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Nigg, Martinz and Lechleitner 17th Plansee Seminar 2009, Vol. 1 RM 55/1<br />

Abstract<br />

<strong>Surface</strong> <strong>Hardening</strong> <strong>of</strong> <strong>Complex</strong> <strong>Molybdenum</strong> <strong>Alloy</strong> <strong>Parts</strong> <strong>by</strong> <strong>Gas</strong><br />

Treatment<br />

B. Nigg*, H.-P. Martinz* and A. Lechleitner*<br />

* PLANSEE SE, Reutte, Austria<br />

<strong>Molybdenum</strong> is the high end material for hot runner nozzles (HRNs) when they are used for injection<br />

moulding <strong>of</strong> corrosive polymers. For better abrasion resistance in addition the outer but especially the<br />

inner surfaces <strong>of</strong> the molybdenum nozzle are hardened <strong>by</strong> SHN ® ( = Super Hard Nitride), a gas nitriding<br />

process. To access longer lifetimes <strong>of</strong> the hot runner nozzles within this work attempts have been made<br />

to enlarge the hardness, to enlarge the thickness and to improve the oxidation resistance <strong>of</strong> the<br />

hardened zone. Variations <strong>of</strong> the process parameters as well as additions <strong>of</strong> elements like carbon or<br />

silicon resulted in reasonable improvements <strong>of</strong> surface properties.<br />

Keywords<br />

<strong>Molybdenum</strong>, TZM, SHN, gas nitriding, oxidation, hardness, pack siliconizing<br />

Introduction<br />

<strong>Molybdenum</strong> and its alloys (like TZM) are the high end materials for hot runner nozzles when they are<br />

used for injection moulding <strong>of</strong> corrosive polymers. For better abrasion resistance in addition the outer but<br />

especially the inner surfaces <strong>of</strong> the molybdenum (alloy) nozzle are hardened <strong>by</strong> SHN ® ( = Super Hard<br />

Nitride), a gas nitriding process which has been derived from literature and internal experience [1 – 5].<br />

As has been stated in the preceding publication <strong>of</strong> this group [6] the hardness pr<strong>of</strong>ile and the oxidation<br />

resistance <strong>of</strong> the surface zone should be improved in order to enlarge lifetime <strong>of</strong> the HRNs (Hot Runner<br />

Nozzles) which are used in plastics injection moulding (PIM) to provide a reproducible connection<br />

between feedstock and moulds. For that reason process parameters have been varied and the elements<br />

carbon (hardness) and silicon (oxidation resistance; [7]) have been implemented into the hard layer.<br />

Experimental<br />

TZM samples were disc like for the parameter variations and the addition <strong>of</strong> methane to the ammonia<br />

and tube shaped with various diameters for the experiments where silicon was added to the diffusion<br />

layer. Table I shows the parameters <strong>of</strong> the experiments which were performed. The hardened samples<br />

were evaluated <strong>by</strong> macroscopy, XRD ( = X-Ray Diffraction) and cross sectioning with subsequent LOM


RM 55/2 17th Plansee Seminar 2009, Vol. 1 Nigg, Martinz and Lechleitner<br />

( = Light Optical Microscopy), SEM-EDX ( = Scanning Electron Microscopy – Energy Dispersive X-Ray<br />

Analysis) and hardness measurements <strong>by</strong> a Nanoindenter.<br />

Results and discussion<br />

The standard SHN process on TZM leads to the formation <strong>of</strong> a zone which mainly consists <strong>of</strong> Mo2N [6].<br />

Table I and fig. 1 show that the substrate below this zone is also hardened slightly. However in a depth<br />

<strong>of</strong> 40 µm below the interphase the hardness is approximately as low as in the bulk substrate material. In<br />

fig. 2 light optical micrographs <strong>of</strong> two cross sections can be seen: on the left hand side that <strong>of</strong> a standard<br />

SHN sample, on the right hand side that <strong>of</strong> an high temperature (HT) SHN sample.<br />

