Difference between revisions of "Team:Slovenia/Mechanosensing/Gas vesicles"

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                        <b>Modeling of ultrasound</b>
 
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                        <h1 class="ui left dividing header"><span id="ach" class="section"> &nbsp; </span>Ultrasound
 
                            controlling device</h1>
 
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                            <ul>
 
                                <li><b>Implementation of 90 W ultrasonic amplifier for pulsed cells stimulation.</b>
 
                                <li><b>Optimization of developed system in a given frequency range around 310 kHz.</b>
 
                                <li><b>User friendly controlling interface of device.</b>
 
                                <li><b>Capability of providing 7 kPa of pressure 4 mm from ultrasonic transducer.</b>
 
                            </ul>
 
                        </div>
 
</div>
 
<div class="ui segment">
 
<h4><span id = "mot" class = "section">&nbsp;</span></h4>
 
<p>The ultrasound (US) wave interacts with tissue and reflects back depending on the
 
properties of the tissues such as velocity of sound in the tissue and its density, which
 
can be modeled using <a href="https://2016.igem.org/Team:Slovenia/Model">wave
 
equation.</a> Higher frequencies have better resolution (shorter wavelengths) but
 
cannot penetrate as deep into the tissues. In diagnostic ultrasound frequencies above 1
 
MHz are used. For better tissue penetration frequencies of interest for our purposes are
 
between 0.3 to 1 MHz yielding sufficient resolution and penetration at the same time
 
<x-ref>Speed2001</x-ref>
 
. Latest studies show that it is possible to use pulsed ultrasound for neurostimulation,
 
ultrasound therapy such as treatment of pain and the repair of various tissues, however
 
without clear knowledge which receptors or cell types we are targeting, and what is the
 
mechanism of the ultrasound stimulation effects
 
<x-ref>Vasquez2014</x-ref>
 
.
 
</p>
 
</div>
 
 
 
                        <h1><span class="section">&nbsp;</span>Results</h1>
 
                        <div class="ui segment">
 
 
<div>
 
<h3><span id="mod" class="section">&nbsp;</span>MODUSON - Generating ultrasonic power
 
pulses for cell stimulation</h3>
 
<p>For the simple setup of the ultrasonic stimulation of cells we initially used ultrasonic
 
baths (<ref>1</ref>) that are used to clean the laboratory equipment, small devices to clean jewelry or
 
ultrasonic cell disruptors, which however offer little control over the intensity,
 
frequency or pulse shapes and numbers of repetitions and are not appropriate to monitor
 
activation of mechanosensors under the fluorescence microscope. However, one member of
 
the team is a student of electrical engineering and this was the right challenge for
 
him.
 
</p>
 
<div style="float:right; width:100%">
 
<figure data-ref="1">
 
<img src=" https://static.igem.org/mediawiki/2016/3/32/T--Slovenia--5.1.15.png">
 
<figcaption><b>Different experiment configurations.</b><br/>
 
  <p style="text-align:justify">Testing homogeneity of pressure in each well with a plate immersed in the
 
ultrasonic bath.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
 
<p>For the generation of specific shapes of ultrasound pulses researchers usually use a
 
setup consisting of two signal generators (one for switching on and off the train of US
 
pulses and the other one to produce the sinusoidal signal of suitable frequency). This
 
signal is further fed to the amplifier and then to the ultrasonic transducer.
 
Furthermore, an ultrasonic sensor is required to evaluate and control the magnitude of
 
the ultrasound. Usually a hydrophone is used in combination with an amplifier and an
 
oscilloscope. This setup is complex to establish and difficult to use. Therefore, the
 
goal of a part of the iGEM 2016 group (student of electrical engineering) was to develop
 
a device (named Moduson), which would be capable of providing appropriate signals
 
required to perform specific ultrasonic experiments in a single apparatus and as such
 
easy to use. The research and development of the device was performed in the Laboratory
 
for Bioelectromagnetics at the Faculty of Electrical Engineering, University of Ljubljana under
 
the supervision of prof. dr. Dejan Križaj and a company Noeto.</p>
 
 
</div>
 
<div>
 
<h3><span id="rel" class="section">&nbsp;</span>The basic requirements for the device and
 
realizations</h3>
 
 
<h5>Adaptability</h5>
 
 
<p>The device should be designed to be as flexible as possible in order to be capable of
 
delivering a wide range and different shapes of stimulation signals to stimulate cells
 
under the microscope, cells in a petri dish, cells in a microplate immersed into a bath
 
and to stimulate animals. In order to fulfill this requirement we selected a dedicated
 
embedded measurement card Red Pitaya acting as an embedded computer. This embedded
 
device is based on Linux system and can be completely customized to the user’s needs.
 
