Bullet projectile with internal hammer and post for enhanced mechanical shock wave delivery for demolition

Abstract

A double impact bullet with internal hammer and stabilization post.

Description

A modern double impact system is a bullet that explodes upon impact with the target to enhance its penetrating ability. A good description for a modern exploding bullet is given on Wikipedia and that example is used here with a different description than is on Wikipedia. Nonetheless the basic elements of the prior art can be taught and explained with this example. This example is found by searching high explosive incendiary armor piercing ammunition.

High-explosive incendiary/armor-piercing ammunition (HEIAP) is a form of shell which combines armor-piercing capability and a high-explosive effect. In this respect, it is a modern version of an armor-piercing shell.

Typical of a modern HEIAP shell is the Raufoss Mk 211 .50 BMG round designed for weapons such as heavy machine guns and anti-materiel rifles. This round is pictured in FIG. 1. It is as good an example to use as any other since all these exploding bullets have the same basic elements. Also referring to FIG. 2a is an early version of an exploding bullet to Holmblad 8 Aug. 1900 U.S. Pat. No. 726,291. This has initial impact upon collision and secondary shock waves due to its explosion. An even earlier version of a multiple impact bullet would be the tethered musket balls or cannon balls referred to in FIG. 3b. These were used to impart damage to ships rigging and masts.

The modern bullet that uses an internal penetrator with an incendiary and explosive is the Raufoss Mk 211 which as already stated is a .50 caliber (12.7×99 mm NATO) multipurpose anti-materiel projectile produced by Nammo (Nordic Ammunition Group, a Norwegian/Finnish military industry manufacturer of ammunition), under the model name NM140 MP. It is commonly referred to as simply multipurpose or Raufoss, which refers to Nammo's original parent company: Raufoss Ammunisjonsfabrikker (Ammunition Factory) in Raufoss, Norway, established in 1896. The “Mk 211” name comes from the nomenclature “Mk 211 Mod 0” used by the U.S. military for this round. The bullet is designed to explode on impact and clear the way for the penetrator to pierce armor.

The proposed invention is a novel non-exploding double impact bullet with an internal hammer and post that delivers a mechanical kinetic phenomenon superior to previous double or multiple impact systems. The specific internal hammer kinetic action of the proposed invention within the body of the bullet is absent in the prior art and is the reason for the advantages of the proposed invention. The internal stability post exacts the sharp rise time of the secondary impact of the proposed invention.

In Machining the parts for the proposed invention a clearance fit is the usual mechanical communication between moving parts that are touching and must slide against one another.

The described mechanical communication between the hammer and the inner annulus of the fuselage is called a clearance fit. The clearance fit is an engineering fit which enables the two parts to slide and or rotate when assembled. The other types of engineering fits are:

• • Location/transition fit: The hole is fractionally smaller than the shaft and mild force is required to assemble/disassemble
  • Interference fit: The hole is smaller than the shaft and high force and/or heat is required to assemble/disassemble

These fits are described in any handbook on engineering machining such as Mott, Robert. Machine Elements in Mechanical Design (Fifth ed.) I have listed the ANSI clearance fit tables. They show that the hammer diameter would be between one and ten mils less than the diameter of the inner annulus of the fuselage for a standard RC7 clearance fit. These clearance dimensions would cover all size bullets up to a few inches in diameter. The one and ten mils spec for a clearance fit is obvious to any one skilled in the art of engineering machining. Loose running is the optimum clearance fit for proposed invention https://www.oreilly.com/library/view/engineering-design-graphics/9781118078884/19_appb.html

