We have developed the means to simultaneously measure the physical size and count catecholamine molecules in individual nanometer transmitter vesicles. This is done by combining resistive pulse (RP) measurements in a nanopore pipet and vesicle impact electrochemical cytometry (VIEC) at an electrode as the vesicle exits the nanopore. Analysis of freshly isolated bovine adrenal vesicles shows that the size and internal catecholamine concentration of vesicles varies with the occurrence of a dense core inside the vesicles. These results might benefit the understanding about the vesicles maturation, especially involving the "sorting by retention" process and concentration increase of intravesicular catecholamine. The methodology is applicable to understanding soft nanoparticle collisions on electrodes, vesicles in exocytosis and phagocytosis, intracellular vesicle transport, and analysis of electroactive drugs in exosomes.
We have developed the means to simultaneously measure the physical size and count catecholamine molecules in individual nanometer transmitter vesicles. This is done by combining resistive pulse (RP) measurements in a nanopore pipet and vesicle impact electrochemical cytometry (VIEC) at an electrode as the vesicle exits the nanopore. Analysis of freshly isolated bovine adrenal vesicles shows that the size and internal catecholamine concentration of vesicles varies with the occurrence of a dense core inside the vesicles. These results might benefit the understanding about the vesicles maturation, especially involving the "sorting by retention" process and concentration increase of intravesicular catecholamine. The methodology is applicable to understanding soft nanoparticle collisions on electrodes, vesicles in exocytosis and phagocytosis, intracellular vesicle transport, and analysis of electroactive drugs in exosomes.
As a crucial organelle to intercellular
communication and modulation of above physiological processes, vesicles
within multiple cells, like neuronal cells,[1−5] beta cells,[6−10] hormonal cells,[11−15] platelets,[16−18] etc., have been investigated in many aspects. Especially,
their involvement in molecular release, exocytosis, has attracted
great interest and been extensively studied in recent years owing
to its importance in many fields such as neuroscience and diabetes.In recent years, micro-/nano-electrochemical approaches have been
developed to realize the quantitative measurement of intravesicular
content and real-time monitoring of their release dynamics.[19−26] Our group developed a new technique, vesicle impact electrochemical
cytometry (VIEC),[27−29] providing a highly effective way to quantify the
intravesicular electroactive contents, such as catecholamines, inside
each single vesicle. However, to the best of our knowledge, the relationship
between size and content concentration of individual vesicle, which
benefits the deeper understanding of the mechanism of exocytosis,
has not yet been disclosed.Although the intravesicular content
of individual vesicles can
be obtained by VIEC, it is currently not possible to measure the size
relating to each measured vesicle. There are several effective commercial
techniques capable of measuring the size of vesicles, such as transmission
electron microscopy (TEM),[30−33] dynamic light scattering (DLS),[34−36] nanoparticle
tracking analysis (NTA),[37−39] and even flow cytometry;[40−42] however, some difficulties still exist. For instance, identifying
vesicles from complex cell debris or corresponding their signal to
the content quantification method, like VIEC, and none of these can
currently be used while simultaneously quantifying the vesicle content.Among those sizing techniques, the resistive pulse (RP) method[43−47] appears compatible with VIEC. With this combination, single vesicles
can be manipulated to move one by one across a solid nanopore with
varying the pore resistance to measure size, then to impact an electrode
surface, release their contents and generate a current transient to
quantify the molecular content.Here we present an effective
strategy to combine RP with the VIEC
technique to simultaneously measure size and content of isolated nanometer
chromaffin vesicles. We then use this to examine the relationship
between content concentration and vesicle size.Periodic pressure
applied to the nanopipette is used to eject vesicles
in solution having a different osmolality inside compared to outside
the tip, and the eluting vesicles are then targeted one at a time
onto an electrode. Two circuits are used for synchronous recording
of the resistive pulses via the nanopipette tip and current spikes
with a carbon fiber microdisk electrode at the VIEC electrode (see Figure A and details in Supporting Information (SI)). A periodic measurement
cycle is used. Application of a pressure pulse (0.5–1 s) is
first used to push out a single vesicle and push away nearby bath
solution (LO in Figure A,C). The ejected solution surrounding the vesicle (HO in Figure A,C) has osmolality
close to that of the intravesicular lumen to avoid swelling and breaking
of vesicles prior to ejection. In the second step, the pressure is
stopped (3–5 s) so the external bath solution, whose osmolality
is lower than the intravesicular solution, will return to the electrode
surface, pushing back the vesicle solution into the nanopipette by
capillary force to stop new particles from flowing out. Vesicles that
attach to the electrode break in a short time (96% of 340 vesicles
open in less than 5 s, see SI, Figure S1). This is facilitated by the low osmolality, and all the intravesicular
catecholamine electrooxidized at the electrode producing current spikes
that can be quantified. When there is only one resistive pulse and
only one current spike appears in one cycle, they can be assumed to
come from the same vesicle (this occurs in 3–7% of pulses empirically;
the vesicle concentration is kept low enough to minimize pulses ejecting
more than one vesicle). This is discussed further in the SI (see Figure S2).
