Basic computational models in neuroscience Flashcards

1
Q

Why make computational models? Isn’t neuroscience complicated enough already?

A

The goal of computational models is to make our life easier: we can easily test a hypothesis in a system that is way less complicated than the real brain.

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2
Q

How does making computational models make our lives easier

A

We can model crucial elements to make simple predictions about process. If our hypothesis has a red flag, we’ll see it quickly without having to go all the way in the training/ surgery/ recording/ analysis cycle. They can also help us to spot things that we missed from the data, and refine our experimental design.

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3
Q

Why is learning to model a good idea even if you want to be a ‘pure’ researcher?

A

Experiment and model are already combined in most cutting-edge research. Even if you plan to be a ‘pure’ experimentalist, knowing about models will make your life much easier when you decide to collaborate with a modeller.

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4
Q

Describe the research Jorge described as a practical example of modelling

A

A recent experimental study in our group showed, using ferrets, that different (low/high) levels of awareness lead to different oscillatory patterns in several brain areas. Changes in awareness may lead to modulations of visual and parietal cortices from frontal cortex, but technical limitations prevented us to precisely identify, in our experiment, the circuits responsible for these effects.

For this reason, we built a computational model to reproduce the patterns of oscillatory brain activity. Among other things, the model predicted which anatomical connections (from the hundreds of possible options) may produce such activity patterns.

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5
Q

Are computational and theoretical models suited for more molecular process or systems processes?

A

Computational and theoretical models can be used to describe neural systems at many different scales –from biophysical processes inside synapses to full brain dynamics. They also embrace different approaches, from highly detailed biophysical descriptions to more abstract models.

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6
Q

What could be inferred from differences in the model predictions and the observed data?

A

Whatever the shape and colour, computational models can use existing knowledge and data to deliver predictions, which then can be used in the design of present and future experiments.

Differences in model predictions could suggest additional mechanisms which are not accounted for in the model. Parameter values and interactions can then be tweaked to become closer to the predicted data.

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7
Q

What else can be derived from models, closely related to predictions?

A

Models can also be used to make postdictions (Abbott, 2008): to explain known phenomena from a different perspective, or to integrate previous findings into a larger, coherent formal framework. Postdictions can tell you if your assumptions are sufficient

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8
Q

From a more methodological point of view, computational models in neuroscience come from different mathematical branches. Name these (3)

A

1) The statistical approach (for example, Bayesian neural models)

2) The computer science approach (such as artificial neural networks, deep learning…);while artificial neural networks are not the same, they can behave like real networks

3) The biophysical approach (such as biophysical models of neurons, tools coming from physics and complex systems science)

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9
Q

Which of these three mathematical branches are we most concerned with? What is it most concerned with?

A

Biophysical; based on what actually happens in the model. The level of detail is up to you

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10
Q

Membrane potential arises from a separation of positive and negative charges across the cell membrane. Where do these excess charges largely stem from?

A

Excess charges are concentrated directly at the membrane (in- and outside). Each excess is only a tiny fraction ot the total number of ions in/outside the cell

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11
Q

What is the use of having a membrane potential? (high energy demand)

A

• rapid electrical signalling possible; rapid transport of signals through CNS

• You only have to open “the gates” to use ion gradients to change the voltage

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12
Q

How do you calculate the membrane potential?

A

Vm= V in– V out
intracellular voltage - extracellular voltage

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13
Q

What is meant by the resting potential and what is the typical voltage?

A

•Resting membrane potential: “undisturbed” state
•Usually RMP ~ -85 to -60 mV. Thus, excess negative charge inside cell at rest

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14
Q

What is meant by polarisation?

A

Any potential difference V in– V out that is different from zero. In practice: Vm is negative

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15
Q

What is meant by de-polarisation

A

loss of (negative) polarization, so Vm moves towards 0 mV

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16
Q

What is meant by hyper-polarisation?

A

Extra (negative) polarisation, so Vm moves away from 0 mV, becomes more negative than rest

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17
Q

What is meant by the direction of current flow? I.e if ions were moving in and out of the cell, which direction would the current be flowing?

A

Direction of current flow is defined as direction of net movement of positive charge e.g. “inward current”: net movement of + charge into cell (or: negative charge leaves cell to outside!)

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18
Q

Name and describe the two driving forces at the membrane

A

Electrical driving force: depends on membrane potential (+ions attracted to inside)

Chemical driving force: depends on concentration difference of ion across membrane

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19
Q

What is meant by an equilibrium potential?

