- Open Access
Field models and numerical dosimetry inside an extremely-low-frequency electromagnetic bioreactor: the theoretical link between the electromagnetically induced mechanical forces and the biological mechanisms of the cell tensegrity
© Mognaschi et al.; licensee Springer. 2014
- Received: 19 June 2014
- Accepted: 9 August 2014
- Published: 27 August 2014
We have implemented field models and performed a detailed numerical dosimetry inside our extremely-low-frequency electromagnetic bioreactor which has been successfully used in in vitro Biotechnology and Tissue Engineering researches. The numerical dosimetry permitted to map the magnetic induction field (maximum module equal to about 3.3 mT) and to discuss its biological effects in terms of induced electric currents and induced mechanical forces (compression and traction). So, in the frame of the tensegrity-mechanotransduction theory of Ingber, the study of these electromagnetically induced mechanical forces could be, in our opinion, a powerful tool to understand some effects of the electromagnetic stimulation whose mechanisms remain still elusive.
- Electromagnetic field models
- Numerical electromagnetic dosimetry
- Magnetic induction field
- Induced electric field
- Induced electric currents
- Induced mechanical forces
The research about the biological effects caused by electromagnetic fields (EMFs) has been of great interest in the past decades. In particular, extremely-low-frequency EMFs (ELF-EMFs), with frequency up to 300 Hz and continuously irradiated by civil and industrial appliances, have been investigated to clarify their possible biological effects on the population unceasingly exposed to them; to this regard, epidemiological studies have shown a relation between the environmental ELF-EMFs and the onset of leukemia (tumor of the lymphoid tissue) (Kheifets et al., 2010) or Alzheimer’s disease (neurodegenerative disorder in the non-lymphoid brain tissue) (Davanipour et al., 2007; Huss et al., 2009; Maes and Verschaeve, 2012).
In both lymphoid and non-lymphoid tissues, the cells regulate the flow of ionic currents across their plasma membrane and internal membranes through specific ion channels, so that one of the simplest ways to affect a biological system is to induce a change in its ionic fluxes (for instance, via an ELF-EMF exposition that elicits conformational changes in the ion channel proteins and modifies, in particular, the calcium currents and the cytosolic calcium concentration), as it is well known that an increased calcium flux can trigger numerous biochemical pathways (Bawin et al., 1978; Walleczek, 1992; Balcavage et al., 1996; Pavalko et al., 2003). As a matter of fact, ELF-EMFs lead to a mitogenic effect in lymphocytes because they can modify the calcium influx (Balcavage et al., 1996; Murabayashi et al., 2004), whereas, in a non-lymphoid tissue such as the brain neuronal tissue, the proposed mechanisms about the electromagnetic stimulation are more complex and involving both ionic fluxes and alterations in the distribution and in the functionality of membrane receptors (e.g. serotonin, dopamine, and adenosine receptors).
In particular, the ELF-EMFs decrease the affinity of the G-protein-coupled 5-HT1B serotonergic receptor with a consequent decreased signal transduction (Massot et al., 2000; Espinosa et al., 2006), decrease the affinity of the G-protein-coupled 5-HT2A serotonergic receptor (Janac et al., 2009), reduce the reactivity of the central dopamine D1 receptor (Sieron et al., 2001), and increase the density of the A2A adenosine receptor (Varani et al., 2011) revealing, as a consequence, a possible treatment of the inflammatory trait in Alzheimer’s disease via a better use of the endogenous adenosine, which is an effective brain anti-inflammatory agent when combined with its A2A receptor (Rosi et al., 2003; Tuppo and Arias, 2005). In addition, the adenosine receptors appear to play an important role during the in vitro ELF-EMF stimulation of other cell types such as neutrophils (Varani et al., 2002; Varani et al., 2003), chondrocytes and fibroblast-like synoviocytes (Varani et al., 2008; De Mattei et al., 2009).
The preceding positive biological effects, which can be described as an electromagnetic modulation of the cellular and tissue functions, have been obtained at extremely low frequencies and very low magnetic fields. In our in vitro experience, in order to enhance the biological effects, we have utilized a similar electromagnetic wave with a frequency of about 75 Hz (instead of the 50 Hz or 60 Hz of the electric devices), a module of the magnetic field equal to circa 3 mT (i.e. about 60-fold the intensity of the Earth magnetic field), and with a solenoids’ spatial configuration to assure, where the cells are seeded, the maximum homogeneity of the magnetic field.
In particular, we have showed that an ELF-EMF stimulus could elicit a cytoprotective response in human neurons in terms of production of the neurotrophic factor sAPPalpha, promotion of the non-amyloidogenic pathways, and protection against cellular stress and oxidation (Osera et al., 2011) via enhanced expressions of the chaperone heat shock protein HSP70 and the free radical scavenger SOD-1, respectively. On the other hand, we have used the same electromagnetic bioreactor to perform bone tissue engineering experiments: to enhance the in vitro culture of biomaterial scaffolds, the electromagnetic stimulus was applied to increase the cell proliferation and the synthesis of type-I collagen, decorin, osteocalcin, and osteopontin, which are fundamental constituents of the physiological bone matrix (Fassina et al., 2006; Fassina et al., 2007; Fassina et al., 2008; Fassina et al., 2009; Fassina et al., 2010; Ceccarelli et al., 2013).
