Effect of TiO2 Doping on the Structure and Microwave Dielectric Properties of Cordierite Ceramics. Issue 6 (20th March 2015)
- Record Type:
- Journal Article
- Title:
- Effect of TiO2 Doping on the Structure and Microwave Dielectric Properties of Cordierite Ceramics. Issue 6 (20th March 2015)
- Main Title:
- Effect of TiO2 Doping on the Structure and Microwave Dielectric Properties of Cordierite Ceramics
- Authors:
- Wu, Song
Song, Kaixin
Liu, Peng
Lin, Huixing
Zhang, Fangfang
Zheng, Peng
Qin, Huibin
Alford, N. - Abstract:
- <abstract abstract-type="main" id="jace13549-abs-0001"> <title> <x xml:space="preserve">Abstract</x> </title> <p>The (1−<italic>x</italic>)Mg<sub>2</sub>Al<sub>4</sub>Si<sub>5</sub>O<sub>18</sub>–<italic>x</italic>TiO<sub>2</sub> |(1−<italic>x</italic>)MAS‐<italic>x</italic>T| (0 ≤ <italic>x</italic> ≤ 0.35) cordierite ceramics are fabricated by solid‐state reaction method for obtaining near‐zero temperature coefficient of resonant frequency (τ<sub>f</sub>). The XRD and SEM results show that (1−<italic>x</italic>)MAS‐<italic>x</italic>T (0 ≤ <italic>x</italic> ≤ 0.10) ceramics exhibit single cordierite solid solution, whereas as 0.15 ≤ <italic>x</italic> ≤ 0.35, present composite phases of Mg<sub>2</sub>Al<sub>4</sub>Si<sub>5</sub>O<sub>18</sub> solution and TiO<sub>2</sub>. Rietveld refinements of XRD data suggest that the [(Si<sub>4</sub>Al<sub>2</sub>)O<sub>18</sub>] hexagonal shape in cordierite structure happens to alternate change from nonsymmetrical hexagonal rings to almost centrosymmetrical equilateral rings as <italic>x</italic> increases to 0.10 comparing to that of <italic>x</italic> = 0. As Ti<sup>4+</sup> ions squeeze into the [(Si<sub>4</sub>Al<sub>2</sub>)O<sub>18</sub>] rings structure, the orientation and shapes of the rings begin to rotate and expand from initial state of [1–20] (<italic>x</italic> = 0) to near [210] direction (<italic>x</italic> = 0.10), and then continue to expand toward close to [110] direction (<italic>x</italic> = 0.25). Due to<abstract abstract-type="main" id="jace13549-abs-0001"> <title> <x xml:space="preserve">Abstract</x> </title> <p>The (1−<italic>x</italic>)Mg<sub>2</sub>Al<sub>4</sub>Si<sub>5</sub>O<sub>18</sub>–<italic>x</italic>TiO<sub>2</sub> |(1−<italic>x</italic>)MAS‐<italic>x</italic>T| (0 ≤ <italic>x</italic> ≤ 0.35) cordierite ceramics are fabricated by solid‐state reaction method for obtaining near‐zero temperature coefficient of resonant frequency (τ<sub>f</sub>). The XRD and SEM results show that (1−<italic>x</italic>)MAS‐<italic>x</italic>T (0 ≤ <italic>x</italic> ≤ 0.10) ceramics exhibit single cordierite solid solution, whereas as 0.15 ≤ <italic>x</italic> ≤ 0.35, present composite phases of Mg<sub>2</sub>Al<sub>4</sub>Si<sub>5</sub>O<sub>18</sub> solution and TiO<sub>2</sub>. Rietveld refinements of XRD data suggest that the [(Si<sub>4</sub>Al<sub>2</sub>)O<sub>18</sub>] hexagonal shape in cordierite structure happens to alternate change from nonsymmetrical hexagonal rings to almost centrosymmetrical equilateral rings as <italic>x</italic> increases to 0.10 comparing to that of <italic>x</italic> = 0. As Ti<sup>4+</sup> ions squeeze into the [(Si<sub>4</sub>Al<sub>2</sub>)O<sub>18</sub>] rings structure, the orientation and shapes of the rings begin to rotate and expand from initial state of [1–20] (<italic>x</italic> = 0) to near [210] direction (<italic>x</italic> = 0.10), and then continue to expand toward close to [110] direction (<italic>x</italic> = 0.25). Due to centrosymmetry adjustment of [(Si<sub>4</sub>Al<sub>2</sub>)O<sub>18</sub>] hexagonal rings and of other microstructure factors improvement, the (1−<italic>x</italic>)MAS‐xT (<italic>x</italic> = 0.10) cordierite solution achieves optimum quality factor <italic>Q</italic><sub>f</sub>: ε<sub>r</sub> = 6.3, <italic>Q</italic><sub>f</sub> = 55 400 GHz (17.6 GHz), τ<sub>f</sub> = −21 ppm/°C. The (1−<italic>x</italic>)MAS‐<italic>x</italic>T (<italic>x</italic> = 0.25) composites obtain a near‐zero temperature coefficient of resonance frequency: ε<sub>r</sub> = 6.8, <italic>Q</italic><sub>f</sub> = 37 800 GHz (18.4 GHz), τ<sub>f</sub> = −0.2 ppm/°C.</p> </abstract> … (more)
- Is Part Of:
- Journal of the American Ceramic Society. Volume 98:Issue 6(2015)
- Journal:
- Journal of the American Ceramic Society
- Issue:
- Volume 98:Issue 6(2015)
- Issue Display:
- Volume 98, Issue 6 (2015)
- Year:
- 2015
- Volume:
- 98
- Issue:
- 6
- Issue Sort Value:
- 2015-0098-0006-0000
- Page Start:
- 1842
- Page End:
- 1847
- Publication Date:
- 2015-03-20
- Subjects:
- Ceramics -- Periodicals
620.1405 - Journal URLs:
- http://catalog.hathitrust.org/api/volumes/oclc/1479639.html ↗
http://onlinelibrary.wiley.com/journal/10.1111/(ISSN)1551-2916 ↗
http://www.ceramicjournal.org/home.html ↗
http://onlinelibrary.wiley.com/ ↗ - DOI:
- 10.1111/jace.13549 ↗
- Languages:
- English
- ISSNs:
- 0002-7820
- Deposit Type:
- Legaldeposit
- View Content:
- Available online (eLD content is only available in our Reading Rooms) ↗
- Physical Locations:
- British Library DSC - 4684.000000
British Library DSC - BLDSS-3PM
British Library HMNTS - ELD Digital store - Ingest File:
- 3068.xml