cation-chloride
transporter proteins, determine the low [Cl–]i which is critical to GABAAR-mediated
inhibition. By using electrophysiological techniques to measure [Cl–]i, we showed that
digestion of the ECM decreases the expression and function of the neuron-specific K+
Cl– cotransporter 2 (KCC2), which normally extrudes Cl– from the neuron, thus
causing an increase in resting [Cl–]i. As a result of ECM degradation, the action of
GABA may be transformed from inhibitory to excitatory. In a third study, we
developed a method for quantifying the largely unknown resting Cl– (leak)
conductance, gCl, and examined the role of gCl for the neuronal Cl– homeostasis. In
isolated preoptic neurons from rat, resting gCl was about 6 % of total resting
conductance, to a major part due to spontaneously open GABAARs and played an
important role for recovery after a high Cl– load. We also showed that spontaneous,
impulse-independent GABA release can significantly enhance recovery when the
GABA responses are potentiated by the neurosteroid allopregnanolone. In a final
commentary, we formulated the mathematical relation between Cl– conductance,
viii
KCC2-mediated Cl– extrusion capacity and steady-state [Cl–]i. In summary, the
present thesis (i) clarifies how well common electrophysiological methods describe
[Cl–]i and gCl, (ii) provides a novel method for quantifying gCl in cell membranes and
(iii) clarifies the roles of the ECM, ion channels and ion transporters in the control of
[Cl–]i homeostasis and GABAAR-mediated signaling in central neurons.
Keywords: chloride concentration, current-voltage relation, interpolation, voltage
ramp, reversal potential, [Cl–]i recovery, KCC2, extracellular matrix, GABAA
receptor, chloride leak conductance, neurosteroid
1
Introduction
Chloride (Cl–) is the most abundant physiological anion, involved in a number of
cellular functions, including pH regulation (Boron & Russell, 1983; Boron, 2004;
Ruffin et al., 2014), gene regulation (Succol et al., 2012; Valdivieso et al., 2016),
trans-epithelial ion transport (Hartzell, 2009; Sun et al., 2009) and cell-volume
regulation (Sardini et al., 2003; MacAulay et al., 2004; MacAulay & Zeuthen, 2010).
In addition, Cl– is crucial for neuronal signaling. Normal function of the central
nervous system (CNS) depends on a delicate balance between neuronal excitation and
inhibition, mediated by signals in the synaptic contacts between neurons. In the brain,
γ-aminobutyric acid (GABA) is by far the most common neurotransmitter that
mediates inhibition. GABA binds to and activates GABA type A receptors
(GABAARs) in the neuronal cell membrane. They are ligand-gated ion channels
largely permeable to Cl– and to a small extent to bicarbonate (HCO3–) (Bormann et
al., 1987). The strength and polarity of GABAAR-mediated signaling is mainly
determined by the number of open ion channels and by the Cl– gradient across the
membrane. In mature neurons, the intracellular Cl– concentration ([Cl–]i) is low, often
5 - 10 mM, due to Cl– extrusion mechanisms (Rivera et al., 1999). As a consequence,
activation of GABAARs leads to a net influx of Cl–, hyperpolarization of the
membrane and neuronal inhibition, that is, a reduced tendency to generate impulses.
Since the inhibitory signaling is associated with Cl– flux through the membrane, it
will also be associated with changes in [Cl–]i. Therefore, to maintain functional
signaling properties, neurons must be equipped with mechanisms to restore [Cl–]i.
There are, however, several conditions under which GABA may excite rather than
inhibit affected neurons. First, this may occur early in development, when [Cl–]i is
much higher than in mature neurons (Ben-Ari et al., 1989; Ben-Ari, 2002). In addition,
there are several pathological conditions where the GABAAR-mediated inhibition is
compromised and an associated maintained change of [Cl–]i (also called [Cl–]i shift)
is evident. These conditions include epilepsy (Kaila & Miles, 2010; Khirug et al.,
2010; Kaila et al., 2014b; Karlócai et al., 2015), chronic pain (Coull et al., 2003; De
Koninck, 2009; Gagnon et al., 2013), autism (Lemonnier & Ben-Ari, 2010; Tyzio et
al., 2014), stress (Hewitt et al., 2009; Maguire, 2014; Bains et al., 2015), and spinal
cord injury (Boulenguez et al., 2010). Despite many studies, the mechanisms and
factors involved in Cl– regulation are not well understood. Thus, for instance, the
causes of the [Cl–]i shifts during transitions to pathological states are not clear (Kaila
et al., 2014a; Wu et al., 2015). As a consequence, understanding Cl– regulation is not
only important to comprehend normal neuronal function but also to understand the
etiology of disease, necessary for the development of therapeutic drugs.
The overall aim of my Ph.D. research project was to clarify the intracellular chloride
homeostasis in central neurons. The present thesis is based on three main projects. In
2
the first project (paper I), we compared two common electrophysiological methods to
understand how [Cl–]i can best be measured and how well the methods reflect the Cl–
conductance, which is determined by the number of Cl–-permeable channels in the
neuronal cell membrane. In the second project (paper II), we studied the role of two
potentially critical factors for setting [Cl–]i and controlling synaptic inhibition: (i) Cl–
-transporting membrane proteins, previously thought to play an important role, but
recently questioned, and (ii) the extracellular matrix (ECM) that normally surrounds
the brain cells, previously not thought directly important for signaling, but recently
shown to influence [Cl–]i. Besides transporters, passive flux through ion channels is
expected to influence the resting [Cl–]i. Therefore, in the third project (paper III) we
developed a new method and measured the Cl– background, “leak”, conductance and
its influence on Cl– homeostasis. We also, in a “general commentary” (paper IV)
clarified the role of a Cl– transporter under different conditions by using a
mathematical model and computer simulations.
GABA- and glycine-receptor mediated neurotransmission
Inhibitory neurotransmission is important for proper neuronal coding and CNS
function. In the adult CNS, GABA and glycine are the most common inhibitory
neurotransmitters. GABA is predominantly present in the brain, whereas glycine is
common in the spinal cord and brainstem. Besides GABAA receptors, GABA acts on
several other types of receptors such as GABAB and GABAC receptors. GABAB
receptors (GABABRs) are metabotropic membrane receptors that mediate neuronal
signaling via G-protein activation. They often underlie slow synaptic signals and are
mainly present in presynaptic sites, where the main function is to reduce
neurotransmitter release (Takahashi et al., 1998). A controversial third type, GABA
C receptors (GABACRs) are ion channels like GABAARs. GABACRs are now usually
considered to be a subtype of GABAARs (Olsen & Sieghart, 2008). Similarly to
GABAARs, glycine receptors (GlyRs) are ligand-gated ion channels, permeable to
anions like Cl– and HCO3–, and mediate fast neurotransmission (Eccles et al., 1977;
Bormann et al., 1987; Kaila et al., 1993).
Receptor structure: GABA- and glycine-gated ion channels are functionally and
structurally similar. They belong to the Cys-loop receptor superfamily. Other
members of this family are cation-selective nicotinic acetylcholine receptors and
serotonin type 3 receptors. GABAARs are assembled in a heteropentameric structure
from a large family of subunits (α1–6, β1–3, γ1–3, δ, ε, θ, π and ρ1–3) encoded by 19
different genes. The major native isoforms are composed of two α, two β and a single
γ, δ or ε subunit (Olsen & Sieghart, 2009; Gunn et al., 2015). GABACRs are
homopentameric receptors composed of ρ subunits. Each subunit contains four
transmembrane (TM1-4) domains (Figure 1A). An extracellular domain includes
GABA- and receptor modulator (see below) binding sites (Olsen & Tobin, 1990). A
3
prominent intracellular domain between TM3 and TM4 is a target of both
serine/threonine and tyrosine protein kinases (Moss et al., 1995; McDonald et al.,
1998; Moss & Smart, 2001). The central ion channel pore is solely formed by the
TM2 domains of each subunit (Macdonald & Botzolakis, 2009) (Figure 1B). Synaptic
GABAARs contain a γ subunit and, compared with δ-subunit containing GABAARs,
display a lower affinity for GABA. Conversely, α4-, α5- and δ-subunit containing
receptors dominate in extrasynaptic sites (Farrant & Nusser, 2005).
Figure 1. Structure of Cys-loop receptor ion channels. A. Individual subunits contain four
transmembrane domains (TM1-4). B. A receptor is assembled in a pentameric structure and
the ion channel is formed by a ring of TM2 domains (blue). (Reproduced from Moss & Smart,
2001, with permission.)
Currents: Presynaptic release of GABA leads to activation of the postsynaptic
GABAARs and opening of the channels that mediate inhibitory postsynaptic currents
(IPSCs), also called phasic currents due to their transient nature. In common
terminology, spontaneous IPSCs (sIPSCs) refer to those generated in the absence of
external stimulation, miniature IPSCs (mIPSCs) refer to those generated
spontaneously when impulse generation is blocked, whereas evoked IPSCs (eIPSCs)
refer to those evoked by stimulation expected to cause presynaptic impulse generation
(Farrant & Nusser, 2005). Besides the action at the synaptic GABA receptors
responsible for the phasic currents, GABA may also escape from the synapse and
activate extrasynaptic GABAARs (Semyanov et al., 2003). Extrasynaptic receptors
have a higher affinity for GABA than their synaptic counterparts and they carry more
sustained, tonic currents (Brickley et al., 1996; Semyanov et al., 2004). Changes in
tonic current influence the neuronal action potential threshold and firing pattern
(Mitchell & Silver, 2003; Semyanov et al., 2004). As noted above, the currents
associated with GABAAR activation, whether phasic or tonic, are accompanied by
changes in Cl– concentrations that must be coped with to maintain normal function.