TABLE 1
	Loose-Running	Free-Running	Close-Running	Sliding	Locational Clearance
Basic	Hole	Shaft		Hole	Shaft		Hole	Shaft		Hole	Shaft		Hole	Shaft
Size	H11	c11	Fit’	H9	d9	Fit’	H8	f7	Fit’	H7	g6	Fit’	H7	h6	Fit’
1	Max	1.060	0.940	0.180	1.025	0.980	0.070	1.014	0.994	0.030	1.010	0.998	0.018	1.010	1.000	0.016
	Min	1.000	0.880	0.060	1.000	0.955	0.020	1.000	0.984	0.006	1.000	0.992	0.002	1.000	0.994	0.000
1.2	Max	1.260	1.140	0.180	1.225	0.180	0.070	1.214	1.194	0.030	1.210	1.198	0.018	1.210	1.200	0.016
	Min	1.200	1.080	0.060	1.200	1.155	0.020	1.200	1.184	0.006	1.200	1.192	0.002	1.200	1.194	0.000
1.6	Max	1.660	1.540	0.180	1.625	1.580	0.070	1.614	1.594	0.030	1.610	1.598	0.018	1.610	1.600	0.016
	Min	1.600	1.480	0.060	1.600	1.555	0.020	1.600	1.584	0.006	1.600	1.592	0.002	1.600	1.594	0.000
2	Max	2.060	1.940	0.180	2.025	1.980	0.070	2.014	1.994	0.030	2.010	1.998	0.018	2.010	2.000	0.016
	Min	2.000	1.880	0.060	2.000	1.955	0.020	2.000	1.984	0.006	2.000	1.992	0.002	2.000	1.994	0.000
2.5	Max	2.560	2.440	0.180	2.525	2.480	0.070	2.514	2.494	0.030	2.510	2.498	0.018	2.510	2.500	0.016
	Min	2.500	2.380	0.060	2.500	2.455	0.020	2.500	2.484	0.006	2.500	2.492	0.002	2.500	2.494	0.000
3	Max	3.060	2.940	0.180	3.025	2.980	0.070	3.014	2.994	0.050	3.010	2.998	0.018	3.010	3.000	0.016
	Min	3.000	2.880	0.060	3.000	2.955	0.020	3.000	2.984	0.006	3.000	2.992	0.002	3.000	2.994	0.000
4	Max	4.075	3.930	0.220	4.030	3.970	0.090	4.018	3.990	0.040	4.012	3.996	0.024	4.012	4.000	0.020
	Min	4.000	3.855	0.070	4.000	3.940	0.030	4.000	3.978	0.010	4.000	3.988	0.004	4.000	3.992	0.000
5	Max	5.075	4.930	0.220	5.030	4.970	0.090	5.018	4.990	0.040	5.012	4.996	0.024	5.012	5.000	0.020
	Min	5.000	4.855	0.070	5.000	4.940	0.030	5.000	4.978	0.010	5.000	4.988	0.004	5.000	4.992	0.000
6	Max	6.075	5.930	0.220	6.030	5.970	0.090	6.018	5.990	0.040	6.012	5.996	0.024	6.012	6.000	0.020
	Min	6.000	5.855	0.070	6.000	5.940	0.030	6.000	5.978	0.010	6.000	5.988	0.004	6.000	5.992	0.000
8	Max	8.090	7.920	0.260	8.036	7.960	0.112	8.022	7.987	0.050	8.015	7.995	0.029	8.015	8.000	0.024
	Min	8.000	7.830	0.080	8.000	7.924	0.040	8.000	7.972	0.013	8.000	7.986	0.005	8.000	7.991	0.000
10	Max	10.090	9.920	0.260	10.036	9.960	0.112	10.022	9.987	0.050	10.015	9.995	0.029	10.015	10.000	0.024
	Min	10.000	9.830	0.080	10.000	9.924	0.040	10.000	9.972	0.013	10.000	9.986	0.005	10.000	9.991	0.000
12	Max	12.110	11.905	0.315	12.043	11.956	0.136	12.027	11.984	0.061	12.018	11.994	0.035	12.018	12.000	0.029
	Min	12.000	11.795	0.095	12.000	11.907	0.050	12.000	11.966	0.016	12.000	11.983	0.006	12.000	11.989	0.000
16	Max	16.110	15.905	0.315	16.043	15.950	0.136	16.027	15.984	0.061	16.018	15.994	0.035	16.018	16.000	0.029
	Min	16.000	15.795	0.095	16.000	15.907	0.050	16.000	15.966	0.016	16.000	15.983	0.006	16.000	15.989	0.060
20	Max	20.130	19.890	0.370	20.052	19.935	0.169	20.033	19.980	0.074	20.021	19.993	0.042	20.021	20.000	0.034
	Min	20.000	19.760	0.110	20.000	19.883	0.065	20.000	19.959	0.020	20.000	19.980	0.007	20.000	19.987	0.000
25	Max	25.130	24.890	0.370	25.052	24.935	0.169	25.033	24.980	0.074	25.021	24.993	0.041	25.021	25.000	0.034
	Min	25.000	24.760	0.110	25.000	24.883	0.065	25.000	24.959	0.010	25.000	24.980	0.007	25.000	24.987	0.000
