|
|
||||||||
Department of Physiology, University of Münster, Germany
1Correspondence: Department of Physiology, University of Münster, Robert-Koch Str. 27a, D-48149 Münster, Germany. E-mail: oberlei{at}uni-muenster.de
| ABSTRACT |
|---|
|
|
|---|
Key Words: nuclear hourglass technique Ca2+ stores nuclear envelope atomic force microscopy
| INTRODUCTION |
|---|
|
|
|---|
Determination of NE electrical conductance, which, in a simplified
view, corresponds to passive ion transport across the NE, has been
confounded by the lack of an appropriate technical approach. The
nuclear patch clamp technique is restricted to preparations with more
or less electrically closed NPCs, whereas microelectrode techniques are
of some use in small somatic nuclei (9)
but fail to
resolve the very low input resistance of the large oocyte nuclei
(reviewed in ref 10
). We recently developed the nuclear
hourglass technique (NHT) (11)
to address this problem and
to measure the NE electrical conductance of Xenopus
laevis oocyte nuclei. The NHT allows the measurement of the
highly conductive NE in an isolated nucleus with great precision.
Several groups, including ours, used the patch clamp technique for
transport studies indicating the existence of ion channels in the NE
directly or indirectly associated with NPCs (12
13
14
15
16
17)
. A
conclusion drawn from these studies was that during patch clamp
experiments most, if not all, of the NPCs are in a closed state
(18)
. The presence of ATP is necessary to maintain the
channels in an open state, thus increasing nuclear ionic permeability
(18)
. Furthermore, Ca2+ and ATP are
directly involved in the modulation of NE passive ionic permeability
(19)
. However, as pointed out by Bustamante and
co-workers, the presence of macromolecule transport through the NPC
central channel also determines (directly or indirectly) single NPC
ionic conductance by promoting transient channel plugging during
macromolecule translocation (20)
.
In contrast to patch clamp experiments, the NHT examines a wide area of
the NE and thus provides information on mean NPC electrical properties.
This approach has the disadvantage that a single NPC event cannot be
detected. However, the NHT offers also an advantage over nuclear patch
clamping that could be crucial for evaluation of the physiological
relevance of the electrical NE conductance: NHT analyses NE conductance
with minimal nuclear manipulations whereas patch clamping of the
double-layered NE (including the Ca2+ stores)
turned out to be invasive (21)
. Using NHT, we recorded
large NE electrical conductances indicating that NPCs are usually
permeable for inorganic ions. (15)
. These recent
observations confirm early microelectrode experiments by Loewenstein
and co-workers indicating that the extremely low electrical resistance
of the NE barrier was due to electrically open NPCs (22
, 23)
.
In a previous study using the NHT we realized that neither block of
macromolecule transport through the NPC central channel nor stimulation
of this pathway affected NE electrical conductance (11)
.
We concluded that separate pathways must exist, one for macromolecules
and another one for inorganic ions. In the present study, we tested
whether Ca2+ and ATP, well-known modulators for
both macromolecule and ion transport, change the conductive properties
of the NE.
| MATERIALS AND METHODS |
|---|
|
|
|---|
Nuclear hourglass technique
The technical aspects of the method and its application in
isolated cell nuclei have been described in detail (11)
.
In short, the method uses a tapered glass tube that narrows in the
middle to two-thirds the diameter of the nucleus. A current of up to 1
mA is injected via two Ag/AgCl electrodes through either end of the
glass tube. The voltage drops across the cell nucleus are measured with
two conventional microelectrodes. The tips of these microelectrodes are
placed near the narrow part of the capillary opposite each other to
measure the electrical resistance of the fluid column between them.
Since current and voltage are simultaneously measured, the resistance
can be calculated online and monitored during the measurements
(Fig. 1
). The nucleus is sucked into the narrow part of the capillary by gentle
fluid movement. Thus, the current flows through the nucleus. The
resulting rise in total electrical resistance indicates the specific
electrical resistance of the cell nucleus.
|
Evaluation of the leak resistance between glass wall and nucleus
(RShunt) was published elsewhere
(11)
. The maximum estimate for the error introduced by
shunt leakage was less than 6%. Thus, we made no attempt to make
corrections for RShunt.
