A shot from a weapon is a method of accelerating a projectile in the barrel to the appropriate initial velocity by employing the pressure of gases produced by the combustion of the propellant charge [1]. The operating cycle of a weapon refers to the series of activities done between two successive rounds. Weapons are categorized as [1] in terms of operating cycle automation:
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single shot firearm – all operations of operating cycle are performed manually by the shooter;
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repeating firearm – part of the operations of the operating cycle is performed manually by the shooter (e.g. opening the breech), part of the operations of the operating cycle is performed automatically (e.g. when manually opening the breech, the empty cartridge is automatically pulled out and ejected);
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semiautomatic firearm – all operations of operating cycle are performed automatically, whereas after one press of trigger by the shooter is only one operating cycle being performed;
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automatic firearm – all operations of operating cycle are performed automatically, whereas after one press of trigger by the shooter is performed more operating cycles than one.
To perform automated tasks on weapons with higher degrees of operating cycle automation (repeating, semiautomatic, and automatic firearms), appropriate mechanisms and equipment are used. In the case of repeating weapons, the shooter's effort is used to ensure that these mechanisms operate properly. The so-called main functional component of the weapon mechanisms is placed in motion utilizing a specific type of propulsion in semiautomatic and automatic firearms, and the kinetic energy of the main functional member is subsequently employed to drive additional weapon mechanisms during firing. The following types of drives are commonly utilized to increase the speed of the main operational part [1]:
A drive by absorbing propellant gas is a fairly common propulsion, especially for higher-powered small arms weapons (submachine guns, assault rifles, and machine guns). The main functional part of the weapon systems is set in motion utilizing a pulse of pressure of the propellant gases taken during the shot from the bore of the barrel in this method of propulsion. The drives with propellant gas collection are split into [1, 2] according to the manner of obtaining gases from the barrel and conveying the pulse of the propellant gas pressure to the main functional member:
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piston system;
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gas trap system;
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moving primer system.
Only the first of them, piston-driven propulsion, is currently employed exclusively for automatic guns. A piston mechanism of the Czech automatic rifle 7.62 mm Sa model 58, which uses a 7.62 x 39 mm cartridge, is an example of this method of propulsion (7.62 mm model 43). The main parts of this device are (see Fig. 1A):
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gas port, in which it is created
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gas cylinder,
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gas piston with piston rod and
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gas channel, which connects the bore of barrel with the gas cylinder.
During the shot, when the projectile's bottom passes through the gas channel, a portion of the propellant gases penetrates the gas cylinder, causing a rapid increase in pressure p and temperature T in the gas cylinder's volume V. The force F created by the pressure of the propellant gases in the gas cylinder acting on the front surface of the gas piston S accelerates the piston and piston rod to the maximum speed vmax. The force F is conveyed to the main functional part of the weapon mechanisms, which is the breech block carrier in the case of the automatic rifle Sa model 58. The kinetic energy of the breech block carrier is then used to drive the other mechanisms of this weapon.
During the shot, there is an intense strain on individual parts of the automatic firearm, including parts of the piston system. These are mainly the following types of stress:
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pressure action of propellant gases;
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temperature action of propellant gases;
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mechanical interaction between moving parts of the weapon (especially dynamic shocks).
In terms of absolute values of individual types of stress, the pressure and temperature action of propellant gases is dominant. Depending on the type, calibre and ballistic power of the weapon and the type of gunpowder used, the maximum values of propellant gas pressure in the bore are mainly in the range of (100–600) MPa. In extreme cases, propellant gas pressures can reach up to 1 GPa, while the maximum propellant gas temperature reaches values in the range (2200–3800) K during the shot [3]. Determination of propellant gas pressure values is possible numerically and experimentally.
Numerical determination of pressure values is the subject of the theory of interior ballistics of firearms [3]. The courses of interior ballistic characteristics (pressure and temperature of propellant gases, trajectory and velocity of the projectile as a function of time) are determined by solving a system of interior ballistics equations, derived on the basis of thermomechanical theory of ideal gas and Newton's laws of motion.
