【发布时间】:2020-04-26 17:23:27
【问题描述】:
现在是完整的代码/问题
我想估计函数 v 的随机波动 - 因此我想计算它的 RMS 值:
import numpy as np
import matplotlib.pyplot as plt
def HHmodel(I,length, area):
v = []
m = []
h = []
z = []
n = []
squares = []
vsquare = (-60)*(-60)
sumsquares = 0
rms = []
a= []
dt = 0.05
t = np.linspace(0,100,length)
#constants
Cm = area#microFarad
ENa=50 #miliVolt
EK=-77 #miliVolt
El=-54 #miliVolt
g_Na=120*area #mScm-2
g_K=36*area #mScm-2
g_l=0.03*area #mScm-2
def alphaN(v):
return 0.01*(v+50)/(1-np.exp(-(v+50)/10))
def betaN(v):
return 0.125*np.exp(-(v+60)/80)
def alphaM(v):
return 0.1*(v+35)/(1-np.exp(-(v+35)/10))
def betaM(v):
return 4.0*np.exp(-0.0556*(v+60))
def alphaH(v):
return 0.07*np.exp(-0.05*(v+60))
def betaH(v):
return 1/(1+np.exp(-(0.1)*(v+30)))
#Initialize the voltage and the channels :
v.append(-60)
rms.append(1)
m0 = alphaM(v[0])/(alphaM(v[0])+betaM(v[0]))
n0 = alphaN(v[0])/(alphaN(v[0])+betaN(v[0]))
h0 = alphaH(v[0])/(alphaH(v[0])+betaH(v[0]))
#t.append(0)
m.append(m0)
n.append(n0)
h.append(h0)
#solving ODE using Euler's method:
for i in range(1,len(t)):
m.append(m[i-1] + dt*((alphaM(v[i-1])*(1-m[i-1]))-betaM(v[i-1])*m[i-1]))
n.append(n[i-1] + dt*((alphaN(v[i-1])*(1-n[i-1]))-betaN(v[i-1])*n[i-1]))
h.append(h[i-1] + dt*((alphaH(v[i-1])*(1-h[i-1]))-betaH(v[i-1])*h[i-1]))
gNa = g_Na * h[i-1]*(m[i-1])**3
gK=g_K*n[i-1]**4
gl=g_l
INa = gNa*(v[i-1]-ENa)
IK = gK*(v[i-1]-EK)
Il=gl*(v[i-1]-El)
v.append(v[i-1]+(dt)*((1/Cm)*(I[i-1]-(INa+IK+Il))))
#v.append(v[i-1]+(dt)*((1/Cm)*(I-(INa+IK+Il))))
meansquare = np.sqrt((np.square(v).sum()))
return v,area,meansquare
spikeEvents = [] #timing each spike
length = 1000*5 #the time period
fluctuations = []
output = []
for j in range(1, 10):
barcode = np.zeros(length)
noisyI = np.random.normal(0,9,length)
area = 1.0+0.1*j
res = HHmodel(noisyI,length,area)
output.append(res[2])
print('Done.')
目标应该是 v 的波动随着 a 的大小以某种方式增加 - 我在这里认为 rms 幅度是一个合理的度量
BR
编辑:
for i in range(1,len(t)):
m.append(m[i-1] + dt*((alphaM(v[i-1])*(1-m[i-1]))-betaM(v[i-1])*m[i-1]))
n.append(n[i-1] + dt*((alphaN(v[i-1])*(1-n[i-1]))-betaN(v[i-1])*n[i-1]))
h.append(h[i-1] + dt*((alphaH(v[i-1])*(1-h[i-1]))-betaH(v[i-1])*h[i-1]))
gNa = g_Na * h[i-1]*(m[i-1])**3
gK=g_K*n[i-1]**4
gl=g_l
INa = gNa*(v[i-1]-ENa)
IK = gK*(v[i-1]-EK)
Il=gl*(v[i-1]-El)
v.append(v[i-1]+(dt)*((1/Cm)*(I[i-1]-(INa+IK+Il))))
z.append(v[i-1]-np.mean(v))
#v.append(v[i-1]+(dt)*((1/Cm)*(I-(INa+IK+Il))))
mean = sum(np.square(v))/len(v)
squared_diffs =[(item-mean)**2 for item in v]
ms_diff = sum(squared_diffs)/len(squared_diffs)
rms_diff =np.sqrt(ms_diff)
return v,area,rms_diff
编辑2: 绘制范围 (1,10) 中的 j - 蓝色:在编辑 1 中计算的 rmsvalue,黄色 1/sqrt(j)
在范围(1,100)内绘制 j - 但波动的“大小”应该增加,而不是减少并在某处居中
【问题讨论】:
-
你为什么要在所有索引上做奇怪的范围和-1?
-
我不能说太多,因为我不是 100% 你想要达到的目标。但是在你的循环中,
meansquare被len(t)划分,尽管循环在除最后一次之外的所有迭代中都没有运行到len(t)。 -
如果您的值存储在
v列表中,我建议您在循环外进行平方。因此,在循环中只需将值附加到v,然后在循环终止后,您可以将平方和计算为np.square(v).sum(),这可能会有所帮助。 -
创建
v后,然后:rms = np.sqrt(np.mean(v**2)) -
但是 v**2 很棘手,因为 v 是一个列表?