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Laser Weaponary

GHOST RIDER

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The AL-1A Airborne Laser (ABL)
YAL-1A-ABL-USAF-1.jpg

The solution of the beam distortion problem paved the way for an operationally viable HEL weapon system.

At the end of the Cold War the SDI program was quietly killed off, but some key proposals survived. The Airborne Laser (ABL), envisaged as a follow-on to the ALL program, but with an operational role, was one of these. In 1996, the US Air Force awarded a US$1.1 billion contract to Boeing, TRW and Lockheed-Martin to develop a prototype ABL system, to be carried in a Boeing 747-400 aircraft. The ABL was to use a MegaWatt class COIL HEL weapon and a system to compensate for atmospheric distortion, to permit boost phase attacks on ballistic missiles.

A single ABL system would thus defend a footprint of hundreds of kilometres diameter, attacking and destroying launched ballistic missiles during their boost phase, when they are most detectable, slowest and most vulnerable due to heavy fuel load, pressurised fuel tanks and structural stresses.

Ballistic missiles have thin load bearing skins, which are heavily stressed during the boost phase, while the missile boosters are largely filled with pressurised high energy propellants. Therefore even slight damage to the booster skin will cause catastrophic failure with results seen many times over during failed launches of satellite launch vehicles.

The ABL would be deployed in time of crisis to the borders of a nation threatening the use of ballistic missiles, and should they be launched, destroy them, ensuring that debris with WMD warheads falls on the launching party. At the time the ABL was conceived, these nations included Iraq, Iran and North Korea. With ongoing growth in Iran's and North Korea's arsenals, and their efforts to deploy nuclear warheads, the ABL could prove to be a vital asset if either of these nations achieves their aims.

One of the design aims of the ABL system was to carry enough laser fuel to destroy twenty to forty missiles during a single 12 to 18 hour sortie. The ABL would orbit near the border of a threat nation and engage missiles as soon as they clear the cloudbase and are within line of sight.

The capabilities of the ABL system have raised the prospect of another operational application, which is the Anti-Satellite (ASAT) role. In this role, the AL-1A would fly an intercept profile to intersect the ground track of a low orbit reconnaissance or surveillance satellite, or manned space vehicle, and damage or destroy it. While satellites are more robust structurally than ballistic missiles, the ABL delivers more power over the same distance when attacking an orbital target, due to the much lower atmospheric density along the beam path, compared to an atmospheric target. Satellites are also equipped with sensitive optics and vulnerable solar panels. Suffice to say even public debate on this application elicited loud complaints from non-US operators of military satellites.

In a crisis the ABL systems would be deployed to the borders of a nation threatening a ballistic missile attack, good candidates now being Iran and the DPRK. Orbiting at the tropopause, the ABL would detect, track, and attack ballistic missiles once they clear the cloudbase, with the debris falling back on the nation which launched the weapon. The latter is a critical consideration for WMD payloads. A design objective for the ABL is to carry enough fuel to destroy 20-40 missiles during an 12 to 18 hour sortie. Other roles canvassed for the ABL include attacks on low orbit reconnaissance satellites.

The airframe used to carry the ABL system is the YAL-1A which is a modified Boeing 747-400F freighter. This is a robust and mature 100 tonne payload class airframe, with a main deck which is comparable to the C-5 Galaxy in payload and capacity.


The most notable external feature of the AL-1A is the nose mounted optical turret for the laser's primary mirror. The turret has a +/-120 degree field of regard in azimuth and is used to point the 1.6 metre primary laser mirror, produced by Corning Glass and Contraves. The roll shell is constructed from composite materials. When the laser is not in use, the 1.8 metre 150 kg window, built by Heraeus/Corning/Contraves, is rotated into a stowed position to protect the optical surface from abrasion by atmospheric dust particles, and birdstrike damage.

The main deck forward of the wing is separated from the aft main deck, which houses the laser system, by a full height bulkhead. The forward fuselage section houses the Battle Management system and the Beam Control Subsystem.

