rxdmath.acos · rxdmath.acosh · rxdmath.asin · rxdmath.asinh · rxdmath.atan · rxdmath.atan2 · rxdmath.ceil · rxdmath.copysign · rxdmath.cos · rxdmath.cosh · rxdmath.degrees · rxdmath.erf · rxdmath.erfc · rxdmath.exp · rxdmath.expm1 · rxdmath.fabs · rxdmath.factorial · rxdmath.floor · rxdmath.fmod · rxdmath.gamma · rxdmath.lgamma · rxdmath.log · rxdmath.log10 · rxdmath.log1p · rxdmath.pow · rxdmath.radians · rxdmath.sin · rxdmath.sinh · rxdmath.sqrt · rxdmath.tan · rxdmath.tanh · rxdmath.trunc · rxdmath.vtrap

Mathematical functions for rate expressions

NEURON’s neuron.rxd.rxdmath module provides a number of mathematical functions that can be used to define reaction rates. These generally mirror the functions available through Python’s math module but support rxd.Species objects.

To use any of these, first do:

from neuron.rxd import rxdmath

Example:

degradation_switch = (1 + rxdmath.tanh((ip3 - threshold) * 2 * m)) / 2
degradation = rxd.Rate(ip3, -k * ip3 * degradation_switch)

For a full runnable example, see this tutorial which as here uses the hyperbolic tangent as an approximate on/off switch for the reaction.

In each of the following, x and y (where present) are arithmetic expressions comprised of rxd.Species, rxd.State, rxd.Parameter, regular numbers, and the functions defined below.

rxdmath.acos()

Inverse cosine.

Syntax:

result = rxdmath.acos(x)
rxdmath.acosh()

Inverse hyperbolic cosine.

Syntax:

result = rxdmath.acosh(x)
rxdmath.asin()

Inverse sine.

Syntax:

result = rxdmath.asin(x)
rxdmath.asinh()

Inverse hyperbolic sine.

Syntax:

result = rxdmath.asinh(x)
rxdmath.atan()

Inverse tangent.

Syntax:

result = rxdmath.atan(x)
rxdmath.atan2()

Inverse tangent, returning the correct quadrant given both a y and an x. (Note: y is passed in before x.) See Wikipedia’s page on atan2 for more information.

Syntax:

result = rxdmath.atan2(y, x)
rxdmath.ceil()

Ceiling function.

Syntax:

result = rxdmath.ceil(x)
rxdmath.copysign()

Apply the sign (positive or negative) of expr_with_sign to the value of expr_to_get_sign.

Syntax:

result = rxdmath.copysign(expr_to_get_sign, expr_with_sign)

The behavior mirrors that of the Python standard library’s math.copysign which behaves as follows:

>>> math.copysign(-5, 1.3)
5.0
>>> math.copysign(-5, -1.3)
-5.0
>>> math.copysign(2, -1.3)
-2.0
>>> math.copysign(2, 1.3)
2.0
rxdmath.cos()

Cosine.

Syntax:

result = rxdmath.cos(x)
rxdmath.cosh()

Hyperbolic cosine.

Syntax:

result = rxdmath.cosh(x)
rxdmath.degrees()

Converts x from radians to degrees. Equivalent to multiplying by 180 / π.

Syntax:

result = rxdmath.degrees(x)
rxdmath.erf()

The Gauss error function; see Wikipedia for more.

Syntax:

result = rxdmath.erf(x)
rxdmath.erfc()

The complementary error function. In exact math, erfc(x) = 1 - erf(x), however using this function provides more accurate numerical results when erf(x) is near 1. See the Wikipedia entry on the error function for more.

Syntax:

result = rxdmath.erfc(x)
rxdmath.exp()

e raised to the power x.

Syntax:

result = rxdmath.exp(x)
rxdmath.expm1()

(e raised to the power x) - 1. More numerically accurate than rxdmath.exp(x) - 1 when x is near 0.

Syntax:

result = rxdmath.expm1(x)
rxdmath.fabs()

Absolute value.

Syntax:

result = rxdmath.fabs(x)
rxdmath.factorial()

Factorial. Probably not likely to be used in practice as it requires integer values. Consider using rxdmath.gamma() instead, as for integers x, rxdmath.factorial(x) = rxdmath.gamma(x + 1).

Syntax:

result = rxdmath.factorial(x)
rxdmath.floor()

Floor function.

Syntax:

result = rxdmath.floor(x)
rxdmath.fmod()

Modulus operator (remainder after division x/y).

Syntax:

result = rxdmath.fmod(x, y)
rxdmath.gamma()

Gamma function, an extension of the factorial. See Wikipedia for more.

Syntax:

result = rxdmath.gamma(x)
rxdmath.lgamma()

Equivalent to rxdmath.log(rxdmath.fabs(rxdmath.gamma(x))) but more numerically accurate.

Syntax:

result = rxdmath.lgamma(x)
rxdmath.log()

Natural logarithm.

Syntax:

result = rxdmath.log(x)
rxdmath.log10()

Logarithm to the base 10.

Syntax:

result = rxdmath.log10(x)
rxdmath.log1p()

Natural logarithm of 1 + x; equivalent to rxdmath.log(1 + x) but more numerically accurate when x is near 0.

Syntax:

result = rxdmath.log1p(x)
rxdmath.pow()

Returns x raised to the y.

Syntax:

result = rxdmath.pow(x, y)
rxdmath.radians()

Converts degrees to radians. Equivalent to multiplying by π / 180.

Syntax:

result = rxdmath.radians(x)
rxdmath.sin()

Sine.

Syntax:

result = rxdmath.sin(x)
rxdmath.sinh()

Hyperbolic sine.

Syntax:

result = rxdmath.sinh(x)
rxdmath.sqrt()

Square root.

Syntax:

result = rxdmath.sqrt(x)
rxdmath.tan()

Tangent.

Syntax:

result = rxdmath.tan(x)
rxdmath.tanh()

Hyperbolic tangent.

Syntax:

result = rxdmath.tanh(x)
rxdmath.trunc()

Rounds to the nearest integer no further from 0. i.e. 1.5 rounds down to 1 and -1.5 rounds up to -1.

Syntax:

result = rxdmath.trunc(x)
rxdmath.vtrap()

Returns a continuous approximation of x / (exp(x/y) - 1) with the discontinuity at x/y near 0 replaced by the limiting behavior via L’Hôpital’s rule. This is useful in avoiding issues with certain ion channel models, including Hodgkin-Huxley. For an example of this in use, see the Hodgkin-Huxley using rxd tutorial (as opposed to using h.hh) .

Syntax:

result = rxdmath.vtrap(x, y)