Furthermore, it can be Wi-Fi controlled so the final application is based on modern
 
programming tools such as JavaScript, C++, HTML, etc. The final application is basically
 
a web page, accessible with any computer capable of the Wi-Fi connection. This
 
application gives complete control of all stimulation parameters and operation of the
 
device. Another advantage of the platform used is its capability of simple integration with
 
Matlab through so-called SCPI commands, usually used in the instrumentation for easy
 
control and data acquisition making the device perfect research and development tool.
 
Simple example of SCPI commands in Matlab for pulsed bursts is shown below:</p>
 
<div style="float:left; width:100%">
 
<figure>
 
<img src=" https://static.igem.org/mediawiki/2016/b/b6/T--Slovenia--5.1.5.png">
 
</figure>
 
</div>
 
 
 
<p style="clear:both">On the
 
<ref>2</ref>
 
a typical sequence of a stimulation signal constructed of a set number of sine waves of
 
defined frequency that is repeated for required number of times with selected repetition
 
period is shown.
 
</p>
 
<div style="float:left; width:100%">
 
<figure data-ref="2">
 
<img src="https://static.igem.org/mediawiki/2016/6/6e/T--Slovenia--5.1.6.png ">
 
<figcaption><b>Signal parameters.</b><br/>
 
<p style="text-align:justify">Parameters that can be set for a typical stimulation signal.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
 
<h5>Simple graphical user interface</h5>
 
<p>Users of the device do not need to be computer experts and do not need to have knowledge
 
on the signal generators, amplifiers and oscilloscopes. Therefore, the motivation was to
 
design and develop a simple user-friendly graphical interface with all the relevant
 
parameters that need to be set in order to run the experiments from the Web page. To
 
accomplish this, dedicated software was written that enables users to design and run the
 
experiment and evaluate the results. <ref>3</ref> presents a developed user interface. On the right side (US burst settings -> STIMULATION
 
PULSE) we can set parameters, such as the amplitude of the signal, frequency and number
 
of sine waves. Below these settings, repetition parameters of the signal (PULSE
 
REPETITION) such as the number of pulse repetitions and its frequency can be set. When
 
all parameters are set, the signal can be previewed by clicking the SHOW BURST button.
 
The pulse sequence is initiated with the START button. The acquired signal from
 
hydrophone is seen on the main plot. At the top of the interface, there are options to
 
export the image of a graph and csv data of the acquired signal. Chosen values of
 
parameters can also be saved for the next use of the device.
 
</p>
 
<div style="margin-left:auto; margin-right:auto; width:50%">
 
<figure data-ref="3">
 
<img onclick="resize(this);"
 
src=" https://static.igem.org/mediawiki/2016/b/bf/T--Slovenia--5.1.7.png">
 
<figcaption><b>Application interface.</b><br/>
 
  <p style="text-align:justify"> Web based interface used for setting of the signal parameters.
 
  </p>
 
</figcaption>
 
</figure>
 
</div>
 
 
<h5 style="clear:both">Signal amplifier</h5>
 
 
<div style="width: 33%; float:left;">
 
<figure data-ref="4">
 
<img class="ui medium image" onclick="resize(this);"
 
src=" https://static.igem.org/mediawiki/2016/7/7e/T--Slovenia--5.1.8.png">
 
<figcaption><b>Simulation scheme.</b><br/>
 
<p style="text-align:justify">Scheme used in LT Spice simulations.
 
  </p>
 
  </figcaption>
 
</figure>
 
</div>
 
<div style="width: 33%; float:left;">
 
<figure data-ref="5">
 
<img class="ui medium image" onclick="resize(this);"
 
src="https://static.igem.org/mediawiki/2016/3/3b/T--Slovenia--5.1.9.png ">
 
<figcaption><b>Model of transducer.</b><br/>
 
<p style="text-align:justify">Equivalent model of ultrasonic transducer based on a BVD model.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
<div style="width: 33%; float:left;">
 
<figure data-ref="6">
 
<img class="ui medium image" onclick="resize(this);"
 
src=" https://static.igem.org/mediawiki/2016/0/0a/T--Slovenia--5.1.10.png">
 
<figcaption><b>Moduson.</b><br/>
 
<p style="text-align:justify">Constructed device with a simple interface; an ON/OFF button, a BNC output for
 
the transducer and a button to trigger stimulation pulses. The pulses can also
 
be triggered directly through the Web interface.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
<p style="clear:both;"></p>
 
