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Measurement of the Electrical Conductivity of zircon at High ...

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high melting temper<strong>at</strong>ure (Tab.1) and <strong>the</strong>refore high chemical activity <strong>of</strong> <strong>the</strong> oxides.<br />

Very <strong>of</strong>ten such physical properties as electrical or <strong>the</strong>rmal conductivity are known only<br />

near <strong>the</strong> normal conditions. D<strong>at</strong>a about electrical properties <strong>at</strong> high temper<strong>at</strong>ures from<br />

reference books very <strong>of</strong>ten are ra<strong>the</strong>r old or contradictory. There are <strong>the</strong>ories describing how<br />

<strong>the</strong>se properties change when physical conditions are varied, but <strong>the</strong>ir results sometimes are<br />

unstable. It is very difficult to verify existing d<strong>at</strong>a under extreme conditions and to get new<br />

experimental d<strong>at</strong>a for fur<strong>the</strong>r calcul<strong>at</strong>ions. Aims <strong>of</strong> this work were:<br />

1. Check <strong>of</strong> <strong>the</strong> ability to make qualit<strong>at</strong>ive measurements <strong>of</strong> <strong>the</strong> electrical resistance <strong>of</strong><br />

<strong>zircon</strong> using an existing equipment <strong>at</strong> high temper<strong>at</strong>ures (above 2400 0 C) ;<br />

2. Calcul<strong>at</strong>ion <strong>of</strong> <strong>the</strong> electrical conductivity <strong>of</strong> <strong>zircon</strong> in order to get <strong>the</strong> temper<strong>at</strong>ure<br />

dependence;<br />

3. Carrying out values <strong>of</strong> activ<strong>at</strong>ion energy <strong>of</strong> <strong>the</strong> sample;<br />

4. Comparison <strong>of</strong> <strong>the</strong> results with liter<strong>at</strong>ure d<strong>at</strong>a.<br />

1. Equipment<br />

1.1. Characteristics <strong>of</strong> Zircon<br />

Zircon ZrSiO 4 (Zr 51% and Si 14.5% <strong>of</strong> weight [6]) was chosen as m<strong>at</strong>erial for our<br />

experiments. Powder <strong>of</strong> <strong>zircon</strong>ium oxide ZrO 2 and powder <strong>of</strong> silicon oxide (SiO 2 ) were used<br />

as primary m<strong>at</strong>erials. Zirconium oxide has a melting temper<strong>at</strong>ure about 2700°C, but when it is<br />

Tab. 2. Interaction temper<strong>at</strong>ures (K) <strong>of</strong> <strong>the</strong> selected high<br />

temper<strong>at</strong>ure m<strong>at</strong>erials [2].<br />

C W Mo ThO 2 ZrO 2 MgO BeO<br />

BeO 2300 2000 1900 2100 1900 1800 ---<br />

MgO 1800 2000 1600 2200 2000 --- 1800<br />

ZrO 2 1600 1600 2200 2200 --- 2000 1900<br />

ThO 2 2000 2200 1900 --- 2200 2200 2100<br />

mixed with silicon oxide, <strong>the</strong><br />

melting temper<strong>at</strong>ure is lower.<br />

Zirconium oxide is<br />

stable in oxidized and<br />

moder<strong>at</strong>e reduction<br />

<strong>at</strong>mospheres in contact with<br />

many metals and o<strong>the</strong>r<br />

oxides. When it is he<strong>at</strong>ed up<br />

to temper<strong>at</strong>ures above<br />

1000°C it has destructive expansion <strong>of</strong> volume [2].<br />

The sample was made by pressing <strong>the</strong> powders toge<strong>the</strong>r. The volume <strong>of</strong> <strong>the</strong> crucible<br />

was complete filled with <strong>the</strong> powder, but during <strong>the</strong> experiment <strong>the</strong> height <strong>of</strong> <strong>the</strong> sample<br />

becomes lower because <strong>of</strong> sintering and vaporiz<strong>at</strong>ion <strong>of</strong> m<strong>at</strong>erials. Zircon can be taken out<br />

from <strong>the</strong> crucible if it was not liquid during <strong>the</strong> he<strong>at</strong>ing process, but if it is he<strong>at</strong>ed above <strong>the</strong><br />

melting temper<strong>at</strong>ure it sticks to <strong>the</strong> walls <strong>of</strong> <strong>the</strong> crucible and it could not be taken out without<br />

melting.<br />

According to <strong>the</strong> st<strong>at</strong>e diagram (Fig. 2) [6] <strong>the</strong> temper<strong>at</strong>ure <strong>of</strong> about 2400°C must be<br />

reached to get a liquid phase <strong>of</strong> <strong>zircon</strong>. But <strong>the</strong> melting temper<strong>at</strong>ure <strong>of</strong> silicon oxide is less<br />

and <strong>the</strong> pressure <strong>of</strong> vapours is about one <strong>at</strong>mosphere <strong>at</strong> 2200°C (temper<strong>at</strong>ure <strong>of</strong> vaporis<strong>at</strong>ion is<br />

1800°C). Because <strong>of</strong> this silicon intensively comes out and it changes <strong>the</strong> chemical<br />

composition <strong>of</strong> <strong>the</strong> sample so th<strong>at</strong> can influence <strong>the</strong> final measurements.<br />

1.2. Experimental Equipment<br />

A crucible made <strong>of</strong> wolfram (W) which has a melting temper<strong>at</strong>ure 3410°C [2] was used<br />

for <strong>the</strong> melting process (Fig. 3). The height <strong>of</strong> <strong>the</strong> crucible was 80 mm, <strong>the</strong> diameter was 80<br />

mm and <strong>the</strong> inner diameter was 64 mm.<br />

136

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