The distance d was usually understood to limit the error-correction capability to ⌊d/2⌋.

We must then obtain the contribution of additional compensatory mutations at distance d + 1.

Consider two opposing point forces F at a distance d apart.

Now, let the distance d approach the limit zero, while M is kept constant.

If we then wish to stop it in a distance d, we must do an equal amount of negative work on the weight.

The overall distance "d" is the distance between levels of the graph.

Select the node n whose distance d from this input is least.

Let us put now a sheet of opposite charge a distance d away from the first sheet (fig. 2.14).

As the distance d approaches λ/4, the wavefront starts becoming narrower.

First the observer measures a straight-line distance D from some observation point O to the object.