Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples
Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions m...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Sawant, S R [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1982 |
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| Schlagwörter: |
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| Anmerkung: |
© the Indian Academy of Sciences 1982 |
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| Übergeordnetes Werk: |
Enthalten in: Bulletin of materials science - Springer India, 1979, 4(1982), 1 vom: März, Seite 11-15 |
|---|---|
| Übergeordnetes Werk: |
volume:4 ; year:1982 ; number:1 ; month:03 ; pages:11-15 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF02744459 |
|---|
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OLC2055175076 |
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| 520 | |a Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. | ||
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10.1007/BF02744459 doi (DE-627)OLC2055175076 (DE-He213)BF02744459-p DE-627 ger DE-627 rakwb eng 600 VZ Sawant, S R verfasserin aut Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples 1982 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1982 Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. Dispersion quenching interfacial polarisation dielectric constant Patil, R N aut Enthalten in Bulletin of materials science Springer India, 1979 4(1982), 1 vom: März, Seite 11-15 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:4 year:1982 number:1 month:03 pages:11-15 https://doi.org/10.1007/BF02744459 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_30 GBV_ILN_70 AR 4 1982 1 03 11-15 |
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10.1007/BF02744459 doi (DE-627)OLC2055175076 (DE-He213)BF02744459-p DE-627 ger DE-627 rakwb eng 600 VZ Sawant, S R verfasserin aut Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples 1982 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1982 Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. Dispersion quenching interfacial polarisation dielectric constant Patil, R N aut Enthalten in Bulletin of materials science Springer India, 1979 4(1982), 1 vom: März, Seite 11-15 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:4 year:1982 number:1 month:03 pages:11-15 https://doi.org/10.1007/BF02744459 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_30 GBV_ILN_70 AR 4 1982 1 03 11-15 |
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10.1007/BF02744459 doi (DE-627)OLC2055175076 (DE-He213)BF02744459-p DE-627 ger DE-627 rakwb eng 600 VZ Sawant, S R verfasserin aut Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples 1982 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1982 Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. Dispersion quenching interfacial polarisation dielectric constant Patil, R N aut Enthalten in Bulletin of materials science Springer India, 1979 4(1982), 1 vom: März, Seite 11-15 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:4 year:1982 number:1 month:03 pages:11-15 https://doi.org/10.1007/BF02744459 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_30 GBV_ILN_70 AR 4 1982 1 03 11-15 |
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10.1007/BF02744459 doi (DE-627)OLC2055175076 (DE-He213)BF02744459-p DE-627 ger DE-627 rakwb eng 600 VZ Sawant, S R verfasserin aut Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples 1982 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1982 Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. Dispersion quenching interfacial polarisation dielectric constant Patil, R N aut Enthalten in Bulletin of materials science Springer India, 1979 4(1982), 1 vom: März, Seite 11-15 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:4 year:1982 number:1 month:03 pages:11-15 https://doi.org/10.1007/BF02744459 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_30 GBV_ILN_70 AR 4 1982 1 03 11-15 |
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10.1007/BF02744459 doi (DE-627)OLC2055175076 (DE-He213)BF02744459-p DE-627 ger DE-627 rakwb eng 600 VZ Sawant, S R verfasserin aut Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples 1982 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © the Indian Academy of Sciences 1982 Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. Dispersion quenching interfacial polarisation dielectric constant Patil, R N aut Enthalten in Bulletin of materials science Springer India, 1979 4(1982), 1 vom: März, Seite 11-15 (DE-627)130547476 (DE-600)781668-6 (DE-576)9130547474 0250-4707 nnns volume:4 year:1982 number:1 month:03 pages:11-15 https://doi.org/10.1007/BF02744459 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_30 GBV_ILN_70 AR 4 1982 1 03 11-15 |
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Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples |
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Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. © the Indian Academy of Sciences 1982 |
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Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. © the Indian Academy of Sciences 1982 |
| abstract_unstemmed |
Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer. © the Indian Academy of Sciences 1982 |
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2024-07-04T01:35:03.512Z |
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1803610387658047488 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2055175076</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402060624.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s1982 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02744459</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2055175076</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02744459-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">600</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Sawant, S R</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Dispersion of dielectric constant and resistivity of $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1982</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© the Indian Academy of Sciences 1982</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract $ Cu_{x} $ $ Zn_{1−x} $ $ Fe_{2} $$ O_{4} $ samples exhibit dispersion of dielectric constant, tanδ and resistivity in the frequency range of 1 kHz to 50 MHz. The dispersion exhibited is in general accord with Koops’ model. However, the details of the conducting and non-conducting regions must be taken into account when composition tends to change interrelationship between the elementary capacitor resistor circuits. On quenching these samples from 800°C the dielectric constantε1 showed an increase for $ CuFe_{2} $$ O_{4} $ and $ Cu_{0·8} $$ Zn_{0·2} $$ Fe_{2} $$ O_{4} $ samples. The dielectric constant of the remaining samples showed no influence on quenching. The compositional variation showed that the dielectric constant has higher value for the ferrite $ Cu_{0·4} $$ Zn_{0·6} $$ Fe_{2} $$ O_{4} $ The results are explained on the basis of cation transfer.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Dispersion</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">quenching</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">interfacial polarisation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">dielectric constant</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Patil, R N</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Bulletin of materials science</subfield><subfield code="d">Springer India, 1979</subfield><subfield code="g">4(1982), 1 vom: März, Seite 11-15</subfield><subfield code="w">(DE-627)130547476</subfield><subfield code="w">(DE-600)781668-6</subfield><subfield code="w">(DE-576)9130547474</subfield><subfield code="x">0250-4707</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:4</subfield><subfield code="g">year:1982</subfield><subfield code="g">number:1</subfield><subfield code="g">month:03</subfield><subfield code="g">pages:11-15</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02744459</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_30</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">4</subfield><subfield code="j">1982</subfield><subfield code="e">1</subfield><subfield code="c">03</subfield><subfield code="h">11-15</subfield></datafield></record></collection>
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