Figure 1
Schematic of RP-VIEC. (A) electrode configuration
for RP-VIEC.
Amplifier 1 records the RP at a potential of +13 mV vs Ag/AgCl reference
electrode. Amplifier 2 records the current spike for VIEC with electrode
potential set to +700 mV vs the same reference electrode. (B–D)
Schematics showing a cycle induced by periodic pressure: (B) Pressure
is applied to push a vesicle across the nanopore and generate an RP
signal. (C) The vesicle attaches on the electrode surface and is surrounded
by the outflowing buffer with relatively high osmolality (similar
to vesicular lumen). LO, low osmolarity; HO, high osmolality. (D)
Suspended pressure results in capillary force (CF) stopping solution
outflow. The vesicle on the surface opens by electroporation aided
by the relatively low osmolarity of the surrounding solution. Electroactive
content of the vesicle is electrooxidized and generates a current
spike.
Schematic of RP-VIEC. (A) electrode configuration
for RP-VIEC.
Amplifier 1 records the RP at a potential of +13 mV vs Ag/AgCl reference
electrode. Amplifier 2 records the current spike for VIEC with electrode
potential set to +700 mV vs the same reference electrode. (B–D)
Schematics showing a cycle induced by periodic pressure: (B) Pressure
is applied to push a vesicle across the nanopore and generate an RP
signal. (C) The vesicle attaches on the electrode surface and is surrounded
by the outflowing buffer with relatively high osmolality (similar
to vesicular lumen). LO, low osmolarity; HO, high osmolality. (D)
Suspended pressure results in capillary force (CF) stopping solution
outflow. The vesicle on the surface opens by electroporation aided
by the relatively low osmolarity of the surrounding solution. Electroactive
content of the vesicle is electrooxidized and generates a current
spike.Chromaffin vesicles, containing
catecholamines, were isolated from
bovine adrenal glands and were investigated after pretreatment through
this strategy. After subtracting the baselines in both traces, some
examples showing the spike following the RP are observed (see Figure and SI, Figure S2). To analyze the RP signal, an algorithm[48] was adopted, and it was used to effectively
relate the magnitude of the RP signal to the ratio of the radius of
the vesicular particle and the nanopore (see details in SI and Figure S4).
Figure 2
An example
an RP vs VIEC signal. The blue trace is the RP recording
and it is shown in the form of normalized current decline, and the
orange trace is VIEC and shown as spike current. The data from both
traces are processed (raw traces in SI, Figure S3). The inset is the magnification of both signals, including
a RP signal and its following VIEC signal (marked with an asterisk
for each). The pink zones indicate when the pressure is applied, and
white zones indicate when it is stopped. RP spikes in the white zone
without corresponding VIEC signals are likely due to dust or other
particles that do not impact or create a signal at the electrode and
so are not considered.
An example
an RP vs VIEC signal. The blue trace is the RP recording
and it is shown in the form of normalized current decline, and the
orange trace is VIEC and shown as spike current. The data from both
traces are processed (raw traces in SI, Figure S3). The inset is the magnification of both signals, including
a RP signal and its following VIEC signal (marked with an asterisk
for each). The pink zones indicate when the pressure is applied, and
white zones indicate when it is stopped. RP spikes in the white zone
without corresponding VIEC signals are likely due to dust or other
particles that do not impact or create a signal at the electrode and
so are not considered.After estimating the
pore size by scanning electron microscopy
(see an example in SI, Figure S5), the
size of individual vesicle can be calculated. The catecholamine content
was evaluated by VIEC as described in the SI. Further, the concentration (C) was calculated
by use of individual vesicle radius (r) and vesicular
catecholamine content in moles (N), using the equation:where NA is Avogadro’s
number (6.022 × 1023 mol–1). We
collected 278 simultaneous measurements of vesicular catecholamine
content and vesicle radius, and these are plotted in Figure with their respective histograms.
The median of vesicle radius is 216 nm, with 2.64 × 106 molecules and a calculated concentration of 0.101 M (see the histogram
of concentration in SI, Figure S6).
Figure 3
Statistical
distribution of vesicle content versus radius of each
individual recorded chromaffin vesicle. The relationship between content
versus radius is shown in a scatter plot in part ①; the normalized
frequency histograms of content are depicted in part ② and
vesicle radius in part ③. Parts ① and ② share
the Y-axis, and parts ① and ③ share
the X-axis. The dotted lines and circle indicate
the median position for each parameter measured.
