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Optical Flow Constraint Equation

Let us suppose that the image intensity is given by I(x,y,t), where the intensity is now a function of time, t, as well as of x and y.

At a point a small distance away, and a small time later, the intensity is
equation1295
where the dots stand for higher order terms.

Now, suppose that part of an object is at a position (x,y) in the image at a time t, and that by a time dt later it has moved through a distance (dx,dy) in the image.

Furthermore, let us suppose that the intensity of that part of the object is just the same in our image before and afterwards.

Provided that we are justified in making this assumption, we then have that
equation1303
and so
equation1305

However, dividing through by dt, we have that
equation1313
as these are the speeds the object is moving in the x and y directions respectively. Thus, in the limit that dt tends to zero, we have
equation1319
which is called the optical flow constraint equation.

Now, tex2html_wrap_inline3706 at a given pixel is just how fast the intensity is changing with time, while tex2html_wrap_inline3708 and tex2html_wrap_inline3710 are the spatial rates of change of intensity, i.e. how rapidly intensity changes on going across the picture, so all three of these quantities can be estimated for each pixel by considering the images.



tex2html_wrap_inline2984 David Marshall 1994-1997