Use the Matlab style code within the Python by connecting octave through Oct2pa Library

In this lesson, we check how we can run without the Matlab style code within the Python by connecting Octave through Oct2 Library. We put the nature in Google Colab, data exchange between Numpy and Octave, write and call .m files, and activate the tool files, Prods, and .MS files. By doing this, we get Python's environmental fluctuations while continuing to update regular syntaxs and matlab / octave in one function. Look Full codes here.
!apt-get -qq update
!apt-get -qq install -y octave gnuplot octave-signal octave-control > /dev/null
!python -m pip -q install oct2py scipy matplotlib pillow
from oct2py import Oct2Py, Oct2PyError
import numpy as np, matplotlib.pyplot as plt, textwrap
from scipy.io import savemat, loadmat
from PIL import Image
oc = Oct2Py()
print("Octave version:", oc.eval("version"))
def show_png(path, title=None):
img = Image.open(path)
plt.figure(figsize=(5,4)); plt.imshow(img); plt.axis("off")
if title: plt.title(title)
plt.show()
We start by setting the Octave and the key libraries to Google Colab, and confirmed that we have octave packages and psychiatric puppies. Then we start the Oct2py session and explain the relief work so that we can display octave sites directly from the Pythali Work. Look Full codes here.
print("n--- Basic eval ---")
print(oc.eval("A = magic(4); A"))
print("eig(A) diag:", oc.eval("[V,D]=eig(A); diag(D)'"))
print("sin(pi/4):", oc.eval("sin(pi/4)"))
print("n--- NumPy exchange ---")
x = np.linspace(0, 2*np.pi, 100)
y = np.sin(x) + 0.1*np.random.randn(x.size)
y_filt = oc.feval("conv", y, np.ones(5)/5.0, "same")
print("y_filt shape:", np.asarray(y_filt).shape)
print("n--- Cells & Structs ---")
cells = ["hello", 42, [1,2,3]]
oc.push("C", cells)
oc.eval("s = struct('name','Ada','score',99,'tags',{C});")
s = oc.pull("s")
print("Struct from Octave -> Python:", s)
We test the bridge between Python and Octave for basic operations of matrix activities, eigensvalue decay, and trigonomic analysis directly to octave. We then change organizing the Arrows and Octave to make a Convolution filter and ensure its formation. Finally, we show that pressing Python lists in octave as the Arraves Arrays, build a arrays, and return to Python by sharing seamless data. Look Full codes here.
print("n--- Writing and calling .m files ---")
gd_code = r"""
function [w, hist] = gradient_descent(X, y, alpha, iters)
% X: (n,m), y: (n,1). Adds bias; returns weights and loss history.
if size(X,2) == 0, error('X must be 2D'); end
n = rows(X);
Xb = [ones(n,1), X];
m = columns(Xb);
w = zeros(m,1);
hist = zeros(iters,1);
for t=1:iters
yhat = Xb*w;
g = (Xb'*(yhat - y))/n;
w = w - alpha * g;
hist
endfor
endfunction
"""
with open("gradient_descent.m","w") as f: f.write(textwrap.dedent(gd_code))
np.random.seed(0)
X = np.random.randn(200, 3)
true_w = np.array([2.0, -1.0, 0.5, 3.0])
y = true_w[0] + X @ true_w[1:] + 0.3*np.random.randn(200)
w_est, hist = oc.gradient_descent(X, y.reshape(-1,1), 0.1, 100, nout=2)
print("Estimated w:", np.ravel(w_est))
print("Final loss:", float(np.ravel(hist)[-1]))
print("n--- Octave plotting -> PNG -> Python display ---")
oc.eval("x = linspace(0,2*pi,400); y = sin(2*x) .* exp(-0.2*x);")
oc.eval("figure('visible','off'); plot(x,y,'linewidth',2); grid on; title('Damped Sine (Octave)');")
plot_path = "/content/oct_plot.png"
oc.eval(f"print('{plot_path}','-dpng'); close all;")
show_png(plot_path, title="Octave-generated Plot")
We write Gradient_Descent of Gradient.m in Octave, call it from Python with notton = 2, and make sure that we recover the right weights and lose weight. We also offer a fracture that has been bound in the Octave in Octave and shows our Pyth Notebook mark. Look Full codes here.
