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I have an array S(i) which contains all of the index values of the x coordinates j which are close to i, i.e. if S(1) = {2,3} this means that x2 and x3 are close to x1. In total I have S(1), ..., S(N) sets.
So this part of the code works fine:
arr = np.array([[1,3], [2,8],[3,1],[6,18], [9,8]])
arr = [item[0] for item in arr] #Extract x-coordinates
def Si(x): #This is the set i want to use
return [[j for j in range(len(x)) if np.abs(x[j] - x[i]) < 2] for i in range(len(x))]
Now i have a subscript of j's, I want to calculate the euclidean distance between (x_i,y_i) to each (x_j,y_j) in S(i), e.g for i=1, if S(1) = {7}, find distance between (x_1, y_1) and (x_7, y_7), for i=2, if S(2) = {3,9}, find distance between (x_2,y_2) and (x_3,y_3) and (x_2,y_2) and (x_9,y_9) and repeat for each i.
I don't know how to implement this, i'm really confused! Here is a Euclidean distance code which finds it for ALL values in the array, but not in the set which i want.
def euc_dist(arr):
arr_x = (arr[:,0,np.newaxis].T - arr[:,0,np.newaxis])**2 ##x-coordinates
arr_y = (arr[:,1,np.newaxis].T - arr[:,1,np.newaxis])**2 ##y-coordinates
arr = np.sqrt(arr_x + arr_y)
return arr
This should work:
S = Si(arr) # get the array
def my_fn(i): # take the value of i
euc_dists = []
for j in S[i]: # iterate over j's in S[i]
if i!= j:
dist = np.linalg.norm(arr[i]-arr[j]) # euclidean distance
euc_dists.append(dist)
return euc_dists
I have a list of 2D points x,y. And I need to find a smooth curve for the upper and lower edges (red and blue curves, correspondingly).
See the picture below:
Here I've found a good example, where the outer edge of x,y points is detected.
Using these I have work I have:
# https://stackoverflow.com/a/50714300/7200745
from scipy.spatial import Delaunay
import numpy as np
def alpha_shape(points, alpha, only_outer=True):
"""
Compute the alpha shape (concave hull) of a set of points.
:param points: np.array of shape (n,2) points.
:param alpha: alpha value.
:param only_outer: boolean value to specify if we keep only the outer border
or also inner edges.
:return: set of (i,j) pairs representing edges of the alpha-shape. (i,j) are
the indices in the points array.
"""
assert points.shape[0] > 3, "Need at least four points"
def add_edge(edges, i, j):
"""
Add an edge between the i-th and j-th points,
if not in the list already
"""
if (i, j) in edges or (j, i) in edges:
# already added
assert (j, i) in edges, "Can't go twice over same directed edge right?"
if only_outer:
# if both neighboring triangles are in shape, it's not a boundary edge
edges.remove((j, i))
return
edges.add((i, j))
tri = Delaunay(points)
edges = set()
# Loop over triangles:
# ia, ib, ic = indices of corner points of the triangle
for ia, ib, ic in tri.vertices:
pa = points[ia]
pb = points[ib]
pc = points[ic]
# Computing radius of triangle circumcircle
# www.mathalino.com/reviewer/derivation-of-formulas/derivation-of-formula-for-radius-of-circumcircle
a = np.sqrt((pa[0] - pb[0]) ** 2 + (pa[1] - pb[1]) ** 2)
b = np.sqrt((pb[0] - pc[0]) ** 2 + (pb[1] - pc[1]) ** 2)
c = np.sqrt((pc[0] - pa[0]) ** 2 + (pc[1] - pa[1]) ** 2)
s = (a + b + c) / 2.0
area = np.sqrt(s * (s - a) * (s - b) * (s - c))
circum_r = a * b * c / (4.0 * area)
if circum_r < alpha:
add_edge(edges, ia, ib)
add_edge(edges, ib, ic)
add_edge(edges, ic, ia)
return edges
def find_edges_with(i, edge_set):
i_first = [j for (x,j) in edge_set if x==i]
i_second = [j for (j,x) in edge_set if x==i]
return i_first,i_second
def stitch_boundaries(edges):
edge_set = edges.copy()
boundary_lst = []
while len(edge_set) > 0:
boundary = []
edge0 = edge_set.pop()
boundary.append(edge0)
last_edge = edge0
while len(edge_set) > 0:
i,j = last_edge
j_first, j_second = find_edges_with(j, edge_set)
if j_first:
edge_set.remove((j, j_first[0]))
edge_with_j = (j, j_first[0])
