alloy
driving band around its base, indicating clockwise spin equipped with winglets inside the bore of a rifled cannon c. 1860 , 1858, designed to engage with clockwise rifling For best performance, the barrel should have a twist rate sufficient to spin-stabilize any
bullet that it would reasonably be expected to fire, but not significantly more. Large-diameter bullets provide more stability, as the larger radius provides more
gyroscopic inertia. In contrast, long bullets are harder to stabilize, as they tend to be very back-heavy and the aerodynamic pressures have a longer arm ("lever") to act on. The slowest twist rates are found in
muzzle-loading firearms meant to fire a round ball; these will have twist rates as low as 1 in , or slightly longer, although for a typical multi-purpose muzzleloader rifle, a twist rate of 1 in is very common. The
M16A2 rifle, which is designed to fire the
5.56×45mm NATO SS109 ball and L110 tracer bullets, has a 1 in or 32 calibers twist. Civilian
AR-15 rifles are commonly found in 1 in (54.8 cal) for older rifles and 1 in (41.1 cal) for most newer rifles. However, some are made with 1 in or 32-caliber twist rates, the same as those used for the M16 rifle. Rifles, which generally fire longer, smaller diameter bullets, will in general have higher twist rates than handguns, which fire shorter, larger diameter bullets. There are three methods in use to describe the twist rate: Traditionally, the most common method expresses the twist rate in terms of the 'travel' (length) required to complete one full revolution of the projectile in the rifled barrel. This method does not provide a straightforward understanding of whether a twist rate is
relatively slow or fast when comparing bores of different diameters. The second method describes the 'rifled travel' required to complete one full projectile revolution in calibers or bore diameters: \text{twist} = \frac{L}{D_\text{bore}}, where \text{twist} is the twist rate expressed in bore diameters; L is the twist length required to complete one full projectile revolution (in mm or in); and D_\text{bore} is the bore diameter (diameter of the lands, in mm or in). The twist travel L and the bore diameter D_\text{bore} must be expressed in a consistent unit of measure, i.e. metric (mm)
or imperial (in). The third method simply reports the angle of the grooves relative to the bore axis, measured in degrees. The latter two methods have the inherent advantage of expressing twist rate as a ratio and provide an easy way to understand whether a twist rate is
relatively slow or fast, even when comparing bores of differing diameters. In 1879,
George Greenhill, a professor of mathematics at the
Royal Military Academy (RMA) at Woolwich, London, UK developed a
rule of thumb for calculating the optimal twist rate for lead-core bullets. This shortcut uses the bullet's length and requires no allowances for weight or nose shape The eponymous
Greenhill Formula, still used today, is: \text{twist} = \frac{C D^2}{L} \times \sqrt{\frac{\mathrm{SG}}{10.9}} where C is 150 (use 180 for muzzle velocities higher than 2,800 f/s); D is the bullet's diameter in inches; L is the bullet's length in inches; and \mathrm{SG} is the bullet's
specific gravity (10.9 for lead-core bullets, which cancels out the second half of the equation). The original value of C was 150, which yields a twist rate in inches per turn, when given the diameter D and the length L of the bullet in inches. This works up to velocities of about 840 m/s (2800 ft/s); above those velocities, a C of 180 should be used. For instance, with a velocity of 600 m/s (2000 ft/s), a diameter of and a length of , the Greenhill formula would give a value of 25, which means 1 turn in . Improved formulas for determining stability and twist rates include the
Miller Twist Rule and the McGyro program developed by Bill Davis and Robert McCoy. , used by both
Confederate and
Union forces in the
American Civil War. If an insufficient twist rate is used, the bullet will begin to
yaw and then tumble; this is usually seen as "keyholing", where bullets leave elongated holes in the target as they strike at an angle. Once the bullet starts to yaw, any hope of accuracy is lost, as the bullet will begin to veer off in random directions as it
precesses. Conversely, a rate of twist that is too high can also cause problems. The excessive twist can cause accelerated barrel wear and, coupled with high velocities, induce a very high spin rate, which can lead to projectile
jacket ruptures, causing high-velocity spin-stabilized projectiles to disintegrate in flight. Projectiles made of a single metal cannot practically achieve flight and spin velocities high enough to cause disintegration in flight.
Smokeless powder can produce muzzle velocities of approximately for spin stabilized projectiles and more advanced propellants used in
smoothbore tank guns can produce muzzle velocities of approximately . A higher twist than needed can also cause more subtle problems with accuracy; any inconsistency within the bullet, such as a void that causes an unequal distribution of mass, may be magnified by the spin. Undersized bullets also have problems, as they may not enter the rifling exactly
concentric and
coaxial to the bore, and excess twist will exacerbate the accuracy problems this causes. A bullet fired from a rifled barrel can spin at over 300,000
rpm (5
kHz), depending on the bullet's
muzzle velocity and the barrel's
twist rate. The general definition of the spin S of an object rotating around a single axis can be written as: S = \frac{\upsilon}{C} where \upsilon is the linear
velocity of a point in the rotating object (in units of distance/time) and C refers to the circumference of the circle that this measuring point performs around the axis of rotation. A bullet that matches the rifling of the firing barrel will exit that barrel with a spin: S = \frac{\upsilon_0}{L} where \upsilon_0 is the muzzle velocity and L is the twist rate. For example, an M4 Carbine with a twist rate of 1 in and a muzzle velocity of will give the bullet a spin of 930 m/s / 0.1778 m ≈ 5.230 kHz (313,835 rpm). Excessive rotational speed can exceed the bullet's designed limits, and the resulting centrifugal force can cause the bullet to disintegrate radially during flight. == Design ==