Opening up [I think]
What does it mean, in science, to be open?
I don’t know.
I wrote a while back, that while I endorse the principles of ‘openness‘, I struggle with the issue of ‘how‘. Since then I have been trying to listen and learn. [Or, better said, shut up and listen.] I started trying to see what hurdles I encountered trying to work exclusively on Open Source Software. I joined the Learning4Content course at WikiEducator. I started looking into platforms that would fit my needs as an open lab notebook. I tried to follow the Open Science Summit. I listened hard at sessions at SciFoo Camp. I went to some New Zealand open data discussions. I became an Academic Editor at PLoS ONE. I joined the panel of the Creative Commons Aotearoa New Zealand.
And after several months of ‘listening’ the one thing that keeps popping in my head is:
kubke, you ain’t gonna figure it out by yourself.
The loudest message that I heard is, perhaps, that there is not a single, simple, one-size-fits-all answer, and that it just may come down to fumbling through until we figure it out.
So, I decided to fumble.
I am taking in Summer students this summer to work on a project that I will try to make as ‘open’ as possible.
I am leaning towards a few things:
- I am pretty sure I want to give Mahara a go as a platform for the day-to-day ‘lab’ stuff.
- I am pretty sure I want to regularly put as much as I can into my space in OpenWetWare.
- I am pretty sure I want to try to shift my imaging to Open Source Software (e.g., Osirix, ImageJ, Cell Profiler)
- am pretty sure I want to put the work out there as it is being gathered.
What I am not so sure about is how this will work. It will be a steep learning curve, but one thing that I am hoping is that by giving it a go I may begin to get the answers.
And hopefully some of the smart people out there might give me a hand and help me steer the boat in the right direction.
#SciFoo lightning talk [Reloaded] – Part 3
(Slides 6,7)
I have always been fascinated by the series of studies in electrophysiology that led to our current understanding of how electrical signalling takes place in neurons. And no collection of classical electrophysiology is complete without the 1952 article by AL Hodgkin and AF Huxley on the sodium and potassium currents in the giant axon of the squid.
Saying that Hodgkin and Huxley were brilliant minds would be an understatement. But I was always fascinated by the following phrase in this paper:
‘These results support the view that depolarization leads to a rapid increase in permeability which allows sodium ions to move in either direction through the membrane.’
The reason it fascinates me is that this phrase would not look out-of-place in any modern neurophysiology textbook. But the state of knowledge at the time about how cell membranes were organised was quite different to that of today. Back at that time, cell membranes were thought to be formed by a layer of lipids ‘sandwiched’ between 2 layers of proteins. That meant that for ions to move in and out of the membrane they would have to break through the protein layers and move through the non-aqueous fatty acid layer (something that would be thermodynamically hard for ions to do). Or, something had to ‘open up’ in the membrane to create an aqueous path for the ions to move.
The idea of pores was not foreign to cell biologists at the time, but the demands of Hodgkin and Huxley’s model of ionic movement in neurons could not be easily reconciled with the (then) current model of the cell membrane structure. Hodgkin and Huxley knew ions had to move rapidly and selectively and that the properties of the membrane changed dynamically for this to happen.
In 1972 Singer and Nicolson published a classic model of the cell membrane. In it they propose that rather than ‘sandwiching’ the lipids, proteins are found in the membranes in two forms: as partially embedded proteins, or as intrinsic proteins that traverse the entirety of the cell membrane. It would not take long to see how these intrinsic proteins could form aqueous channels that would allow ions to move from one side to the other of the membrane. That proteins were able to change their shape had already been shown, and so similar mechanisms could be envisioned for the gating of ion channels.
Neurophysiology would never be the same. By 1976 Neher and Sackmann had published their patch clamp method which allowed them to record currents from single channels (and later won them the Nobel Prize), and only two years later Bertil Hille had written and extensive review on ion channels.
It has never been clear to me (or my friends) how much thought Hodgkin and Huxley put into the structure of the cell membrane and how their work fit into the models of the time. But I like to think that they did and chose to trust and follow their data, regardless of the conflicts and lack of sleep that may have raised for cell biologists.
Citations:
- Hodgkin, A. L., & Huxley, A. F. (1952). Currents carried by sodium and potassium ions through the membrane of the giant axon of Loligo. The Journal of physiology, 116(4), 449.
- Singer, S. J., & Nicolson, G. L. (1972). The fluid mosaic model of the structure of cell membranes. Science (New York, N.Y.), 175(23), 720-731.
- Neher, E., & Sakmann, B. (1976). Single-channel currents recorded from membrane of denervated frog muscle fibres. Nature, 260(5554), 799-802. doi:10.1038/260799a0
- Hille, B. (1978). Ionic channels in excitable membranes. Current problems and biophysical approaches. Biophysical Journal, 22(2), 283-294. doi:10.1016/S0006-3495(78)85489-7
#SciFoo lightning talk [reloaded]
#SciFoo lightning talk [reloaded] – Part 2
(Slides 3,4,5)
One of the articles we read in my biophysics class was a 1942 article by Curtis and Cole. At the time, those working on the electrical properties of neurons were in agreement that during the action potential the membrane did not simply ‘depolarize’ (i.e., lost its electrical polarization) but that it rather reverted its potential: during the action potential the inside of the neuron became more positive than the outside.
Researchers were looking at how this happened, and looking for the ions involved in setting up both the resting potential and the action potential.