Experimental determination of propellant gas pressure values is possible using pressure gauges or piezoelectric pressure sensors, either by measuring directly in the initial combustion chamber using insertion pressure gauges (in the case of artillery weapons), or by measuring on special ballistic barrels using threaded pressure gauges [3]. Experimental determination of the propellant gas temperature during the shot is very problematic and in fact practically impossible due to the small measuring ranges of available temperature sensors (up to 2000 K for thermocouples type B and D) and long sensor response times, which fluctuates for thermocouples and thermistors in the range of (0.1–1) s [4]. Thus, only the maximum, so-called explosion temperature Tv of a given propellant charge is determined experimentally, indirectly by calculation from the experimentally determined explosion heat Qv by burning a certain amount of propellant charge in a calorimetric test pressure vessel immersed in a calorimeter. The course of the propellant gas temperature as a function of time is then determined numerically within the solution of the system of interior ballistics equations for the periods of combustion and expansion of propellant gases [3].
In current design practice, the determination of the pressure and temperature profiles of the propellant gases in the gas cylinder of a piston gas device is carried out only numerically. Experimental determination of propellant gas pressure is not possible due to the requirements for the installation of modern propellant gas pressure sensors, which in the case of piston gas devices cannot be met due to their relatively small dimensions. To determine the course of pressure and temperature in the gas cylinder, the calculation method of prof. Popelínský [2], based on the application of the 1st law of thermodynamics for an open thermodynamic system (energy conservation law) in the form [5] is employed, namely:
$$\frac{\text{d}Q}{\text{d}t}+\sum _{j}\frac{\text{d}{H}_{j}}{\text{d}t}=\frac{\text{d}U}{\text{d}t}+\frac{\text{d}A}{\text{d}t},$$
1
where \(\frac{\text{d}Q}{\text{d}t}\) is change of heat supplied, resp. discharged from the gas cylinder, \(\sum _{j}\frac{\text{d}{H}_{j}}{\text{d}t}\) is the sum of changes in the enthalpies of the gases supplied, resp. discharged from the gas cylinder, \(\frac{\text{d}U}{\text{d}t}\) is change of internal gas energy in a gas cylinder and \(\frac{\text{d}A}{\text{d}t}\) is change in the volumetric work performed by the gas in the gas cylinder.
Furthermore, the equation of state in a gas cylinder applies in the form of
,
where \(p\) is gas pressure in the gas cylinder, \(v\) is specific volume of gas in the gas cylinder, \(r\) is specific gas constant of a gas in a gas cylinder and \(T\) is gas temperature in the gas cylinder.
Furthermore, the 2nd Newton's law of motion is used, applied in the form of the equation of motion of the piston together with the piston rod and the main functional member (hereinafter MFM) in the form
$$m\frac{{d}^{2}x}{d{t}^{2}}=pS,$$
3
where \(x\) is the path of the piston together with the piston rod and MFM, \(m\) is the weight of the piston together with the piston rod and MFM, \(p\) is gas pressure in the gas cylinder and \(S\) is forehead surface of the piston.
Using the law of energy conservation, the equation of state and the equations of motion of the piston together with the piston rod and the MFM, it is possible to determine the time courses of the pressure p and the temperature T acting on the piston. The propellant gas pressure was calculated for a (7.62 x 39) mm cartridge (Fig. 1B).
The results of the calculation were compared with the measurement (differences in the waveforms are caused by the fact that the result of the calculation is the so-called mean ballistic pressure, while the measurement found the course of pressure as a function of time for the cartridge mouth).
The calculated course of pressure and temperature of propellant gases was then used to determine the course of pressure and temperature of propellant gases in the gas cylinder, with the fact that in the energy conservation equation a simplistic assumption was made that there is no heat exchange with the environment, i.e. \(\frac{\text{d}Q}{\text{d}t}=0\). Calculation results for real design parameters of automatic rifle Sa model 58 are shown in the following graphs (Fig. 1C and 1D).
The result of the calculation shows that the moment the bottom of the projectile passes the mouth of the gas channel in the bore of the barrel, the pressure and temperature in the gas cylinder begin to increase. Due to the compression of the gas in the small volume of the gas cylinder, the temperature of the gas in the gas cylinder increases compared to the temperature of the propellant gases in the bore of the barrel. The maximum pressure of propellant gases in the gas cylinder Sa model 58 reaches 34.0 MPa, while the maximum temperature in the gas cylinder reaches 2137.8 K. Furthermore, due to the rapid expansion of the gases in the bore, it happens that from a certain moment the pressure of the gases compressed in the space of the gas cylinder is higher than the current pressure of the gases in the bore of the barrel. This means that the gas starts to flow back into the bore through the gas channel. Nevertheless, due to the high compression and also due to the simplifying assumption that there is no heat transfer from the gas cylinder to the surroundings, the temperature of the gases in the cylinder remains higher than the actual gas temperature in the barrel, by about 240 K.
