上述所有的解决方案都很差，因为它们缺乏

由于本机python而不是numpy向量化实现， 数值稳定性，由于numpy使用不当。cumsum或 由于O(len(x) * w)实现为卷积的速度。

鉴于

import numpy
m = 10000
x = numpy.random.rand(m)
w = 1000

注意x_[:w].sum()等于x[:w-1].sum()。因此，对于第一个平均值，numpy.cumsum(…)加上x[w] / w(通过x_[w+1] / w)，并减去0(从x_[0] / w)。结果是x[0:w].mean()

通过cumsum，您将通过添加x[w+1] / w并减去x[0] / w来更新第二个平均值，从而得到x[1:w+1].mean()。

这将一直进行，直到到达x[-w:].mean()。

x_ = numpy.insert(x, 0, 0)
sliding_average = x_[:w].sum() / w + numpy.cumsum(x_[w:] - x_[:-w]) / w

这个解是向量化的，O(m)，可读且数值稳定。

更新:下面的例子展示了老熊猫。Rolling_mean函数，该函数在最近版本的pandas中已被删除。该函数调用的现代等价函数将使用pandas.Series.rolling:

In [8]: pd.Series(x).rolling(window=N).mean().iloc[N-1:].values
Out[8]: 
array([ 0.49815397,  0.49844183,  0.49840518, ...,  0.49488191,
        0.49456679,  0.49427121])

pandas比NumPy或SciPy更适合这一点。它的函数rolling_mean很方便地完成了这项工作。当输入是一个数组时，它还返回一个NumPy数组。

使用任何定制的纯Python实现都很难在性能上击败rolling_mean。下面是针对两个提议的解决方案的性能示例:

In [1]: import numpy as np

In [2]: import pandas as pd

In [3]: def running_mean(x, N):
   ...:     cumsum = np.cumsum(np.insert(x, 0, 0)) 
   ...:     return (cumsum[N:] - cumsum[:-N]) / N
   ...:

In [4]: x = np.random.random(100000)

In [5]: N = 1000

In [6]: %timeit np.convolve(x, np.ones((N,))/N, mode='valid')
10 loops, best of 3: 172 ms per loop

In [7]: %timeit running_mean(x, N)
100 loops, best of 3: 6.72 ms per loop

In [8]: %timeit pd.rolling_mean(x, N)[N-1:]
100 loops, best of 3: 4.74 ms per loop

In [9]: np.allclose(pd.rolling_mean(x, N)[N-1:], running_mean(x, N))
Out[9]: True

关于如何处理边缘值，也有很好的选项。

有点晚了，但我已经做了我自己的小函数，它不环绕端点或垫与零，然后用于查找平均值。进一步的处理是，它还在线性间隔点上对信号进行重新采样。随意定制代码以获得其他特性。

该方法是一个简单的矩阵乘法与规范化高斯核。

def running_mean(y_in, x_in, N_out=101, sigma=1):
    '''
    Returns running mean as a Bell-curve weighted average at evenly spaced
    points. Does NOT wrap signal around, or pad with zeros.
    
    Arguments:
    y_in -- y values, the values to be smoothed and re-sampled
    x_in -- x values for array
    
    Keyword arguments:
    N_out -- NoOf elements in resampled array.
    sigma -- 'Width' of Bell-curve in units of param x .
    '''
    import numpy as np
    N_in = len(y_in)

    # Gaussian kernel
    x_out = np.linspace(np.min(x_in), np.max(x_in), N_out)
    x_in_mesh, x_out_mesh = np.meshgrid(x_in, x_out)
    gauss_kernel = np.exp(-np.square(x_in_mesh - x_out_mesh) / (2 * sigma**2))
    # Normalize kernel, such that the sum is one along axis 1
    normalization = np.tile(np.reshape(np.sum(gauss_kernel, axis=1), (N_out, 1)), (1, N_in))
    gauss_kernel_normalized = gauss_kernel / normalization
    # Perform running average as a linear operation
    y_out = gauss_kernel_normalized @ y_in

    return y_out, x_out

正弦信号加正态分布噪声的一个简单用法:

我还没有检查这有多快，但你可以试试:

from collections import deque

cache = deque() # keep track of seen values
n = 10          # window size
A = xrange(100) # some dummy iterable
cum_sum = 0     # initialize cumulative sum

for t, val in enumerate(A, 1):
    cache.append(val)
    cum_sum += val
    if t < n:
        avg = cum_sum / float(t)
    else:                           # if window is saturated,
        cum_sum -= cache.popleft()  # subtract oldest value
        avg = cum_sum / float(n)

或用于python计算的模块

在我在Tradewave.net的测试中，TA-lib总是赢:

import talib as ta
import numpy as np
import pandas as pd
import scipy
from scipy import signal
import time as t

PAIR = info.primary_pair
PERIOD = 30

def initialize():
    storage.reset()
    storage.elapsed = storage.get('elapsed', [0,0,0,0,0,0])

def cumsum_sma(array, period):
    ret = np.cumsum(array, dtype=float)
    ret[period:] = ret[period:] - ret[:-period]
    return ret[period - 1:] / period

def pandas_sma(array, period):
    return pd.rolling_mean(array, period)

def api_sma(array, period):
    # this method is native to Tradewave and does NOT return an array
    return (data[PAIR].ma(PERIOD))

def talib_sma(array, period):
    return ta.MA(array, period)

def convolve_sma(array, period):
    return np.convolve(array, np.ones((period,))/period, mode='valid')

def fftconvolve_sma(array, period):    
    return scipy.signal.fftconvolve(
        array, np.ones((period,))/period, mode='valid')    

def tick():

    close = data[PAIR].warmup_period('close')

    t1 = t.time()
    sma_api = api_sma(close, PERIOD)
    t2 = t.time()
    sma_cumsum = cumsum_sma(close, PERIOD)
    t3 = t.time()
    sma_pandas = pandas_sma(close, PERIOD)
    t4 = t.time()
    sma_talib = talib_sma(close, PERIOD)
    t5 = t.time()
    sma_convolve = convolve_sma(close, PERIOD)
    t6 = t.time()
    sma_fftconvolve = fftconvolve_sma(close, PERIOD)
    t7 = t.time()

    storage.elapsed[-1] = storage.elapsed[-1] + t2-t1
    storage.elapsed[-2] = storage.elapsed[-2] + t3-t2
    storage.elapsed[-3] = storage.elapsed[-3] + t4-t3
    storage.elapsed[-4] = storage.elapsed[-4] + t5-t4
    storage.elapsed[-5] = storage.elapsed[-5] + t6-t5    
    storage.elapsed[-6] = storage.elapsed[-6] + t7-t6        

    plot('sma_api', sma_api)  
    plot('sma_cumsum', sma_cumsum[-5])
    plot('sma_pandas', sma_pandas[-10])
    plot('sma_talib', sma_talib[-15])
    plot('sma_convolve', sma_convolve[-20])    
    plot('sma_fftconvolve', sma_fftconvolve[-25])

def stop():

    log('ticks....: %s' % info.max_ticks)

    log('api......: %.5f' % storage.elapsed[-1])
    log('cumsum...: %.5f' % storage.elapsed[-2])
    log('pandas...: %.5f' % storage.elapsed[-3])
    log('talib....: %.5f' % storage.elapsed[-4])
    log('convolve.: %.5f' % storage.elapsed[-5])    
    log('fft......: %.5f' % storage.elapsed[-6])

结果:

[2015-01-31 23:00:00] ticks....: 744
[2015-01-31 23:00:00] api......: 0.16445
[2015-01-31 23:00:00] cumsum...: 0.03189
[2015-01-31 23:00:00] pandas...: 0.03677
[2015-01-31 23:00:00] talib....: 0.00700  # <<< Winner!
[2015-01-31 23:00:00] convolve.: 0.04871
[2015-01-31 23:00:00] fft......: 0.22306

有关现成的解决方案，请参见https://scipy-cookbook.readthedocs.io/items/SignalSmooth.html。 它提供了平窗类型的运行平均值。请注意，这比简单的do-it-yourself卷积方法要复杂一些，因为它试图通过反射数据来处理数据开头和结尾的问题(在您的情况下可能有效，也可能无效……)。

首先，你可以试着:

a = np.random.random(100)
plt.plot(a)
b = smooth(a, window='flat')
plt.plot(b)