Minggu, 26 Februari 2012

Warhead


Types of warheads include:
  • Explosive: An explosive charge is used to disintegrate the target, and damage surrounding areas with a shock wave.
    • Conventional: Chemicals such as gunpowder and high explosives store significant energy within their molecular bonds. This energy can be released quickly by a trigger, such as an electric sparkThermobaric weapons are something of a special case.
      • Blast: A strong shock wave is provided by the detonation of the explosive
      • Fragmentation: Metal fragments are projected at high velocity to cause damage or injury.
      • Continuous rod: Metal bars welded on their ends forming a compact cylinder of interconnected rods, which is violently expanded into a contiguous "zig-zag" shaped ring by an explosive detonation. The rapidly expanding ring produces a unique planar "guillotine" effect that is particularly devastating against military aircraft, which are designed to be resistant to traditional shrapnel.
      • Shaped charge: The effect of the explosive charge is focused onto a specially shaped metal liner to project a hypervelocity jet of metal, to perforate heavy armour.
        • Explosively formed penetrator: Instead of turning a thin metal liner into a focused jet of metal plasma, the shaped charge is directed against a concave metal plate at the front of the warhead, propelling it at super high-velocity while simultaneously deforming it into a dense ogive projectile
    • Nuclear: A runaway nuclear fission or nuclear fusion reaction causes immense energy release.
  • Chemical: A toxic chemical, such as poison gas or nerve gas, is dispersed, which is designed to injure or kill human beings.
  • Biological: An infectious agent, such as anthrax spores, is dispersed, which is designed to sicken or kill humans.
  • Kinetic: Collides with the target at high speed. A detonation is not necessarily required.
Often, a biological or chemical warhead will use an explosive charge for rapid dispersal.
Detonators
TypeDefinition
ContactWhen the warhead makes physical contact with the target, the explosive is detonated. Sometimes combined with a delay, to detonate a specific amount of time after contact.
ProximityUsing radar, sound waves, a magnetic sensor, or a laser the warhead is detonated when the target is within a specified distance. It is often coupled with directional explosion control system that ensures that the explosion sends the fragmentationprimarily towards the target that triggered it.
Remoteremotely detonated via signal from operator (Not normally used for warheads except for self-destruction)
TimedWarhead is detonated after a specific amount of time.
AltitudeWarhead is detonated once it falls to a specified altitude.
CombinedAny combination of the above.

Nuclear force


The nuclear force (or nucleon-nucleon interaction or residual strong force) is the force between two or more nucleons. It is responsible for binding of protons andneutrons into atomic nuclei. The energy released causes the masses of nuclei to be less than the total mass of the protons and neutrons which form them. The force is powerfully attractive between nucleons at distances of about 1 femtometer (fm) between their centers, but rapidly decreases to insignificance at distances beyond about 2.5 fm. At very short distances less than 0.7 fm, it becomes repulsive, and is responsible for the physical size of nuclei, since the nucleons can come no closer than the force allows.
The nuclear force is now understood as a residual effect of the even more powerful strong force, or strong interaction, which is the attractive force that binds particles called quarks together, to form the nucleons themselves. This more powerful force is mediated by particles called gluons. Gluons hold quarks together with a force like that of electric charge, but of far greater power.
The concept of a nuclear force was first quantitatively constructed in 1934, shortly after the discovery of the neutron revealed that atomic nuclei were made of protons and neutrons, held together by an attractive force. The nuclear force at that time was conceived to be transmitted by particles called mesons, which were predicted in theory before being discovered in 1947. In the 1970’s, further understanding revealed these mesons to be combinations of quarks and gluons, transmitted between nucleons that themselves were made of quarks and gluons. This new model allowed the strong forces that held nucleons together, to be felt in neighboring nucleons, as residual strong forces.
The nuclear forces arising between nucleons are now seen to be analogous to the forces in chemistry between neutral atoms called van der Waals forces. Such forces between atoms are much weaker than the electrical forces that hold the atoms themselves together, and their range is shorter, because they arise from spontaneous separation of charges inside the atom. Similarly, even though nucleons are made of quarks and gluons that are in combinations which cancel most gluon forces, some combinations of quarks and gluons nevertheless leak away from nucleons, in the form of short-range nuclear force fields that extend from one nucleon to another close by. These nuclear forces are very weak compared to direct gluon forces inside nucleons, and they extend only over a few nuclear diameters, falling exponentially with distance. Nevertheless, they are strong enough to bind neutrons and protons over short distances, and overcome the electrical repulsion between protons in the nucleus.


balistic missile


RDX

RDX, an initialism for Research Department Explosive, is an explosive nitroamine widely used in military and industrial applications. It was developed as an explosive which was more powerful than TNT, and it saw wide use in WWII. RDX is also known as cyclonite, hexogen (particularly in German and German-influenced languages), and T4. Its chemical name is cyclotrimethylenetrinitramine; name variants include cyclotrimethylene-trinitramine and cyclotrimethylene trinitramine.
In its pure, synthesized state RDX is a white, crystalline solid. It is often used in mixtures with other explosives and plasticizers, phlegmatizers or desensitizers. RDX is stable in storage and is considered one of the most powerful and brisant of the military high explosives

Name

RDX is also known, but less commonly, as cyclonite, hexogen (particularly in German and German-influenced languages), T4 and chemically as cyclotrimethylenetrinitramine. Tenney L Davis, writing in the US in 1943, stated it was generally known in the US as cyclonite; the Germans called it Hexogen, the Italians T4.[2] In the 1930s, the Royal Arsenal, Woolwich, started investigating cyclonite as an explosive to use against German U-boats that were being built with thicker hulls. Britain wanted an explosive that was more powerful than TNT. For security reasons, Britain termed cyclonite as "Research Department Explosive" (R. D. X.).[3] The term RDX appeared in the United States in 1946, but the name RDX is given without explanation.[4] The first public reference in the United Kingdom to the name RDX, or R.D.X. to use the official title, appeared in 1948; its authors were the Managing Chemist, ROF Bridgwater, the Chemical Research and Development Department, Woolwich, and the Director of Royal Ordnance Factories, Explosives; again, it was referred to as simply RDX.[5]
Usage