Although it is known that synaptic activation may be associated with a rise in [Cl–]i
4
(Thompson & Gähwiler, 1989), the influence of receptor activation on the neuronal
Cl– homeostasis in various conditions is still not well understood.
Desensitization: Although GABA-receptor channels are opened by GABA, they may
subsequently close during maintained exposure to GABA. This so-called
desensitization is a property shared with most other ligand-gated ion channels. It may
occur at different time scales and is thought crucial for synaptic communication. In
general, desensitization may be thought to limit the duration of synaptic influence, but
paradoxically the entrance to a desensitized state may imply prolonged synaptic
currents because of subsequent channel re-entry to the open state (Jones & Westbrook,
1995). The currents mediated by GABA- and glycine-gated channels, as commonly
studied under voltage-clamp conditions at steady membrane potentials, usually decay
with time at prolonged exposure to the agonist. This has been interpreted as reflecting
desensitization. However, recently Karlsson et al. (2011) showed that during
activation of GABAARs and GlyRs, the current decay is largely due to dramatic
changes in [Cl–]i whereas true desensitization is slow or even absent. True
desensitization, however, should be reflected by a decay of GABA/glycine-
mediated conductance. To clarify the properties of GABA- and glycine-gated
channels, critically important for synaptic inhibition, it is therefore crucial to be
able to estimate both [Cl–]i and channel-induced conductance. Because of different
conclusions in previous studies (cf e.g. Bianchi & Macdonald, 2002; Karlsson et al.,
2011), we, in paper I, clarified the consequences of the two most common
electrophysiological methods used to estimate conductance and ion concentrations.
As described below, the methods differ dramatically with respect to how correctly
these parameters are given.
Neurosteroids: A GABAAR protein complex has many binding sites, two for the
ligand GABA and several modulatory sites for benzodiazepines, barbiturates and
neurosteroids (Majewska et al., 1986; Barbaccia et al., 2001). Peripherally
synthesized neuroactive steroids may modulate neuronal activity by acting at
GABAARs (Strömberg et al., 2006; Herd et al., 2007). Some steroids are converted to
neuroactive forms by cells within the CNS. However, neurons and glial cells also
express enzymes for de novo synthesis of neurosteroids within the CNS (Corpéchot
et al., 1981; Mellon & Deschepper, 1993). Significant production of neuroactive
steroids or neurosteroids, with resulting changes in the steroid levels within the CNS,
is observed during specific developmental stages or physiological conditions, like
gestation, delivery (Concas et al., 1998; Luisi et al., 2000) and during stress (Purdy et
al., 1991), but also in pathological conditions, like epilepsy (Bäckström, 1976; Grosso
et al., 2003; Mareš et al., 2006). The locally synthesized neurosteroids act in a
paracrine manner by modulating GABAARs in neighboring CNS regions.
Endogenously produced neurosteroids including the progesterone metabolites 5α-
pregnan-3α-ol-20-one (3α,5α-THPROG or allopregnanolone) and 5β-pregnan-3α-ol-
5
20-one (3α,5β-THPROG), and the deoxycorticosterone metabolite 5α-pregnan-3α,21-
diol-20-one (3α,5α-THDOC) are positive modulators of GABAARs (Belelli &
Lambert, 2005; Lambert et al., 2009). Binding of a neurosteroid to a GABAAR leads
to changes in receptor conformation and channel kinetics (Majewska et al., 1986). The
effects depend on the neurosteroid concentration. For instance, at high or low
concentration, allopregnanolone directly activates or potentiates the action of GABA
at GABAARs, respectively (Haage & Johansson, 1999). Since allopregnanolone in
several ways may dramatically increase the GABAAR-mediated Cl– flux, it may
significantly affect the Cl– homeostasis. In the present work (paper III), the effect of
allopregnanolone on passive, channel-mediated recovery after a rise in [Cl–]i was
clarified.
Thermodynamics of Cl– movement
The current mediated by GABAARs (IGABA) can be described by Ohm’s law as a
product of conductance (gGABA; inverse of resistance) and the driving force (DFGABA),
that is, the difference between membrane potential (Vm) and reversal potential
(EGABA):
IGABA = gGABA (Vm – EGABA)
where, gGABA is the GABA-evoked conductance, which depends on the number of
open channels as well as the single-channel conductance. The reversal potential EGABA
is the potential at which no net GABA-mediated current occurs. GABAARs are
permeable to Cl– and HCO3– but the permeability to Cl– is 3 - 5 times higher than that
to HCO3–. Thus, EGABA is more influenced by Cl– than by HCO3
–, and in many
experimental conditions, the influence of HCO3– can be made negligible. In such
cases, EGABA will be equal to the equilibrium potential for Cl– (ECl) as described by
the Nernst equation:
ECl = RT/F ln([Cl–]i/[Cl–]o)
where, R is the gas constant, T is absolute temperature and F is Faraday’s constant. In
physiological conditions, however, EGABA is also influenced by HCO3–, so that
EGABA = (RT/F) ln((PCl[Cl–]i + PHCO3[HCO3–]i)/(PCl[Cl–]o + PHCO3[HCO3
–]o))
where P denotes the relative permeabilities for Cl– and HCO3–, as given by the
subscript. At high [Cl–]i, EGABA is then still relatively close to ECl, but at low [Cl–]i,
significant deviations in positive direction are caused by HCO3– (see e. g. Farrant &
Kaila, 2007).
6
As shown in Figure 2, the relation between ECl and [Cl–]i is logarithmic and suggests
that small changes in Cl– gradient may strongly affect ECl and therefore the driving
force (DFCl = Vm – ECl) that determines the direction of Cl– currents (ICl):
ICl = gCl (Vm – ECl) (1)
where gCl is Cl– conductance. Thus, the effect of ECl on GABAAR-mediated currents
and neuronal excitability is dramatic:
1) When ECl is more negative than Vm, activation of GABAARs will cause
influx of Cl−, membrane hyperpolarization and thereby neuronal inhibition.
GABAAR-mediated inhibition is commonly observed in the mature brain. To maintain
a low ECl, mechanisms to keep [Cl–]i low are required.
Figure 2. Relationship between intracellular chloride concentration [Cl–]i and equilibrium
potential for Cl– (ECl). Small changes in [Cl–]i may lead to profound changes in ECl and in the
effect of GABA action.
2) When ECl is more positive than Vm, GABAAR activation will lead to
outward flux of Cl− ions and depolarization of the membrane. GABA-mediated
depolarization does not always cause excitation. Subthreshold depolarization may
impose a strong inhibitory action, as observed in sensory afferent neurons (Khazipov
et al., 2014; Hammond, 2015). If ECl is more positive than Vm and above threshold for
action potential generation, GABAAR activation will likely, at least temporarily, be
excitatory and thus increase the firing probability. To constantly maintain a high ECl,
as commonly observed in immature neurons, mechanisms for Cl− import may be
required
0 10 20 30 40 50 60 70 80 90 100
-140
-120
-100
-80
-60
-40
-20
0
[Cl-]
i (mM)
EC
l (m
V)
Resting membrane potential (Vm)
ECl
in mature neurons
ECl
in immature neurons
7
3) When ECl is equal or close to Vm, opening of GABAARs may not cause
any significant change in Vm. The open GABAARs, however, may counteract and
prevent depolarization that would otherwise be caused by simultaneous excitatory Na+
influx. Such an effect of the GABA-activated conductance is known as "shunting
inhibition". It is important to note, however, that also during shunting inhibition,
despite that no change in voltage is seen, GABAAR-activation is associated with Cl−
flux that may impose a considerable load on the postsynaptic neuron (Doyon et al.,
2016b), and thus a need for Cl− extrusion mechanisms.
Cation chloride cotransporters (CCCs)
In the CNS, a family of cation chloride cotransporters (CCCs), encoded by the genes
Slc12a 1-9, plays a central role in controlling [Cl–]i. The CCCs are membrane
glycoproteins that mediate ion transport across the plasma membrane (Blaesse et al.,
2009). The family is broadly classified into four categories;
1) Na+-Cl–-cotransporter (NCC)
2) Na+-K+ -Cl–-cotransporters (NKCC1-2)
3) K+-Cl–-cotransporters (KCC1-4)
4) Cation chloride cotransporter 9 (CCC9) and CCC-interacting protein 1
(CIP1).
Regarding neuronal Cl− regulation, NKCC1 and KCC2 are highly important because
they are widely expressed in neurons throughout the CNS.
KCC2: Neurons express four different isoforms of K+-Cl–-cotransporters (KCCs)
KCC1, KCC2, KCC3 and KCC4. KCCs are secondary active transporters which do
not consume energy directly, but rather use the K+ gradient as an energy source to
extrude Cl– (Alvarez-Leefmans & Delpire, 2009). KCC2 is an electroneutral neuron-
specific Cl– transporter responsible for maintaining a low [Cl–]i. In contrast to other
KCCs, which are activated by osmotic changes, KCC2 is also active in isotonic
conditions (Acton et al., 2012). This makes KCC2 the main Cl– extruder that enables
neuronal inhibition mediated by hyperpolarizing influx of Cl– via glycine and GABAA
receptors. KCC2 exists in two splice variants: KCC2a and KCC2b. KCC2a expression
is relatively low but stable throughout the lifespan whereas expression of KCC2b
increases during development (Uvarov et al., 2007). KCC2 is widely expressed in
central neurons with predominant localization in the somato-dendritic compartments.