<p>We built the circuitry with real elements on a prototype board where several additional
 
alterations were required, as the real elements do not have ideal characteristics as the
 
ones included in the simulation. Another challenge was the design of a suitable
 
transformer to increase the voltage amplitude of the signal. The transformer is also
 
required to operate as an impedance transformer. Lowering impedance of the ultrasonic
 
transducer enables higher current levels and consequently higher power values.</p>
 
<p>Once a suitable signal is generated, it needs to be amplified from a signal level
 
(amplitude of 2 V) to several hundred volts or even above 1000 V, which poses a serious
 
engineering challenge. For this purpose, we first designed a circuitry on a conceptual
 
level and simulated it with LT Spice (<ref>4</ref>). In the simulations an electric model of a transducer was considered as a combination
 
of capacitors, inductors and resistors wired in parallel (<ref>5</ref>). This model enables simulation of ultrasonic transducers with several resonant
 
frequencies. Simulations show that our device can reach the power at transducer around
 
92W, which is close to the measured 86W in the real system.
 
</p>
 
</div>
 
<div>
 
<h3><span id="eva" class="section">nbsp;</span>Evaluation of the developed device
 
</h3>
 
 
<p>Functionality of the Moduson was first tested without any connected load. <ref>7</ref> presents a typical output measured with an oscilloscope for a signal of frequency 310
 
kHz.
 
</p>
 
 
<div style="float:left; width:100%">
 
<figure data-ref="7">
 
<img src="https://static.igem.org/mediawiki/2016/5/58/T--Slovenia--5.1.2.png ">
 
<figcaption><b>Typical output signal without load.</b><br/>
 
<p style="text-align:justify">Amplitude of acquired signal depends on the winding of transformer.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
 
<p>Developed device was tested with several transducers with resonance frequencies ranging
 
from 300 kHz up to 1 MHz. Most experiments were performed with an unfocused transducer
 
Olympus V318-SU (<ref>8</ref>) with a waterproof case, allowing it to be used in <i>in vitro</i> experiments.
 
</p>
 
 
<div style="float:left; width:50%">
 
<figure data-ref="8">
 
<img src="https://static.igem.org/mediawiki/2016/f/fe/T--Slovenia--5.1.11.png ">
 
<figcaption><b>Ultrasound transducer V318-SU.</b><br/>
 
<p style="text-align:justify">Handy waterproof case allowed us to use the transducer in most experiments.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
<div style="float:left; width:50%">
 
<figure data-ref="9">
 
<img src="https://static.igem.org/mediawiki/2016/2/2e/T--Slovenia--5.1.4.png ">
 
<figcaption><b>Electric power of ultrasonic transducer before and after
 
compensation.</b><br/>
 
<p style="text-align:justify">Electrical power with compensation was significantly increased with serial
 
compensation.</p>
 
</figcaption>
 
</figure>
 
</div>
 
 
 
<p>
 
<ref>9</ref>
 
presents measured electric power using the transducer V318-SU. After partial
 
compensation of reactive part, the measured real power reached 86 W. This result
 
exceeded the set requirements.
 
</p>
 
 
<p>With compensation, voltage was considerably increased at contacts of transducer and
 
reached around 900Vpp as shown in <ref>10</ref>.
 
</p>
 
<div style="float:left; width:100%">
 
<figure data-ref="10">
 
<img src="https://static.igem.org/mediawiki/2016/3/3d/T--Slovenia--5.1.1.png ">
 
<figcaption><b>Voltage at input of a transducer V318-SU.</b><br/>
 
<p style="text-align:justify">Transducer requires relative high voltage to operate properly.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
 
<p>We measured the emitted ultrasonic pressure indirectly with a hydrophone RP 31l shown in <ref>11</ref>. This hydrophone has a sensitivity of 50mV/100kPa at a frequency of 310kHz. It can be
 
connected directly to the oscilloscope input to detect the pressure of the ultrasonic
 
waves. Pressure measured 4 mm from the transducer reached 7 kPa which gives the
 
intensity of 33 W/cm<sup>2<sup>.</p>
 
 
<div style="float:left; width:50%">
 
<figure data-ref="11">
 
<img src="https://static.igem.org/mediawiki/2016/e/e5/T--Slovenia--5.1.12.png ">
 
<figcaption><b>Hydrophone RP 31l.</b><br/>
 
<p style="text-align:justify">Calibrated hydrophone used to measure pressure.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
 
<p style="clear:both">Example of an output signal measured by a hydrophone is presented in
 
the <ref>12</ref>.
 