Preparation of nuclear envelopes
After placing the oocytes in NIM, nuclei were manually isolated
by piercing the oocyte with two pincers. Individual intact nuclei were
picked up with a Pasteur pipette and transferred to a glass coverslip
placed under a stereo microscope. Then the chromatin was carefully
removed using sharp needles and the nuclear envelope was spread on
poly-L-lysine coated glass, with the nucleoplasmic side facing
downward. Finally, the specimen were washed with deionized water and
dried.
Atomic force microscopy (AFM)
Application of AFM to nuclear envelopes has been described in
detail previously (21)
. We used a MultimodeTM (with a
NanoScope IIIa controller; Digital Instruments, Santa Barbara, CA)
equipped with an optical microscope, a videocamera, and a monitor to
visualize the NE and the AFM tip on the AFM head stage. We used
standard V-shaped 200 µm long silizium nitride cantilevers with
spring constants of 0.06 N/m and pyramidal tips with an estimated tip
diameter of 10 nm (Digital Instruments). The images were recorded with
512 lines per screen at constant force (height mode) in contact mode
with a scan rate of 3 to 10 Hz. The forces applied during the scanning
procedure were minimized by retracting the AFM-tip until it lost
contact with the sample surface and reengaging the tip at a set point
(i.e., force value) minimally above the lift-off value. We could
usually obtain scanning forces below 3 nN with this approach.
Experiments were performed using a so-called fluid cell. Although the
AFM tip physically interacts with the nuclear envelope, we usually were
able to perform multiple scans without damaging the preparation.
Scanning at low forces (3 nN or less) left no visible marks in the
preparation.
Statistics
Data are given either as individual paired measurements or are
shown as mean values ± SE in % of the corresponding
control values (n=number of nuclei). Each experimental group
was compared with its own control. Significance of differences were
tested by the paired Students t test. An asterisk
indicates a significant difference of P < 0.05 or
less.
| RESULTS |
|---|
|
|
|---|
Figure 1
shows the NHT. As indicated in the schematic microphotographs,
the isolated cell nucleus can be positioned in the tapered part of the
capillary (Fig. 1A
) or displaced into the upper or lower
wide part of the glass tube (Fig. 1B
). Correspondingly,
electrical resistance measured across the tapered part of the capillary
changes. From the changes in electrical resistance, the nuclear
envelope electrical resistance (NEER) can be calculated as outlined
above (see Materials and Methods) and described in detail previously
(11)
.
In a first series of experiments, we measured NEER in individual nuclei
with intact perinuclear Ca2+ stores and then
depleted the perinuclear Ca2+ stores by
incubating them in NIM containing the Ca2+ pump
inhibitor thapsigargin and the Ca2+ chelator
BAPTA-AM. Figure 2
(upper) shows the results. NE electrical resistance decreased in all 12
experiments. This was unexpected in view of previous experiments
showing central channel macromolecule plugging by this maneuver
(8)
. Therefore, we designed another series of experiments
with intact NE Ca2+ stores but lacking ambient
ATP (Fig. 2
, lower). Under these conditions, NEER consistently
increased, indicating that passive ion permeability of the NE is
altered. Removal of both ambient ATP and ambient
Ca2+ further increased NEER. Addition of ATP to
the nuclei depleted of ambient (cytosolic) Ca2+
again lowered NEER (Fig. 2
, middle).
|
Figure 3
summarizes the results. They are displayed as NE electrical conductance
(NEEC), which is the reverse value of NEER. The largest NEEC was
measured with empty perinuclear Ca2+ stores (NEEC
increase vs. control: 7.3±0.02%; mean±SE;
n=12). In contrast, the lowest NEEC was measured when both
Ca2+ and ATP were absent in the ambient
(cytosolic) fluid (NEEC decrease vs. control: 20.3±3.7%;
mean±SE; n=10). Removal of either
ambient Ca2+ or ATP also decreased NEEC, but to a
lower extent. Corresponding control experiments applying 0.1% DMSO,
the solvent used in the thapsigargin/BAPTA-AM experiments, revealed no
significant changes in NEEC (NEEC increase vs. control: 0.45±2.16%;
mean±SE; n=10).
|
We applied AFM to search for peripheral channels supposed to be holes
in the range of a few nanometers visible on the cytoplasmic surface of
NPCs. We used isolated NEs spread on glass and visualized the NPCs in
air at native (unfixed) conditions. We tested two conditions:
1) we incubated NEs with control solution containing both
ambient Ca2+ and ATP for 10 min, then washed the
preparation and imaged the NE surface in air; in a second step,
2) we reincubated the same NEs with a solution lacking ATP.