print("n--- Packages (signal/control) ---")
signal_ok = True
try:
oc.eval("pkg load signal; pkg load control;")
print("Loaded: signal, control")
except Oct2PyError as e:
signal_ok = False
print("Could not load signal/control, skipping package demo.nReason:", str(e).splitlines()[0])
if signal_ok:
oc.push("t", np.linspace(0,1,800))
oc.eval("x = sin(2*pi*5*t) + 0.5*sin(2*pi*40*t);")
oc.eval("[b,a] = butter(4, 10/(800/2)); xf = filtfilt(b,a,x);")
xf = oc.pull("xf")
plt.figure(); plt.plot(xf); plt.title("Octave signal package: filtered"); plt.show()
print("n--- Function handles ---")
oc.eval("""
f = @(z) z.^2 + 3*z + 2;
vals = feval(f, [0 1 2 3]);
""")
vals = oc.pull("vals")
print("f([0,1,2,3]) =", np.ravel(vals))
quadfun_code = r"""
function y = quadfun(z)
y = z.^2 + 3*z + 2;
end
"""
with open("quadfun.m","w") as f: f.write(textwrap.dedent(quadfun_code))
vals2 = oc.quadfun(np.array([0,1,2,3], dtype=float))
print("quadfun([0,1,2,3]) =", np.ravel(vals2))
We are uploading signals signals and controls so we can design Butterworth Filter on octabhes and visualize the filtered Waveform back in Python. We also work on jobs by an unknown Octave evaluation of a quadratic Octave. Look Full codes here.
print("n--- .mat I/O ---")
data_py = {"A": np.arange(9).reshape(3,3), "label": "demo"}
savemat("demo.mat", data_py)
oc.eval("load('demo.mat'); A2 = A + 1;")
oc.eval("save('-mat','demo_from_octave.mat','A2','label');")
back = loadmat("demo_from_octave.mat")
print("Keys from Octave-saved mat:", list(back.keys()))
print("n--- Error handling ---")
try:
oc.eval("no_such_function(1,2,3);")
except Oct2PyError as e:
print("Caught Octave error as Python exception:n", str(e).splitlines()[0])
print("n--- Simple Octave benchmark ---")
oc.eval("N = 2e6; a = rand(N,1);")
oc.eval("tic; s1 = sum(a); tv = toc;")
t_vec = float(oc.pull("tv"))
oc.eval("tic; s2 = 0; for i=1:length(a), s2 += a(i); end; tl = toc;")
t_loop = float(oc.pull("tl"))
print(f"Vectorized sum: {t_vec:.4f}s | Loop sum: {t_loop:.4f}s")
print("n--- Multi-file pipeline ---")
pipeline_m = r"""
function out = mini_pipeline(x, fs)
try, pkg load signal; catch, end
[b,a] = butter(6, 0.2);
y = filtfilt(b,a,x);
y_env = abs(hilbert(y));
out = struct('rms', sqrt(mean(y.^2)), 'peak', max(abs(y)), 'env', y_env(1:10));
end
"""
with open("mini_pipeline.m","w") as f: f.write(textwrap.dedent(pipeline_m))
fs = 200.0
sig = np.sin(2*np.pi*3*np.linspace(0,3,int(3*fs))) + 0.1*np.random.randn(int(3*fs))
out = oc.mini_pipeline(sig, fs, nout=1)
print("mini_pipeline -> keys:", list(out.keys()))
print("RMS ~", float(out["rms"]), "| Peak ~", float(out["peak"]), "| env head:", np.ravel(out["env"])[:5])
print("nAll sections executed. You are now running MATLAB/Octave code from Python!")
We exchange between Python and octave files, ensures that data flows both methods without problems. We also check to handle an error by holding an octave error as a different python. Next, it is made Benchmark vector to compare summaries included in Octave, indicating the operation of the vectorization. Finally, we build a pipe for many files that uses the sorting and the availability of the envelope, which is important Psython, show how we can edit the Octave code in our usable parts within Python Workflow.
In conclusion, we see how we can associate by combining the relevant Octave features have directed directly to Python and Colab. We are successfully testing data exchange, custom activities, package uses, and measuring performance, indicating that we can mix with mattlab / octave functioning without leaving our textbook. By combining the power of both areas, we put ourselves in line to solve the effects of problems and effectively.
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