Important: Please read the installation page for details about how to install the toolboxes. $\newcommand{\dotp}[2]{\langle #1, #2 \rangle}$ $\newcommand{\enscond}[2]{\lbrace #1, #2 \rbrace}$ $\newcommand{\pd}[2]{ \frac{ \partial #1}{\partial #2} }$ $\newcommand{\umin}[1]{\underset{#1}{\min}\;}$ $\newcommand{\umax}[1]{\underset{#1}{\max}\;}$ $\newcommand{\umin}[1]{\underset{#1}{\min}\;}$ $\newcommand{\uargmin}[1]{\underset{#1}{argmin}\;}$ $\newcommand{\norm}[1]{\|#1\|}$ $\newcommand{\abs}[1]{\left|#1\right|}$ $\newcommand{\choice}[1]{ \left\{ \begin{array}{l} #1 \end{array} \right. }$ $\newcommand{\pa}[1]{\left(#1\right)}$ $\newcommand{\diag}[1]{{diag}\left( #1 \right)}$ $\newcommand{\qandq}{\quad\text{and}\quad}$ $\newcommand{\qwhereq}{\quad\text{where}\quad}$ $\newcommand{\qifq}{ \quad \text{if} \quad }$ $\newcommand{\qarrq}{ \quad \Longrightarrow \quad }$ $\newcommand{\ZZ}{\mathbb{Z}}$ $\newcommand{\CC}{\mathbb{C}}$ $\newcommand{\RR}{\mathbb{R}}$ $\newcommand{\EE}{\mathbb{E}}$ $\newcommand{\Zz}{\mathcal{Z}}$ $\newcommand{\Ww}{\mathcal{W}}$ $\newcommand{\Vv}{\mathcal{V}}$ $\newcommand{\Nn}{\mathcal{N}}$ $\newcommand{\NN}{\mathcal{N}}$ $\newcommand{\Hh}{\mathcal{H}}$ $\newcommand{\Bb}{\mathcal{B}}$ $\newcommand{\Ee}{\mathcal{E}}$ $\newcommand{\Cc}{\mathcal{C}}$ $\newcommand{\Gg}{\mathcal{G}}$ $\newcommand{\Ss}{\mathcal{S}}$ $\newcommand{\Pp}{\mathcal{P}}$ $\newcommand{\Ff}{\mathcal{F}}$ $\newcommand{\Xx}{\mathcal{X}}$ $\newcommand{\Mm}{\mathcal{M}}$ $\newcommand{\Ii}{\mathcal{I}}$ $\newcommand{\Dd}{\mathcal{D}}$ $\newcommand{\Ll}{\mathcal{L}}$ $\newcommand{\Tt}{\mathcal{T}}$ $\newcommand{\si}{\sigma}$ $\newcommand{\al}{\alpha}$ $\newcommand{\la}{\lambda}$ $\newcommand{\ga}{\gamma}$ $\newcommand{\Ga}{\Gamma}$ $\newcommand{\La}{\Lambda}$ $\newcommand{\si}{\sigma}$ $\newcommand{\Si}{\Sigma}$ $\newcommand{\be}{\beta}$ $\newcommand{\de}{\delta}$ $\newcommand{\De}{\Delta}$ $\newcommand{\phi}{\varphi}$ $\newcommand{\th}{\theta}$ $\newcommand{\om}{\omega}$ $\newcommand{\Om}{\Omega}$
This numerical tour explores local differential operators (grad, div, laplacian) and their use to perform edge detection.
options(warn=-1) # turns off warnings, to turn on: "options(warn=0)"
library(imager)
library(png)
for (f in list.files(path="nt_toolbox/toolbox_general/", pattern="*.R")) {
source(paste("nt_toolbox/toolbox_general/", f, sep=""))
}
for (f in list.files(path="nt_toolbox/toolbox_signal/", pattern="*.R")) {
source(paste("nt_toolbox/toolbox_signal/", f, sep=""))
}
source("nt_toolbox/toolbox_wavelet_meshes/meshgrid.R")
options(repr.plot.width=3.5, repr.plot.height=3.5)
To obtain robust edge detection method, it is required to first remove the noise and small scale features in the image. This can be achieved using a linear blurring kernel.
Size of the image.
n <- 256*2
Load an image $f_0$ of $N=n \times n$ pixels.
f0 <- as.matrix(load_image("nt_toolbox/data/hibiscus.png",n))
Display it.
imageplot(f0)
Blurring is achieved using convolution: $$ f \star h(x) = \sum_y f(y-x) h(x) $$ where we assume periodic boundary condition.
This can be computed in $O(N\log(N))$ operations using the FFT, since $$ g = f \star h \qarrq \forall \om, \quad \hat g(\om) = \hat f(\om) \hat h(\om). $$
cconv <- function(f, h){
c <- fft(f)*fft(h)
return( Re(fft(c, inverse=T )/length(c)) ) }
Define a Gaussian blurring kernel of width $\si$: $$ h_\si(x) = \frac{1}{Z} e^{ -\frac{x_1^2+x_2^2}{2\si^2} }$$ where $Z$ ensure that $\hat h(0)=1$.
t <- c(0:round(n/2), (round(-n/2)+1):(-1))
X2 <- meshgrid_2d(t, t)$X ; X1 <- meshgrid_2d(t, t)$Y
normalize <- function(h){ h/sum(h) }
h <- function(sigma){ normalize(exp(-(X1**2 + X2**2)/ (2*sigma**2))) }
Define blurring operator.
blur <- function(f, sigma){ cconv(f, h(sigma)) }
Exercise 1
Test blurring with several blurring size $\si$.
options(repr.plot.width=7, repr.plot.height=7)
source("nt_solutions/segmentation_1_edge_detection/exo1.R")
## Insert your code here.
The simplest edge detectors only make use of the first order derivatives.
For continuous functions, the gradient reads $$ \nabla f(x) = \pa{ \pd{f(x)}{x_1}, \pd{f(x)}{x_2} } \in \RR^2. $$
We discretize this differential operator using first order finite differences. $$ (\nabla f)_i = ( f_{i_1,i_2}-f_{i_1-1,i_2}, f_{i_1,i_2}-f_{i_1,i_2-1} ) \in \RR^2. $$ Note that for simplity we use periodic boundary conditions.
Compute its gradient, using (here decentered) finite differences.
s <- c(n, 1:(n-1))
nabla <- function(f){
dx <- f - f[s,]
dy <- f - f[,s]
grad <- array(rep(0, length=2*n*n), c(n,n,2))
grad[,,1] <- dx ; grad[,,2] <- dy
return(grad)
}
One thus has $ \nabla : \RR^N \mapsto \RR^{N \times 2}. $
v <- nabla(as.matrix(f0))
One can display each of its components.
options(repr.plot.width=7, repr.plot.height=3.5)
imageplot(v[,,1], "d/dx", c(1,2,1))
imageplot(v[,,2], "d/dy", c(1,2,2))
A very simple edge detector is obtained by simply thresholding the gradient magnitude above some $t>0$. The set $\Ee$ of edges is then $$ \Ee = \enscond{x}{ d_\si(x) \geq t } $$ where we have defined $$ d_\si(x) = \norm{\nabla f_\si(x)}, \qwhereq f_\si = f_0 \star h_\si. $$
Compute $d_\si$ for $\si=1$.
sigma <- 1
d <- sqrt(apply(nabla(blur(as.matrix(f0), sigma))**2, c(1,2), sum))
Display it.
options(repr.plot.width=3.5, repr.plot.height=3.5)
imageplot(d)