examples/example_13_post_processing/main.py
def run_neuron(traj):
    """Runs a simulation of a model neuron.

    :param traj:

        Container with all parameters.

    :return:

        An estimate of the firing rate of the neuron

    """

    # Extract all parameters from `traj`
    V_init = traj.par.neuron.V_init
    I = traj.par.neuron.I
    tau_V = traj.par.neuron.tau_V
    tau_ref = traj.par.neuron.tau_ref
    dt = traj.par.simulation.dt
    duration = traj.par.simulation.duration

    steps = int(duration / float(dt))
    # Create some containers for the Euler integration
    V_array = np.zeros(steps)
    V_array[0] = V_init
    spiketimes = []  # List to collect all times of action potentials

    # Do the Euler integration:
    print('Starting Euler Integration')
    for step in range(1, steps):
        if V_array[step-1] >= 1:
            # The membrane potential crossed the threshold and we mark this as
            # an action potential
            V_array[step] = 0
            spiketimes.append((step-1)*dt)
        elif spiketimes and step * dt - spiketimes[-1] <= tau_ref:
            # We are in the refractory period, so we simply clamp the voltage
            # to 0
            V_array[step] = 0
        else:
            # Euler Integration step:
            dV = -1/tau_V * V_array[step-1] + I
            V_array[step] = V_array[step-1] + dV*dt

    print('Finished Euler Integration')

    # Add the voltage trace and spike times
    traj.f_add_result('neuron.$', V=V_array, nspikes=len(spiketimes),
                      comment='Contains the development of the membrane potential over time '
                              'as well as the number of spikes.')
    # This result will be renamed to `traj.results.neuron.run_XXXXXXXX`.

    # And finally we return the estimate of the firing rate
    return len(spiketimes) / float(traj.par.simulation.duration) *1000
def run_neuron(traj):
    """Runs a simulation of a model neuron.

    :param traj:

        Container with all parameters.

    :return:

        An estimate of the firing rate of the neuron

    """

    # Extract all parameters from `traj`
    V_init = traj.par.neuron.V_init
    I = traj.par.neuron.I
    tau_V = traj.par.neuron.tau_V
    tau_ref = traj.par.neuron.tau_ref
    dt = traj.par.simulation.dt
    duration = traj.par.simulation.duration

    steps = int(duration / float(dt))
    # Create some containers for the Euler integration
    V_array = np.zeros(steps)
    V_array[0] = V_init
    spiketimes = []  # List to collect all times of action potentials

    # Do the Euler integration:
    print('Starting Euler Integration')
    for step in range(1, steps):
        if V_array[step-1] >= 1:
            # The membrane potential crossed the threshold and we mark this as
            # an action potential
            V_array[step] = 0
            spiketimes.append((step-1)*dt)
        elif spiketimes and step * dt - spiketimes[-1] <= tau_ref:
            # We are in the refractory period, so we simply clamp the voltage
            # to 0
            V_array[step] = 0
        else:
            # Euler Integration step:
            dV = -1/tau_V * V_array[step-1] + I
            V_array[step] = V_array[step-1] + dV*dt

    print('Finished Euler Integration')

    # Add the voltage trace and spike times
    traj.f_add_result('neuron.$', V=V_array, nspikes=len(spiketimes),
                      comment='Contains the development of the membrane potential over time '
                              'as well as the number of spikes.')
    # This result will be renamed to `traj.results.neuron.run_XXXXXXXX`.

    # And finally we return the estimate of the firing rate
    return len(spiketimes) / float(traj.par.simulation.duration) *1000
def run_neuron ( traj ) : # Extract all parameters from `traj` V_init = traj . par . neuron . V_init I = traj . par . neuron . I tau_V = traj . par . neuron . tau_V tau_ref = traj . par . neuron . tau_ref dt = traj . par . simulation . dt duration = traj . par . simulation . duration steps = int ( duration / float ( dt ) ) # Create some containers for the Euler integration V_array = np . zeros ( steps ) V_array [ 0 ] = V_init spiketimes = [ ] # List to collect all times of action potentials # Do the Euler integration: print ( 'Starting Euler Integration' ) for step in range ( 1 , steps ) : if V_array [ step - 1 ] >= 1 : # The membrane potential crossed the threshold and we mark this as # an action potential V_array [ step ] = 0 spiketimes . append ( ( step - 1 ) * dt ) elif spiketimes and step * dt - spiketimes [ - 1 ] <= tau_ref : # We are in the refractory period, so we simply clamp the voltage # to 0 V_array [ step ] = 0 else : # Euler Integration step: dV = - 1 / tau_V * V_array [ step - 1 ] + I V_array [ step ] = V_array [ step - 1 ] + dV * dt print ( 'Finished Euler Integration' ) # Add the voltage trace and spike times traj . f_add_result ( 'neuron.$' , V = V_array , nspikes = len ( spiketimes ) , comment = 'Contains the development of the membrane potential over time ' 'as well as the number of spikes.' ) # This result will be renamed to `traj.results.neuron.run_XXXXXXXX`. # And finally we return the estimate of the firing rate return len ( spiketimes ) / float ( traj . par . simulation . duration ) * 1000
Runs a simulation of a model neuron.

    :param traj:

        Container with all parameters.

    :return:

        An estimate of the firing rate of the neuron
Runs a simulation of a model neuron .