As a consequence, the aim of the present work is to accomplish a detailed numerical dosimetry inside our electromagnetic bioreactor in order to show the specific and effective physical stimulus transduced by the cells in vitro, not only by describing the local time-dependent magnetic field, but also by discussing the local hydrostatic forces (perpendicular to the cell membranes) and the local shear forces (parallel to the cell membranes), both caused by the magnetic field; in other words, we aim to frame this kind of stimulation not only under an electromagnetic viewpoint, but also under the tensegrity-mechanotransduction theory of Ingber (Mammoto and Ingber, 2010).
Experimental setup of the electromagnetic bioreactor
In order to create a finite element model, some electric measurements were performed. The coils are powered via a Burndy connector, of which two terminals are used for delivering current to the coils. Current and voltage measurements were simultaneously performed as shown in Figure 2.
The preceding measurements were then used to estimate the resistance R and the inductance L of the coils via a custom-made script in Matlab language (The MathWorks, Inc., Natick, MA). In particular, given an applied voltage in the lumped-element RL series circuit, the script identified R and L in a current transient by minimizing an error functional based on the measured current and the estimated one (minimization via the simplex method; error functional tolerance less than 10-4; measurement error of about 2–3%). The estimated coils’ parameters were R = 545 Ω and L = 595 mH. After that, in order to validate the estimated resistance R, a measurement with a digital multimeter was also carried out: R resulted equal to 548 Ω, that is, in good agreement with the estimated value. As a consequence, because of the coils were connected in series, each coil was approximately characterized by L = 298 mH and R = 272 Ω.
Finite element models
In order to simulate the magnetic field produced by the electromagnetic bioreactor, two 3D finite element models were implemented: a linear/static (Problem 1) and a linear/time-dependent (Problem 2). A third problem (Problem 3) was solved to calculate the field effects due to the metallic plates of the incubator where the bioreactor was placed during the in vitro experiments. The third problem was time-dependent and both linear and non-linear materials were considered.
Formulation of the models in terms of dual potentials
If a model subregion contains a ferromagnetic material, the relevant magnetic permeability depends on the unknown field and, for this reason, the Equations 1 and 2 are non-linear and can be solved by an iterative procedure. The method is cost-effective in the case of 3D models because the vector potential is defined only in the conductive subregions, while the scalar potential is defined elsewhere. As a consequence, using a numerical grid to discretise the field domain, there are three unknowns per node in the conductive subregions, whereas one unknown in the other nodes.
We have solved the Problems 1, 2, and 3 by the method implemented in the finite element tool MagNet (version 7, Infolytica Corporation, Montréal, Canada) and running on a 64 bit PC with 8-core CPU and 16 GB of RAM.
Static problem without culture medium (Problem 1)
The total current flowing in the 1/4 coil was assumed equal to the measured peak current of 319 A (as discussed above).
Time-dependent problem with culture medium (Problem 2)
A 3D linear/time-dependent problem was implemented to calculate the magnetic field in the real electromagnetic bioreactor. The current flowing in the 1/4 coil was considered time-dependent as shown in Figure 2. A culture well-plate with real dimensions was included and filled by a physiological saline solution with an electrical conductivity of 1.84 S/m (Figure 3). The problem was solved according to the Equations 1, 2, 3, 4, 5, and 6.
Effects of metallic plates near the electromagnetic bioreactor (Problem 3)
In order to assess our finite element implementation with an internal control, the inductance L and the resistance R of the coils were calculated and compared with the measured ones: L resulted equal to 369 mH in agreement with its measure (L is a function of the magnetic energy Em; Em = 4.69 × 10-3 J in the present model) (Stratton, 1941; Panofsky and Phillips, 1962), whereas R was equal to 278 Ω in very good concordance with the measured value (R is a function of the Joule losses P; P = 7.06 W in the present model) (Stratton, 1941; Panofsky and Phillips, 1962).