A

For a given molecule, what the membrane potential must be at for them to be at their concentration potential. Orin other words:

Equilibrium potential (=reversal potential): the potential at which the electrical driving force equals the chemical (diffusional) driving force

20
Q

Give the equilibrium potentials for the four main ions involved in the whole transmembrane community

A

ion | Inside Mm | Outside Mm | Eq pot

Na+ 50| 440| +55mV|
Cl - 52| 560| -60mV|
K + 400| 20| -75mV|
Organic ions (A-) 385| ~0| –|
Ca 2+ 0.0001| 2| +120 mV|

21
Q

What does the Nernst equation tell us?

A

It gives the equilibrium potential for each ion

22
Q

Give the Nernst equation and what each variable represents

A

Ek = ( RT / zF ) ( ln [K+]out / K+ in )

R: gas constant
T: temperature (Kelvin)
z: ion valence
F: Faraday constant

RT/F ~ 25 mV at 25 oC

23
Q

What is meant by the faraday constant and what is it for potassium?

A

In physical chemistry, the Faraday constant, denoted by the symbol F, is the electric charge per mole of elementary charges. It represents the amount of electric charge carried by one mole, or Avogadro’s number, of electrons.

24
Q

What do we assume in the Nernst equation? (2)

A

We assume that pumps establish a gradient in the 1st place, and that membrane is somewhat permeable to K+ ions (for calculating K+)

25
Q

Describe the situation with multiple ion species (Na+ and K+) from rest to modest depolarisation and further

A

•At rest, electrical and chemical equilibrium is maintained.
•The opening of Na+ channels (stimulus) drives Na+ ions inside the cell, depolarising the cell membrane.
• As a reaction to this depolarization, K+ electrical forces become weaker and K+ flows out of the cell, restoring balance.

26
Q

If concentration gradient of K+ is present, when does equilibrium (i = 0) arise?

A

If concentration gradient of K+ is present, equilibrium (i=0) only arises if potential is negative

27
Q

What is the Goldman-Hodgkin-Katz equation used for and how does it do it?

A

Membrane potential is determined by a weighted sum
of equilibrium potentials, where weight is determined
by the relative permeability of the ion

28
Q

Give the Goldman-Hodgkin-Katz equation and name the variables

A

Vm=R.T / F ln( ( Pk .[K+]out + Pcl . [Cl-]in ) / ( Pk .[K+]in + Pcl . [Cl-]in ) )

R: gas constant
T: temperature (Kelvin)
F: Faraday constant
Pk: Permeability of K

29
Q

Why is temperature important in these models

A

It is indicative of the amount of movement (Kinetic energy?) of the ions and therefore the diffusion process

30
Q

How is the electrical driving force represented in neural depictions as circuits?

A

electrical driving force represented by “battery” symbol.

31
Q

How is current-voltage relation calculated/ represented mathematically?

A

Through Ohm’s law:
Ik= γ*(Vm-Ek)

Where Ik is the current generated by an ion equation; shows the relationship between this and the membrane

32
Q

How would you describe the relationship between current and voltage?

A

Current-voltage plot is linear (ohmic)

and i=0 if V=0 in absence of ionic gradient

33
Q

How are ionic channel groups represented as electric circuits?

A

Several K+channels situated in parallel: lump into one
conductance. conductance placed in series with battery (=electromotive force). Different types of channels in parallel: different equilibrium potentials => different battery-conductance combinations.

34
Q

What is the Hodgkin-Huxley model meant to model? How was this model formulated (methods)?

A

Electrophysiological (voltage clamp) recordings of the giant axon of the squid. These recordings were
followed by a computational model of the ionic contributions to the membrane potential. The model provided a biophysical description of the generation of action potentials (APs).

35
Q

What are the Hodgkin-Huxley model assumptions?

A

• Two types of ion channels (Na+ and K+) regulate the membrane potential dynamics of the cell.

• “Active membrane”: the ion channel conductance varies as a function of time and voltage.

36
Q

What resisitences did Hodgkin and Huxley consider for their model and how accurate were they?

A

They considered three different resistances in their model; Na, K and C, passive resistances. They assumed chloride had a significant role in generating individual action potentials. While it does play a role it is not a fundamental part as suggested. You can test your model to reveal things like this

37
Q

What does C represent in these circuitry models?