<p>
 
 
<div style="float:left; width:100%">
 
<figure data-ref="12">
 
<img src=" https://static.igem.org/mediawiki/2016/b/b8/T--Slovenia--5.1.3.png">
 
<figcaption><b>Voltage signal detected using the hydrophone.</b><br/>
 
<p style="text-align:justify">With calibration data, we can determine pressure which corresponds to acquired
 
voltage amplitude.
 
</p>
 
</figcaption>
 
</figure>
 
</div>
 
<p style="clear:both;">
 
</p>
 
</div>
 
<div>
 
                            <h3><span id="set" class="section">nbsp;</span>Set-up for experiments with ultrasonic
 
                                pulses</h3>
 
 
                            <p>After we successfully tested the Moduson device, we aimed to design measurement set-up
 
                                for stimulation of cells cultivated in plastic 6-well plates, which allows insertion of
 
                                the ultrasound transducer. In order to ensure repeatable conditions in every experiment
 
                                the position of a transducer was fixed with a suitable holder. Several models of holders
 
                                were designed for different experimental configurations and a 3D-printer was used to
 
                                fabricate a dedicated holder (<ref>13</ref>). This allowed positioning of the transducer at the fixed height above the bottom of a
 
                                well (<ref>14</ref>), which was crucial due to the series of maximal and minimal intensity of generated
 
                                pressure.
 
                            <p>
 
                            <div style="float:left; width:50%">
 
                                <figure data-ref="13">
 
                                    <img src="https://static.igem.org/mediawiki/2016/8/88/T--Slovenia--5.1.13.png ">
 
                                    <figcaption><b>3D printer.</b><br/>
 
                                        <p style="text-align:justify">Printing a holder for the ultrasonic transducer that we used for a 6-well plate.
 
</p>
 
                                    </figcaption>
 
                                </figure>
 
                            </div>
 
 
                            <div style="float:left; width:50%">
 
                                <figure data-ref="14">
 
                                    <img src=" https://static.igem.org/mediawiki/2016/e/ea/T--Slovenia--5.1.14.png">
 
                                    <figcaption><b>Ultrasound based experiments on the microscope.</b><br/>
 
                                        <p style="text-align:justify">Ultrasonic transducer with a 3D printed holder in a 6-well plate.
 
</p>
 
                                    </figcaption>
 
                                </figure>
 
                            </div>
 
 
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Revision as of 17:07, 18 October 2016

Gas vesicles

 Enhanced mechanosensitivity by gas vesicles expressed in mammalian cells

  • Addition of synthetic lipid microbubbles improved the responsiveness of cells to low-power ultrasound.
  • Gas vesicle-forming proteins were expressed in mammalian cells where they improved sensitivity of cells to ultrasound.
  • Combination of the ectopic expression of the mechanosensing bacterial channel MscS and gas vesicle-forming proteins sensitized cells to mechanical stimulation.

 

For activation of mechanoreceptors TRPC1 or MscS, a high-power ultrasound wave (900 Vpp) is required. Our aim was to improve responsiveness of cells to respond to the lower power of ultrasound as this would increase the selectivity, avoiding stimulation of endogenous channels and prevent cell damage. We decided to test gas-filled lipid microbubbles, since it has been reported that microbubbles can amplify the ultrasonic signal Ibsen2015 .

Further explanation ...

Microbubbles are small gas-filled lipid vesicles which are used as contrast agents in medicine. Their size is in the range of micrometers. They work by resonating in an ultrasound beam, rapidly contracting and expanding in response to the pressure changes of the sound wave Blomley2001. Ibsen et al. Ibsen2015 have used microbubbles for transduction of the ultrasonic wave in order to make neurons of C.elegans sensitive to ultrasound.

  Results

  Lipid microbubbles

Synthetic lipid microbubbles.

(A) Schematic of a cell with an increased sensitivity to ultrasound stimulation in the presence of microbubbles. When exposed to mechanical stimuli the microbubbles contract and expand, resulting in activation of mechanosensitive channels on the cell membrane. (B) Mixed size distribution of lipid microbubbles was obtained. Stabilized lipid microbubbles were prepared by sonication and detected by microscopy.