boundary.append(edge_with_j)
last_edge = edge_with_j
elif j_second:
edge_set.remove((j_second[0], j))
edge_with_j = (j, j_second[0]) # flip edge rep
boundary.append(edge_with_j)
last_edge = edge_with_j
if edge0[0] == last_edge[1]:
break
boundary_lst.append(boundary)
return boundary_lst[0]
#generating of random points
N = 1000
r = 1 - 2*np.random.random((N,2))
r_norm = np.linalg.norm(r, axis=1)
points = r[r_norm <= 1]
plt.figure(figsize=(10,10))
plt.scatter(points[:,0], points[:,1], color='k', s=1)
# Computing the alpha shape
edges = alpha_shape(points, alpha=1, only_outer=True)
#order edges
edges = stitch_boundaries(edges)
plt.axis('equal')
edge_points = np.zeros((len(edges),2))
k=0
for i, j in edges:
edge_points[k,:] = points[[i, j], 0][0] , points[[i, j], 1][0]
k += 1
plt.plot(edge_points[:,0],edge_points[:,1])
#theoretical/expected edges
# xx = np.linspace(-1,1, 100)
# yy_upper = np.sqrt(1 - xx**2)
# yy_lower = -np.sqrt(1 - xx**2)
# plt.plot(xx, yy_upper, 'r:')
# plt.plot(xx, yy_lower, 'b:')
Right now the cloud of points is black. Blue line is obtained from the algorithm above.
UPDATE:
the starting and final points can be chosen the most left point (OR by hand it is no problem)
I am expecting the following result:
You can use the fact (see the scipy.spatial.Delaunay documentation) that
"for 2-D, the triangle points are oriented counterclockwise".
Therefore, the outer edge points constructed in the Alpha shape will always be oriented counterclockwise i.e., the inner side of the shape will be to their left (if this was not certified in the documentation we could have checked it ourselves and flipped if necessary, but here there is no need).
This means that the points along the polygon between the leftmost point and the rightmost point are the lower hull, and the points between the rightmost and the leftmost are the upper hull. The code below implements this idea.
min_x_ind = np.argmin(edge_points[:, 0])
max_x_ind = np.argmax(edge_points[:, 0])
if min_x_ind < max_x_ind:
lower_hull = edge_points[min_x_ind:max_x_ind+1, :]
upper_hull = np.concatenate([edge_points[max_x_ind:, :], edge_points[:min_x_ind+1, :]])
else:
upper_hull = edge_points[max_x_ind:min_x_ind+1, :]
lower_hull = np.concatenate([edge_points[min_x_ind:, :], edge_points[:max_x_ind+1, :]])
and the result can be visualized for example with:
plt.plot(upper_hull[:,0],upper_hull[:,1], "r", lw=3)
plt.plot(lower_hull[:,0],lower_hull[:,1], "b", lw=3)
I am trying to make my own CFD solver and one of the most computationally expensive parts is solving for the pressure term. One way to solve Poisson differential equations faster is by using a multigrid method. The basic recursive algorithm for this is:
function phi = V_Cycle(phi,f,h)
% Recursive V-Cycle Multigrid for solving the Poisson equation (\nabla^2 phi = f) on a uniform grid of spacing h
% Pre-Smoothing
phi = smoothing(phi,f,h);
% Compute Residual Errors
r = residual(phi,f,h);
% Restriction
rhs = restriction(r);
eps = zeros(size(rhs));
% stop recursion at smallest grid size, otherwise continue recursion
if smallest_grid_size_is_achieved
eps = smoothing(eps,rhs,2*h);
else
eps = V_Cycle(eps,rhs,2*h);
end
% Prolongation and Correction
phi = phi + prolongation(eps);
% Post-Smoothing
phi = smoothing(phi,f,h);
end
I've attempted to implement this algorithm myself (also at the end of this question) however it is very slow and doesn't give good results so evidently it is doing something wrong. I've been trying to find why for too long and I think it's just worthwhile seeing if anyone can help me.
If I use a grid size of 2^5 by 2^5 points, then it can solve it and give reasonable results. However, as soon as I go above this it takes exponentially longer to solve and basically get stuck at some level of inaccuracy, no matter how many V-Loops are performed. at 2^7 by 2^7 points, the code takes way too long to be useful.