A

Capacity: How much energy the neuron is able to store

38
Q

When is an electric current generated in the neuron?

A

If the membrane potential is different to the charge of an ion then a current is generated. If not they are satisfied

39
Q

Describe two different ion channels as described by the hodgkin huxley model

A

Potassium channel:
• The K+ channel has four similar subunits
• Each subunit can open or close independently.
• The channel is open if (and only if) all four subunits are open.

Sodium channel:
• The Na+ channel has three “fast” subunits and one “slow” subunit.
• Each subunit can open or close independently.
• The channel opens if all four subunits are open. In practice, the slow subunit works as an inactivation mechanism due to its particular “inverse” dynamics. This means they tend to open and close at opposite times but small windows of opportunity.

40
Q

Break down the Hodgkin-Huxley model without the inclusion of ion channel dynamics

A

the extracellular current (Iext) is the sum of the other currents (Ina + Ik + IL + Ic). The current is given by the ion conductance (g) multiplied by the membrane potential (difference in voltages; Vx - Vna ). E.g the sodium current is given by (Ina = gna (V- Vna )). The current of the capacitor is calculated by the derivative of the capcitor (C dv/dt). These are then summed to get the model:

Iext = gna (V- Vna ) + gK (V- VK ) + gL (V- VL ) + C dv/dt

Which can be rewritten as

C dv/dt = gna (Vna- V ) + gna (Vk- V ) + gna (VL- V ) + Iext

41
Q

Break down the inclusion of the ion channel dynamics in the model

A

If we consider:
• The probability of one subunit being open as 𝒏
• The probability that the channel is open as 𝒏^4
• The maximal K+ conductance for all channels open as
𝒈𝑲
Then the K+ conductance is given by:
𝒈𝑲 . 𝒏^4 (Vk - V )

If we consider:
• The probability of a fast subunit being open as 𝒎
• The probability of a slow subunit being open as 𝒉(controls inactivation)
• The probability that the channel is open as 𝒎𝟑𝒉
• The maximal Na+ conductance for all channels open as “𝒈𝑵𝒂
Then the Na+ conductance is given by:
𝒈𝑵𝒂 . m^3 . h (V𝑵𝒂 - V )

So the equation becomes:
C dv/dt = 𝒈𝑵𝒂 . m^3 . h (V𝑵𝒂 - V ) + 𝒈𝑲 . 𝒏^4 (Vk - V ) + gna (VL- V ) + Iext

42
Q

How are the dynamics of the K+ and Na + subunits given?

A

Tn dn/dt = -n + n∞ (activation of potassium)
Tm dm/dt = -m + m∞ (activation of sodium)
Th dh/dt = -h+ h∞ (inactivation of sodium)

Here, the variables 𝜏&,(,)and [𝑛,𝑚,ℎ]*depend on the membrane potential V (and therefore, also vary on time with V).

43
Q

What do these subunit equations interact to give?

A

These equations interact to generate action potentials in the model i.e the depolarisation peak and the after-spike hyper-polarisation (see in docs)

44
Q

Give the time course of an AP according to the HH model

A

1) Initial depolarisation needed
2) Na+channels open
3) They depolarise the membrane further (not in V-clamp)
4) More Na+channels open => more depolarisation (positive feedback loop!)
5) K+channels start to open: repolarising effect
6) Na+channels inactivate
7) K+conductance outlasts Na+ conductance: hyperpolarisation

45
Q

Give four examples of how different types of ion channels can have a variety of cell firing behaviours

A

(A) N. tractus solitarius: hyperpolarize cell tonically => depolarising pulse triggers spikes, but delayed
due to A-current (carried by potassium ions)

(B) Thalamic neurons: hyperpolarise cell tonically => depolarising pulse triggers burst of spikes,
due to low-threshold Ca-current

(C) Thalamocortical relay neuron: spontaneous burst of action potentials, due to:
1) H-current, switches on during hyperpolarisation but acts to depolarise cell;
2) low-threshold Ca-current, triggering Na-action potentials
3) repolarisation due to shut-down of H- and Ca-current, versus resting K+ currents

D) Neurotransmitter ACh closes M-current channels in sympathetic ganglion (ANS)
M-current is a K+current that slowly opens upon depolarisation;
cell can fire only one spike when depolarised; ACh => closes M-current => more spikes