Now consider a portion of a **cylindric** film of length x terminated by two equal disks of radius r and containing a certain volume of air.

Now let us consider a **cylindric** film contained between two equal fixed disks A and B, and let a third disk, C, be placed midway between.

Hence if the length of the **cylindric** film is less than its circumference, it is in stable equilibrium.

But if the length of the **cylindric** film is greater than its circumference, and if we suppose the disk C to be placed midway between A and B, and to be moved towards A, the pressure on the side next A will diminish, and that on the side next B will increase, so that the resultant force will tend to increase the displacement, and the equilibrium of the disk C is therefore unstable.

Hence the equilibrium of a **cylindric** film whose length is greater than its circumference is unstable.

But the surface-tension, acting on a **cylindric** column of liquid whose length exceeds the limit of stability, begins to produce enlargements and contractions in the stream as soon as the liquid has left the orifice, and these inequalities in the figure of the column go on increasing till it is broken up into elongated fragments.

Vegetative cells **cylindric** (rodlets), ellipsoid or ovoid, and straight.

Sporogenous rodlets **cylindric**, not altered in shape: - Bacillus (Cohn), non-motile; Bactrinium (Fischer), motile, with one polar flagellum (monotrichous); Bactrillum (Fischer), motile, with a terminal tuft of cilia (lophotrichous); Bactridium (Fischer), motile, with cilia all over the surface (peritrichous) .

Vegetative cells, **cylindric** but curved more or less spirally.