Table I: Process parameters and results <strong>of</strong> the various hardening processes<br />

process <strong>Gas</strong> / Pack Temperature mass gain thickness <strong>of</strong> HV* in HV* - 10µm HV* - 40µm HV* - 100µm<br />

denomination composition in °C in mg / cm 2<br />

standard SHN<br />

zone in µm hardened zone deep in base deep in base deep in base<br />

TZM<br />

HT SHN<br />

NH3 1000 1,05 16 16 6 3,5 3<br />

TZM<br />

Carbo SHN<br />

NH3 1200 1,55 12 17 8 7,5 7<br />

TZM<br />

Silico SHN<br />

NH3 + CH 4 1100 0,70 11,5 17 7 5 3<br />

Mo Si + NaF + H2 1100 10,00 30 14 2,9 2,9 2,7<br />

NH3 1000<br />

1800<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

Hardness<br />

(HV 0,01)<br />

in kg/(mm) 2<br />

* all HV ( = Vickers Hardness) values in GPa<br />

Hardness vs. Depth - SHN<br />

-15 -10<br />

200<br />

-5 0 5 10 15 20 25 30 35 40 45 50 55 60 65 70 75 80 85 90<br />

Depth (µm) from the interface<br />

Fig. 1: Hardness pr<strong>of</strong>ile for two TZM samples hardened with the standard SHN process<br />

Hardness sample 1<br />

Hardness sample 2


Nigg, Martinz and Lechleitner 17th Plansee Seminar 2009, Vol. 1 RM 55/3<br />

Fig. 2: Light optical micrograph <strong>of</strong> cross sections <strong>of</strong> a standard SHN (left) and a HT-SHN (right) TZM sample<br />

The HT (1200°C) SHN process leads to a less homogeneous diffusion zone with a lower mean<br />

thickness. However the hardness pr<strong>of</strong>ile is different (see table I and fig. 3): starting from a slightly higher<br />

hardness <strong>of</strong> the diffusion zone even in a <strong>of</strong> depth 100 µm from the interface the TZM exhibits a hardness<br />

<strong>of</strong> 700 kg/(mm) 2 , which is more than double compared to the bulk value (300 at approx. 200 µm depth).<br />

1800<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

Hardness<br />

(HV 0,01)<br />

in kg/(mm) 2<br />

Hardness vs. Depth HT - SHN<br />

200<br />

-25 -15 -5 5 15 25 35 45 55 65 75 85 95 105 125 145 165 185 205 225 245 265 285 305 325 345<br />

Depth (µm) from the interface<br />

Fig. 3: Hardness pr<strong>of</strong>ile for two TZM samples hardened with the HT SHN process<br />

Hardness sample 1<br />

Hardness sample 3<br />

This is a very promising result. Less successful was the carbo nitridation at 1100°C. Although the<br />

diffusion layer which was formed is rather uniform (fig. 5, left) the hardness pr<strong>of</strong>iles look very different<br />

depending on the location where they were measured (fig. 4). As the carbo nitrided samples showed<br />

locally blackened areas soot formation from the gas phase can be assumed. This can probably be<br />

suppressed <strong>by</strong> lowering the methane content in the gas mixture so that more uniform hardening<br />

conditions can be established in future. XRD measurements revealed that Mo2C, MoC, MoN and locally<br />

Mo2N contribute to the composition <strong>of</strong> the hard zone. This mixture is slightly less hard than the hard


RM 55/4 17th Plansee Seminar 2009, Vol. 1 Nigg, Martinz and Lechleitner<br />

zones formed <strong>by</strong> ammonia exposure (Mo2N, much less MoN). The right hand sided light optical<br />

micrograph <strong>of</strong> fig. 5 was prepared from a pack siliconized Mo sample which was subsequently submitted<br />

to a standard SHN process. The horizontal thick layer on top consists mainly <strong>of</strong> MoSi2, the greyish<br />

uneven phase on top is most probably Si3N4 (XRD – results). The vertical zone was formed during the<br />

SHN process on the pure cutted Mo surface: it consists mainly <strong>of</strong> Mo2N.<br />

1800<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

Hardness<br />

(HV 0,01)<br />

in kg/(mm) 2<br />

Hardness vs. Depth - Carbo-SHN<br />

-15<br />

200<br />

-5 5 15 25 35 45 55 65 75 85 95 105 115 125 135 145 155 165 175 185 195 205<br />

Depth (µm) from interface<br />

Fig. 4: Hardness pr<strong>of</strong>ile for two TZM samples hardened with the HT SHN process<br />

Hardness 3 long. a<br />

Hardness 3 long. b<br />

Hardness 3 transv.<br />

Fig. 5: LO micrograph <strong>of</strong> the cross section <strong>of</strong> a carbo nitride TZM (left) and <strong>of</strong> a silico nitrided Mo (right) sample


