UNDERSTANDING ABOUT THE OGIVES OF THE PROJECTILES
UNDERSTANDING ABOUT THE OGIVE OF THE PROJECTILES
The ogive in the context of projectiles
refers to the curved, tapered shape of a projectiles nose or front section. It
is a crucial design feature that influences the aerodynamic performance,
stability, and efficiency of a projectile as it moves through air or other
media.
An ogive is a curved that connects the cylindrical body of a
projectile to its pointed tip. It is designed to reduce drag by allowing air
flow smoothly around the projectile, minimizing turbulence and energy loss.
In engineering and ballistics, the ogive refers to the
curved or conical shape of the forward nose section of a projectile, such as a
projectile, missile, or artillery shell. The design and characteristics of the
ogive play a crucial role in determining the projectiles aerodynamic
efficiency, stability, and overall performance.
Definition and Geometrical Basis: The term ogive
originates from architecture, referring to a pointed, arch-like shape. In
projectiles, the ogive is the curve or contour that transitions form the
projectiles cylindrical body to its tip. This shape reduces drag by providing a
smooth airflow around the projectile during its flight.
To find the ogive number generally we can use the
formula
Ogive number = R / D
R is the radius of
curvature and D is the diameter of the projectile, for military projectile the
ogive number falls between 0.5 to 1.0 and for sporting and long range
projectiles the ogive number falls between 1.0 to 2.0
Ogive profiles are usually defined mathematically
using geometric curves like:
Circular or tangent ogive: Formed by a portion of a circle.
Elliptical ogive: Part of an ellipse.
Parabolic ogive: Derived from a parabola for better supersonic
performance.
Secant ogive: A circular curve that intersects the cylindrical body
rather than being tangent to it, reducing drag further.
The ogive shape significantly impacts the projectiles
drag coefficient; in aerodynamics a sharper ogive minimizes drag but can reduce
structural strength. And blunter ogives may produce more drag but provide
better structural integrity and stability.
Supersonic Flight Stability: Pointed ogives like parabolic and secant designs
perform well at high speeds.
Range and Accuracy: A well-designed ogive reduces aerodynamic drag,
extending the range and improving accuracy.
Mach Number Adaptation: The optimal ogive shape depends on the speed range of
the projectile, particularly whether it operates in subsonic, transonic, or
supersonic regimes.
Here are the essential mathematical equations for an
ogive-shaped nose in projectile design.
Round Nose Ogive: A classic, semi-circular curve that is less
aerodynamic than other ogives, the main advantages are reliable feeding in
lever action and semi-automatic firearms and high energy transfer on impact.
For a round nose ogive, the curve is a segment of a
circle. To calculate the length of the curve, you can use the formula for the
arc length of a circle.
Arc length S = R x theta
S = is the arch length (the length of the round nose
ogive)
R = radius of the circular arc.
Theta = is the central angle of the arc (in radians)
The angle theta can be calculated based on the
dimensions of the ogive (like the desired nose length) and the overall design.
For simplicity, the round nose ogive will generally be a small segment of the
full circle.
You can calculate the height h of the ogive
(form the tip of the base of the curve) using the following relation, assuming
the circular arc is symmetric.
Height of the round nose
h = R. (1- Cos (theta / 2)
h is the vertical height from the center of the circle
to the tip of the projectiles nose.
R is the radius of the circle.
Theta is the central angle in radians (the same angle
as in the arc length formula)
Spitzer Ogive: Spitzer ogive refers to a pointed nose shape that is
more aerodynamically efficient compared to round nose or blunt designs. The
term spitzer is derived from the German word spitz meaning sharp or pointed.
The ogive is the curved section of the projectile nose, and in a spitzer
design, this curve is often a secant ogive, which has more pronounced, sharper
point compared to a tangent ogive. The curve of a spitzer ogive typically
intersects the projectile body at an angle, leading to a more gradual
transition between the nose and the cylindrical body. The sharp point at the
tip of the projectile allows for reduced air resistance as the projectile
travels through the atmosphere. The angle of the point is critical in
determining the projectiles aerodynamic performance. A sharper point reduces
drag but might increases the tendency to tumble upon impact unless designed for
controlled expansion for fragmentation. The main advantages of the spitzer
shape is Lower drag, High Ballistic Co efficient and Improve accuracy.
To calculate the height of the ogive that is base to
the tip of the projectile.
h = R. (1 – cos (theta / 2)
h is the height of the ogive.
R radius of the circle defining the ogive.
Theta is the central angle of the arc in radians.
To calculate the arc length of the projectile is
L = R. Theta
L is the length of the ogive from the tip to the
transition to the cylindrical body.