RDX was widely used during World War II, often in explosive mixtures with TNT such as Torpex, Composition B, Cyclotols, and H6. RDX was used in one of the first plastic explosives. RDX is believed to have been used in many bomb plots including terrorist plots. The bouncing bomb depth charges used in the "Dambusters Raid" each contained 6,600 pounds (3,000 kg) of Torpex.[6]
RDX forms the base for a number of common military explosives:
Composition A: Granular explosive consisting of RDX and plasticizing wax. Such as, composition A-5 (RDX coated with 1.5% stearic acid) and composition A-3 (91% RDX coated with 9% wax)
Composition B: Castable mixtures of 40% RDX and 60% TNT, with an extra 1% of wax added (desensitizer)
Composition C: The original composition C was used in World War II, but there have been subsequent variations including C-2, C-3, and C-4. C-4 consists of RDX (91%), a plasticizer (which can be dioctyl adipate {DOA}, diethylhexyl, or dioctyl sebacate) (5.3%), a binder, which is usually polyisobutylene (2.1%), SAE 10 non-detergent motor oil (1.6%).
Composition CH-6: 97.5% RDX, 1.5% calcium stearate, 0.5% polyisobutylene, and 0.5% graphite.[7]
DBX (Depth Bomb Explosive): Castable mixture consisting of 21% RDX, 21% aluminium nitrate, 40% TNT, and 18% powdered aluminium. Developed during World War II, it was to be used in underwater munitions as a substitute for Torpex employing only half the amount of then-strategic RDX.[1][8] As the supply of RDX became more adequate, the mixture was shelved.
Cyclotol: Castable mixture of RDX (50-80%) with TNT (20-50%) designated by the amount of RDX/TNT, such as Cyclotol 70/30.
HBX: Castable mixtures of RDX, TNT, powdered aluminium, and D-2 wax with calcium chloride.
H-6: Castable mixture of RDX, TNT, powdered aluminum, and paraffin wax.
PBX: RDX is also used as a major component of many polymer-bonded explosives (PBX). RDX-based PBX's typically consist of RDX and a polymer/co-polymer binder. Examples of RDX-based PBX formulations include, but are not limited to: PBX-9007, PBX-9010, PBX-9205, PBX-9407, PBX-9604, PBXN-106, PBXN-3, PBXN-6, PBXN-10, PBXN-201, PBX-0280, PBX Type I, PBXC-116, PBXAF-108, etc.
Semtex: (Trade name): Plastic demolition explosives containing RDX and PETN as major energetic components.
Torpex: 42% RDX, 40% TNT, and 18% powdered aluminium. The mixture was designed during World War II and used mainly in underwater ordnance.
Outside of military applications, RDX is also used in controlled demolition to raze structures. The demolition of the Jamestown Bridge in the US state of Rhode Island is one example where RDX shaped charges were used to remove the span.
Properties

The velocity of detonation of RDX at a density of 1.76 g/cm³ is 8750 m/s.
It is a colourless solid, of crystal density 1.82 g/cm³. It is obtained by reacting concentrated nitric acid with hexamine.[9]
(CH2)6N4 + 10HNO3 → (CH2-N-NO2)3 + 3CH2(ONO2)2 + NH4NO3 + 3H2O
It is a heterocycle and has the molecular shape of a ring. It starts to decompose at about 170 °C and melts at 204 °C. Its structural formula is: hexahydro-1,3,5-trinitro-1,3,5-triazine or (CH2-N-NO2)3.
At room temperature, it is very stable. It burns rather than explodes and detonates only with a detonator, being unaffected even by small arms fire. (This is one of the properties that make it a useful military explosive.) It is less sensitive than pentaerythritol tetranitrate (PETN). However, it is very sensitive when crystallized, below −4 °C.[citation needed] Under normal conditions, RDX has a figure of insensitivity of exactly 80 (RDX defines the reference point.).
RDX sublimes in vacuum, which limits its use in pyrotechnic fasteners for spacecraft.
RDX when exploded in air has about 1.5 times the explosive power of TNT per unit weight and about 2.0 times per unit volume.[10][11]

