From the earliest days of radiology the reduction of the amount of scattered radiation reaching the film has engaged the attention of both radiologists and apparatus manufacturers. The interposition of a grid between patient and film has been the device most widely used for this purpose, and much effort has been devoted to the improvement of grids both in design and manufacture. Nevertheless, despite the pleas made at intervals in the radiological literature for the introduction of a method of specifying the performance of a grid in terms of its ultimate effect upon the radiograph, it is still customary to define the grid simply in terms of its “ratio”, the number of lines to the inch, and, where appropriate, the radius. In practice differences in film quality are frequently caused by differences between grids that are nominally the same as judged by these parameters. The evidence available suggests that only a grid of exceptional quality, whose stated ratio would be about 10 : 1, would be suitable for use over the wide range of kilovoltage say, 60 to 120, now being used. Because of the difficulty in selecting such a grid a high ratio grid is frequently used for all work regardless of the kilovoltage. In most cases such grids absorb a higher proportion of the image-forming radiation than do low ratio grids.