Lecture handout including QS - Department of Materials Science ...
Lecture handout including QS - Department of Materials Science ...
Lecture handout including QS - Department of Materials Science ...
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Qu.Sheet 8 MATERIALS SCIENCE BQ4<br />
Course B: <strong>Materials</strong> for Devices<br />
Question Sheet 8<br />
1. (a) Sketch a unit cell <strong>of</strong> CaF 2 viewed down [001].<br />
(b) Describe the coordination <strong>of</strong> Ca by F, and <strong>of</strong> F by Ca.<br />
(c) Comment on the packing <strong>of</strong> Ca ions and the location <strong>of</strong> the F ions. How does this<br />
compare with the zinc blende structure<br />
(d) In δ-Bi 2 O 3 , the Bi sub-lattice is the same as that <strong>of</strong> Ca in CaF 2 and S in ZnS, but the<br />
stoichiometry means that there are vacant anion sites, randomly distributed. Sketch a<br />
possible unit cell <strong>of</strong> δ-Bi 2 O 3 .<br />
(e) Comment on why δ-Bi 2 O 3 is a fast ionic conductor whilst stoichiometric CaF 2 and ZnS<br />
are not.<br />
(f) Calculate the composition <strong>of</strong> YSZ (i.e. Y 2 O 3 doped ZrO 2 , Zr 1-x Y x O [2-(x/2)] ) which would<br />
give just one quarter <strong>of</strong> the oxygen vacancy concentration as in δ-Bi 2 O 3 .<br />
2. (Tripos Question; 2008)<br />
How is a high-temperature cubic zirconia phase stabilised at room temperature and what<br />
are the consequences for its oxygen mobility Describe how such a material might be<br />
used in a hydrogen fuel cell. In your answer refer to the chemical reactions involved and<br />
explain how a voltage is generated. [40%]<br />
Different amounts <strong>of</strong> yttria (Y 2 O 3 ) are added to zirconia (ZrO 2 ) to produce two ceramic<br />
materials: Y 0.1 Zr 0.9 O x and Y 0.15 Zr 0.85 O y . The molar cation compositions are readily<br />
determined, but what are the molar oxygen compositions x and y [10%]<br />
Both ceramic materials are cubic and give an X-ray diffraction pattern characteristic <strong>of</strong><br />
the fluorite structure, in which the first and largest peak is a reflection from the {111}<br />
planes. Using CuKα radiation this peak occurs at 2θ = 30.147° for Y 0.1 Zr 0.9 O x whereas it<br />
is shifted to 2θ = 29.732° for Y 0.15 Zr 0.85 O y . Give a reason for this change in the<br />
diffraction pattern between the two materials. [15%]<br />
(i) What are the oxygen vacancy concentrations, n, in Y 0.1 Zr 0.9 O x and in Y 0.15 Zr 0.85 O y <br />
(ii) At 1000°C the ionic conductivity <strong>of</strong> Y 0.1 Zr 0.9 O x is 2.5 × 10 -4 Ω -1 m -1 . What is the<br />
ionic conductivity <strong>of</strong> Y 0.15 Zr 0.85 O y at the same temperature<br />
(iii) Determine the diffusivity <strong>of</strong> oxygen in Y 0.15 Zr 0.85 O y at 1000°C. [35%]<br />
[ionic radii: Y 3+ = 1.159 Å, Zr 4+ = 0.98 Å, O 2- = 1.28 Å]<br />
3. (a) From the Arrhenius plot in your <strong>handout</strong> (BH47), showing ionic conductivity versus<br />
inverse temperature for a number <strong>of</strong> ionic conductors, estimate the activation energy for<br />
ion transport in yttria-stabilised zirconia (YSZ).<br />
(b) In Zr 0.8 Y 0.2 O 1.9 how many oxygen vacancies are there per unit cell If the lattice<br />
parameter <strong>of</strong> (cubic) YSZ is 0.54 nm, calculate the number density <strong>of</strong> vacancies.<br />
MT13