I think my main issue is that my implementation of a jacobian iteration is using linear algebra to calculate the update at each step. This should, in general, be fast however, the update matrix A is an n*m sized matrix, and calculating the dot product of a 2^7 * 2^7 sized matrix is expensive. As most of the cells are just zeros, should I calculate the result using a different method?
if anyone has any experience in multigrid methods, I would appreciate any advice!
Thanks
my code:
# -*- coding: utf-8 -*-
"""
Created on Tue Dec 29 16:24:16 2020
#author: mclea
"""
import numpy as np
import matplotlib.pyplot as plt
from scipy.signal import convolve2d
from mpl_toolkits.mplot3d import Axes3D
from scipy.interpolate import griddata
from matplotlib import cm
def restrict(A):
"""
Creates a new grid of points which is half the size of the original
grid in each dimension.
"""
n = A.shape[0]
m = A.shape[1]
new_n = int((n-2)/2+2)
new_m = int((m-2)/2+2)
new_array = np.zeros((new_n, new_m))
for i in range(1, new_n-1):
for j in range(1, new_m-1):
ii = int((i-1)*2)+1
jj = int((j-1)*2)+1
# print(i, j, ii, jj)
new_array[i,j] = np.average(A[ii:ii+2, jj:jj+2])
new_array = set_BC(new_array)
return new_array
def interpolate_array(A):
"""
Creates a grid of points which is double the size of the original
grid in each dimension. Uses linear interpolation between grid points.
"""
n = A.shape[0]
m = A.shape[1]
new_n = int((n-2)*2 + 2)
new_m = int((m-2)*2 + 2)
new_array = np.zeros((new_n, new_m))
i = (np.indices(A.shape)[0]/(A.shape[0]-1)).flatten()
j = (np.indices(A.shape)[1]/(A.shape[1]-1)).flatten()
A = A.flatten()
new_i = np.linspace(0, 1, new_n)
new_j = np.linspace(0, 1, new_m)
new_ii, new_jj = np.meshgrid(new_i, new_j)
new_array = griddata((i, j), A, (new_jj, new_ii), method="linear")
return new_array
def adjacency_matrix(rows, cols):
"""
Creates the adjacency matrix for an n by m shaped grid
"""
n = rows*cols
M = np.zeros((n,n))
for r in range(rows):
for c in range(cols):
i = r*cols + c
# Two inner diagonals
if c > 0: M[i-1,i] = M[i,i-1] = 1
# Two outer diagonals
if r > 0: M[i-cols,i] = M[i,i-cols] = 1
return M
def create_differences_matrix(rows, cols):
"""
Creates the central differences matrix A for an n by m shaped grid
"""
n = rows*cols
M = np.zeros((n,n))
for r in range(rows):
for c in range(cols):
i = r*cols + c
# Two inner diagonals
if c > 0: M[i-1,i] = M[i,i-1] = -1
# Two outer diagonals
if r > 0: M[i-cols,i] = M[i,i-cols] = -1
np.fill_diagonal(M, 4)
return M
def set_BC(A):
"""
Sets the boundary conditions of the field
"""
A[:, 0] = A[:, 1]
A[:, -1] = A[:, -2]
A[0, :] = A[1, :]
A[-1, :] = A[-2, :]
return A
def create_A(n,m):
"""
Creates all the components required for the jacobian update function
for an n by m shaped grid
"""
LaddU = adjacency_matrix(n,m)
A = create_differences_matrix(n,m)
invD = np.zeros((n*m, n*m))
np.fill_diagonal(invD, 1/4)
return A, LaddU, invD
def calc_RJ(rows, cols):
"""
Calculates the jacobian update matrix Rj for an n by m shaped grid
"""
n = int(rows*cols)
M = np.zeros((n,n))
for r in range(rows):
for c in range(cols):
i = r*cols + c
# Two inner diagonals
if c > 0: M[i-1,i] = M[i,i-1] = 0.25
# Two outer diagonals
if r > 0: M[i-cols,i] = M[i,i-cols] = 0.25
return M
def jacobi_update(v, f, nsteps=1, max_err=1e-3):
"""
Uses a jacobian update matrix to solve nabla(v) = f
"""
f_inner = f[1:-1, 1:-1].flatten()
n = v.shape[0]
m = v.shape[1]
A, LaddU, invD = create_A(n-2, m-2)
Rj = calc_RJ(n-2,m-2)
update=True
step = 0
while update:
v_old = v.copy()
step += 1
vt = v_old[1:-1, 1:-1].flatten()
vt = np.dot(Rj, vt) + np.dot(invD, f_inner)
v[1:-1, 1:-1] = vt.reshape((n-2),(m-2))
err = v - v_old
if step == nsteps or np.abs(err).max()<max_err:
update=False
return v, (step, np.abs(err).max())