Representative images are shown in Fig. 4
. NPCs deprived of ATP are shown on the left. NPC surface is smooth and
no channel openings are detected other than the central channel
entrance. In contrast, ATP incubation led to a dramatic shift in NPC
surface topography. Multiple small pores are detectable in the NPC
periphery.
|
| DISCUSSION |
|---|
|
|
|---|
10 kDa)
through the central NPC channel. It became obvious that passive
macromolecule transport is regulated by the filling state of the NE
Ca2+ store (7)
Ambient ATP and Ca2+ seem to be necessary for
normal function of the putative peripheral channels. This finding
agrees with patch clamp experiments in nuclei of Xenopus
laevis oocytes (18)
and of mouse liver
(19)
. From time-lapse experiments applying atomic force
microscopy on nuclear envelopes of Xenopus laevis
oocytes, we know that both ATP and Ca2+ contract
NPCs (27
, 28)
. We used high Ca2+
concentrations (10 µM) in our experiments. It can be assumed that
Ca2+ is released into the nucleoplasm through
inositol 1,3,4 trisphosphate-activated Ca2+
channels of the nuclear envelope accumulating for seconds at high
concentrations near NPCs (14
, 29
, 30)
.
ATP and a sufficiently high concentration of Ca2+
trigger macromolecule transport through the central channel, probably
by a peristaltic wave of contractions. It has been proposed that a
contractile apparatus may be involved in the nucleocytoplasmic
transport of macromolecules through the NPC (31)
. A model
was developed proposing that the nuclear pore contains eight myosin
molecules arranged in an octagonal array, with their heads facing the
cytoplasm and their tails pointing toward the nucleus. These molecules
are in contact with another eight myosin molecules arranged in an
opposite direction, with their heads facing the nucleoplasm. According
to this model, macromolecule transport through the pore would be
accomplished by contractions generated by ATP hydrolysis in the myosin
heads (32)
. In light of the present experiments, we want
to modify the peristaltic transport model by separating the route
of the macromolecules from the route taken by ions. We assume that
under physiological conditions, i.e., when karyophilic proteins are
present for transport, the central channel is usually plugged by
proteins in transit. This view is derived from the original model by
Bustamante and co-workers (12)
. It means that passive
electrical permeability of the plugged central channel must be very
low. However, the passive NE electrical permeability is usually large.
Therefore, we need to postulate peripheral channels that operate in
parallel to the central NPC channel.
When the cytoplasmic aspects of NPCs are carefully analyzed by AFM
using unfixed, native preparations, multiple dimples can be discovered
on the NPC surface. These dimples are found only in NPCs challenged
with ATP before scanning. They could represent the cytoplasmic openings
of the putative peripheral channels described by electron microscopy
several years ago (4)
. Due to limitations of the AFM
technique, we cannot identify them in more detail. The limitation of
the AFM used for imaging the rather complex native NE is based on the
physical extension of the AFM stylus that interacts with the surface.
Therefore, the smaller the lateral dimension of a hole is in an
individual NPC the more the respective hole will be imaged as a shallow
dimple. Taking this limitation into account, the dimples are likely to
represent the entrances of the small peripheral channels. The dimples
were spread over the whole NPC surface and it was not possible to count
them. The main reason we cannot determine the exact number of dimples
per NPC is the irregularity in NPC structure. This irregularity is the
price we must pay for using a native, nonfixed NE preparation that
still responds to physiological stimuli as ATP.
Figure 5
shows the model we propose. The NPC structure is based on a
3-dimensional model developed a few years ago (33)
and
includes the observations of the present paper:
|
1. The existence of small peripheral channels is derived from the observation that blockage of central channel transport by NE calcium store depletion is not paralleled by a comitant decrease of the passive electrical conductance. To the contrary, the electrical conductance is increased.