History

RDX was used by both sides in World War II. The US produced about 15,000 long tons (15,000 t) per month during WW II and Germany about 7,000 long tons (7,100 t) per month.[12] RDX had the major advantages of possessing greater explosive power than TNT used in the First World War, and requiring no additional raw materials for its manufacture.[12]
Germany
The discovery of RDX dates from 1898 when Georg Friedrich Henning obtained a German patent (patent No. 104280) for its manufacture, by nitrating hexamine nitrate (hexamethylenetetramine nitrate) with concentrated nitric acid.[13] In this 1898 patent, its properties as a medical compound were mentioned; however, three further German patents obtained by Henning in 1916 proposed its use in smokeless propellants.[13] The German military started investigating its use in 1920 and referred to it as hexogen.[14] Research and development findings were not published further until Edmund von Herz,[15] described as an Austrian and later a German citizen, obtained a British patent in 1921[16] and a United States patent in 1922.[17] Both patent claims were initiated in Austria; and described the manufacture of RDX by nitrating hexamethylenetetramine.[16][17] The British patent claims included the manufacture of RDX by nitration, its use with or without other explosives, and its use as a bursting charge and as an initiator.[16] The US patent claim was for the use of a hollow explosive device containing RDX and a detonator cap containing RDX.[17] In the 1930s, Germany developed improved production methods.[14]
During the Second World War, Germany used the code names W Salt, SH Salt, K-method, the E-method and the KA-method. These represented the names of the developers of the various chemical processes used to prepare RDX. The W-method was developed by Wolfram in 1934 and gave RDX the code name "W-Salz". It used sulphamic acid, formaldehyde and nitric acid.[18] SH-Salz (SH salt) was from Schnurr who developed a batch-process in 1937–38 based on nitrating hexamine.[19] The K-method was from Knõffler and was based on adding ammonium nitrate to the hexamine / nitric acid process.[20] The E-method was developed by Ebele, in Germany, and turned out to be identical to the Ross and Schiessler process described later.[21] The KA-method was developed by Knöffler, in Germany, and turned out to be identical to the Bachmann process described later.[22]
UK
In the United Kingdom (UK), RDX was manufactured from 1933 by the Research Department in a pilot plant at the Royal Arsenal in Woolwich, London; a larger pilot plant being built at the RGPF Waltham Abbey just outside London in 1939.[23][24] In 1939 a twin-unit industrial-scale plant was designed to be installed at a new 700 acres (280 ha) site, ROF Bridgwater, away from London; and production of RDX started at Bridgwater on one unit in August 1941.[23][25] The ROF Bridgwater plant brought in ammonia and methanol as raw materials: the methanol was converted to formaldehyde and some of the ammonia converted to nitric acid, which was concentrated for RDX production.[5] The rest of the ammonia was reacted with formaldehyde to produce hexamine. The hexamine plant was supplied by Imperial Chemical Industries; and it incorporated some features based on data obtained from the United States (US).[5] RDX was produced by continually adding hexamine and concentrated nitric acid to a cooled mixture of hexamine and nitric acid in the nitrator.[5] The RDX was purified and processed for its intended use; and recovery and reuse of some methanol and nitric acid was also carried out.[5] The hexamine-nitration and RDX purification plants were duplicated (i.e. twin-unit) to provide some insurance against loss of production due to fire, explosion or air attack.[23]
The United Kingdom and British Empire were fighting without allies against Nazi Germany until the middle of 1941 and had to be self-sufficient. At that time (1941), the UK had the capacity to produce 70 long tons (71 t) (160,000 lb) of RDX per week; both Canada, an allied country and self-governing dominion within the British Empire, and the US were looked upon to supply ammunition and explosives, including RDX.[26] By 1942 the Royal Air Force's annual requirement was forecast to be 52,000 long tons (53,000 t) of RDX, much of which came from North America (Canada and the US).[25]
Canada
A different method of production to the Woolwich process, was found and used in Canada, possibly at the McGill University Department of Chemistry. This was based on reacting paraformaldehyde and ammonium nitrate in acetic anhydride.[27] A UK patent application was made by Robert Walter Schiessler, Pennsylvania State College and James Hamilton Ross, at McGill, Canada, in May 1942 and the UK patent was issued in December 1947.[28] Gilman states that the same method of production had been independently discovered by Ebele in Germany prior to Schiessler and Ross, but that this was not known by the Allies.[13][27] Urbański provides details of five methods of production: this is listed as the (German) E-method.[21]
UK, US and Canadian production and development
At the beginning of the 1940s, the major US explosive manufacturers, E. I. du Pont de Nemours & Company and Hercules had several decades of experience of manufacturing Trinitrotoluene (TNT) and had no wish to experiment with new explosives; a view also held by the US Army Ordnance, who proposed to continue using TNT.[29] RDX had been tested by Picatinny Arsenal in 1929 and it was regarded as too expensive and too sensitive.[26] The Navy proposed to continue using ammonium picrate.[29] In contrast, the view that new explosives were unnecessary was not shared by the National Defense Research Committee (NDRC), who had visited The Royal Arsenal, Woolwich.[29] James B. Conant, chairman of Division B, wished to involve academic research into this area. Conant therefore set up an Experimental Explosives Research Laboratory at the Bureau of Mines, Bruceton, Pennsylvania using direct Office of Scientific Research and Development (OSRD) funding.[26]
In 1941, the UK's Tizard Mission visited the US Army and Navy departments and part of the information handed over included details of the "Woolwich" method of manufacture of RDX and its stabilisation by mixing it with beeswax.[26] The UK was asking that the US and Canada, combined, supply 220 short tons (200 t) (440,000 lb) of RDX per day.[26] A decision was taken by William H. P. Blandy, Chief of the Bureau of Ordnance to adopt RDX for use in mines and torpedoes.[26] Given the immediate need for RDX, the US Army Ordnance, at Blandy's request, built a plant that just copied the equipment and process used at Woolwich. The result was the Wabash River Ordinance Works run by E. I. du Pont de Nemours & Company.[30] This works had the largest nitric acid plant in the world, at that time.[26] The Woolwich process was expensive; it needed 11 pounds (5.0 kg) of strong nitric acid for every pound of RDX.[31]
By early 1941, the NDRC was researching new processes.[31] The Woolwich or direct nitration process has at least two serious disadvantages: (1) it used large amounts of nitric acid and (2) at least one-half of the formaldehyde is lost. One mole of hexamethylenetetramine could produce at most one mole of RDX.[32] At least three laboratories with no previous explosive experience were tasked to develop better production methods for RDX; they were based at Cornell, Michigan and Penn State universities.[26][33] Werner Emmanuel Bachmann, from Michigan, successfully developed the "combination process" by combining the Canadian process with direct nitration.[22][26] The combination process required large quantities of acetic anhydride instead of nitric acid in the old British "Woolwich process". Ideally, the combination process could produce two moles of RDX from each mole of hexamethylenetetramine.[32]
Vast increases in production of RDX could not continue to rely on the use of the beeswax, first used in the Woolwich process, to desensitize the RDX. A substitute based on petroleum was developed at the Bruceton Explosives Research Laboratory.[26]
[edit]Bachmann process
The NDRC tasked three companies to develop pilot plants. They were the Western Cartridge Company, E. I. du Pont de Nemours & Company and Tennessee Eastman Company, part of Eastman Kodak.[26] The Eastman Chemical Company (TEC), Kingsport, Tennessee, a leading manufacturer of acetic anhydride, Werner Emmanuel Bachmann successfully developed a continuous-flow manufacturing process for RDX. RDX was crucial to the war effort and the current batch-production process could not keep up. In February 1942, TEC built the Wexler Bend pilot plant and began producing small amounts of RDX. This led to the US government authorizing TEC to design and build Holston Ordnance Works (H.O.W.) in June 1942. By April 1943, RDX was being manufactured there.[34] At the end of 1944, the Holston plant and the Wabash River Ordinance Works (which used the Woolwich process) were making 25,000 short tons (23,000 t) (50 million pounds) of Composition B per month.[35]
The US Bachmann process for RDX was found to be richer in HMX than the United Kingdom's RDX. This later led to a RDX plant using the Bachmann process being set up at ROF Bridgwater in 1955, to produce both RDX and HMX.
Military compositions
The United Kingdom's intention in World War II was to use "desensitised" RDX: in the original Woolwich process RDX coated with beeswax, but changed to a RDX coated with petroleum-based product, based on the work carried out at Bruceton. In the event the UK was unable to obtain sufficient RDX to meet its needs.[25] Some of this shortfall was met by substituting a mixture of ammonium nitrate and TNT.[25]
Karl Dönitz was reputed to have claimed that "an aircraft can no more kill a U-boat than a crow can kill a mole".[36] However, by May 1942 Wellington bombers began to deploy depth charges containing Torpex, a mixture of RDX, TNT and aluminium, which had up to 50 percent more destructive power than TNT-filled depth charges.[36] Considerable quantities of the RDX–TNT mixture were produced at the Holston Ordnance Works, with Tennessee Eastman developing an automated mixing and cooling process based around the use of stainless steel conveyor belts.[11]
Terrorism
The 1993 Bombay bombings were the first terrorist blasts in Mumbai which used RDX by placement into several vehicles as bombs. RDX was main component used for the 2006 Mumbai train bombings and the Jaipur bombings in 2008.[37][38] It is also believed to be the explosive in the 1999 Russian apartment bombings,[39] 2004 Russian aircraft bombings,[40] and 2010 Moscow Metro bombings.[41]
Ahmed Ressam, the al-Qaeda Millennium Bomber, used a small quantity of RDX as one of the components in the explosives that he prepared to bomb Los Angeles International Airport on New Year's Eve 1999/2000; the combined explosives could have produced a blast forty times greater than that of a devastating car bomb.[42][43]

