I thought I would show this rather unusual Fuze. Normally fitted to 3.5" Rocket HE shells for anti-tank use as I understand.
Does anyone have a sectioned diagram they could post?
The Fuze Percussion L5 is, as far as I'm aware, a copy of one of the US M404 models. Possibly the M404A1, as the UK text I have says M404 'Mark 1', which doesn't exist, but the M404A1 does. The M404 series were used with the US developed 3.5" M20 'HEAT' (aka shaped charge) and M30 busting WP smoke rockets for the M20 series 'Super Bazooka'.
Hi Barney,
Don't think this is for the 3.5" Rocket Launcher round. So far as I am aware all were HEAT hollow cone and therefore required a base fuze. A point fuze would destroy the jet and make it ineffective.
As well as the penetrating jet, the 3.5 RL round had a copper slug that was supposed to be inserted into the tank through the hole burnt by the jet, thus really spoiling the day for the crew.
Here is an example of the slug picked up by me on the ranges after firing, it was VERY hot.
Alan1.
Yes, I concur, as mentioned above, that the L5 were for a 3.5" rocket. Obviously, just like the US 'M' (standard Model) code system, there are a multitude of 'L5' things, and likely other fuzes.
A nose-mounted fuze would cause loss of penetration capability for a shaped charge (aka HEAT) equipped munition, but it would not "destroy the jet". Anything at in front jet is simply penetrated, the jet tip eroding slightly as it passes through.
As to shaped charge "burning holes" in the structures hit is a very, very common misconception. The physical mechanism by which the jet penetrates the structure hit has nothing really to do with heat (temperature). The primary penetrating mechanism is pressure.
The velocity of the jet tip is commonly in the 7-12 km/s (approx. 23,000-39,000 ft/s, approx. 16,000-27,000 mph) velocity range. The velocity of the jet is not constant, the tip is far higher than the rear, as such it stretches. With older shaped charge designs, about 30% of the shaped charge liner goes into the stretching jet, whilst 70% goes into the slug at the rear, which is far slower; commonly 100s of m/s.
Due to this very high velocity, the pressure exerted on the material struck by the jet tip exceeds, by at least an order of magnitude (aka 10 times), the material's strength. The pressure experienced can be calculated using Bernoulli's principles, but it's essentially the faster and denser the material (fluid), the higher the pressure.
Due to the pressure exerted by the jet tip being over ten times the strength of the material, the material it is simply pushed out of the way. No "burning" takes place, though things do get rather hot as they are rapidly moved around.
The pressure experienced by material the jet is made of is also way above its strength and as such it is also pushed out of the way as penetration occurs. In general as the target material is pushed out of the way to form a crater, the eroded jet material coats the outside of the crater. In reality, some target and jet material flows backwards towards the incoming jet, which can cause problems.
Penetration continues until the pressure exerted by the jet is less than that required to deform the target material. Hence when the velocity drops below a level that results in a pressure that is less than target material's plastic deformation strength.
At this point, what's left of the jet and slug are present in the bottom area of the hole the jet created.
However if the target is thinner than the amount of target material the jet can penetrate, this results in the jet, bits of the target, high pressure and temperature detonation product gases, and sometimes the slug, all passing into the target. The jet and slug tend to have a straight line flight path, whilst the spalled off target material forms a cone of lethal high velocity fragments.
If the jet, slug, or target spall fragments hits a person, or energetic materials (propellant, high explosive fillings, etc.), the result is commonly catastrophic.