def MGV(f, v):
"""
Solves for nabla(v) = f using a multigrid method
"""
# global A, r
n = v.shape[0]
m = v.shape[1]
# If on the smallest grid size, compute the exact solution
if n <= 6 or m <=6:
v, info = jacobi_update(v, f, nsteps=1000)
return v
else:
# smoothing
v, info = jacobi_update(v, f, nsteps=10, max_err=1e-1)
A = create_A(n, m)[0]
# calculate residual
r = np.dot(A, v.flatten()) - f.flatten()
r = r.reshape(n,m)
# downsample resitdual error
r = restrict(r)
zero_array = np.zeros(r.shape)
# interploate the correction computed on a corser grid
d = interpolate_array(MGV(r, zero_array))
# Add prolongated corser grid solution onto the finer grid
v = v - d
v, info = jacobi_update(v, f, nsteps=10, max_err=1e-6)
return v
sigma = 0
# Setting up the grid
k = 6
n = 2**k+2
m = 2**(k)+2
hx = 1/n
hy = 1/m
L = 1
H = 1
x = np.linspace(0, L, n)
y = np.linspace(0, H, m)
XX, YY = np.meshgrid(x, y)
# Setting up the initial conditions
f = np.ones((n,m))
v = np.zeros((n,m))
# How many V cyles to perform
err = 1
n_cycles = 10
loop = True
cycle = 0
# Perform V cycles until converged or reached the maximum
# number of cycles
while loop:
cycle += 1
v_new = MGV(f, v)
if np.abs(v - v_new).max() < err:
loop = False
if cycle == n_cycles:
loop = False
v = v_new
print("Number of cycles " + str(cycle))
plt.contourf(v)
I realize that I'm not answering your question directly, but I do note that you have quite a few loops that will contribute some overhead cost. When optimizing code, I have found the following thread useful - particularly the line profiler thread. This way you can focus in on "high time cost" lines and then start to ask more specific questions regarding opportunities to optimize.
How do I get time of a Python program's execution?
I have a face made from 4 xyz vertices.
I want to align it with the z axis so it is parallel with it.
If I calculate the normals I can calculate the angle between them but that is just the angle. I need an x rotation and a y rotation.
I am using numpy on Python 3.
Thanks.
To rotate a unit vector to the, say, 1st axis you can use QR decomp, like so:
normal = np.random.random(3)
normal /= np.sqrt(normal#normal)
some_base = np.identity(3)
some_base[:, 0] = normal
Q, R = np.linalg.qr(some_base)
Q.T#normal
# array([-1.00000000e+00, -2.77555756e-17, 1.11022302e-16])
As you can see you may have to flip one or two of the columns of Q:
if (Q.T#normal)[0] < 0:
if np.linalg.det(Q) < 0:
rot = (Q * [-1, 1, 1]).T
else:
rot = (Q * [-1, -1, 1]).T
else:
if np.linalg.det(Q) < 0:
rot = (Q * [1, -1, 1]).T
else:
rot = Q.T
edit: I'm not looking for you to debug this code. If you are familiar with this well-known algorithm, then you may be able to help. Please note that the algorithm produces the coefficients correctly.
This code for cubic spline interpolation is producing linear splines and I can't seem to figure out why (yet). The algorithm comes from Burden's Numerical Analysis, which is just about identical to the pseudo code here, or you can find that book from a link in the comments (see chapter 3, it's worth having anyway). The code is producing the correct coefficients; I believe that I am misunderstanding the implementation. Any feedback is greatly appreciated. Also, i'm new to programming, so any feedback on how bad my coding is also welcome. I tried uploading pics of the linear system in terms of h, a, and c, but as a new user i can not. If you want a visual of the tridiagonal linear system that the algorithm solves, and which is set up by the var alpha, see the link in the comments for the book, see chap 3. The system is strictly diagonally dominant, so we know there exists a unique solution c0,...,cn. Once we know the ci values, the other coefficients follow.