The compartmentalization of KCC2 often results in local differences in [Cl–] and
EGABA, for instance in soma as compared with dendrites (Raimondo et al., 2012).
8
The secondary and tertiary structures of KCC2 and all other CCC family members are
yet to be resolved. However, the structure predicted on basis of hydrophobicity
suggests that KCC2 has 12 transmembrane domains, intracellularly located N- and C-
termini and short loops connecting the transmembrane domains (Payne et al., 1996;
Gamba, 2005; Hartmann & Nothwang, 2014) (Figure 3). The C- and N-termini
contain several amino acid residues (serine, threonine and tyrosine; Figure 3) that may
be selectively and specifically de/phosphorylated by several phosphatases/kinases
(Kahle et al., 2013). This occurs in many different physiological and
pathophysiological conditions, dynamically affecting KCC2 activity and thereby local
[Cl–]i distribution (for review Kelsch et al., 2001; Kahle et al., 2005; Lee et al., 2007).
The C-terminal of KCC2 also contains an ISO domain which is necessary for KCC2
activity in isotonic conditions (Acton et al., 2012).
Figure 3. Putative structure of the KCC2 protein, with amino acid residues important for
transport activity and membrane stability indicated. Phosphorylation, mutation or deletion of
these amino acid residues result in changes of ion-transport or surface stability. (Reproduced
from Medina et al., 2014, with permission).
KCC2 may form di- and oligomeric complexes in the membrane, but the functional
significance of KCC2 oligomerization remains unclear as experimental evidence on
the oligomerization-dependent transport activity of KCC2 is still sparse and highly
contradictory (Medina et al., 2014). Age-dependent upregulation of KCC2 expression
mediates a developmental switch of the mode of GABAAR signaling in the CNS
9
(Ganguly et al., 2001; Tyzio et al., 2008). Early in development, the relatively low
level of KCC2 function in immature neurons keeps the Cl– gradient inefficient for
driving hyperpolarizing influx of Cl–. Instead, activation of GABAAR then usually
leads to depolarizing efflux of Cl– and an excitatory action of GABA. With
development, upregulation of KCC2 leads to a much lower [Cl–]i, compatible with Cl–
influx and enabling the GABA-evoked inhibition typical for the mature CNS.
Perturbed KCC2 activity may result in altered GABAAR-mediated signaling, as
documented in stress (Hewitt et al., 2009; Bains et al., 2015; MacKenzie & Maguire,
2015) and in pathological conditions, including epilepsy (Kaila & Miles, 2010;
Khirug et al., 2010; Kaila, et al., 2014b; Karlócai et al., 2015), chronic pain (Coull et
al., 2003; De Koninck, 2009; Gagnon et al., 2013), autism (Lemonnier & Ben-Ari,
2010; Tyzio et al., 2014) and spinal cord injury (Boulenguez et al., 2010).
Figure 4. Main types of neuronal Cl– transport. KCC2-mediated Cl– extrusion is driven by the
K+ gradient generated by the Na+-K+-ATPase. Extrusion of Cl– generates an inwardly directed
electrochemical gradient for Cl– resulting in hyperpolarizing currents through Cl– permeable
channels (top). NKCC1-mediated Cl– uptake is driven by the Na+ gradient generated by the
Na+-K+-ATPase. Uptake of Cl– by NKCC1 generates an outwardly directed electrochemical
gradient for Cl– resulting in depolarizing currents through Cl– permeable channels (bottom).
NKCC1: Na+-K+-Cl– cotransporter 1 (NKCC1) is highly expressed in immature
neurons, promoting intracellular Cl– accumulation and thereby depolarizing GABAAR
10
responses (Delpire, 2000). NKCC1 uses the Na+ gradient as energy source to transport
K+ and Cl– into the cell and it mediates electroneutral transport with 1Na+:1K+:2Cl–
stoichiometry (Alvarez-Leefmans & Delpire, 2009). The expression of NKCC1 is
downregulated in the first three weeks of postnatal development (Li et al., 2002). In
mature neurons, the distribution of NKCC1 is poorly studied but recent results
indicate that NKCC1 is highly expressed in the axon initial segment where the action
of GABA may be depolarizing even in mature neurons (Khirug et al., 2008). In
contrast to mature central neurons, primary sensory (Delpire & Austin, 2010) and
olfactory neurons (Kaneko et al., 2004) maintain a high [Cl–]i and exhibit depolarizing
GABA responses as a consequence of a high level of NKCC1. Figure 4 shows the
main types of Cl– transport by KCC2 and NKCC1.
Thermodynamics of KCC2 and NKCC1
KCC2 mediates electroneutral transport of 1K+:1Cl–. This means that the overall
transport of K+ and Cl– neither generates a net current across the membrane nor
depends on the membrane potential. Thus, the driving force (UKCC2) for KCC2-
mediated K+ and Cl– transport solely depends on the chemical potential differences
for K+ and Cl–:
UKCC2 = RT ln([Cl–]i/[ Cl–]o) + RT ln([K+]i/[K+]o)
At equilibrium UKCC2 = 0 and thus:
RT ln([Cl–]i/[ Cl–]o) + RT ln([K+]i/[K+]o) = 0
[Cl–]i/[Cl–]o = [K+]o/[K+]i
[Cl–]i = [Cl–]o[K+]o/[K+]i (2)
If [K+]i is set by the Na+-K+-ATPase or by experimental solutions, then equation (2)
provides the [Cl–]i at KCC2 equilibrium. With the experimental values used in this
study ([Cl–]o = 146.4 mM, [K+]o = 5 mM and [K+]i = 140 mM), [Cl–]i will be 5.2 mM,
and thus, according to the Nernst equation, ECl = –83 mV. This is below the average
Vm, implying that GABAAR activation will usually hyperpolarize the cell.
In the absence of other mechanisms than KCC2 for Cl– transport, steady-state [Cl–]i
(and ECl) can thus be obtained from equation (2). Then, ECl = EK. However, all neurons
likely display at least some gCl, which will drive ECl towards the resting (or prevailing)
potential. This also means that if KCC2 is blocked, [Cl–]i will redistribute passively
and at equilibrium ECl = Vm. With KCC2 present, as we have expressed in paper IV,
steady-state ECl will settle somewhere between EK and resting Vm, depending on the
11
relative contribution of KCC2 and gCl. Papers III and IV of this thesis clarify the
influence of gCl on the Cl– homeostasis.
Since KCC2 functions near thermodynamic equilibrium (Payne, 1997; Payne et al.,
2003), relatively small perturbations in Cl– or K+ concentrations may affect the
transport markedly. Thus, for instance, even a moderate increase in [K+]o, such as
often detected in epileptic conditions (Viitanen et al., 2010), may reverse Cl− transport
by KCC2 to become inwardly directed (Payne, 1997; Thompson & Gähwiler, 1989).
Similarly as KCC2, NKCC1 mediates electroneutral transport. Thus, the equilibrium
for NKCC1 depends on the chemical gradients of Na+, K+ and Cl– and at equilibrium:
[Cl–]i = [Cl–]o ([Na+]o [K+]o / ([Na+]i [K+]i))1/2
However, in contrast to KCC2 and as a consequence of the physiological ion
concentrations, NKCC1 usually operates far from equilibrium and mediates Cl–
transport in inward direction only (Alvarez-Leefmans & Delpire, 2009).
Role of impermeant anions in setting [Cl–]i
Neurons are surrounded by a complex network of extracellular matrix (ECM). The
ECM is mostly composed of chondroitin sulphate proteoglycans (CSPGs) and
hyaluronic acid (Dityatev et al., 2010; Soleman et al., 2013). The CSPGs contain very
many fixed negative charges. Similarly, the cell cytoplasm contains negatively
charged macromolecules, such as nucleic acids and proteins, which cannot pass the
plasma membrane. It has recently been proposed that the negatively charged
macromolecules on the in- and outside of the cell membrane play a critical role in
setting the resting [Cl–]i (Glykys et al., 2014a). This idea, which contrasts with the
view that [Cl–]i is determined by the CCCs (Kaila et al., 2014a; Rivera et al., 1999),
rests on the knowledge that impermeant ions may affect the distribution of permeant
ions via a so called Gibbs-Donnan effect (see e.g. Kutchai, 2004, for a pedagogical
description). In support of their proposal, Glykys et al. (2014a) reported that digestion
of the ECM was associated with a rise in [Cl–]i. The report by Glykys et al. (2014a),
which also stated that CCCs do not determine resting [Cl–]i, has been intensely
debated (Ben-Ari, 2014; Cho, 2014; Delpire & Staley, 2014; Glykys et al., 2014b;
Luhmann et al., 2014; Voipio et al., 2014; Vogt, 2015; Doyon et al., 2016b; Robel &
Sontheimer, 2016). It therefore remains unclear if the ECM does play a critical role
in setting the resting [Cl–]i. This question was addressed in paper II of the present
thesis.