B z and B x for y = 0 cm, z = 4.5 cm, and t = 1.36 ms (B y was negligible)
x = 0 cm
x = 3 cm
|ΔB| = |Bi(x = 0 cm)-Bi(x = 3 cm)| [mT]
|ΔB|/Bi(x = 0 cm) [%]
B z [mT]
B x [mT]
B z and B x for y = 4.5 cm, z = 4.5 cm, and t = 1.36 ms (B y was negligible)
x = 0 cm
x = 3 cm
|ΔB| = |Bi(x = 0 cm)-Bi(x = 3 cm)| [mT]
|ΔB|/Bi(x = 0 cm) [%]
B z [mT]
B x [mT]
B z and B y for x = 0 cm, z = 4.5 cm, and t = 1.36 ms (B x was negligible)
y = 0 cm
y = 4.5 cm
|ΔB| = |Bi(y = 0 cm)-Bi(y = 4.5 cm)| [mT]
|ΔB|/Bi(y = 0 cm) [%]
B z [mT]
B y [mT]
B z and B y for x = 3 cm, z = 4.5 cm, and t = 1.36 ms (B x was negligible)
y = 0 cm
y = 4.5 cm
|ΔB| = |Bi(y = 0 cm)-Bi(y = 4.5 cm)| [mT]
|ΔB|/Bi(y = 0 cm) [%]
B z [mT]
B y [mT]
Induced electric currents and induced mechanical forces inside the culture wells
Magnetic, induced electric, and induced mechanical parameters at the side surface of a cylindrical culture well according to the Faraday-Neumann-Lenz and Lorentz laws (z = 4.5 cm)
t = 0.64 ms
Left neighborhood of t = 1.36 ms
Right neighborhood of t = 1.36 ms
B z [mT]
B x [mT]
B y [mT]
|J|, induced current density [mA/m 2 ]
|F|, induced force [pN]
2.7 (maximum compression)
4.9 (maximum traction)
The preceding analytical solution was numerically confirmed and the forces were comparable to those applied in the study of cellular mechanics (Diz-Munoz et al., 2010), so, we could state that the seeded cells were also stimulated with time varying mechanical forces acting onto their plasma membrane at the frequency of 75 Hz. In addition, these forces belonged to planes parallel to the coils’ planes and, consequently, under the tensegrity-mechanotransduction theory of Ingber (Mammoto and Ingber, 2010), they could be discomposed into their perpendicular/hydrostatic and tangent/shear components acting onto the cellular membranes.
It is well known that the physiological functions of cells and tissues can be influenced not only by molecules, but also by mechanical stimuli. In particular, according to the theory of Ingber (Ingber, 2003a; Ingber, 2003b; Ingber, 2006a; Ingber, 2006b; Mammoto and Ingber, 2010), during the in vitro culture inside bioreactors, the mechanical forces may change a specific cell status of force equilibrium, named isometric tensional prestress or “tensional integrity” or “tensegrity”, inducing, via mechanotransduction, biochemical responses that may lead to changes to the transcriptional profile.
Inside our electromagnetic bioreactor, as shown above, the magnetic induction was able to elicit time varying mechanical forces acting perpendicularly or tangentially onto the cell membrane; as a consequence, these forces were able to modulate the cell tensegrity via tensile, compressive, and shear deformations.
Understanding how cells sense and react to mechanical forces has been shown to be crucial. For example, when osteoblasts are subjected to fluid shear stress, stretch-gated ion channels are opened and, due to the increased calcium concentration, numerous biochemical pathways are activated that lead to an enhanced transcription of bone matrix genes (Pavalko et al., 2003; Fassina et al., 2005; Young et al., 2009). In addition, both tension (i.e. traction) and compression affect the cell tensegrity: these forces alter the activities of intracellular signaling molecules such as Rho GTPases, guanine nucleotide exchange factors, GTPase activating proteins, and the MAPK pathway, consequently modulating the expression of transcription factors essential for the homeostasis of bone, cartilage and tooth tissues (Mammoto et al., 2012). Tension and compression may also influence the transcription activity more rapidly when their action is transmitted directly into the nucleus via the cytoskeleton linked to nuclear envelop proteins (Kim et al., 2012).
The biological effects inside our electromagnetic bioreactor could be also explained via the opening of voltage-gated Ca2+ channels in the cell membrane. In particular, the electromagnetic stimulation can raise the net Ca2+ flux in human cells and, according to Pavalko’s diffusion-controlled/solid-state signaling model (Pavalko et al., 2003), the increase in the cytosolic Ca2+ concentration is the starting point for numerous biochemical pathways.
In conclusion, in this study, we have performed a detailed numerical dosimetry inside our extremely-low-frequency electromagnetic bioreactor which has been successfully used in in vitro Biotechnology and Tissue Engineering researches (Fassina et al., 2006; Fassina et al., 2007; Fassina et al., 2008; Fassina et al., 2009; Fassina et al., 2010; Saino et al., 2011; Osera et al., 2011; Ceccarelli et al., 2013). The numerical dosimetry permitted to map the magnetic induction and to discuss its biological effects in terms of electromagnetically induced mechanical forces. In fact, the finite element method was shown to be effective in field calculations for a broad range of engineering (Di Barba et al., 2012) and of bioengineering (Di Barba et al., 2007; Di Barba et al., 2009; Di Barba et al., 2011) applications. So, in the intriguing frame of the tensegrity-mechanotransduction theory (Mammoto and Ingber, 2010), the study of these electromagnetically induced mechanical forces could be, in our opinion, a powerful tool to understand some effects of the electromagnetic stimulation whose mechanisms remain still elusive.
The authors are grateful to Dr. R. Cadossi and Dr. S. Setti, who provided us, generously, the Biostim SPT Pulse Generator (Igea, Carpi, Italy). The authors are also grateful to Infolytica Corporation (Montréal, Canada), who provided us, generously, the MagNet software for the finite element analysis. The research was funded by the INAIL Grants 2010 to LF and FN.
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