project:
POLYMers

«Querverbindungen in Polymer Netzwerken »

–Mussel threads and spaghetti in the computer

Here you will find the proposed materials framed in a  coloured box . The code next to it identifies each item (foto, video, etc.) individually. You will need this code to fill in the form. Additionally, you can have an overview of the materials from all research groups at matter.soundsof.net/materials.

One can think of polymers as being long chain-molecules-a bit like spaghetti. In our case the spaghetti are even cooked, because the polymers are very flexible. Similar to a pile of spaghetti also a pile of polymers does not possess any mechanical stability, unless one ”glues” different parts of the spaghetti or polymers together. In this way one creates a continuous network out of the pile of independent threads. This network now possesses some mechanical stiffness and is not as easily deformable as the original threads. It is possible to use this process of cross-linking to specifically tailor the mechanical properties of the polymers.

 

Biological materials like bone, wood, silk or mussel-threads use cross-links that are relatively weak in strength, but are reversible. This means that a ruptured cross-link can re-form after the load is released. This mechanism provides some kind of self-healing. In a standard theoretical description a cross-link is described as an additional bond between two parts of one or two polymers. In the picture of the spaghetti this means that the cooked, sticky pasta are glued together at the positions where the pasta touches. Nevertheless, in nature a cross-link is often formed between more than only two partners. Using computer-simulations we aim at closing this gap in the theoretical description by explicitly investigating the influence of the number of contacts on the mechanical performance of cross-linked polymers.

The picture shows a network made from differently colored polymers (spaghetti) that is held together by cross-links, made of three contacts. The cross-links are depicted by black balls and connecting bars. An important question to answer is how this network deforms, when one changes the size of the simulation box. Other questions that are investigated are how the deformation changes (i) if one changes the length of the spaghetti or (ii) if one switches from cooked to un-cooked spaghetti, i.e. if the polymers are not flexible like a thread, but stiff like un-cooked pasta.

Mytilus with Byssus

Brocken Inaglory  [Poly2]

The picture shows a mussel that uses fine threads, i.e. its byssus, to adhere to a stone. These threads have to resist the high forces stemming from the waves and tides. The byssus threads are perfectly adapted to this task : they are relatively stiff, they can be extended up to the double of their original length without rupture, they possess a wear-resistant outer coating, they show self-healing and they naturally adhere under water. Responsible for these extraordinary properties are metal-coordination bonds that cross-link this material. These cross-links are most stable, when they form connections between three different parts of the polymers.

Zebra Mussel [Poly3] Negative consequences of mussel adhesion 

The pictures shows the negative consequences of mussel adhesion. In the process of biofouling these materials adhere on wetted materials. Especially on ship hulls this is unwanted, because fouling significantly increases drag and, thus, increases fuel consumption. Due to the high adhesion strength of marine mussels cleaning is complex, time consuming and consequently expensive. A possible medical application is to implant a drug depot in arteries to treat arteriosclerosis . Currently, one main problem is to maintain the depot in place resisting the strong forces due to blood flow. A more detailed understanding of the adhesion process and the mechanics of marine mussel byssus threads is consequently of technological as well as medical importance.

The model

 

Schematic of cross-linking a single chain with a metal-ion

The picture shows a schematic of cross-linking a single chain with a metal-ion. The ion cross-links three parts of one or of different polymers. The number of cross-links changes the mechanical behavior of the chain. Where the number of cross-links is large, the deformation is small and where the number of cross-links is low, the deformation is high.

Screenshot of the computer code  [Poly5]

The picture on the left shows a screenshot of the used computer code. The detail shows part of the sub-routine that is used to calculate the energetic contribution of the cross-links. The used methods are Monte-Carlo simulations. This method relies heavily on the use of random numbers, quite similar to playing roulette in the world-famous casino of Monte Carlo. This analogy gave the game its name.

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Displacement

 

Simulation of the force needed to pull different kinds of cross-links. The black symbols show a polymer where a cross-links connects three parts of a polymer, while the grey points correspond to cross-links that form solely between two partners.

 

The graph suggests a different mechanical behaviour: in the case of the three-fold coordinated structures (black) the curve is smoother, while the maximum force is smaller.

A typical result of a simulation. A cross-linked polymer is pulled in the computer and the force needed to do so is calculated. The figure shows two polymers that have the same number of cross-links, but where the cross-links are of different type. The black symbols show a polymer where a cross-links connects three parts of a polymer, while the grey points correspond to cross-links that form solely between two partners. The different mechanical behaviour is obvious. The curve is smoother for the three-fold coordinated structures, while the maximum force is smaller. This behavior will prove beneficial in network systems, because peak loads stemming from two-fold coordinated structures will be attenuated.

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Trajectory

 

Deformation of a polymer with
exactly one cross-link that connects
three parts of the polymer

The movie shows the deformation of a polymer with exactly one cross-link that connects three parts of the polymer. This cross-link consists of three bonds. During deformation first the two outermost parts of the polymer are stretched. Doing so the bond connecting the two most distant parts of the polymer fails. The two remaining bonds are not very stable and soon a single remaining bond between two parts of the polymers forms. It is this two-stage process of failing that makes a significant difference between three- and two-fold coordinated cross-links. For the latter, the rupture of one bond means the total loss of mechanical stability.

Research team

 

Principal Investigator: Dr. Markus A. Hartmann

 

 - H. Shabbir 

Source Material - Attribution

[Poly1]  Network © Markus Hartmann, Universität Wien

[Poly2]  Brocken Inaglory, via Wikimedia Commons  [CC BY-SA 3.0]

[Poly3]  Zebra mussel photo by NOAA/GLERL (Public Domain) 

[Poly4]  The model © Shabbir et al, 2017, New Journal of Physics, in press. [CC BY 3.0]

[Poly5]  Program code © Markus Hartmann, Universität Wien

[Poly6]  Displacement © Markus Hartmann, Universität Wien

[Poly7]  Trajectorie © Markus Hartmann, Universität Wien

 
 
 
 

Polymer network

 

Network made of differently coloured 

polymers (Spaghetti).The cross-links are depicted by black balls and connecting bars.

   

     

                          (Click image to enlarge)

 
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