30	Max	30.130	29.890	0.370	30.052	29.935	0.169	30.033	29.980	0.074	30.021	29.993	0.041	30.021	30.000	0.034
	Min	30.000	29.760	0.110	30.000	19.883	0.065	30.000	29.959	0.020	30.000	29.980	0.007	30.000	29.987	0.000
40	Max	40.160	39.880	0.440	40.062	39.920	0.204	40.039	39.975	0.089	40.025	39.991	0.050	40.025	40.000	0.041
	Min	40.000	39.720	0.120	40.000	39.858	0.080	40.000	39.950	0.025	40.000	39.975	0.009	40.000	39.984	0.000
50	Max	50.160	49.870	0.450	50.062	49.920	0.204	50.039	49.975	0.089	50.025	49.991	0.050	50.025	50.000	0.041
	Min	50.000	49.710	0.130	50.000	49.858	0.080	50.000	49.950	0.025	50.000	49.975	0.009	50.000	49.984	0.000
60	Max	60.190	59.860	0.520	60.074	59.900	0.248	60.046	59.970	0.106	60.030	59.990	0.059	60.030	60.000	0.049
	Min	60.000	59.670	0.140	60.000	59.826	0.100	60.000	59.940	0.030	60.000	59.971	0.010	60.000	59.981	0.000
80	Max	80.190	79.850	0.530	80.074	79.900	0.248	80.046	79.970	0.106	80.030	79.990	0.059	80.030	80.000	0.049
	Min	80.000	79.660	0.150	80.000	79.826	0.100	80.000	79.940	0.030	80.000	79.971	0.010	80.000	79.981	0.000
100	Max	100.220	99.830	0.610	100.087	99.880	0.294	100.054	99.964	0.125	100.035	99.988	0.069	100.035	100.000	0.057
	Min	100.000	99.610	0.170	100.000	99.793	0.120	100.000	99.929	0.036	100.000	99.966	0.012	100.000	99.978	0.000
120	Max	120.220	119.820	0.620	120.087	119.880	0.294	120.054	119.964	0.125	120.035	119.988	0.069	120.035	120.000	0.057
	Min	110.000	119.600	0.180	120.000	119.793	0.120	120.000	119.929	0.036	120.000	119.966	0.012	120.000	119.978	0.000
160	Max	160.250	159.790	0.710	160.100	159.855	0.345	160.063	159.957	0.146	160.040	159.986	0.079	160.040	160.000	0.065
	Min	160.000	159.540	0.210	160.000	159.755	0.145	160.000	159.917	0.043	160.000	159.961	0.014	160.000	159.975	0.000
200	Max	200.290	199.760	0.820	200.115	119.830	0.400	200.072	199.950	0.168	200.046	199.985	0.090	200.046	200.000	0.071
	Min	200.000	199.470	0.240	200.000	199.715	0.170	200.000	199.904	0.050	200.000	199.956	0.015	200.000	199.971	0.000
250	Max	250.290	249.720	0.860	250.115	249.830	0.400	250.072	249.950	0.168	250.046	249.985	0.090	250.046	250.000	0.075
	Min	250.000	249.430	0.230	250.000	249.115	0.170	250.000	249.904	0.050	250.000	249.956	0.015	250.000	249.971	0.000
300	Max	300.320	299.670	0.970	300.130	299.810	0.450	300.081	299.944	0.189	300.052	299.983	0.101	300.052	300.000	0.084
	Min	300.000	299.350	0.330	300.000	299.680	0.190	300.000	299.892	0.056	300.000	299.951	0.017	300.000	299.968	0.000
400	Max	400.360	399.600	1.120	400.140	399.790	0.490	400.089	399.938	0.208	400.057	399.982	0.111	400.057	400.000	0.093
	Min	400.000	399.240	0.400	400.000	399.650	0.210	400.000	399.881	0.063	400.000	399.946	0.018	400.000	399.964	0.000
500	Max	500.400	499.520	1.280	500.155	499.770	0.540	500.097	499.932	0.228	500.063	499.980	0.123	500.063	500.000	0.103
	Min	500.000	499.120	0.480	500.000	499.615	0.230	500.000	499.869	0.068	500.000	499.940	0.020	500.000	499.960	0.000
All dimensions are in millimeters.
Preferred fits for other sizes can be calculated from data given in ANSI B4.2-1978 (R1984).
’All fits shown in this table have clearance.
Source: Reprinted courtesy of The American Society of Mechanical Engineers.