The Battle Management System (BMS) comprises the computers which manage the weapon system, the operator consoles for the weapon system, and supporting communications. Built around open systems COTS hardware and software, the system is the nerve centre of the ABL. It performs the identification, tracking, determines the priority and nomination of targets, and controls the engagement.

To do this, the battle management system relies on offboard sensors and an onboard infrared tracking and rangefinding sensor. The latter is a derivative of the legacy LANTIRN targeting pod, using the existing longwave FLIR sensor to tracking the missile, and a new carbon dioxide 10.6 micron band rangefinding laser and sensor, to supplement angle track data with accurate range. The intent is to produce an accurate trajectory projection for the target missile to facilitate 'prioritising' targets for attack. The sensor is mounted in a dorsal pod, carryied on a short pylon.

The third subsystem in the forward fuselage is the Beam Control System (BCS). This is the critical component which ensures that the laser's power can be effectively delivered to the target. The BCS comprises the wavefront sensor and control system for beam distortion control, the systems for beam jitter control, beam alignment and beam 'walk' control, calibration hardware, and target acquisition and tracking equipment. The deformable mirror has 341 actuators which update the shape of the mirror at 1,000 Hz frequency – this means 1/1000 sec is required not only to measure the distortion but also to calculate and control the mirror actuator.
ABL-Cutaway-1S.jpg


The lower forward cargo hold is retained and intented for carrying equipment to support deployments.

The aft main deck area carries the HEL subsystem and supporting hardware. Immediately aft of the wing are the two supporting lasers, built by Raytheon and Northrop-Grumman. These are the Tracking Illuminator Laser (TIL) and Beacon Illuminator Laser (BIL), both diode pumped solid state devices. The TIL is used to illuminate the target to facilitate fine tracking, while the BIL is used to measure atmospheric distortion to compensate beam wavefront shape, via the wavefront sensor.


A single stage of the COIL laser
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Beam Control Subsystem
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COIL Turret Assembly
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COIL-1st-Stage-1S.jpg

Aft of these are the main laser power stages, using 1.315 micron band COIL technology. Plastics, composites and titanium are used extensively to save structural weight. Despite this, each of the six laser modules weight around 1.5 tonnes. Each of the modules vents exhaust efflux via six ventral exhaust ducts and ports (see photo).

The laser stages are complex. The gaseous atomic oxygen fuel for the COIL is produced in a reactor which mixes Helium (He) hydrogen peroxide liquid (H2O2) and potassium hydroxide (KOH) producing waste heat and potassium chloride (KCl). The hydrogen peroxide is recycled in a closed loop system until it has been exhausted. US sources claim that 1,200 USG of propellant is to be carried.

The atomic Oxygen produced is then mixed with gaseous Iodine (I), to produce the excited Iodine required for laser operation. The gaseous mix is then flowed through a supersonic expansion nozzle, which also acts as the laser cavity.


Ventral aft fuselage exhaust ports for the COIL laser.
ABL-Exhaust-1S.jpg


The high power beam is flowed through all six laser stages gaining power with each stage, for an aggregate output of the order of a MegaWatt of continuous wave power. The full power beam is directed via a system of mirrors to the beam control subsystem and then the optical turret in the nose.

In an operational environment the AL-1A would be positioned into an orbit near enough to cover the territory of interest and loiter awaiting target tracks. Surveillance systems such as orbital early warning satellites, AEW&C where equipped with suitable radar, and UAVs would detect the initial launch of the missiles, relaying this data via Link-16 to the AL-1A. Once the ABL system is cued, the aircraft positions for a shot - if required the aircraft will turn to face the threat sector to afford the best possible field of regard for the laser weapon.

As the ballistic missiles break through the overcast, their enormous heat signatures would be detected by the LANTIRN sensor and coarse tracking initated. The BMS would attempt to establish missile trajectories as early as possible to determine priority for engagement. While the US Air Force have not disclosed how they intend to do this, it is reasonable to speculate that the value of the target and the distance to the missile would both be factors in the beam scheduling algorithm. Not unlike phased array radars used for missile defence, there is a finite time window to attack each target and a finite amount of laser time available within this window. Therefore judicious scheduling of laser use is essential to provide opportunities for reattack if needed. More distant targets will require that the laser 'dwell' on the target much longer to achieve effect, compared to nearer targets.