Composition B

Composition B, colloquially "comp B", is an explosive consisting of castable mixtures of RDX and TNT. It is used as the main explosive filling in artillery projectiles, rockets, land mines, hand grenades, sticky bombs and various other munitions.[1] It was also used for the explosive lenses in the first implosion-type nuclear weapons developed by the United States.

Ingredients

The standard ratio of ingredients (by weight) is 59.5% RDX (detonation velocity of 8,750 m/s) and 39.4% TNT (detonation velocity of 6,900 m/s), together with an additional 1% paraffin wax[4] to improve handling qualities. Most commonly it is described as 60/40 RDX/TNT with 1% wax added.
Properties

Density: 1.65 g/cm3-
Velocity of detonation: 8,050 m/s
Use

Composition B was extremely common in United States and other western nations' munitions and was the standard explosive filler from early World War II until the early 1950s, when less sensitive explosives began to replace it in many weapons systems.[citation needed] Some NATO-approved munitions suppliers such as Mecar[5] have continued to use Composition B in their products.
Composition B is related to Cyclotol, which has a higher proportion of RDX (up to 75%).

C-4 (explosive)

C-4 or Composition C-4 is a common variety of the plastic explosive known as Composition C.

Composition and manufacture


C4 is made up of explosives, plastic binder, plasticizer and usually marker or odorizing taggant chemicals such as 2,3-dimethyl-2,3-dinitrobutane (DMDNB) to help detect the explosive and identify its source.[1]
The explosive in C4 is RDX (cyclonite or cyclotrimethylene trinitramine), which makes up around 91% of C4 by mass.[1] The plasticizer is diethylhexyl (5.3%)[1] or dioctyl sebacate and the binder is usually polyisobutylene (2.1%).[1] Another plasticizer used is dioctyl adipate (DOA). A small amount of SAE 10 non-detergent motor oil (1.6%) is also added.[1]
C4 is manufactured by combining the noted ingredients with binder dissolved in a solvent. The solvent is then evaporated and the mixture dried and filtered. The final material is an off-white solid with a texture similar to modelling clay.

Characteristics and uses

C4 has a detonation velocity of 8,092 m/s (26,550 ft/s)
A major advantage of C4 is that it can easily be molded into any desired shape. C4 can be pressed into gaps, cracks, holes and voids in buildings, bridges, equipment or machinery. Similarly, it can easily be inserted into empty shaped charge cases of the type used by military engineers.
C4 is very stable and insensitive to most physical shocks. C4 cannot be detonated by a gunshot or by dropping it onto a hard surface. It does not explode when set on fire or exposed to microwave radiation. Detonation can only be initiated by a combination of extreme heat and a shockwave, such as when a detonator inserted into it is fired.
The British military uses a plastic explosive referred to as PE4. Like C4, it is an off-white colored solid and its explosive characteristics are nearly identical to C4. The type and proportion of plasticizer used differs, and PE4 has a slightly greater velocity of detonation, 8,210 m/s (26,900 ft/s). Semtex is a somewhat similar plastic explosive.

Peluru kendali




Peluru kendali (disingkat: rudal), peluru berpandu atau misil adalah senjata roket militer yang bisa dikendalikan atau memiliki sistem pengendali otomatis untuk mencari target atau menyesuaikan arah. Dalam penggunaan sehari-hari, istilah "misil" merujuk kepada roket dengan sistem kendali, sedangkan "roket" digunakan untuk roket tanpa sistem kendali. Perbedaan utama di antara dianggap sangat sedikit selain perbedaan sistem kendali.
Peluru kendali pertama digunakan dalam sebuah operasi adalah peluru kendali Jerman dalam Perang Dunia II. Yang paling terkenal adalah V-1 dan V-2, keduanya menggunakan sistem autopilot sederhana untuk menjaga arah terbang peluru agar tetap pada yang rute telah ditentukan sebelumnya.

Jenis peluru kendali
Peluru kendali balistik adalah peluru kendali yang memakai lintasan trayektori yang ditentukan oleh balistik dalam sistem pengirimannya. Peluru kendali ini hanya dikendalikan dalam masa peluncuran saja. Peluru kendali balistik yang pertama adalah roket V-2 yang dikembangkan oleh Nazi Jerman pada 1930-an dan 1940-an atas instruksi dari Walter Dornberger. Peluru kendali balistik dapat diluncurkan dari lokasi tetap seperti silo misil, kendaraan peluncur, pesawat, kapal atau kapal selam. Tahap peluncuran dapat berlangsung dari puluhan detik sampai beberapa menit dan dapat terdiri sampai dengan tiga tingkat roket. Trayektori rudal balistik terdiri dari tiga tahap yaitu tahap peluncuran, tahap terbang bebas dan fase memasuki kembali atmosfer Bumi.