12
Specific aims of the thesis
The overall aim of the present thesis is to clarify the mechanisms involved in the
neuronal chloride homeostasis, which is critically important for the fast neuronal
inhibition in the central nervous system. The more specific aims are:
1. To clarify how to accurately estimate the intracellular Cl– concentration,
[Cl–]i, by electrophysiological methods.
2. To clarify the role of the extracellular matrix (ECM) in setting [Cl–]i.
3. To develop a method for estimating the resting Cl– conductance of the
neuronal membrane.
4. To elucidate the role of passive, conductive Cl– flux for the neuronal [Cl–]i
homeostasis.
5. To establish the theoretical relation between the Cl– equilibrium potential
(ECl), Cl– extrusion capacity and synaptic input.
13
Methodological considerations
In the present thesis, the regulation of neuronal [Cl–]i was investigated using
electrophysiological, biochemical and computational techniques. A brief summary of
the methods is provided below and the detailed experimental procedures are presented
in the methods section of each original publication and manuscript.
Cell and tissue preparation
The present work was made using neurons from the preoptic hypothalamic region of
Sprague-Dawley rats. The main reason for the choice of preparation is that we have a
large amount of available information on the electrophysiological signaling properties
of these neurons. It is known that GABA signaling undergoes a developmental
transition from excitation to inhibition. Since this transition is completed during the
first two weeks of postnatal development (Tyzio et al., 2008), we used 3-5 weeks old
rats to ensure that GABA signaling is inhibitory. Older rats were not used since in
general, neurons form younger rats survive better and are more easily accessed with
the techniques used.
Experiments were mainly performed on neurons from the medial preoptic nucleus
(MPN). These neurons express functional GABAARs and GlyRs (Karlsson et al.,
1997a) and as such, they provide an excellent experimental model for studying [Cl–]i
regulation. One advantage of cells with two types of Cl–-permeable channels is that
we may estimate [Cl–]i by using an agonist to one receptor/channel type while
simultaneously blocking the other type to understand its role for the [Cl–]i
homeostasis.
In this study, two acute in vitro preparations were used: 1) slice preparation 2) acutely
dissociated neurons.
Brain slices, 200-300 µm thick and containing the preoptic area were prepared as
described in detail in the Methods section of paper I-III (see also e. g. Johansson et
al., 1995; Karlsson et al., 2011)) The major advantage of the slice preparation is the
near-physiological conditions, with intact neurites, synaptic connections, surrounding
glial cells and ECM. However, neurons in slice preparation preserve extensive
dendritic branches which makes it impossible to control the distal membrane voltage
by the voltage-clamp technique.
An enzyme-free, mechanical dissociation method was used to dissociate neurons from
brain slices as described previously by Vorobjev (1991) with the modifications
according to Karlsson et al. (1997b). To dissociate neurons, a vibrating glass rod was
applied to the site of the MPN. Dissociated neurons lack the majority of neurites,
14
enabling excellent control of the membrane potential in voltage-clamp conditions.
They also allow rapid application of pharmacological drugs. In addition, this
preparation preserves many functional presynaptic nerve terminals and their
properties can be tested in this preparation. However, since neurites and natural
environment is lost, a comparison with neurons in slice preparations is often
warranted.
Electrophysiological recording
The present work was mainly carried out by using patch-clamp techniques. Patch-
clamp was first introduced by Neher & Sakmann (1976). Since then it has been widely
used in studying ionic transport mediated through ion channels and transporter
proteins. This study was conducted using different patch-clamp recording
configurations, viz conventional whole-cell recording (Hamill et al., 1981),
amphotericin (Rae et al., 1991) or gramicidin (Abe et al., 1994; Ebihara, et al., 1995;
Kyrozis & Reichling, 1995) perforated-patch recording and cell-attached recording
(Hamill et al., 1981; Alcami et al., 2012).
To carry out patch-clamp recordings, a borosilicate-glass pipette with a tip of ~1 µm
dimeter was produced in a standard electrode puller. A patch pipette filled with
pipette-filling solution, usually mimicking the natural intra- or extracellular ionic
composition, and with a resistance of 3.5- 4.5 MΩ was approached to the cell. When
the pipette touched the cell, weak suction was applied to form a tight seal of resistance
usually > 1 GΩ. To achieve an electrical continuity with the interior of the cell, the
membrane was ruptured by applying a pulse of negative pressure. This conventional
whole-cell configuration was used in the experiments to dialyze the cytoplasm of the
cell with intracellular pipette-filling solution. Despite its simplicity, conventional
whole-cell configuration has limitations, which include run-down of currents over
time due to washout of essential cytoplasmic components (Pusch & Neher, 1988). To
avoid this problem, either amphotericin- or gramicidin-perforated patch-clamp
technique was used. Amphotericin forms non-selective monovalent ion pores in the
patch membrane and allows electrical access to the cell interior (Rae et al., 1991). To
achieve an amphotericin-perforated patch, amphotericin was added to the intracellular
solution in the pipette and a GΩ seal between pipette and cell membrane was formed.
Amphotericin pores are permeable to Cl– ions, implying a disturbed [Cl–]i via
Cl– exchange between cytosol and recording pipette. Thus, to study unperturbed
[Cl–]i, the gramicidin-perforated patch technique was used. Since the pores formed by
gramicidin in the cell membrane are impermeable to Cl–, [Cl–]i is not affected by flux
into or out of the recording pipette (Ebihara et al., 1995).
In slice preparations, spontaneous neuronal activity was recorded either in the cell-
attached configuration or with perforated-patch recording. We also stimulated the
15
presynaptic fibers within the MPN and recorded the evoked and spontaneous
postsynaptic responses as described previously by Malinina et al. (2006). The current
recorded in the cell-attached configuration during neuronal action potential generation
is composed of a capacitive component as well as a resistive component. The resistive
component has a time course similar to the transmembrane potential, while the
capacitive component has a time course that corresponds to the derivative of that
potential (Johansson & Århem, 1992).
During all electrophysiological recordings, neurons were continuously perfused with
extracellular solution via a gravity-fed perfusion system. Exchange to solution
containing GABA, glycine and/or other substances was controlled by solenoid valves
via a computer. The majority of electrophysiological studies were performed at room
temperature, 21-23 C. (Exceptions are noted in paper II.)
Electrophysiological measuring of [Cl–]i
[Cl–]i, was obtained from the Cl– equilibrium potential, ECl, as given by the current-
voltage (I-V) relation for the current component carried exclusively by Cl–. First, the
I-V relation for “leak” currents was recorded in the absence of ligands for Cl–
permeable channels. The I-V relation was obtained from a voltage ramp at a rate of
±1.6 V s-1 (Karlsson et al., 2011). To obtain the current carried by Cl–, leak currents
were subtracted from the current measured in the presence of GABA or glycine.
[Cl–]i was estimated from the known concentration of extracellular Cl– ([Cl–]o) and
ECl, as defined by the Nernst equation. Measuring [Cl–]i requires activation of Cl–
permeable channels that, depending on DFCl, may affect [Cl–]i during the
measurement. Thus, to minimize artificial changes, [Cl–]i was always measured at a
holding membrane potential close to the reversal potential (ECl), where Cl– flux is
small. Further, a technique with symmetric ramps in negative and positive direction
was used to avoid artificial [Cl–]i perturbations. That this technique gives negligible
perturbation of [Cl–]i was shown theoretically in Fig. 2F,G of paper I.
Electrophysiological measurement of [Cl–]i provides some clear advantages over
optical Cl– imaging. Electrophysiological techniques are usually called “invasive”
since contact between pipette and cytoplasm is achieved. However, as noted above,
the gramicidin-perforated patch technique enables recordings that do not perturb
[Cl–]i. Further, ECl provides the probably most direct and sensitive method available
for quantifying [Cl–]i. “Non-invasive” optical imaging requires artificial introduction
of fluorescent Cl–-binding sensors into the cell and is far from reliable in estimating
[Cl–]i (Berglund et al., 2011). The main two limitations of Cl– imaging to measure
[Cl–]i are:
16
1) Changes in pH are commonly observed during neuronal excitation and all
available Cl– sensors have a high sensitivity to H+ ions. Therefore, measuring
[Cl–]i highly depends on changes in pH.
2) Commonly used Cl– sensors have a high Kd (~ 90 mM) and low Cl–
sensitivity. In physiological conditions, changes in [Cl–]i are often in a range
of a few mM. This implies that the sensitivity of Cl– sensors in physiological
conditions is limited.
Cl– transporter activity and [Cl–]i homeostasis
The neuronal [Cl–]i homeostasis involves two major mechanisms of Cl– transport: one
being mediated by CCCs and the other one being passive and mediated by the flux of
Cl– via available channels. CCCs mediate electroneutral ion transport and therefore,
an electrophysiological approach to directly monitor the ion flux mediated by CCCs
is not possible. However, the activity of CCCs can be estimated by monitoring
changes in [Cl–]i. To study the [Cl–]i homeostasis, cells were loaded to a high [Cl–]i,
by a combination of membrane depolarization and activation of Cl– channels by either
GABA or glycine. Depolarization generates a driving force that drives Cl– into the
cell. During [Cl–]i loading as well as during recovery, [Cl–]i was estimated as
previously described and plotted against time. The time constant of [Cl–]i recovery
was obtained from a single-exponential fit. To study Cl– transporter-mediated [Cl–]i
changes during recovery, contribution of passive channel-mediated leak was
minimized by keeping the command voltage close to ECl. Pharmacological blockers
were applied to discriminate different transporters involved in the [Cl–]i recovery.