2. Ambient ATP and Ca2+ are important prerequisites for maintaining the peripheral channels in an open state. This is shown functionally by the increased electrical conductance and structurally by the appearance of small channels on the NPC surface.
3. The large NE electrical conductance is explained by the passive electrical permeability of peripheral channels, at least under conditions when karyophilic macromolecules are available for NPC central channel plugging.
4. The central channel itself does not explain the passive electrical NPC permeability. Obviously, inorganic ions do not pass through the central channel as long as the latter is occupied by macromolecules.
However, the functional state of the NPC central channel can modify
peripheral channel function. Thus, macromolecule transport pathway and
ion transport pathways can interfere with each other as previously
shown (12)
.
| ACKNOWLEDGMENTS |
|---|
Received for publication November 28, 2000.
Revision received April 9, 2001.
| REFERENCES |
|---|
|
|
|---|
This article has been cited by other articles:
![]() |
I. Liashkovich, W. Hafezi, J. E. Kuhn, H. Oberleithner, A. Kramer, and V. Shahin Exceptional mechanical and structural stability of HSV-1 unveiled with fluid atomic force microscopy J. Cell Sci., July 15, 2008; 121(14): 2287 - 2292. [Abstract] [Full Text] [PDF] |
||||
![]() |
A. Kramer, Y. Ludwig, V. Shahin, and H. Oberleithner A Pathway Separate from the Central Channel through the Nuclear Pore Complex for Inorganic Ions and Small Macromolecules J. Biol. Chem., October 26, 2007; 282(43): 31437 - 31443. [Abstract] [Full Text] [PDF] |
||||
![]() |
B. Naim, V. Brumfeld, R. Kapon, V. Kiss, R. Nevo, and Z. Reich Passive and Facilitated Transport in Nuclear Pore Complexes Is Largely Uncoupled J. Biol. Chem., February 9, 2007; 282(6): 3881 - 3888. [Abstract] [Full Text] [PDF] |
||||
![]() |
V. Shahin, W. Hafezi, H. Oberleithner, Y. Ludwig, B. Windoffer, H. Schillers, and J. E. Kuhn The genome of HSV-1 translocates through the nuclear pore as a condensed rod-like structure J. Cell Sci., January 1, 2006; 119(1): 23 - 30. [Abstract] [Full Text] [PDF] |
||||
![]() |
A. Wiedlocha, T. Nilsen, J. Wesche, V. Sorensen, J. Malecki, E. Marcinkowska, and S. Olsnes Phosphorylation-regulated Nucleocytoplasmic Trafficking of Internalized Fibroblast Growth Factor-1 Mol. Biol. Cell, February 1, 2005; 16(2): 794 - 810. [Abstract] [Full Text] [PDF] |
||||
![]() |
C. Perez-Terzic, A. Behfar, A. Mery, J. M.A. van Deursen, A. Terzic, and M. Puceat Structural Adaptation of the Nuclear Pore Complex in Stem Cell-Derived Cardiomyocytes Circ. Res., March 7, 2003; 92(4): 444 - 452. [Abstract] [Full Text] [PDF] |
||||
![]() |
X. Wei, V. G. Henke, C. Strubing, E. B. Brown, and D. E. Clapham Real-Time Imaging of Nuclear Permeation by EGFP in Single Intact Cells Biophys. J., February 1, 2003; 84(2): 1317 - 1327. [Abstract] [Full Text] [PDF] |
||||
![]() |
P. P. Dzeja, R. Bortolon, C. Perez-Terzic, E. L. Holmuhamedov, and A. Terzic Energetic communication between mitochondria and nucleus directed by catalyzed phosphotransfer PNAS, July 23, 2002; 99(15): 10156 - 10161. [Abstract] [Full Text] [PDF] |
||||
![]() |
C. Schafer, V. Shahin, L. Albermann, M. J. Hug, J. Reinhardt, H. Schillers, S. W. Schneider, and H. Oberleithner Aldosterone signaling pathway across the nuclear envelope PNAS, May 14, 2002; 99(10): 7154 - 7159. [Abstract] [Full Text] [PDF] |
||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
| HOME | HELP | FEEDBACK | SUBSCRIPTIONS | ARCHIVE | SEARCH | TABLE OF CONTENTS |