Peluru kendali jelajah adalah peluru kendali yang memakai sayap dan menggunakan jet sebagai tenaga penggerak. Peluru kendali jelajah intinya adalah bom terbang. Peluru kendali jelajah dirancang untuk membawa hulu ledak konvensional dalam jumlah besar atau nuklir dan dapat menjangkau ratusan mil dengan tingkat akurasi tinggi. Peluru kendali jelajah modern dapat terbang mencapai kecepatan supersonik atau di atas subsonik, menggunakan sistem kendali otomatis dan terbang pada ketinggian rendah untuk menghindari radar. Rudal jelajah pertama yang dikembangkan adalah Kettering Bug yang dikembangkan oleh Amerika Serikat pada 1917 untuk digunakan dalam Perang Dunia I. Rudal ini terbang lurus untuk waktu yang telah ditentukan sebelumnya kemudian sayapnya akan dilepaskan untuk kemudian badan rudal yang mengandung hulu ledak jatuh menghujam tanah. Rudal ini tidak pernah digunakan dalam perang karena Perang Dunia I selesai sebelum rudal ini dapat digunakan. Rudal jenis ini yang terkenal antara lain adalah BGM-109 Tomahawk AS yang dapat mencapai jangkauan 1.100 km.

Peluru kendali anti-kapal adalah rudal yang fungsi utamanya adalah untuk menghancurkan kapal permukaan. Kebanyakan rudal anti-kapal menggunakan sistem pemandu inersial dan pelacak radar aktif. Rudal anti-kapal adalah salah satu dari sekian rudal jarak pendek yang digunakan dalam Perang Dunia II. Jerman menggunakannya untuk menenggalamkan banyak kapal sekutu sebelum pihak sekutu menemukan cara untuk mengatasinya (prinsipnya dengan radio jamming). Rudal anti-kapal dapat diluncurkan dari kapal, kapal selam, pesawat, helikopter dan kendaraan darat. Rudal anti-kapal yang terkenal dalam sejarah adalah rudal Jerman, Fritz X dan Henschel Hs 293.
Contoh peluru kendali anti kapal :
Boeing Harpoon (USA) - 221 kg warhead, 93-315 km range depending on platform
C-802/YJ-82 CSS-N-8 'Saccade' (China) - 165 kg warhead, 500+ km range
Exocet (France) - 165 kg warhead, 70-180 km range
RBS-15 (Sweden) - 200 kg warhead, 200 km range
Sea Eagle (UK) - 230 kg warhead, 110+ km range
Kh-35 (Rusia) - 1645 kg warhead, 130 km range

Peluru kendali darat ke udara adalah peluru kendali yang diluncurkan dari darat untuk menghancurkan pesawat. Istilah terkenal untuk rudal jenis ini adalah SAM yang merupakan singkatan dari rudal darat ke udara dalam bahasa Inggris yaitu suface-to-air missile. Rudal darat ke udara dapat diluncurkan dari lokasi tetap atau kendaraan peluncur. SAM terkecil yang dikembangkan oleh Uni Soviet dapat dibawa dan diluncurkan oleh seorang tentara. SAM juga dapat diluncurkan dari kapal, contoh dari jenis ini adalah Aegis.

Peluru kendali udara ke udara adalah rudal yang dipasang di pesawat terbang dengan target menghancurkan pesawat musuh. Rudal udara ke udara yang terkenal antara lain adalah AIM-9 Sidewinder buatan Amerika Serikat. Rudal jenis ini dapat mendeteksi target dengan menggunakan pelacak radar, inframerah atau laser. Rudal udara ke udara umumnya berbentuk panjang, silinder tipis untuk mengurangi efek gesekan pada kecepatan tinggi. Rudal ini umumnya digerakkan oleh satu atau lebih roket berbahan bakar padat atau cair. MBDA Meteor buatan Britania Raya menggunakan ramjet dan dapat mencapai kecepatan Mach 4.

Peluru kendali anti-tank adalah rudal yang fungsi utamanya untuk menghancurkan tank atau kendaraan lapis baja lainnya. Rudal anti-tank generasi pertama seperti AG-3 Sagger dikendalikan dengan menggunakan joystick. Rudal anti-tank generasi kedua seperti BGM-71 TOW dan AGM-114 Hellfire menggunakan radio, penanda laser atau kamera di ujung rudal. Rudal anti-tank generasi ketiga seperti FGM-148 Javelin buatan AS dan Nag buatan India adalah dari jenis "tembak dan lupakan". Nag menggunakan pelacak inframerah serta gelombang milimeter.

Peluru kendali anti-balistik
adalah peluru kendali dengan fungsi utama untuk menyergap dan menghancurkan peluru kendali balistik lawan. Rudal anti-balistik jarak pendek antara lain Arrow buatan Israel dan MIM-104 Patriot buatan AS. Sedangkan rudal anti-balistik yang dirancang untuk melawan ICBM sebelumnya hanya ada dua yaitu Safeguard AS yang menggunakan LIM-49A Spartan dan Sprint serta A-35 Rusia. A-35 kemudian dikembangkan menjadi A-135 yang menggunakan Gorgon dan Gazelle. Amerika Serikat kemudian mengembangkan Ground-Based Midcourse Defense.

Peluru kendali anti-satelit
adalah rudal yang memiliki fungsi untuk menghancurkan satelit buatan musuh. Rudal jenis ini antara lain adalah Anti-satellite weapons (ASAT) yang diluncurkan dari pesawat. Rudal jenis ini relatif masih dalam tahap pengembangan.

