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Wikipedia says that

Dynamic instability refers to the coexistence of assembly and disassembly at the 'ends' of a microtubule.

but Karp's Cell Biology, 7th edition says

Dynamic instability is an inherent property of microtubule itself, more specifically, of the plus end of the microtubule.

I was of the opinion that the GTP bound to the minus end does not hydrolyse and so no depolymerisation take place at the minus end.

But again from The Cell: A Molecular Approach. 2nd edition I found that

treadmilling is a dynamic behavior in which tubulin molecules bound to GDP are continually lost from the minus end and replaced by the addition of tubulin molecules bound to GTP to the plus end of the same microtubule.

The concept I have developed so far is completely shattered by this treadmilling thing. Can somebody explain,

i) Whether GTP remains attached to the minus end?

ii) Whether depolymerisation occurs at the minus end?

iii) If depolymerisation does not occur, then is treadmilling a special condition?

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  • $\begingroup$ I think the reason why the literature contain these contradictions is that all these phenomena do happen, but in most conditions the dynamics is strongly dominated by the plus-end dynamics (growth and catastrophies), leading most research to disregard minus ends completely. $\endgroup$ – Joce May 10 '16 at 11:12
  • $\begingroup$ Treadmilling, AFAIK, happens in actin filaments not tubulin. $\endgroup$ – WYSIWYG May 10 '16 at 11:24
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    $\begingroup$ @WYSIWYG no, it happens in microtubules. See this. $\endgroup$ – MattDMo May 10 '16 at 13:07
  • $\begingroup$ @MattDMo Interesting. The textbook that I used to read never mentioned that even though the article you mention is quite old. I found a more recent article on this topic. Thanks for correcting me. $\endgroup$ – WYSIWYG May 10 '16 at 15:58
  • $\begingroup$ @WYSIWYG no problem. I found that article while researching an answer I've decided not to write - seems the idea of treadmilling has been around for a long time. $\endgroup$ – MattDMo May 10 '16 at 18:23
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Often microtubule (MT) dynamics and actin dynamics are taught side by side, which can be quite confusing as MTs display unique characteristics relative to actin filaments. Indeed, treadmilling is an in vivo behavior primarily associated with actin, while dynamic instability characterizes MT growth. But why?

Both actin filaments and MTs are "sided" (polar), with actin having barbed- and pointed-ends and MTs having plus- and minus-ends. This polarity emerges from two properties: 1) the energetic state of the individual monomers that make up the filament and 2) the rate of growth.

For actin, the barbed-end is compromised mostly of ATP-actin (high energy), while the pointed-end is made up of ADP-actin (low energy). This composition preferentially adds new ATP-monomers to the ATP-rich barbed-end, yielding a faster rate of growth than at the pointed-end. Disassembly at the pointed-end occurs more readily as ATP-actin is converted to lower energy ADP-actin. Treadmilling occurs when the rate of assembly at the barbed-end is equal to the rate of disassembly at the pointed-end (Pollard and Borisy, 2003).

Similarly to actin filaments, MTs are polar, with their plus-ends made up of GTP-tubulin monomers and GDP-tubulin concentrated at their minus-ends (Desai and Mitchison, 1997). Unlike actin filaments, which can form sporadically almost anywhere in the cell (Pollard and Borisy, 2003), MTs are initiated at what we call a microtubule organizing center, or MTOC (Kollman, 2011).

The bulk of MTs within the cell are attached to the MTOC through their minus-ends, though there are unattached sub-populations. Both in vivo and in vitro data indicate that growth and shrinkage at the minus-ends does occur, but that the rates are slow relative to those occurring at the plus-ends (Hendershott, 2014). In these instances, MTs can undergo treadmilling in a manner similar to that as actin and this behavior is readily observed in vitro (Waterman-Storer, 1997). Recent studies have suggested that MT minus-ends are under tight regulation in vivo, likely limiting their dynamics (Akhmanova, 2015). Therefore, MT growth and shrinkage primarily occurs at thee plus-ends. Enter dynamic instability.

MT plus-ends undergo a cyclical process of growth and shrinkage known as dynamic instability (Mitchison and Kirschner, 1984). The key to this process is the difference in shape between GDP-tubulin and GTP-tubulin (Buey, 2006). One can imagine GTP-tubulin as a rectangle, with perfectly straight lines connecting its angles. On the other hand, GDP-tubulin has a small bend in the center of one of its long ends.

As a MT grows, GTP-tubulin is added to the plus-end forming a "GTP cap." The role of this cap is to counteract the inherent desire of GDP-tubulin to bend outward, thereby forming a straight filament and ensuring continued growth of the MT (Desai and Mitchison, 1997). However, the MT will lose its cap when the rate of GTP-tubulin addition drops below the rate of GTP to GDP conversion, thereby exposing GDP-tubulin. This event characterizes the "catastrophe" stage of dynamic instability (Mitchison and Kirschner, 1984). The shape of GDP-tubulin is no longer constrained in this stage, and instead, bends outward causing rapid disassembly of the MT. Because the cell is chock full of GTP-tubulin, recovery of the GTP cap rapidly occurs and the MT re-enters productive growth. This cycle of growth-catastrophe-recovery is the hallmark of MT dynamic instability.

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  • $\begingroup$ Answer is mostly fine, but, as per the earlier comments on the original post, MTs can become detached from the MTOC, and then undergo treadmilling. $\endgroup$ – AJK Dec 29 '17 at 1:40

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