To study the contribution of Cl– leak conductance in [Cl–]i recovery, cells were loaded
to a high [Cl–]i and during the recovery phase, the membrane was voltage clamped
close to the resting membrane potential (in this case -74 mM) and transporter proteins
were blocked. This provided the essential driving force for Cl– leak-mediated [Cl–]i
recovery.
Estimating relative Cl– conductance by a novel method
In paper III, we have developed a novel electrophysiological method for measuring
relative resting Cl– conductance (gCl). We have formulated a simple mathematical
relation which is based on the conductance version of the Goldman-Hodgkin-Katz
equation (Goldman, 1943; Hodgkin & Katz, 1949). We showed that the relative
resting gCl can be obtained from the change in resting membrane potential (ΔErev) and
the change in Cl– equilibrium potential (ΔECl) under conditions where [Cl–]i is altered.
[Cl–]i-dependent changes in Erev and ECl were estimated by using electrophysiological
techniques. This method depends on the simple, and experimentally verified,
assumption that the total membrane conductance does not change before and after Cl–
17
loading. To minimize the effect of other factors, the experiments were performed in
presence of a cocktail of blockers: Tetraethylammonium and tetrodotoxin were used
to block unwanted gating of voltage-dependent K+ and Na+ channels, Cd2+ was used
to block presynaptic-release and VU0255011‐1 was used to block KCC2 activity.
In principle, the method for estimating gCl may be used for all preparations accessible
to common electrophysiological recording techniques. In cases where [Cl–]i cannot
easily be manipulated, [Cl–]o can be changed instead. Then, offset changes in liquid-
junction potentials and electrode potentials must also be taken into account.
Immunoblotting
Whole-cell KCC2 protein from MPN-containing coronal slices was extracted using
RIPA buffer containing a protease inhibitor. Membrane-expressed proteins were
extracted using a plasma membrane protein extraction kit. Following extraction,
proteins in individual samples were measured and separated by sodium dodecyl
sulfate polyacrylamide gel electrophoresis (SDS-PAGE) and transferred from the gel
to a polyvinylidene difluoride (PVDF) membrane. Then, the PVDF membranes were
incubated with the primary antibodies against KCC2, transferrin receptor, calnexin or
β-tubulin. The membranes were subsequently incubated with the appropriate HRP-
conjugated secondary antibody and incubated with western HRP chemiluminescence
substrate. The chemiluminescent signals in the membranes were acquired using an
Odyssey Fc Imaging System and quantified using Image studio version 3.1. Western
blot experiments were repeated at least 8-10 times on independent samples (animals).
For analysis, all signals from the membrane fraction were normalized to transferrin
whereas those from the whole-cell fraction were normalized to β-tubulin or calnexin.
Obtained data were compared using non-parametrical tests.
Computational modeling
In this thesis, computational modeling was used to either complement
electrophysiological data or to address a specific question that is difficult to
understand using electrophysiological experiments only.
In paper I, a computational model of GABA-activated currents was used to clarify the
changes in [Cl–]i that are expected from the Cl– current under voltage-clamp
conditions. The model was based on that made by Karlsson et al. (2011) and the
kinetics of GABA-mediated currents observed by Haage et al. (2005), but here we
omitted the desensitization. Initially, the model parameter values were adopted to the
experimental conditions used by Bianchi & Macdonald (2002), to achieve roughly
similar currents as observed experimentally by those authors. Subsequently, we
18
computed the Cl– current and the changes in [Cl–]i. Further, we used this model to
complement our electrophysiological data obtained from MPN neurons.
In paper III, the computational model described by Karlsson et al. (2011) was used to
study the influence of resting gCl on the [Cl–]i homeostasis. Thus, the model was
modified to account for resting gCl as well as for KCC2-mediated transport. The
KCC2-mediated transport capacity was expressed in terms of a proportionality
constant (gKCC2) that may be seen as an “equivalent conductance” although the
cotransport with K+ makes Cl– transport by KCC2 electroneutral. The constants gKCC2
and gCl were first adjusted to match experimental [Cl–]i changes with KCC2-mediated
or conductive Cl– transport in isolation. Subsequently, the time course of theoretically
expected [Cl–]i recovery at various combinations of gKCC2, gCl and membrane potential
was computed.
In paper IV, to clarify how [Cl–]i depends on Cl– extrusion capacity and synaptic input,
we formulated, in mathematical terms, the relation between steady-state ECl, gKCC2,
total gCl and Vm and illustrated this in graphical form. The basic idea behind the
interpretation in terms of steady synaptic input is that synaptic inhibition will mainly
affect gCl (as for GABA- or glycine-gated channels) whereas synaptic excitation,
which is most often due to non-selective (e. g. glutamate-gated) cation channels, will
be equivalent to a positive change of Vm.
19
Results and discussion
Project 1: Estimating [Cl–]i by electrophysiological methods
To study the Cl– homeostasis, it is crucial that an appropriate method for measuring
Cl– dynamics is selected. The method should be accurate and sufficiently sensitive to
detect small changes in [Cl–]i. Several electrophysiological or imaging techniques are
available to measure [Cl–]i in neurons. Common electrophysiological methods are
based on an estimate of ECl which is used together with the known extracellular Cl–
concentration, [Cl–]o, to calculate [Cl–]i from the Nernst equation. ECl is measured as
the voltage of zero current (reversal potential) under conditions where the current is
carried by Cl– only. In principle, ECl reflects [Cl–]i directly and if ECl can be measured
with mV-precision, [Cl–]i can usually, for physiological levels, be obtained with at
least mM-precision. (As noted above, on the contrary, recently developed, non-
invasive Cl– sensors have a low Cl– sensitivity in the physiological range of [Cl–]i
(Berglund et al., 2011)). When estimating ECl on basis of membrane currents, care
must be taken to separate the current component carried by Cl– from other current
components. In the present work, GABA and glycine were used to induce currents
carried by Cl–, since the studied cells express Cl–-permeable ligand-gated ion channels
(GABAA and glycine receptors) sensitive to these substances. Although these
channels also show some permeability for HCO3–, the contribution of HCO3
– was
excluded by using a HCO3–-free extracellular solution. Further, leak current
components were quantified in the absence of ligands and subtracted from the total
membrane current.
To estimate ECl, the I-V relation of the studied Cl– currents must be established. The
two most common techniques, here called the interpolation and the voltage-ramp
methods, differ with respect to the voltage protocol used. Since the introduction of the
voltage-clamp technique (Hodgkin & Huxley, 1952), the interpolation method has
been the most widely used. For studies of ligand-gated channels, it usually implies
that the ligand is applied repeatedly, each time at a different steady voltage. The I-V
relation for a specific time point after the start of ligand application (or at the time of
peak current) is subsequently obtained by interpolation of the current amplitudes
recorded at each voltage.
In the voltage-ramp method, on the other hand, voltage is increased or decreased
gradually at a steady rate while continuously recording the current in the presence of
a ligand. Recently, by using the voltage ramp method Karlsson et al. (2011) showed
that desensitization of GABAARs is significantly slower than previously reported and
that changes in [Cl–]i largely define the decay of GABA-evoked current. These
findings contradict previous ideas that GABAARs desensitize (i. e. channels close at
prolonged GABA exposure) rapidly and that [Cl–]i does not change much during a
20
typical experiment with activation of GABA- or glycine activated channels. Earlier
conclusions were, however, to a large extent based on analysis with the interpolation
method. For instance, in a previous study, Bianchi & Macdonald (2002) concluded,
on basis of analysis with the interpolation method, that in roughly similar conditions
as in the study by Karlsson et al. (2011), the decay of GABA-evoked current is mainly
due to receptor desensitization and changes in [Cl–]i are negligible. The discrepancy
between conclusions based on the two methods, led us to the hypothesis that the
interpolation and the voltage-ramp methods differ with respect to how correctly
[Cl–]i and gCl are described by the two methods. To clarify which method is the most
correct one and to what degree the two methods agree with theoretical expectations
of [Cl–]i and gCl, we made a direct comparison between the two methods.
To clarify the theoretically expected changes in ECl and gCl, we used a computational
model, based on that described by Karlsson et al. (2011), to compare the GABA-
evoked currents expected with the two types of voltage protocol. For simplicity, we
assumed that the studied channels showed no true desensitization, that is, the channels
stay open in the continued presence of GABA. The model was adopted to the
conditions for GABA-evoked currents as observed by Bianchi & Macdonald (2002).
Most essentially, the model accounted for the changes in [Cl–]i that would be expected
from the Cl– flux through the GABA-activated channels. For simplicity, we assumed
that no other channels or transporters contributed to changes in [Cl–]i.