JDAM(Joint Direct Attack Munition) adalah perlengkapan pemandu yang mengubah bom gravitasi tak berpandu, atau "bom bodoh", menjadi mesiu "pandai" di segala cuaca. Perlengkapan JDAM bom adalah digunakan untuk memandu pada target dengan suatu sistem pemandu inersial terintegrasi yang dipasangkan sebuah penerima Global Positioning System (GPS) untuk menambah akurasi, memberikan daerah peluncuran lebih dari 15 nautikal mil (28 km) dari titik peluncuran.
Varian JDAM :
GBU-29 250-lb MK-81
GBU-30 500-lb MK-82
GBU-31 2000-lb MK-84 or BLU-109
GBU-32 1000-lb MK-83
GBU-35 1000-lb BLU-110
GBU-38 500-lb MK-82

Torpedo adalah proyektil berpenggerak sendiri yang diluncurkan dari atas permukaan atau di bawah permukaan air yang kemudian meluncur di bawah permukaan air, dirancang untuk meledak pada kontak atau jarak tertentu dengan target. Torpedo dapat diluncurkan dari kapal, kapal selam, helikopter, pesawat dan ranjau laut. Beberapa contoh torpedo modern antara lain MK 48 AS yang diluncurkan dari tabung torpedo kapal selam dan menggunakan sonar pasif atau aktif, serta VA-111 Shkval buatan Rusia yang menggunakan efek superkavitasi dapat mencapai kecepatan 200 knot atau 370 km/jam.

BY :ADITYA AS

Senjata nuklir

Senjata nuklir


Senjata nuklir adalah senjata yang mendapat tenaga dari reaksi nuklir dan mempunyai daya pemusnah yang dahsyat - sebuah bom nuklir mampu memusnahkan sebuah kota. Senjata nuklir telah digunakan hanya dua kali dalam pertempuran - semasa Perang Dunia II oleh Amerika Serikat terhadap kota-kota Jepang, Hiroshima dan Nagasaki.Pada masa itu daya ledak bom nuklir yg dijatuhkan di Hiroshima dan Nagasaki sebesar 20 kilo(ribuan) ton TNT. Sedangkan bom nuklir sekarang ini berdaya ledak lebih dari 70 mega(jutaan) ton TNT
Negara pemilik senjata nuklir yang dikonfirmasi adalah Amerika Serikat, Rusia, Britania Raya (Inggris), Perancis, Republik Rakyat Cina, India, Korea Utara dan Pakistan. Selain itu, negara Israel dipercayai mempunyai senjata nuklir, walaupun tidak diuji dan Israel enggan mengkonfirmasi apakah memiliki senjata nuklir ataupun tidak. Lihat daftar negara dengan senjata nuklir lebih lanjut.


Bentuk bom nuklir yang dijatuhkan di Hiroshima dan Nagasaki
Senjata nuklir kini dapat dilancarkan melalui berbagai cara, seperti melalui pesawat pengebom, peluru kendali, peluru kendali balistik, dan Peluru kendali balistik jarak benua.

Tipe senjata nuklir

Senjata nuklir mempunyai dua tipe dasar. Tipe pertama menghasilkan energi ledakannya hanya dari proses reaksi fisi. Senjata tipe ini secara umum dinamai bom atom (atomic bomb, A-bombs). Energinya hanya diproduksi dari inti atom.
Pada senjata tipe fisi, masa fissile material (uranium yang diperkaya atau plutonium) dirancang mencapai supercritical mass - jumlah massa yang diperlukan untuk membentuk reaksi rantai- dengan menabrakkan sebutir bahan sub-critical terhadap butiran lainnya (the "gun" method), atau dengan memampatkan bulatan bahan sub-critical menggunakan bahan peledak kimia sehingga mencapai tingkat kepadatan beberapa kali lipat dari nilai semula. (the "implosion" method). Metoda yang kedua dianggap lebih canggih dibandingkan yang pertama. Dan juga penggunaan plutonium sebagai bahan fisil hanya bisa di metoda kedua.
Tantangan utama di semua desain senjata nuklir adalah untuk memastikan sebanyak mungkin bahan bakar fisi terkonsumsi sebelum senjata itu hancur. Jumlah energi yang dilepaskan oleh pembelahan bom dapat berkisar dari sekitar satu ton TNT ke sekitar 500.000 ton (500 kilotons) dari TNT.
Tipe kedua memproduksi sebagian besar energinya melalui reaksi fusi nuklir. Senjata jenis ini disebut senjata termonuklir atau bom hidrogen (disingkat sebagai bom-H), karena tipe ini didasari proses fusi nuklir yang menggabungkan isotop-isotop hidrogen (deuterium dan tritium). Meski, semua senjata tipe ini mendapatkan kebanyakan energinya dari proses fisi (termasuk fisi yang dihasilkan karena induksi neutron dari hasil reaksi fusi.) Tidak seperti tipe senjata fisi, senjata fusi tidak memiliki batasan besarnya energy yang dapat dihasilkan dari sebuah sejata termonuklir.


Dasar kerja desain Tellr-Ulam pada bomb hidrogen: sebuah bomb fisi menghasilkan radiasi yang kemudian mengkompresi dan memanasi butiran bahan fusi pada bagian lain.
Senjata termonuklir bisa berfungsi dengan melalui sebuah bomb fisi yang kemudian memampatkan dan memanasi bahan fisi. Pada desain Teller-Ulam, yang mencakup semua senjata termonuklir multi megaton, metoda ini dicapai dengan meletakkan sebuah bomb fisi dan bahan bakar fusi (deuterium atau lithium deuteride) pada jarak berdekatan di dalam sebuah wadah khusus yang dapat memantulkan radiasi. Setelah bomb fisi didetonasi, pancaran sinar gamma and sinar X yang dihasilkan memampatkan bahan fusi, yang kemudian memanasinya ke suhu termonuklir. Reaksi fusi yang dihasilkan, selanjutnya memproduksi neutron berkecepatan tinggi yang sangat banyak, yang kemudian menimbulkan pembelahan nuklir pada bahan yang biasanya tidak rawan pembelahan, sebagai contoh depleted uranium. Setiap komponen pada design ini disebut "stage" (atau tahap). Tahap pertama pembelahan atom bom adalah primer dan fusi wadah kapsul adalah tahap sekunder. Di dalam bom-bom hidrogen besar, kira-kira separuh dari 'yield' dan sebagian besar nuklir fallout, berasal pada tahapan fisi depleted uranium. Dengan merangkai beberapa tahap-tahap yang berisi bahan bakar fusi yang lebih besar dari tahap sebelumnya, senjata termonuklir bisa mencapai "yield" tak terbatas. Senjata terbesar yang pernah diledakan (the Tsar Bomba dari USSR) merilis energi setara lebih dari 50 juta ton (50 megaton) TNT. Hampir semua senjata termonuklir adalah lebih kecil dibandingkan senjata tersebut, terutama karena kendala praktis seperti perlunya ukuran sekecil ruang dan batasan berat yang bisa di dapatkan pada ujung kepala roket dan misil.
Ada juga tipe senjata nuklir lain, sebagai contoh boosted fission weapon, yang merupakan senjata fisi yang memperbesar 'yield'-nya dengan sedikit menggunakan reasi fisi. Tetapi fisi ini bukan berasal dari bom fusi. Pada tipe 'boosted bom', neutron-neutron yand dihasilkan oleh reaksi fusi terutama berfungsi untuk meningkatkan efisiensi bomb fisi. contoh senjata didesain untuk keperluan khusus; bomb neutron adalah senjata termonuklir yang menghasilkan ledakan relatif kecil, tetapi dengan jumlah radiasi neutron yang banyak. Meledaknya senjata nuklir ini diikuti dengan pancaran radiasi neutron. Senjata jenis ini, secara teori bisa digunakan untuk membawa korban yang tinggi tanpa menghancurkan infrastruktur dan hanya membuat fallout yang kecil. Membubuhi senjata nuklir dengan bahan tertentu (sebagain contoh cobalt atau emas) menghasilkan senjata yang dinamai "salted bomb". Senjata jenis ini menghasilkan kontaminasi radioactive yang sangat tinggi. Sebagian besar variasi di disain senjata nuklir terletak pada beda "yield" untuk berbagai keperluan, dan untuk mencapai ukuran fisik yang sekecil mungkin.