import matplotlib.pyplot as plt
# need some zero vectors...
def zeroV(m):
z = [0]*m
return(z)
#INPUT: n; x0, x1, ... ,xn; a0 = f(x0), a1 =f(x1), ... , an = f(xn).
def cubic_spline(n, xn, a, xd):
"""function cubic_spline(n,xn, a, xd) interpolates between the knots
specified by lists xn and a. The function computes the coefficients
and outputs the ranges of the piecewise cubic splines."""
h = zeroV(n-1)
# alpha will be values in a system of eq's that will allow us to solve for c
# and then from there we can find b, d through substitution.
alpha = zeroV(n-1)
# l, u, z are used in the method for solving the linear system
l = zeroV(n+1)
u = zeroV(n)
z = zeroV(n+1)
# b, c, d will be the coefficients along with a.
b = zeroV(n)
c = zeroV(n+1)
d = zeroV(n)
for i in range(n-1):
# h[i] is used to satisfy the condition that
# Si+1(xi+l) = Si(xi+l) for each i = 0,..,n-1
# i.e., the values at the knots are "doubled up"
h[i] = xn[i+1]-xn[i]
for i in range(1, n-1):
# Sets up the linear system and allows us to find c. Once we have
# c then b and d follow in terms of it.
alpha[i] = (3./h[i])*(a[i+1]-a[i])-(3./h[i-1])*(a[i] - a[i-1])
# I, II, (part of) III Sets up and solves tridiagonal linear system...
# I
l[0] = 1
u[0] = 0
z[0] = 0
# II
for i in range(1, n-1):
l[i] = 2*(xn[i+1] - xn[i-1]) - h[i-1]*u[i-1]
u[i] = h[i]/l[i]
z[i] = (alpha[i] - h[i-1]*z[i-1])/l[i]
l[n] = 1
z[n] = 0
c[n] = 0
# III... also find b, d in terms of c.
for j in range(n-2, -1, -1):
c[j] = z[j] - u[j]*c[j+1]
b[j] = (a[j+1] - a[j])/h[j] - h[j]*(c[j+1] + 2*c[j])/3.
d[j] = (c[j+1] - c[j])/(3*h[j])
# This is my only addition, which is returning values for Sj(x). The issue I'm having
# is related to this implemention, i suspect.
for j in range(n-1):
#OUTPUT:S(x)=Sj(x)= aj + bj(x - xj) + cj(x - xj)^2 + dj(x - xj)^3; xj <= x <= xj+1)
return(a[j] + b[j]*(xd - xn[j]) + c[j]*((xd - xn[j])**2) + d[j]*((xd - xn[j])**3))
For the bored, or overachieving...
Here is code for testing, the interval is x: [1, 9], y:[0, 19.7750212]. The test function is xln(x), so we start 1 and increase by .1 up to 9.
ln = []
ln_dom = []
cub = []
step = 1.
X=[1., 9.]
FX=[0, 19.7750212]
while step <= 9.:
ln.append(step*log(step))
ln_dom.append(step)
cub.append(cubic_spline(2, x, fx, step))
step += 0.1
...and for plotting:
plt.plot(ln_dom, cub, color='blue')
plt.plot(ln_dom, ln, color='red')
plt.axis([1., 9., 0, 20], 'equal')
plt.axhline(y=0, color='black')
plt.axvline(x=0, color='black')
plt.show()
Ok, got this working. The problem was in my implementation. I got it working with a different approach, where the splines are constructed individually instead of continuously. This is fully functioning cubic spline interpolation by method of first constructing the coefficients of the spline polynomials (which is 99% of the work), then implementing them. Obviously this is not the only way to do it. I may work on a different approach and post that if there is interest. One thing that would clarify the code would be an image of the linear system that is solved, but i can't post pics until my rep gets up to 10. If you want to go deeper into the algorithm, see the text book link in the comments above.
import matplotlib.pyplot as plt
from pylab import arange
from math import e
from math import pi
from math import sin
from math import cos
from numpy import poly1d
# need some zero vectors...
def zeroV(m):
z = [0]*m
return(z)
#INPUT: n; x0, x1, ... ,xn; a0 = f(x0), a1 =f(x1), ... , an = f(xn).
def cubic_spline(n, xn, a):
"""function cubic_spline(n,xn, a, xd) interpolates between the knots
specified by lists xn and a. The function computes the coefficients
and outputs the ranges of the piecewise cubic splines."""