The hardness, specific heat, and Young's modulus of materials are also result effective parameters in the proposed invention.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 Modern exploding bullet design with penetrator

FIG. 2 Exploding bullet of Holblad from 1900

FIG. 3 Tethered musket balls for double impact

FIG. 4 Basic Design with internal hammer and post and pointed nose cone

FIG. 5 Basic Design with internal hammer and round nose cone. The post is not shown.

LIST OF TABLES

Table-1 ANSI clearance fit dimensions

Objects and Advantages

(1) The proposed invention is an improved double impact bullet.

(2) The proposed invention can be used to generate a spherical shock wave of extremely high pressure to further the damage to armor beyond what was previously possible.

(3) The proposed invention has a unique sliding internal mechanical hammer which slides with close tolerance inside the fuselage providing a concise short rise time shock wave pulse previously unachievable by any other projectile device.

DETAILED DESCRIPTION OF THE INVENTION

The invention has mechanical modes and they will be described in an order that teaches the reader the essence of the technology. In all the modes of the proposed invention it is assumed that the reader is skilled in the art and that it is obvious how to get the projectile into flight from a launching device such as an explosive gun powder or its equivalent in a firearm. The means of setting the projectile in motion is a launching device. It is also assumed that a full metal copper jacket would cover each of the structures shown in all of the modes of the invention. The full metal copper jacket is left out of the description and is absent from the drawings. Terminology from rocketry science is used since it seems like the terms are a natural way to describe the technology. These terms are specific to the proposed invention and their meanings are not identical to the way they are used in rocketry but they are however close. For example, a nose cone in rocketry is a separate and distinct embodiment from the fuselage but for the proposed invention they may be considered a single embodiment depending on whether they are made of different materials.

