Physical principles of nanofiber production Theoretical background (3) Electrical bi-layer

1 / 27

# Physical principles of nanofiber production Theoretical background (3) Electrical bi-layer - PowerPoint PPT Presentation

Physical principles of nanofiber production Theoretical background (3) Electrical bi-layer. D. Lukáš 2010. Electric bi-layer. Boltzmann equation Poisson Equation Debye ‘s length.

I am the owner, or an agent authorized to act on behalf of the owner, of the copyrighted work described.

## PowerPoint Slideshow about 'Physical principles of nanofiber production Theoretical background (3) Electrical bi-layer' - abrienda-flores

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript

### Physical principles of nanofiber productionTheoretical background (3)Electrical bi-layer

D. Lukáš

2010

Electric bi-layer

Boltzmann equation

Poisson Equation

Debye‘s length

Electric bi-layer is another object with nano-dimension in electrospinning. Referring to second part of (Figure 3.2), one may consider a plane surface of polymer solution, containing ions both in polymer macromolecules and their solvent. Let the ion valence be considered as one for simplification and e denotes the elementary electric charge. In electrospinning, electric potential, 0, at the liquid / polymer solution surface is generated by the electrostatic field in between two electrodes.

Fig. 3.2:A cloud of ions (3) in a polymer solution (4) is induced by an electrostatic field between a collector (5) and an electrode (6). The thickness of the ionic atmosphere at the vicinity of the solution surface is called the ‘Debye’s length’, D.

Figure 3.2: A charged colloid particle - (1): A positively charged colloid particle is surrounded by a cloud of negative ions - (2). Potential j is quenched with increasing distance, x, from the surface.

An electrospinner, from the point of view of ion distribution, resembles the situation in the vicinity of a charged colloid particle. The similitude is indicated in (Figure 3.2), where the collector plays the role of organised groups of charges on colloid particles. The only difference between colloid particle and electrospinner is the gap coined by the space between the collector and liquid surface.

+

+

+

+

+

Prodleva!!!

D

‘Debye’s length‘

The electric potential, , having the value, o, at the solution surface, decreases with the depth in the solution as quenched by the ion distribution in the solution surface layer, i.e. as quenched by induced charges that shield the electric field towards the bulk of the solution.

For the sake of simplification relative parallel placement of both the collector and the solution surface will be considered henceforth. The parallel configuration gives rise to simple symmetric equipotential surfaces that are parallel to them too. So, the electrostatic potential (x) can be considered as the function of the only variable x, which is the distance measured along the axis, perpendicular to the collector and solution surfaces, with its origin located at the solution surface, pointing to the polymer solution bulk.

N… Number of space cells

n… Number of particles

Configuration vector

Boltzmann

equation

Non-interacting free particles

1 nm

100 km

To derive - x relationship, one has to start with a rule that governs the distribution of ions acted upon by the external electrostatic field as well as the field generated by ions themselves. The probability, p(x), of finding an ion at a particular depth, x, in the solution depends on its energy

through the Boltzmann equation

where kB is the Boltzmann constant, and T being the absolute temperature in Kelvin.

Kittel and Kroemer [29]

The electrolyte for this moment comprises two kinds of ions of opposite charge +e and –e. Their volumetric concentrations are:

Wheren0 is the concentration of charges, when the solution is not affected by any external electrostatic field. The concentration n0 is universal for both the ions as the solution is electro-neutral as a whole.

The charge distribution is also governed by the one-dimensional Maxwell’s first law of electrostatics, generally expressed in the form of Poisson Equation with the potential gradient

having the nonzero component along the x axis only. Mathematically, the particular shape of the Equation (3.7) for this case becomes:

(3.10)

(3.11)

Nonlinear differential equation!!!

‘Debye’s length‘

D

D

several units or tens of nanometres

Conductive body (liquid body)

+

Intensity inside conductive body is zero.

Intensity vectors (on the surface of conductive body) are perpendicular to body surface.

Surface of body is equipotentials.

With respect to electrospinning, one can underline that Debye’s length is the thickness of the ion cloud at the vicinity of the liquid surface.

As this thickness in conductive liquids is generally not more than several units or tens of nanometres, the external electrostatic field is able to influence directly only the molecules that are close to the liquid surface.

It is convenient to underline on this place that the electrostatic field grasps during electrospinning preferably the surface layer of the liquid where net charges are enormously concentrated.

The surface husk of the liquid is transmitted into a jet that is hence supposed to be highly charged too.