h = zeroV(n-1)
# alpha will be values in a system of eq's that will allow us to solve for c
# and then from there we can find b, d through substitution.
alpha = zeroV(n-1)
# l, u, z are used in the method for solving the linear system
l = zeroV(n+1)
u = zeroV(n)
z = zeroV(n+1)
# b, c, d will be the coefficients along with a.
b = zeroV(n)
c = zeroV(n+1)
d = zeroV(n)
for i in range(n-1):
# h[i] is used to satisfy the condition that
# Si+1(xi+l) = Si(xi+l) for each i = 0,..,n-1
# i.e., the values at the knots are "doubled up"
h[i] = xn[i+1]-xn[i]
for i in range(1, n-1):
# Sets up the linear system and allows us to find c. Once we have
# c then b and d follow in terms of it.
alpha[i] = (3./h[i])*(a[i+1]-a[i])-(3./h[i-1])*(a[i] - a[i-1])
# I, II, (part of) III Sets up and solves tridiagonal linear system...
# I
l[0] = 1
u[0] = 0
z[0] = 0
# II
for i in range(1, n-1):
l[i] = 2*(xn[i+1] - xn[i-1]) - h[i-1]*u[i-1]
u[i] = h[i]/l[i]
z[i] = (alpha[i] - h[i-1]*z[i-1])/l[i]
l[n] = 1
z[n] = 0
c[n] = 0
# III... also find b, d in terms of c.
for j in range(n-2, -1, -1):
c[j] = z[j] - u[j]*c[j+1]
b[j] = (a[j+1] - a[j])/h[j] - h[j]*(c[j+1] + 2*c[j])/3.
d[j] = (c[j+1] - c[j])/(3*h[j])
# Now that we have the coefficients it's just a matter of constructing
# the appropriate polynomials and graphing.
for j in range(n-1):
cub_graph(a[j],b[j],c[j],d[j],xn[j],xn[j+1])
plt.show()
def cub_graph(a,b,c,d, x_i, x_i_1):
"""cub_graph takes the i'th coefficient set along with the x[i] and x[i+1]'th
data pts, and constructs the polynomial spline between the two data pts using
the poly1d python object (which simply returns a polynomial with a given root."""
# notice here that we are just building the cubic polynomial piece by piece
root = poly1d(x_i,True)
poly = 0
poly = d*(root)**3
poly = poly + c*(root)**2
poly = poly + b*root
poly = poly + a
# Set up our domain between data points, and plot the function
pts = arange(x_i,x_i_1, 0.001)
plt.plot(pts, poly(pts), '-')
return
If you want to test it, here's some data you can use to get started, which comes from the
function 1.6e^(-2x)sin(3*pi*x) between 0 and 1:
# These are our data points
x_vals = [0, 1./6, 1./3, 1./2, 7./12, 2./3, 3./4, 5./6, 11./12, 1]
# Set up the domain
x_domain = arange(0,2, 1e-2)
fx = zeroV(10)
# Defines the function so we can get our fx values
def sine_func(x):
return(1.6*e**(-2*x)*sin(3*pi*x))
for i in range(len(x_vals)):
fx[i] = sine_func(x_vals[i])
# Run cubic_spline interpolant.
cubic_spline(10,x_vals,fx)
Comments on your coding style:
Where are your comments and documentation? At the very least, provide function documentation so that people can tell how your function is supposed to be used.
Instead of:
def cubic_spline(xx,yy):
Please write something like:
def cubic_spline(xx, yy):
"""function cubic_spline(xx,yy) interpolates between the knots
specified by lists xx and yy. The function returns the coefficients
and ranges of the piecewise cubic splines."""
You can make lists of repeated elements by using the * operator on a list.
Like this:
>>> [0] * 10
[0, 0, 0, 0, 0, 0, 0, 0, 0, 0]
So that your zeroV function can be replaced by [0] * m.
Just don't do this with mutable types! (especially lists).
>>> inner_list = [1,2,3]
>>> outer_list = [inner_list] * 3
>>> outer_list
[[1, 2, 3], [1, 2, 3], [1, 2, 3]]
>>> inner_list[0] = 999
>>> outer_list
[[999, 2, 3], [999, 2, 3], [999, 2, 3]] # wut
Math should probably be done using numpy or scipy.
Apart from that, you should read Idiomatic Python by David Goodger.