Once a coarse track for a specific missile has been established and the laser scheduled to shoot, the turret is slewed to point at the target and the TIL illuminator is lit up to initiate fine tracking. Once the fine track is established, the BIL beacon is lit up to generate continuous data on atmospheric distortion along the beam path. With the BIL operating the COIL laser is engaged and a multi-MegaWatt beam of 1.315 micron infrared radiation is put on to the target. In a viable engagement scenario, this would lead, within seconds, to the breakup of the target missile. Once this has happened, the system is cued to the second highest priority target and the same engagement sequence repeated. This would continue until laser fuel is exhausted or all of the targets killed, or out of reach.

What defences exist against the ABL? Given the signature size of a ballistic missile, detection and tracking is unavoidable once the missile clears any cloud. At that point the only defence lies in improving the missile's resistance to laser attack.

Years ago a physicist remarked to this author that this was 'simple, you cover the missile with a mirror coating to reflect the laser'. This is of course easier said than done, since any dirt, dust, moisture droplets, ice particles or other material on the surface of even a perfect mirror will vapourise and the superheated plasma will eat into the surface, destroying its reflectivity. At best mirror surfaces increase required laser dwell time to destroy the target.

Another strategy proposed has been to impart a rotation to the missile, effectively causing it to spin around its longitudinal axis, to minimise local exposure time to the laser, the idea being that through the remainder of each rotation the skin would cool. But this strategy also at best delays the inevitable, and could at best impact required dwell time.

A third strategy proposed has been the use of ablative surface coatings which would evaporate and so both cool the surface and block the beam in a layer of superheated vapour. A variation on this theme is the use of highly heat resistant skin materials. Both of these strategies would significantly add to the cost and weight of a missile, impacting deployable numbers and useful warhead size.

A fourth strategy proposed has been the use of higher rocket thrust per payload so the missile climbs out of the atmosphere in a much shorter time, thus reducing firing opportunities for the laser. If the missile can complete its boost pahse in half the time, the time available for attack is halved, which during a massed launch would allow some fraction of missiles to get past the laser. As with the preceding strategy, cost/numbers becomes a major issue since a much bigger missile first and second stage is required for the same warload.

Let us assume that a player develops a fast burn, spinning ballistic missile with an ablative coating, covered by a mirror coating. What it means is that more ABL platforms will need to patrol a given area to ensure that the increased dwell time does not allow any missiles to escape. The attacker will have to spend a lot more on his missiles. Like all missile defence technologies, the ABL drives up the cost of mounting a successful missile attack, to the point where it may not be economically viable. Suffice to say the intensive interest of China and Iran in cruise missiles indicates that the ABL, and ground based interceptor missiles, are already having impact well before they have even achieved full operational capability.

The ABL program has been controversial, to say the least. As it is directly competing for funds with capabilities such as interceptor missiles, be they silo, warship or air launched, there is an added element to the controversy, as all players attempt to maximise their slice of the budgetary pie.

The COIL laser achieved 'First Light' in November, 2004, with an initial test run. However, significant integration and testing remains before the system will be viable for operational use. This February the buy of five production airframes was put on hold, until such time as the capabilities of the prototype could be proven. Current planning envisages a trial shot against a target ballistic missile in late 2008.

Recent US reports indicate that many problems remain to be resolved. One is that of atmospheric dust particles in the main beam, termed 'fireflies'. Given the intensity of the beam, dust particles vapourise and the plasma exacerbates local turbulence and soaks up energy from the beam, reducing effective range. It also has the potential of interfering with the fine tracking function, which relies on infrared reflections off the target.