by:ADITYA ARIF SETYAWAN

E = mc2

E = mc2



dalam ilmu fisika adalah sebuah rumus yang sering dikenal dan sangat penting dalam menjelaskan persamaan nilai antara energi (E) dan massa (m), yang disetarakan secara langsung melalui konstanta kuadrat laju cahaya dalam vakum ( c 2 )
,
yang mana:
E = energi (J)
m = massa (kg)
c = kecepatan cahaya (m.s-1)
Faktor c 2 bernilai 89.88 PJ/kg = 21.48 Mt TNT per kg = 149.3 pJ/u = 931.5 MeV/u.
Jika energi yang dimaksud dalam persamaan di atas adalah energi diam, maka massa yang terkait adalah juga massa diam atau massa invarian.

Albert Einstein menurunkan formula ini didasarkan atas pengamatannya pada tahun 1905 atas kelakuan obyek yang bergerak dengan laju mendekati laju cahaya. Kesimpulan terkenal yang ditariknya dari pengamatan ini adalah bahwa massa sebuah benda sebenarnya adalah sebuah ukuran dari kandungan energi benda tersebut. Sebaliknya, persamaan yang dimaksud mengisyaratkan bahwa semua energi yang ada dalam sistem tertutup memengaruhi massa diam dari sistem.

Menurut persamaan ini, jumlah maksimum energi yang "dapat diperoleh" dari suatu obyek untuk melakukan kerja aktif adalah massa obyek dikalikan kuadrat dari laju cahaya.
Rumus ini juga digunakan untuk mengukur besarnya energi yang dihasilkan dalam reaksi nuklir. Perubahan massa isotop sebelum dan sesudah reaksi nuklir diperhitungkan. Dimana jumlah massa yang hilang sesudah reaksi nuklir (Δm) dikalikan dengan kuadrat kecepatan cahaya, hasilnya sama dengan energi yang dilepaskan dalam reaksi nuklir tersebut.