The numerically computed currents at different steady holding voltages showed a
substantial decay during the activation of the GABA-mediated conductance. The I-V
relations constructed from current amplitude at four different time points showed a
roughly constant interpolated reversal potential, which if taken to reflect ECl suggests
that there is no change in [Cl–]i. Further, the slope of the I-V relation decreased with
time and, if taken to reflect gCl, suggests a substantial desensitization. However, since
the model did not include any channel desensitization, the current decay must have
another cause. One advantage with the model, in comparison with wet experiments,
is that [Cl–]i can be obtained directly from the computations. Here, the model clearly
demonstrated that [Cl–]i changed dramatically during the currents recorded at steady
voltages. Thus, in essence, the computations show that the I-V relation obtained by
the interpolation method gives a reversal potential that does not correctly reflect ECl
and [Cl–]i and a slope that does not correctly reflect gCl, contrary to common
assumptions, such as made by Bianchi & Macdonald (2002). On the other hand,
computations of the currents and [Cl–]i during voltage ramps showed that I-V relations
obtained from these ramps correctly reflected the changes in [Cl–]i and also correctly
reflected the constant gCl of the model. The model also displayed that although the
altered Cl– flux induced by the voltage ramps to some degree changes [Cl−]i, the use
of symmetrical ramps in negative and positive direction minimizes such changes to
non-significant levels.
21
Wet experiments with dissociated MPN neurons confirmed the differences between
the two protocols to estimate [Cl–]i and gCl. Since the biological GABAARs show some
degree of true desensitization, the slope of the I-V curves from the living neurons
decay, although slowly, with time in the presence of GABA.
The difference between the two methods for constructing I-V plots depend on the
interpolation used in the non-accurate method. As explained in Fig. 5 of paper I, this
implies that artificial I-V relations (colored in the figure) are obtained whereas the
true I-V relations (black and gray in the figure) remain undetected.
The principle that flux through ion channels may be associated with changes in ion
concentrations apply to all type of channels and need to be considered in every
experiment involving currents through ion channels. Our findings suggest that the
voltage-ramp method is to be preferred when I-V relations reflecting [Cl–]i and gCl are
needed. This also means that a number of earlier studies may need reinterpretation.
The study by Bianchi & Macdonald (2002) provides a particularly clear example.
However, the interpolation method has been used even in the first papers where the
voltage-clamp technique was introduced (Hodgkin & Huxley, 1952). This should not
be taken to imply that all such studies are mistaken. In many cases, for instance most
likely for the fast Na+ channels studied by Hodgkin & Huxley (1952), the magnitude
and time course of ion flux are so limited with respect to the volumes affected that
significant changes in ion concentrations may not take place. In case of channels with
slow kinetics, such as GABAA- and glycine receptors and several types of voltage-
gated K+ channels, however, interpretation of the results from the interpolation
method should be made with caution.
22
Project 2: Role of Cl– transporters and extracellular matrix in [Cl–]i
homeostasis
The effect of GABAAR-meditated signaling depends critically on the transmembrane
Cl− electrochemical gradient. It has been widely accepted that cation-chloride
cotransporters (CCCs) play a primary role in setting [Cl–]i and the transmembrane
Cl− electrochemical gradient. Recently, Glykys et al. (2014a) used a genetically
expressed Cl– sensor to measure the resting [Cl–]i in young hippocampal neurons.
Surprisingly, the authors concluded that CCCs are not involved in setting resting
[Cl–]i. Furthermore, they observed an increased [Cl–]i upon digesting the negatively
charged proteoglycans in the extracellular matrix (ECM). Thus, the authors claimed
that [Cl–] is not actively maintained by CCCs, but rather passively distributed
according to a Gibbs-Donnan equilibrium under the influence of fixed local anionic
charges (Glykys et al., 2014a). The mechanism proposed by Glykys et al. (2014a) has
been intensely debated (Ben-Ari, 2014; Cho, 2014; Delpire & Staley, 2014; Glykys
et al., 2014b; Luhmann et al., 2014; Voipio et al., 2014; Silayeva et al., 2015; Vogt,
2015; Doyon et al., 2016b; Robel & Sontheimer, 2016).
Paper II of the present thesis is an attempt to at least partly resolve the debated role of
the ECM and of CCCs for [Cl–]i and synaptic transmission, using electrophysiological
measurements in a slice preparation containing MPN neurons. [Cl–]i, was estimated
on the basis of gramicidin-perforated recordings and I-V relations constructed from
voltage ramps as described in paper I. First, we quantified resting [Cl–]i, which was
significantly lower than expected from a thermodynamic equilibrium (or passive
distribution). This clearly contradicts the findings of Glykys et al. (2014a) while
indicating (likely indirectly active) Cl– extrusion involved in setting [Cl–]i. Another
controversial finding of Glykys et al. (2014a) was that inhibiting KCC2 or NKCC1
activity had no effect on ECl, directly contradicting the previously assumed role of
CCCs for [Cl–]i (Rivera et al., 1999; Kaila et al., 2014a) and also contradicting their
own earlier findings (Dzhala & Staley, 2003; Dzhala et al., 2005, 2008; Glykys et al.,
2009). However, when we, in the present work, blocked KCC2 activity by a KCC2-
specific blocker, [Cl–]i increased significantly. These results clearly show that [Cl–]i
is maintained below thermodynamic equilibrium by the activity of KCC2.
As noted above, Glykys et al. (2014a) observed an increased [Cl–]i upon digesting the
negatively charged proteoglycans (chondroitin sulfate) in the ECM. Surprisingly, in
our experimental conditions too, degradation of the ECM with chondroitinase
increased basal [Cl–]i. Recently, Delpire & Staley (2014), in support of the findings
by Glykys et al. (2014a), proposed that digestion of local impermeant anionic charges
increases local [Cl–]o (thus differing from [Cl–]o in the bulk solution) thereby changing
the driving force for Cl– (but see Kaila et al., 2014a). The analysis in the present work,
showed that the [Cl–]o contributing to the driving force for GABA-evoked currents,
23
was not affected by ECM degradation and was, when Cl– leak was minimized, not
significantly different from bulk [Cl–]o. This contradicts the idea that digestion of local
impermeant anionic charges affects the local [Cl–]o.
Our results thus showed that although the ECM affects [Cl–]i in MPN neurons, this is
not likely via effects of the macromolecular anionic charges. Since our results also
demonstrated that [Cl–]i is dependent on KCC2 activity, we hypothesized that the
action of ECM digestion may be mediated by effects on KCC2. Such effects would
be consistent with the dynamic control of KCC2 expression by several factors, e.g.
neuronal activity (Rivera et al., 2004; Khirug et al., 2010; Puskarjov et al., 2012),
changes in cell volume (Kahle et al., 2005; Friedel et al., 2015; Jentsch, 2016),
neurotrophic factors (Rivera et al., 2004; Boulenguez et al., 2010), interaction with
other molecules (Gauvain et al., 2011; Ivakine et al., 2013; Mahadevan et al., 2014)
and [Cl–]i (Piala et al., 2014). We tested our hypothesis by studying KCC2 activity as
reflected by the recovery after loading to a high [Cl–]i. (We here used the voltage-
ramp method analyzed in paper I.) The [Cl–]i recovery showed an exponential time
course and was clearly dependent on KCC2. The slowing of [Cl–]i recovery upon
digesting the ECM thus suggests that KCC2 is affected.
Alterations in KCC2 protein level have been associated with several physiological
and pathological conditions (Kahle et al., 2013). Therefore, we asked whether the
suggested effect of ECM digestion on KCC2 function was due to an altered KCC2
protein level. KCC2 protein is present in monomeric, dimeric and oligomeric forms
(Blaesse et al., 2006; Watanabe et al., 2009), but the importance of monomer/oligomer
KCC2 remains debatable (Jaenisch et al., 2010; Medina et al., 2014; Leonzino et al.,
2016). We found that ECM digestion reduced the amount of KCC2 monomers, in
whole-cell as well as plasma membrane fractions, but did not affect KCC2 dimers.
The parallell reduction of KCC2 monomers and Cl– extrusion capacity, suggests that
monomers are likely to be functional for Cl– transport.
We also investigated the mechanism underlying the KCC2 downregulation. KCC2
can be downregulated by the Ca2+-dependent protease calpain (Puskarjov et al., 2012)
and via an NMDA-receptor-dependent pathway (Lee et al., 2011). In our samples,
blocking NMDA receptors did not inhibit the ChABC-dependent downregulation of
KCC2. At the same time, in presence of the calpain-inhibitor calpeptin (Puskarjov et
al., 2012) or high-threshold Ca2+-channel blocker Cd2+ (Sundgren-Andersson &
Johansson, 1998), ChABC failed to reduce the KCC2 level, suggesting that ECM
removal triggers influx of Ca2+ that mediates calpain-dependent cleavage of KCC2.
Potentially, different types of Ca2+ channels could mediate Ca2+ entry (Takahashi &
Momiyama, 1993). Previously, Kochlamazashvili et al. (2010) reported that
enzymatic removal of another component of ECM, hyaluronic acid, reduces L-type
voltage-dependent Ca2+ currents and had profound impact on long-term potentiation.
24
Our western blot data in paper II, however, suggests that Ca2+ influx through N-type
Ca2+ channels contribute to the KCC2 downregulation upon ECM degradation. This
is consistent with the idea that digestion of ECM leads to activation/potentiation of
N-type Ca2+ channels and thereby downregulation of KCC2. However, further
experiments are warranted to unravel the mechanism behind the ECM-dependent
modulation of N-type Ca2+ channels.