Properties of microbubbles for example rigidity, are affected by the composition of the lipid membrane and the gas core. We prepared our lipid microbubbles from a mixture of DSPC:DSPE. Before sonication we added gas perfluorohexane (as described in the Protocols section), which facilitates compression and expansion of the microbubbles upon ultrasound stimulation (3.3.1.A). A heterogeneous mixture of microbubbles in the range from 5 to 100 µm in size were generated by this procedure (3.3.1.B). Microbubbles are most effective in the size range corresponding to the resonance frequency of the ultrasound. However, care has to be taken in the applied energy to prevent cavitation, that can sonoporate cell membranes.

Application of microbubbles to cells expressing mechanosensitive channel MscS significantly improved calcium influx after mechanical stimulation using low-power ultrasound wave (450 Vpp) (3.3.2.). The same experimental setup was used a previusly described in ultrasound stimulation of mechanosensitive channels.

Ultrasound response of cells is amplified by the use of lipid microbubbles.

(A) Presentation of the ultrasound stimulation sequence and (B) signal parameters used for the stimulation. (C, D) Lipid microbubbles strongly enhanced response of cells expressing MscS channels. HEK293 cells expressing MscS channels were stimulated with ultrasound for 10 s and calcium influx was recorded in real time (D) using a confocal microscope. For comparison cells without ectopic MscS were used. Fluo-4 (D, green line) and Fura Red dyes (D, red line) were used for ratiometric calcium imaging. (D) Ratio (blue line) was calculated from fluorescence intensities of Fura Red and Fluo-4 using CaPTURE.

However, there are some drawbacks related to the use of lipid microbubbles, as their delivery requires injection into the selected tissue. Additionally lifetime of lipid microbubbles is limited in the tissue to tens of minutes and they need to be prepared freshly at least once a week.

  Gas vesicles

To overcome the described drawback we thought of alternative options. One idea that initially looked too crazy to work was to use genetically encoded gas vesicles that are produced in bacteria. Bacterial gas vesicles have been used as contrasting agents for ultrasonography in animals Shapiro2014. This demonstrated that ultrasound can have effect on gas vesicles. However adding bacterial gas vesicles instead of microbubbles would not solve the problem. The best solution would be if the gas vesicles could be produced in the functional form in mammalian cells. iGEM team OUC-China 2012 demonstrated that only two protein components were sufficient to prepare functional gas vesicles in E.coli. Since gas vesicles are compressible their size should vary with pressure variations in the ultrasound or by mechanical stimulus, which would strongly influence the cytoskeleton or cell membrane. Therefore, they would likely amplify activation of mechano-channels (s1).

Schematic of a cell expressing gas vesicle-forming proteins for increased sensitivity to ultrasound stimulation.

When exposed to mechanical stimuli the gas vesicles contract and expand, resulting in activation of mechanosensitive channels on the cell membrane.


Further explanation ...

Gas vesicles are stable gas-filled structures, which provide buoyancy in a wide variety of planktonic prokaryotes Buchholz1993. Two structural proteins have been identified in the gas vesicles of cyanobacteria and the halophilic archaea. The major protein, GvpA, is small hydrophobic protein that forms the ribs of the gas vesicle wall, while the minor gas vesicle protein, GvpC, is larger, hydrophilic protein that stabilizes the structure Hayes1986.


Expression of gas vesicle forming proteins in mammalian cells.

Expression of (A) GvpC and (B) GvpA protein was determined by Western blot using (A) anti-FLAG and (B) anti-AU1, respectively. Expected sizes (marked with arrow) are 22,5 kDa and 8,5 kDa for GvpC and GvpA, respectively.

HEK293 cells were transfected with plasmids expressing both gas vesicle forming proteins, GvpA and GvpC. We could obtain GvpC from the Registry and added to its characterization, while the plasmid for GvpA could not be recovered and its coding sequence was synthesized using mammalian codon usage. Expression of both proteins was confirmed by the western blot (3.3.3.) and colocalization was observed by confocal microscopy (3.3.4.).

GvpA and GvpC were both expressed in the cytosol and colocalized.

HEK293T cells were transfected with plasmids encoding gas vesicle proteins, GvpA and GvpC. 24 h after transfection cells were fixed, permeabilized and immunostained with anti-FLAG (upper row) and anti-AU1 (lower row). Both GvpA and GvpC are located in cytosol as expected. Colocalization is presented in the overlay picture.

Cell viability was not affected by expression of gas vesicle forming proteins.