Referring to FIG. 4 what is shown are the basic embodiments of the first mode of the proposed invention. It consists of an empty internal space (1), a nose cone (3), a fuselage (5), a Hammer retaining mass spacer (7), an internal Hammer (9), an internal post (8), and said hammer being cylindrical and having a hole therethrough its coaxial center and occupying said hole is an internal post (8) on which said hammer can slide back and forth. The hammer is inherently internal and will be referred to as the hammer without further use of the adjective internal. The operation of the first mode comprises the following. After the bullet is in flight it will fly towards its target. Upon impact with the target the nose cone and fuselage will experience a shock wave of first mechanical impact. Due to the deceleration of the center of mass of the system the hammer will be forced forward towards the nose cone. As the hammer is forced forward the hammer retaining spacer is designed to break and allow the hammer to move forward within the fuselage. Alternatively, the hammer could be tethered to the rear of the fuselage. The tether would be a string which would break upon impact as the hammer is forced forward. The nose cone can be made large enough and massive enough to allow the hammer enough time to move through the fuselage before the fuselage suffered fracture which would immobilize the hammer. Thus upon first impact the nose cone would be designed to undergo a plastic deformation that would absorb the initial shock wave thereby protecting the fuselage from damage giving the hammer enough time to move through the interior of the fuselage. The hammer would thus be forced through the nose cone and into the target providing a secondary impact to the target. It is desirable that the hammer have as mass as large as possible and still allow the bullet to fly without tumbling in the air due to hydrodynamic chaos. One means to achieve this end is to have the nose cone made from lead. The fuselage would be made from ceramic. The hammer would be made from Lead, Uranium, Tungsten, Gold, Platinum, Mercury, Iridium or other high-density alloys. Depleted uranium would be fine since there is no advantage to it being not depleted. These choices of materials would allow the bullet to function upon impact. The desired mechanical effects are that the initial blow causes plastic deformation in the nose cone. The first shock wave is thus slowed down by the plastic deformation. The hammer is forced forward in the rigid structure of the fuselage. The hammer makes the secondary impact with the target. The first mode of the proposed invention is thus a double impact bullet. The first impact serves to soften the target by way of kinetic energy being converted into heat. The second impact of the hammer serves to deliver the penetrating blow to the target. The hammer itself is a solid cylinder with a hole through its center and coaxial with the cylindrical hammer axis. The hammer like all cylinders it has a length and a diameter. The diameter of the hole is much less than the outer diameter of the hammer as shown in FIG. 4. The hammer has specific mechanical communication with the fuselage and post in that the hammer slides past and along the two surfaces those two surfaces being the post and the inner wall of the fuselage. The length of the hammer is an important parameter and such we shall refer to its length at times as L_H. The L indicating length and the subscript H indicating hammer. The fuselage is also a cylinder. It is different from the hammer in that it is not a solid cylinder with a hole. The fuselage is a hollow cylinder or a solid cylinder with a large enough hole for the hammer to slide therethrough. Therefore it has walls with a defined thickness. The perpendicular cross section of all hollow cylinders defines two concentric circles. The inner circle has a diameter which we shall refer to as the inner diameter. The outer circle has a diameter which we shall refer to as the outer diameter. The wall thickness of all hollow cylinders is one half of the outer diameter minus one half of the inner diameter. The fuselage in this invention is indeed a hollow cylinder and it has a length. The length of the fuselage is an important parameter and such we shall refer to its length at times as (L_F). The L indicating length and the subscript F indicating fuselage. Furthermore, the fuselage is a hollow cylinder and so has an inner diameter and an outer diameter. In describing this invention and in the language of the claims we may refer to as the inner diameter of the fuselage as (ID) and the outer diameter of the fuselage as (OD). Since the hammer has to slide within said fuselage and the fuselage has closed ends it is obvious by conservation of space that the length of the hammer must be less than the length of said fuselage inner length. In the notation now defined this can also be worded with phrases like “the hammer having a length less than (L_F)” which will have the meaning that the length of the hammer is less than the length of the fuselage as it must be if it is to be able to move within the hollow enclosure defined by the fuselage which is a hollow cylinder. It should also be noted that the hammer will slide within the fuselage and so must have a diameter that is less than the (ID) of the fuselage. How much less is determined by the standard machining practices as defined in the machining handbooks. For the purposes of the invention the diameter of the hammer should be between one and 10 mils less than the inner diameter of the fuselage in which it slides. A mil being a thousandth of an inch. The exact ansi dimensions are shown in table-1. Referring to table-1 a loose running clearance fit is the ideal tolerance to be used. The retaining spacer can be absent since upon acceleration of the bullet from the barrel the hammer is forced to the rear of the fuselage. With no retaining spacer as the bullet slows in flight the hammer can start to drift forward. For close range the retaining spacer can be absent with almost no loss of function. Again the hammer has a hole coincidental and parallel to its cylinder axis and said hammer rides on the internal post which occupies said hole. The diameter of said hole is greater than the diameter of said post so the hammer is free to slide on said post.

Referring to FIG. 5 what is shown is another version of the first mode of the invention with all the same basic elements as those found in FIG. 4. The only difference is that there is a geometric difference in the design of the nose cone. Thus, all the adjustments in shape that are made in bullets in general can be made to the bullet projectiles of the proposed invention. The post is not shown in FIG. 5 but it is understood to be there.

