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CPT International 04/2016

The leading technical journal for the global foundry industry – Das führende Fachmagazin für die weltweite Gießerei-Industrie

The leading technical journal for the
global foundry industry – Das führende Fachmagazin für die
weltweite Gießerei-Industrie

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Figure 6: Meshed geometry, red:<br />

melt, blue: die<br />

Figure 7: Calculated temperature distribution after the end of solidification,<br />

left: 1.2343, right: D185<br />

mation of a solid shell, leading to an<br />

additional heat resistance.<br />

For the heat transported through the<br />

die material the result is<br />

Q˙ = 4 kW.<br />

It can be seen immediately that the<br />

amount of heat transferred to the die<br />

surface is much greater than the amount<br />

of heat which can be removed by the die<br />

material. The same situation is given<br />

when the die surface is quenched rapidly<br />

by die spraying. In the case of die<br />

spraying the heat amount induced by<br />

water eva poration is also much greater<br />

than the heat which can be transported<br />

to the die surface. These circumstances<br />

lead to the formation of temperature<br />

peaks and subsequently to peaks<br />

in the thermal stresses especially at the<br />

surface of the die. The abrupt change<br />

of compressive and tensile stresses at<br />

the die surface is a well-known mechanism<br />

leading to fire cracks. A second<br />

effect of the limited heat conduction is<br />

that the cooling rates that are achievable<br />

by the implementation of cooling<br />

channels are limited by the die material.<br />

Higher thermal conductivity of the<br />

die material would lower the stress and<br />

temperature peaks and also potentially<br />

lower cycle times. Therefore benefits<br />

can be expected for both die life time<br />

and productivity.<br />

Comparison of heat conductivities<br />

As already mentioned materials with<br />

higher heat conductivities than the<br />

most commonly used die material, the<br />

hot working steel 1.2343, have been developed<br />

in the recent past. One example<br />

is the material HTCS 130 which<br />

was developed by Rovalma S.A., Barcelona,<br />

Spain. The heat conductivity of<br />

this steel at room temperature is close<br />

to that of pure iron so that it almost<br />

reaches the theoretical limit for iron<br />

based materials. The thermo-physical<br />

properties at room temperature and<br />

elevated temperatures have been published<br />

in [2]. If the heat conductivity<br />

potentials of iron based materials become<br />

insufficient for a certain purpose<br />

one has to switch to other material<br />

families. One possibility is the use<br />

of tungsten or molybdenum-based alloys.<br />

Their heat conductivities are way<br />

higher than that ones of iron based<br />

materials. Figure 1 shows a comparison<br />

of the heat conductivities of the<br />

materials 1.2343, HTCS 130 and D185.<br />

(All data in figure 1 were obtained at<br />

the Austrian Foundry Institute). It is<br />

remarkable that the heat conductivity<br />

of D185 is almost constant over the<br />

whole temperature range. This is quite<br />

advantageous for the hpdc-process.<br />

For that reason D185 was tested more<br />

comprehensively in technological test<br />

facilities representing industrial hpdc-conditions.<br />

Experimental – Trials at the<br />

test facility<br />

In order to quantify the heat removal<br />

capacities of different cooling concepts<br />

in hpdc with respect to cooling<br />

media (water, oil), flow properties and<br />

geometries as well as die materials a<br />

test facility was developed at the Austrian<br />

Foundry Institute. The trials with<br />

D185 were part of a larger investigation<br />

programme with different die materials.<br />

The results of this series of trials<br />

with several iron based materials have<br />

been published in [3] and [4]. The testing<br />

concept is similar to that presented<br />

here.<br />

Each testing device consists of an axially<br />

symmetrical body which is fabricated<br />

from the material which is requested<br />

to be tested. This body is heated<br />

up to a pre-set temperature of 260 °C<br />

by a conventional oil tempering device.<br />

The heat input of the liquid metal<br />

is simulated by six electrical cartridge<br />

heaters. In the center of the body is a<br />

bore hole where the cooling medium is<br />

passing through. The cooling media are<br />

directed by different standardized flow<br />

geometries. Figure 2 shows a schematic<br />

view of the construction. The body<br />

has 18 positions for thermocouples logging<br />

temperature values at six different<br />

distances from the surface of the bore<br />

hole and at three different length positions<br />

of the bore hole. A more detailed<br />

description is given in [3].<br />

The trial itself is divided into 5 stages:<br />

» Preheating of the body via oil tempering<br />

up to 260 °C,<br />

» Heating up to 350 °C via oil tempering<br />

and cartridge heaters,<br />

» Activating the cooling at active electrical<br />

heating with cartridges until<br />

an equilibrium temperature T equ.<br />

is<br />

reached,<br />

Casting Plant & Technology 4 / <strong>2016</strong> 27

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