Based on the above results, it is clear that the gas piston must withstand high stress during operation, the piston forehead is exposed to dynamic shocks, high temperatures and pressures. The piston surface must withstand friction and wear, corrosion and erosion, and oxidation [6, 7, 8]. Failure of the piston function leads to limited of operation or malfunction of the weapon.
One of the ways to increase the service life of exposed weapon components, such as gas pistons, barrel bores, parts of the breech mechanism (locking piece, breech block, breech block carrier etc.), is the application of suitable coatings. Due to their suitable chemical and physical properties, mainly chromium coatings are used, created by the process of hard chromium plating (sometimes referred to as functional chromium plating) [9, 10, 11]. Hard chromium plating is an electrochemical process used to deposit a layer of chromium on a substrate. It is used in applications where high hardness and abrasion resistance or prolonging the service life of the functional surfaces of components is required. These coatings are formed in thicknesses of 10 µm to 100 µm. The hard chrome plating process itself has both advantages and disadvantages. Advantages, such as relatively low acquisition costs, have recently been overshadowed by a number of disadvantages, including low current efficiency, low resistance to chlorides, sulphuric acids and tensile residual stresses, causing lower corrosion resistance and reduced fatigue strength. [12, 13]. However, one of the biggest disadvantages is certainly the unecological nature of the whole process. During the coating process, compounds containing hexavalent chromium are present, which is very dangerous and one of the substances with the highest potential to cause cancer [14, 15, 16]. Furthermore, it is necessary to prepare acid baths, which again represent a significant environmental burden in the entire process.
Currently, the trend is to find suitable replacements for hard chrome plating technology, which is still used for a wide range of applications. These substitutes include, for example, the deposition of hard, abrasion-resistant coatings using PVD (Physical Vapor Deposition) and CVD (Chemical Vapor Deposition) technologies. For example, the application of PVD coatings based on FeinAl (designation of the AlCrN coating) showed that the application of this coating to the gas piston did not lead to its visible wear even after 3,000 shots [17]. However, it should be added that the FeinAl coating was applied to the original hard chrome coating. Another possible substitute for hard chrome plating is the use of thermal spraying, e.g. HVOF (High Velocity Oxygen Fuel) technology [18, 19, 20, 21]. However, HVOF technology is not suitable for all applications, as the coatings created by this technology must in many cases be further processed, e.g. by grinding or polishing. [22, 23]. Another disadvantage of this method is the porosity of the formed coating, although it is significantly lower compared to other thermal spraying methods (e.g. TWAS – Twin Wire Arc Spraying, APS – atmospheric plasma spraying) [24, 25, 26].
Chromium nitride (CrN) coated by Physical Vapor Deposition (PVD) has proven to be a promising replacement for hard chromium plating due to its high hardness, low internal stress, toughness and ability to improve corrosion, oxidation and wear resistance [27, 28]. The useful properties of this coating can be increased by chemical-heat treatment of the base material (substrate), i.e. by creating a hard layer-coating duplex system [29, 30, 31]. The diffusion layer formed, for example, by the nitriding process, increases the hardness of the substrate surface, which improves the adhesion of hard coatings on soft substrates and further increases the load-bearing capacity and fatigue strength of the substrate [32]. In general, with this technology, great emphasis is placed on the preparation of the functional surfaces of the components before coating. The surface texture achieved by the production technology is largely copied to the texture of the coating (so-called technological inheritance), so it is appropriate to use a suitable finishing method (e.g. polishing, sandblasting, etc.) [33], before applying the coating (so-called surface pretreatment) or suitably finish the surface of the deposited coating (e.g. wet sanding, µlap, etc.).
In this work, selected mechanical and tribological properties of CrN coating deposited by PVD technology on a substrate in the form of 42CrMo4 steel, which is widely used for the production of exposed weapon components, including gas pistons, were compared. The properties of both the CrN coating itself and the duplex system plasma nitriding + deposition of the CrN coating (PN + CrN) were investigated. The results of the investigation of the properties of the CrN coating and the PN + CrN duplex system were compared with the results of the hard chromium coating formed by a standard electrochemical process. Hard chromium was deposited on 42CrMo2 steel in the tempered state. The aim of the study was to investigate the possibility of replacing hard chromium with a CrN coating or a PN + CrN duplex system.