Statistical
distribution of vesicle content versus radius of each
individual recorded chromaffin vesicle. The relationship between content
versus radius is shown in a scatter plot in part ①; the normalized
frequency histograms of content are depicted in part ② and
vesicle radius in part ③. Parts ① and ② share
the Y-axis, and parts ① and ③ share
the X-axis. The dotted lines and circle indicate
the median position for each parameter measured.Notably, our results appear to provide insight into the quantitative
aspect of vesicle maturation, especially regarding the dense core
within vesicles. The vesicular dense core, consisting of polyanionic
protein, is thought to largely complex the catecholamines via electrostatic
interaction. We sorted the current transients for VIEC of single vesicles
by curve fitting the falling phase (after the peak) of the current
spikes.[49] The previous theoretical analysis
considered only vesicles with dense cores and yet provided a potential
framework to explain events that have single versus multiple exponential
declines on the falling part of the event. However, as exocytosis
is partial,[2,50−52] this means
that release is more complex with single exponential events for release
from the spaces vs double exponential events from both the spaces
and the dense core in the vesicle. In VIEC where the entire vesicle
content is measured, we interpret events with single exponential to
represent immature vesicles (NDCVs). If the falling phase is fit by
a single exponential decline, we interpret this to indicate that the
vesicle does not have a protein dense core, and a double exponential
fit reflects the existence of a dense core. We then classified all
the simultaneous measurements of catecholamine amount (VIEC) and radius
(RP) for vesicles into two groups via a fit of one or two exponentials
in the respective current spike. With the assumptions above, this
allowed us to divide spikes into those having dense cores (DCV, n = 150) and those apparently without dense cores (NDCV, n = 128). In SI, Figure S7, we
show the statistical distribution of the vesicle radii and their catecholamine
concentrations for both groups. The median concentration of the DCVs
is higher than the NDCVs (0.116 M for DCVs versus 0.062 M for NDCVs, P < 0.01, see the inset in SI, Figure S7②), and the median radius of the DCVs is slightly
smaller (216 nm for DCVs versus 218 nm for NDCVs, P < 0.1, see the inset in SI, Figure S7③). Also, the median catecholamine numbers are higher for
DCVs (2.8 × 106 molecules for DCVs versus 2.1 ×
106 molecules for NDCVs, P < 0.01,
see SI, Figure S8).DCVs are usually
considered to be more mature vesicles than NDCVs.
Our results provide a novel perspective on the hypothetical process
called “sorting by retention” for protein recycling
(see SI, Figure S9)[53,54] during vesicle maturation. Briefly, after being formed from the trans-Golgi network and homotypic fusion, immature vesicles
will expel those proteins not destined for mature vesicles via budding
off of small clathrin-coated vesicles, possibly leading to a slight
decrease in vesicle size. Subsequently, the following condensation
and acidification of the vesicular lumen will increase the concentration
of intravesicular catecholamines as the dense core is formed.[55−57] Our data are consistent with this process.In conclusion,
our work presents an effective approach to simultaneously
correlate the size of an individual chromaffin vesicle and its intravesicular
catecholamine content. By use of the resistive pulses caused by a
vesicle exiting a nanopore and then capturing the vesicle on an electrode
for analysis, the RP-VIEC approach allows us to examine individual
vesicles for size and molecular content and to examine the distribution
of these two parameters. Furthermore, with vesicle size and content,
we can calculate catecholamine concentration in each vesicle separately
and examine its variation, whereas this was only possible for populations
of vesicles in previous experiments. Analysis of isolated chromaffin
vesicles indicates size and catecholamine concentration are different
between DCVs and NDCVs. Thus, this might be a means to provide quantitative
information about the vesicle maturation process. The strategy presented
here should benefit further investigation of vesicle-related physiology
processes, including exocytosis, phagocytosis, intracellular vesicle
transport, as well as analysis of electroactive drugs in exosomes.
Authors: Samuel A Stoner; Erika Duggan; Danilo Condello; Abraham Guerrero; James R Turk; Padma K Narayanan; John P Nolan Journal: Cytometry A Date: 2015-10-20 Impact factor: 4.355
Authors: Xianchan Li; Soodabeh Majdi; Johan Dunevall; Hoda Fathali; Andrew G Ewing Journal: Angew Chem Int Ed Engl Date: 2015-08-12 Impact factor: 15.336
Authors: Keke Hu; Rui Jia; Amir Hatamie; Kim Long Le Vo; Michael V Mirkin; Andrew G Ewing Journal: J Am Chem Soc Date: 2020-09-28 Impact factor: 15.419