In 1942 Curtis and Cole reported on an experiment in which they changed the extracellular concentration of potassium and measured the effects this had on resting and action potentials:
What they saw when they measured the amplitude of the action potential was that as they increased the concentration of potassium outside the cell, the amplitude of the action potential was reduced. But they failed to control for what turned up to be an important variable: Sodium. The way they reduced the concentration of potassium was by replacing it with sodium. Their data could be interpreted in two ways: that the amplitude of the action potential was decreased as potassium concentration was increased or that the amplitude of the action potential was decreased as sodium was decreased. This may not have been a huge oversight on their part given the state of knowledge of the time, but turned out to be a big mistake (and one that they should have controlled for).
A few years later, Hodgkin and Katz published a paper in which they showed that the second explanation was the correct one.
In 1949 they showed that the ion carrying the current during the action potential was indeed sodium, something that would become known as the sodium hypothesis. Future work by Hodgkin and co-workers would define the mathematical functions that described the electrical properties of neurons, models that continue to be used today.
In 1963 Hodgkin shared the Nobel prize with his collaborator Andrew Huxley and John Eccles. My friends from the biophysics course always wondered how things would have turned out had Curtis and Cole realized the effect of sodium.
Citations:
- Curtis, HJ and Cole KS (1942) Membrane Resting and Action Potentials from the Squid Giant Axon. Journal of Cellular and Comparative Physiology Vol 19 (2) 135-144
- Hodgkin AL and Katz B (1949) The effect of Sodium Ions on the Electrical Activity of the Giant Axon of the Squid. J. Physiol. 108, 37-77 (PMID: 16991839)
#SciFoo lightning talk [reloaded]
#SciFoo Lightning talk [reloaded] – Part 1
At SciFoo I got a chance to give a lightning talk. These are 5 minute talks, similar to Ignites and PechaKuchas. It is fair to say that is was nerve-wracking! And 5 minutes seem like an eternity when you are that nervous!
But I am rehashing it here as an extended version of the 5 minutes, 2 or 3 slides at a time, over several posts.
[Slides 1 and 2]
When I started University in Argentina, there wasn’t a neuroscience programme. (I had actually gotten interested in science after reading the microbe hunters as a kid, so I should have really been a microbiologist.) But neuroscience was taught pretty much in every course, and I became fascinated with it, and by the middle of my 6 year undergraduate I had joined a research group to study brain development.
At about that time, I took a course in biophysics. One of the best I think I took and loved it. It was common back then that all courses had several hours a week dedicated to reading and discussing (and dissecting!) the primary literature. But biophysics did something different. We didn’t just read *the* papers, but also all of the work that led to those significant papers. And the results were discussed taking into account the historical context during which they were obtained.
This was really interesting for two reasons: First, we were not only learning a discipline but also the evolution of ideas within the discipline: the evolution of scientific thought. Second, it gave me an appreciation of the treasures that were hidden in old volumes of journals.
I think I owe to this course my love for the history of science, and my eagerness to blow off the dust of old journal covers in search of science gems. In the process, I have come to realise that many of what we may consider new or groundbreaking results, are actually answering questions that were posed long ago.
Throughout the history of science I find heaps of questions that remain unanswered waiting for the development of technology that lets scientists take the next step. Some of these questions resurface, many times without reference to the original ideas, some remain buried waiting to be rediscovered by someone willing to browse through old archives and willing to reexamine them with modern tools.
I decided to talk about this because this is something I love about science: that serendipitous marriage between scientific ideas and technological development, which I also think aligns with the spirit of SciFoo.
How to build a [water] brain
Whenever I try to teach some aspects of neuronal integration in class, I run into trouble, since most of the neuronal properties are defined by mathematical formulae that describe the electrical properties of neurons that are sometimes difficult for the students to grasp. Without a basic knowledge of electricity, it is hard to build a conceptual image of what neurons are doing.
Or is it?
I was invited to talk about the brain to a group of 9-11 year old pupils in a primary school in the North Shore yesterday, when I thought it might be fun to try to build neurons and discover how they worked. So, here is my water neuron:
It turns out, this little water neuron (which can be built with pretty much household items) has a lot to show about the passive properties of neurons.
Synaptic currents:
The pipette dropper was used to inject [current] water into the different dendrites. Because of the properties of the dropper, there is a limit to the amount of current that can be injected at a given time, and the injection of current is not instantaneous but has a time course that is analogout to the time course of the synaptic potential.
Spatial and temporal integration:
Current can be injected in one or more dendrites with different time patterns. Injecting into all dendrites at the same time, or into one or more dendrites at different time intervals provides a good idea of how the output of the neuron is shaped by spatial and temporal integration.
Threshold:
By tilting the ‘soma’ to different degrees the amount of current needed to be injected into the dendrites to allow for an output of the axon will increase. Therefore, one can build neurons with different thresholds and see how that affects the output of the neuron.
Leak currents:
One can poke tiny holes into the soma so that some of the current injected into the neuron leaks out. Combining this with changing threshold and the temporal patterns of injection into the dendrites is a good way of showing how temporal and spatial integration work in different ways to produce an output through the axon. One can also put some leaks into the axon, and ‘myelinate’ it with saran wrap to show the insulating properties of the myelin sheath.
Although this ‘water neuron model’ cannot illustrate the active properties of the neurons, it does contribute to an intuitive construct of how currents may be acting in individual neurons. The different neurons can be connected to form a circuit, and then one could examine how the output of the circuit is affected by changing things likethreshold, leak and number of inputs into individual neurons.
Well, it was fun. I may give this a go in my next neuro class at Uni.











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