Theta is the central angle of the arc in radians.
To calculate the central angle of the projectile is
Theta = 2. arccos (1- h/R)
Tangent Ogive: The tangent ogive shape is the most familiar in
projectiles, the profile of this shape is formed by a segment of a circle such
that the projectile body is tangent to the curve of the nose cone at its base,
and the base is on the radius of the circle. The popularity of this shape is
largely due to the ease of constructing its profile, as it is simply a circular
section.
The radius of the circle
that forms the ogive is called the ogive radius, ρ, and
it is related to the length and base radius of the nose cone as expressed by
the formula:
The radius y at any point x, as x varies from 0 to L is:
The nose cone
length, L, must be less than or equal to ρ. If they are
equal, then the shape is hemisphere.
L is
the overall length of the nose cone
R is
the radius of the base of the nose cone.
y is
the radius at any point x, as x varies
from 0, at the tip of the nose cone, to L.
The equations define the
two-dimensional profile of the nose shape. The full body of revolution of
the nose cone is formed by rotating the profile around the center line C⁄L.
While the equations
describe the "perfect" shape, practical nose cones are often blunted
or truncated for manufacturing, aerodynamic, or thermodynamic reasons.
Spherically Blunted
Tangent Ogive or Soft Point: A tangent ogive nose is
often blunted by capping it with a segment of a sphere. The tangency
points where the sphere meets the tangent ogive can be found from:
L is
the overall length of the nose cone
R is
the radius of the base of the nose cone.
y is
the radius at any point x, as x varies
from 0, at the tip of the nose cone, to L.
where rn is
the radius and xo are the center of the spherical
nose cap.
Secant Ogive: The
profile of this shape is also formed by a segment of a circle, but the base of
the shape is not on the radius of the circle defined by the ogive radius. The Projectile
body will not be tangent to the curve of the nose at its base.
The ogive radius ρ is not determined by R and L (as
it is for a tangent ogive), but rather is one of the factors to be chosen to
define the nose shape. If the chosen ogive radius of a secant ogive is greater
than the ogive radius of a tangent ogive with the same R and L,
then the resulting secant ogive appears as a tangent ogive with a portion of
the base truncated.
Secant ogive nose cone render and profile with parameters and ogive circle shown above
Alternate
secant ogive render and profile which show a bulge due to a smaller radius
shown above
Then the radius y at any point x as x varies
from 0 to L is:
If the chosen ρ is less than the tangent ogive ρ and greater than half the length of the nose cone, then the result will be a secant ogive that bulges out to a maximum diameter that is greater than the base diameter. A classic example of this shape is the nose cone of Honest John.
Elliptical Ogive: The
profile of this shape is one-half of an ellipse, with the major axis being the
centreline and the minor axis being the base of the nose cone. A rotation of a
full ellipse about its major axis is called a prolate spheroid, so an
elliptical nose shape would properly be known as a prolate hemispheroid. This
shape is popular in subsonic flight (such as model rocketry) due to the blunt
nose and tangent base. [further explanation needed] This is not a shape
normally found in professional rocketry, which almost always flies at much
higher velocities where other designs are more suitable. If R equals L, this is
a hemisphere
An elliptical ogive is a
nose cone generated by the segment of an ellipse where, the base of the ogive
lies along the minor axis of the ellipse and the curve extends from the base to
the tip, forming a smooth continuous shape.
Descriptive Geometry of the Spitzer Projectile:
Ogive: The ogive shape forms the front of the bullet. The ogive shape is formed from the arcs of two circles. The ogive may or may not be tangent at the point of intersection to the cylindrical portion of the bullet. When the circles are tangent to the cylinder portion, we call say this is a tangent ogive. When the circles are not tangent to the cylinder portion, we say we have a secant ogive. The rationale behind the use of the term "secant" can be seen in Figure 6, where there are two horizontal reference lines (brown colour) that are both secant lines.
Cylinder: The cylindrical portion of the bullet is what engages the rifling of the barrel.
Frustum: The back of the bullet (aka "boattail") geometrically is in the shape of the frustrum of the cone Tapering the back of the bullet reduces drag, particularly at speeds less than supersonic.
Projectile Mass Calculation:
We will compute the volume of the spitzer bullet as follows.
Compute the volume of the frustum portion (VFrustum)
Compute the volume of the cylinder portion (VCylinder)
Compute the volume of the ogive portion (VOgive)
Compute the total volume by summing all the volumes of the pieces
Compute the mass using the density of lead Frustum Volume: Cylinder Volume:Ogive Volume:
The ogives circular arc is not tangent to the cylinder at the point of intersection. This case results in a rather pointy projectile.
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