From 90cae6c018131e05405c20528eb7c3c385792421 Mon Sep 17 00:00:00 2001 From: Jan Grewe Date: Sun, 22 Jan 2017 13:55:59 +0100 Subject: [PATCH] [project] fixes to input resistance project --- .../input_resistance.tex | 31 +++++++++++-------- 1 file changed, 18 insertions(+), 13 deletions(-) diff --git a/projects/project_input_resistance/input_resistance.tex b/projects/project_input_resistance/input_resistance.tex index 8cff3f4..189aefa 100644 --- a/projects/project_input_resistance/input_resistance.tex +++ b/projects/project_input_resistance/input_resistance.tex @@ -30,18 +30,20 @@ %%%%%%%%%%%%%% Questions %%%%%%%%%%%%%%%%%%%%%%%%% \section*{Estimating cellular properties of different cell types.} -You will analyse data from intracellular \texit{in vitro} recordings +You will analyze data from intracellular \textit{in vitro} recordings of pyramidal neurons from two different maps of the electrosensory lateral line lobe (ELL) of the weakly electric fish -\textit{Apteronotus leptorhynchus}. The resistance and capacitance of -the membrane are typically estimated by injecting hyperpolarizing -current pulses into the cell. From the respective responses we can -calculate the membrane resistance by applying Ohm's law ($U = R \cdot -I$). To estimate the membrane capacitance we need to fit an -exponential function $y = a \cdot e^{(b \cdot x)}$to the response to -get the membrane time-constant $\tau$. With the knowledge of $R$ and -$\tau$ we can estimate the capacitance $C$ from the simple relation -$\tau = R \cdot C$. +\textit{Apteronotus leptorhynchus}. The membrane resistance and the +membrane capacitance are fundamental properties of a neuron that have +a great influence on the coding properties of the cell. They are +typically estimated by injecting pulses of hyperpolarizing current +into the cell. From the respective responses we can calculate the +membrane resistance by applying Ohm's law ($U = R \cdot I$). To +estimate the membrane capacitance we need to fit an exponential +function of the form $y = a \cdot e^{(-x/\tau)}$ to the response to get the +membrane time-constant $\tau$. With the knowledge of $R$ and $\tau$ we +can estimate the capacitance $C$ from the simple relation $\tau = R +\cdot C$. \begin{questions} \question{} The accompanying dataset (input\_resistance.zip) @@ -59,13 +61,16 @@ $\tau = R \cdot C$. a function of time. This plot should also show the across-trial variability. Also plot the time-course of the injected current. \\[0.5ex] - \part{} Estimate the imput resistances of each cell.\\[0.5ex] + \part{} Estimate the input resistances of each cell.\\[0.5ex] \part{} Fit an exponential to the initial few milliseconds of the current-on response. Use a gradient-descent approach to do - this.\\[0.5ex] + this.\\ It is very important to understand the exponential decay + function. If you are unsure, play with the function and understand + how the parameters influence the decay. (Hint: It might be + necessary to transform the data a bit.)\\[0.5ex] \part{} Estimate the membrane capacitance of each cell. Compare $R$, $I$ and $\tau$ between cells of the two segments.\\[0.5ex] - \part{} Optional: use a double exponential and see, if the fit gets better. + \part{} Optional: use a double exponential and see, if the fit improves. \end{parts} \end{questions}