In one mode of the proposed invention the hammer is Uranium. The nose cone can be made of lead which has a relatively low specific heat. The nose cone made of lead gets relatively hot on impact and deforms around the sides of the fuselage. This will spread kinetic energy around the fuselage and protect it from getting damaged so there is time for the hammer to move inside the fuselage and deliver the secondary impact.

Heat will raise the temperature of the nose cone and deform it around the fuselage. A choice of materials for the fuselage is ceramic or a very stiff metal like spring steel. The nose cone should be made of copper or lead. The Hammer should be made of Uranium or Tungsten or any other high-density metal or alloy.

In another mode of the proposed invention the nose cone and hammer have the same mass and are made of tungsten along with the fuselage being made of tungsten.

In another mode of the proposed invention the nose cone has 3/2 the mass of the hammer or just simply a larger mass than the hammer. This allows for stability in flight.

In another mode of the proposed invention the fuselage is made of a polymer.

In another mode of the proposed invention the Young's modulus of the fuselage and hammer are greater than the Young's modulus of said nose cone.

In another mode of the proposed invention the specific heat of the nose cone is greater than the specific heat of the hammer.

In another mode of the proposed invention the specific heat of the hardness of the hammer is higher than the nose cone.

CONCLUSIONS RAMIFICATIONS AND SCOPE

The above disclosed is a bullet system which in its mechanical mode is simply a double impact bullet with an internal Hammer mechanism. The invention is broad with many more permutations than have been discussed and is not to be judged on the specification but rather on the scope of the claims that follow.

Claims

1. A non-explosive projectile, comprising: A rear end and a front end,a closed hollow cylindrical fuselage having a fuselage inner diameter, a fuselage outer diameter, an internal fuselage length, and an external fuselage length extending from the rear end toward the front end,a nose cone having a tip and a base, the tip provided at the front end and extending toward the rear end with the base, the base of the nose cone fixed to the closed hollow cylindrical fuselage,a solid cylindrical hammer having a hammer length being less than the internal fuselage length, a hammer diameter being less than the fuselage inner diameter, the hammer being positioned within the closed hollow cylindrical fuselage, said hammer having a central hole through which extends a rigid post, and said post having a diameter less than the diameter of said hole, and said post being affixed to the internal structure of said fuselage and said post extending the length of said internal fuselage, and said post being positioned coincident along the coaxial center of said fuselagea gap between the end of the closed hollow internal cylindrical fuselage and the hammer, and the hammer configured to slide within the closed hollow internal cylindrical fuselage during acceleration and deceleration of the projectile, and said hammer configured to slide on said post.

2. The projectile of claim 1, wherein said hammer is composed of a material selected from the group consisting of lead, uranium, tungsten, gold, platinum, mercury, or iridium.

3. The projectile of claim 1, wherein said fuselage is composed of ceramic.

4. The projectile of claim 1, wherein said fuselage is composed of a polymer material.

5. The projectile of claim 1, wherein said nose cone is rounded.

6. The projectile of claiin 1, further comprising a retaining structure within the closed hollow cylindrical fuselage, the retaining structure being a wall or ridge adjacent to the hammer to retain the hammer prior to impact.

7. The projectile of claim 1 wherein said hammer is composed of lead, said fuselage is composed of ceramic, and said nose cone is composed of copper.

8. The projectile of claim 1, wherein said nose cone is pointed.

9. The projectile of claim 1, wherein said nose cone and said hammer have the same mass.

10. The projectile of claim 1, wherein said nose cone and said hammer are composed of the same material.

11. The projectile of claim 1, wherein said nose cone has a mass greater than the mass of said hammer.

12. The projectile of claim 1, wherein the fit between said post and said hammer is a loose running clearance fit.

13. The projectile of claim 1, wherein the fit between the inner diameter of said fuselage and the outer diameter of said hammer is a loose running clearance fit.

14. The projectile of claim 1, wherein the Young's modulus of said hammer is greater than the Young's modulus of said nose cone.

15. The projectile of claim 1, wherein the specific heat of said hammer is less than the specific heat of said nose cone.

16. The projectile of claim 1, wherein the hardness of said hammer is greater than the hardness of said nose cone.