HEK293 cells were transfected with GvpA and/or GvpC. 24 h after the transfection viability of cells was measured using trypan blue.

A toxicity test was performed in order to ensure that gas vesicles were not toxic to mammalian cells. 3.3.5. shows that the viability of cells was not altered when expressing gas vesicle forming proteins.

HEK293 cells expressing gas vesicle-forming proteins exhibited increased sensitivity to ultrasound stimulation, even in the absence of exogenous mechanosensitive channels (3.3.6.), which was most likely due to activation of the endogenous mechanosensitive channels in mammalian cells.

Gas protein vesicles improve the sensitivity of cells to ultrasound.

(A) Presentation of the ultrasound stimulation sequences for 900 Vpp (red) and 450 Vpp (grey) ultrasound waves and (B) signal parameters used for stimulation. (C, D) Genetically encoded gas vesicle-forming proteins greatly increased cell response at high-power (900 Vpp) in comparison to low-power ultrasound (450 Vpp). HEK293 cells expressing Gvps were stimulated with ultrasound for 10 s and calcium influx was recorded in real time (D). Fluo-4 (D, green line) and Fura Red dyes (D, red line) were used for ratiometric calcium imaging. (D) Ratio (blue line) was calculated from fluorescence intensities of Fura Red and Fluo-4 using CaPTURE.

In order to maximize the sensitivity of cells to ultrasound, we transfected cells with a combination of mechanosensitive channel MscS and gas vesicle-forming proteins. By decreasing the power of ultrasound stimulation we demonstrated that cells expressing a combination of both ectopic channels and gas vesicles were activated as a result of the ultrasound stimulation (3.3.7.).

Coexpression MscS with Gvps in mammalian cells improves sensitivity of cells to ultrasound even at lower voltages.

(A) Presentation of the ultrasound stimulation sequence and (B) signal parameters used for stimulation. (C, D) Co-expression of mechanosensitive channels and gas vesicle-forming proteins increased sensitivity to ultrasound stimulation in comparison to the cells without exogenous mechanosensitive channels. HEK293 cells expressing gas vesicle-forming proteins GvpA and GvpC with or without MscS were stimulated with ultrasound for 10 s and calcium influx was recorded in real time (D) using a confocal microscope. Changes in fluorescence intensity of calcium indicators Fluo-4 (green line) and Fura Red (red line) are shown. (D) Ratio (blue line) was calculated from fluorescence intensities of Fura Red and Fluo-4 using CaPTURE.

To prove that calcium influx was the mediator of activation of mechanosensitive channels, we used an inhibitor of ion channels gadolinium (Gd3+), which has a similar ionic radius, but a higher charge density to Ca2+. By blocking the pore of the channel it acts as an general inhibitor of calcium ion channels Bourne1982. As shown on 3.3.8., the addition of gadolinium prevented calcium influx triggered by ultrasound stimulation.

Calcium influx after ultrasound stimulation is mediated by activation of mechanosensitive channels.

(A) Presentation of the ultrasound stimulation sequence and (B) signal parameters used for stimulation. (C, D) Gadolinium inhibits activation of mechanosensitive ion channels after ultrasound stimulation. HEK293 cells expressing gas vesicle-forming proteins GvpA and GvpC with or without MscS were treated with gadolinium (red line) or not (grey line) and stimulated with ultrasound for 10 s and calcium influx was recorded in real time (D). Changes in fluorescence intensity of calcium indicators Fluo-4 (green line) and Fura Red (red line) are shown. (D) Ratio (blue line) was calculated from fluorescence intensities of Fura Red and Fluo-4 using CaPTURE.



This is the first time demonstration that that gas vesicle-forming proteins can be expressed in human cells and that they improve the sensitivity of mechanosensitive channels for ultrasound. Moreover when the gas vesicle-forming proteins were co-expressed with ectopic ion channels the calcium influx could be achieved with low-power ultrasound stimulation.

Ultrasound is a type of mechanical stimulus, therefore we reasoned that cells might exhibit response also to other types of stimulus such as the touch. The next task was to couple the response of mechanosensitive channels to the mediator of signaling or to the genetically encoded reporter. Mediator of this activation are Ca2+ ions, which are sensed by different cellular proteins and which have been in the literature detected by several designed sensors. The mechanosensing device was then coupled to the calcium split luciferase reporter based on M13 and calmodulin or can be coupled to the protease split system and response of cells was determined against mechanical stimulus in a Touchpaint implementation.