There has been considerable speculation on the use of the ABL for other roles, excluding the previously mentioned ASAT role. One idea has been to use the ABL to attack cruise missiles. If these are high flying supersonic weapons like the Kh-22 Burya/Kitchen flying a relatively flat trajectory, then the ABL will be highly effective. If they are low flying cruise missiles in the class of the Tomahawk or ALCM, then effectiveness is apt to be poor. The same is true of low flying aircraft targets or surface targets. The reality is that the troposphere, below 36,000 ft, is a poor propagation environment with a lot of water vapour and dust particles, or water droplets in cloud. The tropospheric 'soup' absorbs and dissipates the energy in the laser beam a lot faster than the dry/cold/thin stratosphere does. Physics are physics and cannot be easily beaten. The result will be very poor effective range, and an unusuable weapon if any cloud gets between the laser and the target. Much the same constraints apply if the target is an aircraft. A high flying UAV, reconnaissance aircraft or even hypersonic vehicle is extremely vulnerable to the ABL. A low flying aircraft is not.

In perspective the AL-1A ABL is a revolutionary weapon which once mature will render ineffective arsenals of short, intermediate and intercontinental ballistic missiles, and high flying aircraft and cruise missiles, where conditions permit the ABL to operate within lethal range of the target. How soon the ABL matures into an operationally viable system remains to be seen.
 
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YAL-1A-ABL-1S.jpg

The YAL-1A ABL will be the first large laser weapon to become operational. Its purpose is to destroy ballistic missiles during the boost phase (Boeing).
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Advanced Tactical Laser (ATL)
ATL-C-130-Prototype-2S.jpg

The ATL program is an effort to exploit the technology developed for the ABL to provide a cheaper and smaller system, suitable for carriage on aircraft such as the AC-130 Spectre or V-22 Osprey, as a close air support weapon. In January 2006, U.S. Air Force's 46th Test Wing provided Boeing with a C-130H Hercules for trials of the prototype weapon, claimed to be in the MegaWatt class, using COIL technology. The intent was to mount the laser prototype in the aircraft and perform lethality trials in 2007 against a range of ground targets. L-3 Communications/Brashear developed the optical turret, and the laser is being built by AFRL at Kirtland Air Force Base in Albuquerque, New Mexico. The laser was successfully fired in May, 2008.
ATL-CONOPS-Kirtland-2008-1S.jpg
 
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HP lasers as weapons are inevitable, but I think we will see them more for close-in, terminal defense rather than that described here. As the ranges go up, so do the aiming and focus problems.

We have already tested a laser point-defense system that is capable of popping three heavy mortar shells inflight simultaneously... kind of like a CIWS for land. The beauty f lasers, of course, is near zero time of flight. The geometry of target lead and intercept is greatly simplified.
 
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HP lasers as weapons are inevitable, but I think we will see them more for close-in, terminal defense rather than that described here. As the ranges go up, so do the aiming and focus problems.

We have already tested a laser point-defense system that is capable of popping three heavy mortar shells inflight simultaneously... kind of like a CIWS for land. The beauty f lasers, of course, is near zero time of flight. The geometry of target lead and intercept is greatly simplified.

Personally I think the best environment for long range lasers would be the space vacuum. You have no atmospheric distortion/blooming and targets may engage one another at tremendous lengths (like fractions of light seconds) so the speed of the "projectile" may be important. The problem would be tackling the energy generation and heat dissipation.
 
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Personally I think the best environment for long range lasers would be the space vacuum. You have no atmospheric distortion/blooming and targets may engage one another at tremendous lengths (like fractions of light seconds) so the speed of the "projectile" may be important. The problem would be tackling the energy generation and heat dissipation.

For a powerful laser as is fitted upon that Boeing...atmospheric distortions will not drastically effect laser effectiveness. I must say that much claims are seen that threat elimination & especially with respect to Ballistic warheads travelling ~7-10km/s can be successfully engaged because they still are unmatched relative to light speed 3E8 m/s....However its no the laser speed but its the hardware components [tracking/guiding] that STILL are limiting factors in effectively using the much professed SPeED Of LIGHT
 
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Personally I think the best environment for long range lasers would be the space vacuum. You have no atmospheric distortion/blooming and targets may engage one another at tremendous lengths (like fractions of light seconds) so the speed of the "projectile" may be important. The problem would be tackling the energy generation and heat dissipation.

space basedaser was tried and then a.andoned in ronald raygon's time.
 
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