我在Jupyter Notebook工作。当我想在cython中编译.pyx时,会抛出类似这样的错误:
%run -i setup.py build_ext --inplace
unable to find vcvarsall.bat
setup.py文件如下所示:
from distutils.core import setup
from Cython.Build import cythonize
setup(
ext_modules=cythonize("hh_vers_vector.pyx"),
)
然而,这只发生在我工作的计算机上。在家里的那个,它运作得很好。
Visual Studio可能是一个问题,如here所述。问题是,我在两台计算机上安装了相同版本的Visual Studio 2017社区。最新的Anaconda 3版本安装在两台计算机上。两者都使用Python 3.6.2和IPython 6.1.0。那怎么可能呢?两者都运行在Windows 10.我还会向您显示我的.pyx文件。如果您需要更多信息,我将编辑我的帖子。
from math import exp
import numpy as np
import time
def hhModel(*params, Iext, float dt, int Vref):
## Unwrap params argument: these variables are going to be optimized
cdef float ENa = params[0]
cdef float EK = params[1]
cdef float EL = params[2]
cdef float GNa = params[3]
cdef float GK = params[4]
cdef float GL = params[5]
## Input paramters
# I : a list containing external current steps, your stimulus vector [nA]
# dt : a crazy time parameter [ms]
# Vref : reference potential [mV]
def alphaM(float v, float vr): return 0.1 * (v-vr-25) / ( 1 - exp(-(v-vr-25)/10) )
def betaM(float v, float vr): return 4 * exp(-(v-vr)/18)
def alphaH(float v, float vr): return 0.07 * exp(-(v-vr)/20)
def betaH(float v, float vr): return 1 / ( 1 + exp( -(v-vr-30)/10 ) )
def alphaN(float v, float vr): return 0.01 * (v-vr-10) / ( 1 - exp(-(v-vr-10)/10) )
def betaN(float v, float vr): return 0.125 * exp(-(v-vr)/80)
## steady-state values and time constants of m,h,n
def m_infty(float v, float vr): return alphaM(v,vr) / ( alphaM(v,vr) + betaM(v,vr) )
def h_infty(float v, float vr): return alphaH(v,vr) / ( alphaH(v,vr) + betaH(v,vr) )
def n_infty(float v, float vr): return alphaN(v,vr) / ( alphaN(v,vr) + betaN(v,vr) )
## parameters
cdef float Cm, gK, gL, INa, IK, IL, dv_dt, dm_dt, dh_dt, dn_dt, aM, bM, aH, bH, aN, bN
cdef float Smemb = 4000 # [um^2] surface area of the membrane
cdef float Cmemb = 1 # [uF/cm^2] membrane capacitance density
Cm = Cmemb * Smemb * 1e-8 # [uF] membrane capacitance
gNa = GNa * Smemb * 1e-8 # Na conductance [mS]
gK = GK * Smemb * 1e-8 # K conductance [mS]
gL = GL * Smemb * 1e-8 # leak conductance [mS]
# numSamples = int(T/dt);
cdef int numSamples = len(Iext);
# DEF numSamples = 200000
# initial values
cdef float[:] v = np.empty(numSamples, dtype=np.float)
cdef float[:] m = np.empty(numSamples, dtype=np.float)
cdef float[:] h = np.empty(numSamples, dtype=np.float)
cdef float[:] n = np.empty(numSamples, dtype=np.float)
#cdef float v[numSamples]
#cdef float m[numSamples]
#cdef float h[numSamples]
#cdef float n[numSamples]
v[0] = Vref # initial membrane potential
m[0] = m_infty(v[0], Vref) # initial m
h[0] = h_infty(v[0], Vref) # initial h
n[0] = n_infty(v[0], Vref) # initial n
## calculate membrane response step-by-step
for j in range(0, numSamples-1):
# ionic currents: g[mS] * V[mV] = I[uA]
INa = gNa * m[j]*m[j]*m[j] * h[j] * (ENa-v[j])
IK = gK * n[j]*n[j]*n[j]*n[j] * (EK-v[j])
IL = gL * (EL-v[j])
# derivatives
# I[uA] / C[uF] * dt[ms] = dv[mV]
dv_dt = ( INa + IK + IL + Iext[j]*1e-3) / Cm;
aM = 0.1 * (v[j]-Vref-25) / ( 1 - exp(-(v[j]-Vref-25)/10))
bM = 4 * exp(-(v[j]-Vref)/18)
aH = 0.07 * exp(-(v[j]-Vref)/20)
bH = 1 / ( 1 + exp( -(v[j]-Vref-30)/10 ) )
aN = 0.01 * (v[j]-Vref-10) / ( 1 - exp(-(v[j]-Vref-10)/10) )
bN = 0.125 * exp(-(v[j]-Vref)/80)
dm_dt = (1-m[j])* aM - m[j]*bM
dh_dt = (1-h[j])* aH - h[j]*bH
dn_dt = (1-n[j])* aN - n[j]*bN
# calculate next step
v[j+1] = (v[j] + dv_dt * dt)
m[j+1] = (m[j] + dm_dt * dt)
h[j+1] = (h[j] + dh_dt * dt)
n[j+1] = (n[j] + dn_dt * dt)
return v