Recently, Doyon et al. (2016a) showed by computer simulations that mild alteration
in KCC2 activity may cause incorrect neuronal coding via altered GABAAR-mediated
transmission. In paper II, we tested directly and experimentally the hypothesis that
ChABC-dependent downregulation of KCC2 affects the efficacy of GABAAR-
mediated transmission, in the MPN-containing slice preparation. The preparation is
suitable for studying inhibition, since even in the absence of excitatory glutamatergic
inputs, many MPN neurons are spontaneously active. Thus, presynaptic stimulation
readily induce inhibition seen as a clear reduction of postsynaptic impulse frequency.
Since our results, at low stimulus frequency, showed a clear inhibition also in ChABC-
treated brain slices, the effect of ECM digestion on KCC2, [Cl–]i and ECl apparently
was not sufficient to prevent the inhibitory action of GABA, although it may have
been mediated by shunting rather than hyperpolarization (cf Khazipov et al., 2014).
Intense neuronal activity may, however, accentuate accumulation of internal Cl–
(Staley et al., 1995). In agreement, we found that high-frequency presynaptic
stimulation was followed by significantly reduced GABAAR-mediated inhibition or
even by excitation in ChABC-treated cells, but not in control cells. Thus, intense
neuronal activity after ECM digestion may change a dominant inhibitory GABA
action to excitatory. In summary, paper II highlights a critical role of the ECM for
GABAAR-mediated signaling. Although digestion of the ECM increases [Cl–]i, the
mechanism is not compatible with that proposed by Glykys et al. (2014a). Rather,
digestion of the ECM decreases the expression and function of KCC2, consequently
causing an increase in resting [Cl–]i as well as an impaired capacity to handle a high
Cl– load.
The ECM has an important role in development (Bonnans et al., 2014), plasticity
(Kerrisk et al., 2014) and in the pathogenesis of injuries and disease (Fawcett, 2015).
Degradation of the ECM (Lendvai et al., 2000; Stern et al., 2001; Trachtenberg &
Stryker, 2001) and reduction of neuronal inhibition (Harauzov et al., 2010) is critical
for experience-dependent plasticity. Thus, our findings may provide the underlying
mechanism of experience-dependent changes in neuronal excitability. These results
also offer novel insights into understanding pathological conditions, such as epilepsy,
spinal cord injury and chronic pain, where the ECM may be degraded (Wilczynski et
al., 2008; Soleman et al., 2013) and the effect on [Cl–]i may result in increased
neuronal activity (Coull et al., 2003; Coull et al., 2005; Boulenguez et al., 2010;
25
Nardou et al., 2011). Further experiments are needed to differentiate the role of
different ECM components in physiological and pathological conditions.
26
Project 3: Influence of Cl– leak conductance on [Cl–]i homeostasis
According to the predominant view, the resting neuronal membrane shows some
conductance for K+, Na+ and Cl– ions (Goldman, 1943; Hodgkin & Katz, 1949;
Forsythe & Redman, 1988). The resting leak (or background) conductance is
important for setting the resting membrane potential as well as for the control of
neuronal excitability, and ionic homeostasis (Hille, 2001). Although it has long been
known that the neuronal membrane possesses some resting Cl– conductance
(Goldman, 1943; Hodgkin & Katz, 1949; Forsythe & Redman, 1988), data on gCl in
central neurons is extremely scarce. First, the quantity of resting gCl is not well known.
Secondly, in spite of a number of characterized Cl– channel types (Jentsch et al.,
2002), the molecular identity of Cl– leak channels is unknown. Recently, Rinke et al.
(2010) proposed that ClC-2, a voltage-dependent Cl– channel, may mediate a major
part of the leak conductance. The single-channel conductance of ClC-2 channels is
~2-3 pS and the presence of these channels influences [Cl–]i in hippocampal neurons.
However, the expression of ClC-2 is highly restricted to specific neuronal types
(Smith et al., 1995) and even restricted to specific neuronal compartments (Földy et
al., 2010). On the other hand, in central neurons, GABAARs are the main mediators
of Cl– conductance and they are widely expressed in the brain. It has been known that
extrasynaptic GABAARs are non-desensitizing, high-affinity receptors (Belelli &
Lambert, 2005; Kullmann et al., 2005) that may mediate a large leak Cl– conductance
(single-channel conductance ~30 pS) (Wagner, 2005). In paper III, an attempt was
made to clarify the molecular identity of Cl– leak channels in MPN neurons. Further,
we studied the influence of Cl– leak conductances on the [Cl–]i homeostasis. We have
also developed a novel method to estimate the relative Cl– leak conductance and used
it to obtain as estimate of resting gCl in MPN neurons.
It has been proposed that inwardly rectifying ClC-2 channels control [Cl–]i by acting
as one-way Cl– exit valves or Cl– efflux pathways (Staley, 1994; Földy et al., 2010;
Rinke et al., 2010; Smart, 2010). Contrary to that, Ratté & Prescott (2011) claim that
ClC-2 cannot acts as an efflux pathway because of its imperfect inward rectification.
Rather, ClC-2s act as Cl– leak channels. To clarify the role of Cl– leak (or passive)
conductances, their influence must be separated from that of transporters involved in
[Cl–]i regulation. Therefore, we first studied [Cl–]i recovery as described previously
(paper II), in the presence of a KCC2- or NKCC1-blocker. The KCC2 blocker
significantly slowed the [Cl–]i recovery, whereas the NKCC1 blocker did not affect
the time course of [Cl–]i recovery. Further, we did not observe ClC-2 mediated
currents in the MPN neurons. These results indicate that [Cl–]i recovery after a high
load is mainly mediated by KCC2 while NKCC1 and ClC-2 are not involved. In paper
III, we also showed that even with KCC2 blocked, [Cl–]i recovers from a high Cl– load
if the voltage is kept near the resting potential, but not at a depolarized level. These
results clearly demonstrate that Cl– extrusion depends on voltage as expected for Cl–
27
leak channels, where voltage contribute to the driving force for Cl– (cf equation 1).
The level of [Cl–]i will, in the absence of transporter proteins, be dictated by the
voltage, with steady ECl settling at the membrane potential.
GABAARs are widely expressed in the CNS where they mediate a Cl– conductance in
several different conditions. Spontaneous GABA release and tonic activation of
GABAARs may contribute to a more or less steady Cl– conductance (Farrant &
Nusser, 2005). We therefore tested whether GABAARs contribute to the conductance
underlying the passive [Cl–]i extrusion. However, neither a GlyR blocker nor a
competitive GABAAR antagonist affected conductive [Cl–]i recovery. This indicates
that [Cl–]i recovery does not depend on activation by glycine or GABA of their
respective receptor types. However, the open-channel GABAAR blocker picrotoxin
reduced conductive [Cl–]i recovery. Our interpretation is that spontaneously open
GABAARs, such as shown by Birnir et al. (2000) and Wlodarczyk et al. (2013), may
contribute to the gCl important for conductive [Cl–]i recovery. It is known that a low
concentration of ambient GABA activates tonic GABAARs which are primarily
expressed in extrasynaptic sites (Semyanov et al., 2003) and that δ-subunit containing
GABAARs are commonly expressed at such sites (Gunn et al., 2015). We here showed
that pharmacological activation of δ-subunit containing GABAARs dramatically
potentiated the conductive [Cl–]i recovery. With respect to the role of increased [Cl–]i
for epileptic conditions (Khalilov et al., 2003), this may be taken to support the idea
that enhancing tonic inhibition may help in preventing epilepsy. In addition, there is
a number of neurological conditions where perturbed signaling by δ-subunit
containing GABAARs has been reported, such as e.g. mood disorders (Maguire et al.,
2005; Maguire & Mody, 2008; Sequeira et al., 2009), schizophrenia (Maldonado-
Avilés et al., 2009) and fragile X syndrome (Curia et al., 2009) for which our findings
may be helpful in better understanding the etiology of disease.
Neurosteroids are endogenous substances shown to have anti-seizure effects and may
be important in pathological conditions like stress and epilepsy. A high concentration
(20 nM - 100 nM) of the endogenous GABAAR-active neurosteroid allopregnanolone
has been detected in the brain (Purdy et al., 1991; Mareš et al., 2006; Biagini et al.,
2010). Therefore, we studied whether allopregnanolone-mediated potentiation of
synaptic GABAARs affects the [Cl–]i recovery. Our results show that spontaneous
GABA release does not contribute to conductive [Cl–]i recovery in basal conditions.
However, allopregnanolone enhanced the speed of recovery. Since the effect was
observed already at low steroid concentration shown to affect GABAARs activated by
GABA and with impulse generation blocked, this was interpreted as due to enhanced
effects of spontaneously released GABA (cf Haage & Johansson, 1999). At higher
concentration, known to directly activate GABAARs in MPN neurons (Haage &
Johansson, 1999), allopregnanolone had a dramatic effect on conductive [Cl–]i
28
recovery. Thus our results indicate that if Vm is sufficiently hyperpolarized, then the
neurosteroid has the capacity to strongly enhance [Cl–]i recovery.
In this project we developed a novel, but simple, method for estimating the resting
gCl. Such a method is needed since previous attempts to estimate gCl were associated
with considerable problems and depended on many assumptions (cf Forsythe &
Redman, 1988). We derived a simple mathematical expression where the relative gCl
is obtained from the experimentally accessible shift in reversal potential of total
current (corresponding to the resting potential) relative to the shift in ECl under
conditions where [Cl–]i is altered. The method depends on the assumption that the
total membrane conductance does not change with Cl– loading, a condition that was
experimentally verified. The method should be relatively easy to apply to many other
preparations. An attractive alternative to changing [Cl–]i by Cl– loading, as done here,
may be to simply alter [Cl–]o. If that is done, care has to be taken to account for
changes in liquid-junction and electrode potentials that accompany changes in [Cl–]o.