Fisika atom

Fisika atom
adalah fisika "hull" elektron atom.
Orang awam biasanya menghubungkan istilah fisika atom dengan tenaga nuklir dan bom nuklir, dikarenkan penggunaan sinonim dari kata atom dan nuklir dalam standar Inggris. Namun, fisikawan membedakan antara fisika atom (berhadapan dengan efek hull elektron dan spin keseluruhan nukleus dan muatan listrik) dan fisika nuklir (berhadapan dengan gaya dalam nukleus atom dan reaksi yang mengubah, menyatukan atau memisahkan mereka).
Awal dari fisika atom ditandai dengan penemuan dan penelitian garis spektral. Hal ini menggambarkan garis yang jelas dalam spektrum panas dan cahaya.
Penelitian dari garis-garis ini menuju ke model atom Bohr dan sampai ke pengertian kita sekarang tentang hull elektron atom seperti dijelaskan oleh model atom orbital yang merupakan dasar dari seluruh pemahaman kimia. Kesimpulan ini tidak secara langsung, tetapi merupakan hasil dari riset lebih dari satu abad, yang telah sukses dalam menaruh kimia sebagai suatu dasar dan juga memberikan banyak aplikasi baru.
Fisika nuklir
adalah ilmu yang mempelajari mengenai inti atom, serta perubahan-perubahan pada inti atom. Dalam fisika nuklir, sebuah reaksi nuklir adalah sebuah proses di mana dua nuklei atau partikel nuklir bertubrukan, untuk memproduksi hasil yang berbeda dari produk awal. Pada prinsipnya sebuah reaksi dapat melibatkan lebih dari dua partikel yang bertubrukan, tetapi kejadian tersebut sangat jarang. Bila partikel-partikel tersebut bertabrakan dan berpisah tanpa berubah (kecuali mungkin dalam level energi), proses ini disebut tabrakan dan bukan sebuah reaksi.
Dikenal dua reaksi nuklir, yaitu reaksi fusi nuklir dan reaksi fisi nuklir. Reaksi fusi nuklir adalah reaksi peleburan dua atau lebih inti atom menjadi atom baru dan menghasilkan energi, juga dikenal sebagai reaksi yang bersih. Reaksi fisi nuklir adalah reaksi pembelahan inti atom akibat tubrukan inti atom lainnya, dan menghasilkan energi dan atom baru yang bermassa lebih kecil, serta radiasi elektromagnetik. Reaksi fusi juga menghasilkan radiasi sinar alfa, beta dan gamma yang sagat berbahaya bagi manusia.
Contoh reaksi fusi nuklir adalah reaksi yang terjadi di hampir semua inti bintang di alam semesta. Senjata bom hidrogen juga memanfaatkan prinsip reaksi fusi tak terkendali. Contoh reaksi fisi adalah ledakan senjata nuklir dan pembangkit listrik tenaga nuklir.
Unsur yang sering digunakan dalam reaksi fisi nuklir adalah Plutonium dan Uranium (terutama Plutonium-239, Uranium-235), sedangkan dalam reaksi fusi nuklir adalah Lithium dan Hidrogen (terutama Lithium-6, Deuterium, Tritium).
REAKSI NUKLIR
Dalam fisika nuklir, sebuah reaksi nuklir adalah sebuah proses di mana dua nuklei atau partikel nuklir bertubrukan, untuk memproduksi hasil yang berbeda dari produk awal. Pada prinsipnya sebuah reaksi dapat melibatkan lebih dari dua partikel yang bertubrukan, tetapi kejadian tersebut sangat jarang. Bila partikel-partikel tersebut bertabrakan dan berpisah tanpa berubah (kecuali mungkin dalam level energi), proses ini disebut tabrakan dan bukan sebuah reaksi.
Dikenal dua reaksi nuklir, yaitu reaksi fusi nuklir dan reaksi fisi nuklir. Reaksi fusi nuklir adalah reaksi peleburan dua atau lebih inti atom menjadi atom baru dan menghasilkan energi, juga dikenal sebagai reaksi yang bersih. Reaksi fisi nuklir adalah reaksi pembelahan inti atom akibat tubrukan inti atom lainnya, dan menghasilkan energi dan atom baru yang bermassa lebih kecil, serta radiasi elektromagnetik. Reaksi fusi juga menghasilkan radiasi sinar alfa, beta dan gamma yang sagat berbahaya bagi manusia.
Contoh reaksi fusi nuklir adalah reaksi yang terjadi di hampir semua inti bintang di alam semesta. Senjata bom hidrogen juga memanfaatkan prinsip reaksi fusi tak terkendali. Contoh reaksi fisi adalah ledakan senjata nuklir dan pembangkit listrik tenaga nuklir.
Unsur yang sering digunakan dalam reaksi fisi nuklir adalah Plutonium dan Uranium (terutama Plutonium-239, Uranium-235), sedangkan dalam reaksi fusi nuklir adalah Lithium dan Hidrogen (terutama Lithium-6, Deuterium, Tritium).
REPRESENTASI
Persamaan reaksi nuklir ditulis serupa seperti persamaan dalam reaksi kimia. Setiap isotop ditulis dalam bentuk: simbol kimianya dan nomor massa. Partikel neutron dan elektron, masing-masing ditulis dalam simbol n dan e. Partikel proton atau protium (sebagai inti atom hidrogen) ditulis dalam simbol p. Partikel deuterium dan tritium, masing-masing ditulis dalam simbol D dan T.
Contohnya:
Lithium-6 + Deuterium -> Helium-4 + Helium-4

6Li + D -> 4He + 4He

6Li + D -> 2 4He

isotop helium-4, disebut juga partikel alfa, bisa ditulis dalam simbol α
Jadi, bisa juga ditulis:
6Li + D -> α + α

atau:
6Li(D,α)α (bentuk yang dipadatkan)

ENERGI

Untuk menghitung energi yang dihasilkan, perubahan massa isotop sebelum dan sesudah reaksi nuklir diperhitungkan. Jumlah massa yang hilang, dikalikan dengan kuadrat kecepatan cahaya; hasilnya sama dengan energi yang dilepaskan dalam reaksi itu.

(lihat Tabel isotop)


massa isotop Lithium-6 : 6,015122795
massa isotop Deuterium : 2,0141017778
massa isotop Helium-4 : 4,00260325415

Lithium-6 + Deuterium -> Helium-4 + Helium-4
6,015122795 + 2,0141017778 -> 4,00260325415 + 4,00260325415

8,0292245728 -> 8,0052065083

Massa yang hilang: 8,0292245728 - 8,0052065083 = 0,0240180645 u (0,3%)

(dibulatkan)


E = mc2


E = mc2 = 1u x c2
= 1,660538782×10−27 kg x (299.792.458 m/s)2
= 149241782981582746,248171448×10−27 Kg m2/s2
= 149241782981582746,248171448×10−27 J
= 931494003,23310656815183435498209 ev
= 931,49 Mev (dibulatkan)
Jadi, massa 1u = 931,49 Mev



E = mc2 = 1 Kg x c2
= 1 kg x (299.792.458 m/s)2
= 89875517873681764 Kg m2/s2
= 89875517873681764 J
= 89,875 PJ (dibulatkan)
Jadi, massa 1 Kg = 89,875 PJ



Jadi energi yang dapat dihasilkan = 89,875 PJ/kg = 21,48 Mt TNT/kg
=149,3 pJ/u = 931,49 MeV/u


E = 0,0240180645 u x 931,49 MeV

E = 22,372586901105 MeV (dengan keakuratan 1%)
E = 22,4 Mev (dibulatkan)


Jadi, persamaan reaksinya:

6Li + D -> 4He (11.2 MeV) + 4He (11.2 MeV)

6Li + D -> 2 4He + 22,4 MeV


massanya hilang sebanyak 0,3 % (dibulatkan dari 0,2991330517938 %)

0,3 % x 21,48 Mt TNT/kg = 64 Kt/kg (dibulatkan)


jadi, Jumlah energi yang bisa dihasilkan (dengan 100 % efisien )
melalui reaksi fusi nuklir berbahan materi:

Lithium-6 + Deuterium = 64 Kt/kg (dibulatkan)

ENERGI RATA-RATA

Berikut adalah jumlah energi nuklir yang bisa dihasilkan per kg materi:
Fisi nuklir:
Uranium-233: 17,8 Kt/kg = 17800 Ton TNT/kg
Uranium-235: 17,6 Kt/kg = 17600 Ton TNT/kg
Plutonium-239: 17,3 Kt/kg = 17300 Ton TNT/kg
Fusi nuklir:
Deuterium + Deuterium: 82,2 Kt/kg = 82200 Ton TNT/kg
Tritium + Deuterium: 80,4 Kt/kg = 80400 Ton TNT/kg
Lithium-6 + Deuterium: 64,0 Kt/kg = 64000 Ton TNT/kg

BY :aditya arif setyawan