Nigg, Martinz and Lechleitner 17th Plansee Seminar 2009, Vol. 1 RM 55/5<br />

Fig. 6 shows the hardness pr<strong>of</strong>ile through the silicide zone down to the Mo substrate. There is a thin<br />

layer in between, most probably Mo5Si3 (EDX). As can be seen also from table I the hardness has a<br />

steep gradient into the molybdenum substrate. The layer hardness is lower compared to the nitrided or<br />

carbo nitrided substrates. This may – to a small extent – be caused <strong>by</strong> the s<strong>of</strong>ter base material Mo<br />

instead <strong>of</strong> TZM. From literature [7] it is known that MoSi2 should be s<strong>of</strong>ter than Mo nitrides or Mo<br />

carbides, but much more oxidation resistant. The pack siliconizing <strong>of</strong> the samples was performed in a<br />

way that the inner volume was not filled with pack mixture in case <strong>of</strong> the long and thin tubes (fig. 7, left).<br />

Nevertheless the inner cylindrical surface (diameter 2.4 x length 23.2 mm 3 ) was siliconized completely <strong>by</strong><br />

the evaporation <strong>of</strong> silicon fluoride which is formed from NaF and Si. The thickness <strong>of</strong> the silicide layer<br />

inside the long tube <strong>of</strong> fig. 7 lies between 20 and 50 µm (fig. 8). This result is important because the real<br />

parts which eventually have to be hardened in that way – the HRNs (Hot Runner Nozzles; fig. 7, right) –<br />

also have thin channels. More work must be done especially to control the thickness distribution and<br />

roughness <strong>of</strong> the layers, furthermore to check the oxidation and abrasion resistance.<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

0<br />

Hardness<br />

(HV 15mN)<br />

in kg/(mm) 2<br />

-60 -40 -20 0 20 40 60 80 100 120<br />

Fig. 6: Nanoindentation Hardness pr<strong>of</strong>ile for a sample hardened with the silico SHN process<br />

Summary and outlook<br />

Hardness vs. Depth - Silico SHN<br />

Depth [µm] from the interface<br />

Up to now for the plastic injection moulding <strong>of</strong> very corrosive and abrasive polymer melts TZM<br />

or SHN treated TZM HRNs are used. For further improvement <strong>of</strong> the standard SHN diffusion<br />

layer various measures were performed and evaluated: Higher process temperatures for SHN<br />

lead to a flater hardness pr<strong>of</strong>ile, addition <strong>of</strong> hydrocarbon to the ammonia and a higher process<br />

temperature show a comparable, but significantly weaker effect and – finally – silico nitriding (in<br />

two steps) causes a modified silicide layer which has to be investigated intensely and optimized<br />

in future.


RM 55/6 17th Plansee Seminar 2009, Vol. 1 Nigg, Martinz and Lechleitner<br />

Fig. 7: Macros <strong>of</strong> silico SHN treated Mo tubes (left) and <strong>of</strong> a variety <strong>of</strong> TZM HRNs for PIM application<br />

Fig. 8: LO micrograph <strong>of</strong> the cross sections <strong>of</strong> a silico nitrided Mo tube: longitudinal (left), transversal (right)<br />

References<br />

1. H.-P. Martinz and K. Prandini, Int. J. <strong>of</strong> Refractory & Hard Materials 12, pp.179 – 186 (1994)<br />

2. I. Jauberteau., J.L. Jauberteau, M. Cahoreau and J. Aubreton, Appl. Phys. 38, pp. 3654 – 3663<br />

(2005)<br />

3. Y. M. Lakhtin and Y. D. Kogan, Metal Science and Heat Treatment 10 / 1, pp. 24 – 28 (1968)<br />

4. T. Nakajima and T. Shirasaki, J. Electrochem. Soc. 144 /6, pp. 2096 – 2100 (1997)<br />

5. W. D. Sproul, Contract No. NAS 8-37686 – Final Report for NASA Marshall Space Flight Center<br />

(1993)<br />

6. H.-P. Martinz and B. Nigg, Proceedings 20 th International Conference on <strong>Surface</strong> Modification<br />

Technologies, Vienna, pp. 100 – 106, ASM (2006)<br />

7. D. Manomaisupat, D.S. Wilkinson and A. Petric, Journal <strong>of</strong> Materials Science, Volume 33, Number<br />

9, pp. 2319-2330 (1998)

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