With this method, we showed that in MPN neurons, gCl accounts for ~ 6 % of the total
resting conductance. Here the measured resting gCl represents the relative Cl– leak
conductance in the cell body of the MPN neuron. However, it is possible that the Cl–
leak conductance is compartment specific, so that dendrites or neurons with intact
dendrites have different relative Cl– leak conductance. The majority of the Cl– leak
conductance was blocked by picrotoxin, an open channel blocker of GABAARs,
suggesting that GABAARs account for a major fraction of resting gCl. Alterations in
synaptic and extrasynaptic GABAAR subunits and expression have been reported in
many neurological disorders, such as epilepsy (Stell et al., 2003), chronic pain (Iura
et al., 2016), autism (Fernandez et al., 2007; Braudeau et al., 2011), stress (Gauthier
& Nuss, 2015; for excellent review, see Hines et al., 2012). Such alterations should
be associated with altered Cl– leak conductance. Therefore, our method likely paves
the way for new approaches in understanding the role of an altered Cl– leak
conductance and thereby neuronal excitability in physiological and pathological
conditions.
Our electrophysiological experimental results clearly indicate that MPN neurons
express a resting gCl that influences the recovery of [Cl–]i. To complement the
experimental results, we used a computational model with parameters matching the
experimental values. The reason for this study was to clarify the role of conductive
Cl– flux in [Cl–]i homeostasis. It was clear that at negative potentials, conductive Cl–
flux may account for a substantial [Cl–]i recovery, with a time course roughly similar
to that of KCC2 dependent recovery. Interestingly, our simulations showed that at a
negative resting potential, the computed [Cl–]i recovery with gCl as well as KCC2-
mediated transport was significantly quicker than with KCC2 alone. Taken together,
our findings offer new insights into understanding [Cl–]i homeostasis and normal
inhibition via the control of the Cl– leak conductance.
29
Dissociated MPN neurons had a roughly exponential Cl– recovery with a time
constant ~500 s. The obtained time constant was dramatically slower than the 82 s
observed in slice preparations (paper II) and the few seconds reported in some earlier
studies (Staley & Proctor, 1999; Wagner et al., 2001). The difference is likely, at least
partly, due to recording techniques, since previous measurement of [Cl–]i was
performed either with sharp-electrodes or by whole-cell patch clamp which dialyze
the cell and cause ionic equilibration with the patch pipette solution. As shown by
Pusch & Neher (1988), the latter equilibration may occur within a few seconds. Thus,
the quicker [Cl–]i recovery in studies with sharp-electrodes or by whole-cell patch
clamp may be artefactual. The different time course seen in dissociated cells as
compared with slice preparations may possibly be attributed to either difference in
surface-to-volume ratio in these preparations or absence of ECM in the former
preparations. As a consequence of greater number of remaining neurites, the surface-
to-volume ratio should be higher for neurons in slice preparations, and it seems
possible that they may express more KCC2 than dissociated neurons. In slice
preparations, neurons are surrounded by the ECM, whereas dissociated neurons lack
the integrity of the ECM which is crucial for expression of KCC2 (paper II). It seems
possible that dissociation of individual neurons from slices may damage the ECM and
downregulate KCC2 which may lead to slower [Cl–]i recovery.
30
Project 4: Clarifying the role of KCC2 under conditions with different
inhibitory or excitatory conductances
Neurons constantly receive inhibitory and excitatory signals that work by altering the
ion conductance of the membrane. The efficiency of GABAAR-mediated inhibition
relies heavily on ECl which is dependent on the clearance of Cl– from the intracellular
cytosol by KCC2 (Doyon et al., 2016b). There is a large body of evidence showing
that, in pathological conditions, downregulation of KCC2 activity leads to altered
[Cl–]i homeostasis (Price et al., 2005). Recently, Doyon et al. (2016a) emphasized that
the effects on [Cl–]i by even small changes in KCC2 activity may have dramatic
consequences for neuronal coding. As previously described (paper III), the membrane
Cl– conductance, gCl, can also profoundly influence the [Cl–]i homeostasis. To
understand the control of [Cl–]i, it is important not only to separately clarify the
transport capacity by KCC2 and the influence of gCl, but also how these factors
interact to determine ECl and [Cl–]i. Since the effect of gCl (but not that of KCC2)
depends on the membrane potential, Vm, also this has to be considered as a
determinant of [Cl–]i. In paper IV, we formulated the relation between the above
factors in mathematical terms, to enable a graphical description and better
understanding of their influence on ECl. We thus showed that in a manner that strongly
depends on gCl, ECl will vary between the equilibrium potential for K+ ions, EK, and
Vm (The dependence on EK is due to the co-transport of Cl– with K+ by KCC2). Our
finding that the influence of the transport capacity by KCC2 (expressed as gKCC2) is
reduced with increased gCl, is in stark contrast with the recent claim by Doyon et al.
(2016b) that ECl is sensitive to changes in KCC2 activity only when gCl is large. Doyon
et al. (2016b) used this idea to explain the controversial findings of Glykys et al.
(2014a) who did not observe changes in the resting [Cl–]i upon blocking KCC2.
Doyon et al. (2016b) proposed that the findings of Glykys et al. (2014a) could be
explained by their use of a slice preparation that lacked strong inhibitory synaptic
activity. They concluded that “Testing under low Cl– load conditions will, therefore,
lead to gross underestimation of the contribution of KCC2 and overestimation of the
contribution of the Donnan effect” (Doyon et al., 2016b). However, the relation
between gCl and transport capacity was not correctly formulated by Doyon et al.
(2016b). As we showed in paper IV, at low steady (inhibitory or resting) gCl, [Cl–]i
will strongly depend on KCC2 activity, whereas at high steady gCl, [Cl–]i will depend
more on the prevailing membrane potential. In contrast, a lack of excitatory synaptic
input, which affects [Cl–]i mainly via Vm, will reduce the dependence of [Cl–]i on
KCC2 and could in principle contribute to the controversial findings of Glykys et al.
(2014a).
31
Overall Summary
In the first project (paper I), we compared the most common methods to study ion
channel properties and the associated interpolation and voltage-ramp methods for
constructing I-V relations. The two methods clearly generate different results: the
popular interpolation method may fail to detect conductance and ion concentration
changes during prolonged channel activation, whereas the voltage-ramp method
accurately detects such changes.
In the second project (paper II), we clarified the role of the ECM for resting [Cl–]i and
Cl– transport capacity. Our results showed that digestion of the ECM increases [Cl–]i.
In parallel, digestion of the ECM decreases the expression and function of KCC2, thus
explaining the increase in resting [Cl–]i. Further, ECM degradation together with
intense neuronal activity may change the effect of GABA-mediated signaling from
inhibitory to excitatory. We also clarified severeal steps in the ECM-dependent
signaling pathway that leads to the downregulation of KCC2.
In the third project (paper III), we clarified the influence of the Cl– leak conductance
on [Cl–]i homeostasis in MPN neurons. We first developed a novel method to estimate
the relative Cl– leak conductance and obtained a measure of about 6 % in MPN
neurons. We also showed that, at resting potential, the Cl– leak conductance
contributes significantly, and in the same order of magnitude as KCC2, to the recovery
from a raised [Cl–]i. We identified spontaneously open GABAARs as the major
molecular contributors to resting Cl– leak conductance and conductive [Cl–]i recovery.
We also showed that an endogenous neurosteroid as well as a synthetic GABA-active
substance may enhance conductive [Cl–]i recovery.
In the fourth project (paper IV), we formulated the mathematical relationship between
ECl, gCl, Vm and KCC2 transport activity at steady state. We showed that [Cl–]i strongly
depends on KCC2 transport capacity when gCl is low. We also showed that, in the
absence of other transporters than KCC2, ECl will settle between Vm and EK,
depending on the relative magnitude of gCl and KCC2 transport capacity.
32
Acknowledgements
First and foremost, I would like to express my sincere thanks to my supervisor Prof.
Staffan Johansson for scientific and personal mentorship. You have been an inspiring
teacher and a scientifically- rigorous mentor. I remain indebted to you for all that I
learnt in the lab under your constant guidance.
I also would like to thank my co-supervisor Dr. Micheal Druzin for introducing me to
patch-clamp. I can’t thank you enough for your scientific guidance, constructive
comments and suggestions.
I also owe many thanks to past and present members of the lab especially Evgenya,
Tatiana, Erii, Olga and Nazanin.
Thank you Anita Dreyer-Perkiomaki for the timely administrative help.
I also thank Paul Kingham and Mallappa for your help and advice.
I would also like to thank Vahid, Cecilia, Stylianous, Paolo and all colleagues at IMB
for enriching the working atmosphere.
Edward, Sebastian and Vaishnavi- I owe you many thanks for your help, support and
friendship.
Joydeep, Prashant, Shrikant, Pratibha, Dilip, Anjana, Amol, Sonali, Chinmay,
Chaitanya, Dharmesh, Edvin, Brijesh and Manoj- you all have been amazing friends.
Thanks for making my stay in Umeå memorable.
I would also like to thank Abhilasha and my family for your unconditional love,
support and patience.
33
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