{"id":449,"date":"2013-11-18T21:56:03","date_gmt":"2013-11-18T19:56:03","guid":{"rendered":"https:\/\/wissen.science-and-fun.de\/chemistry\/?p=449"},"modified":"2013-12-02T20:55:09","modified_gmt":"2013-12-02T18:55:09","slug":"dysprosium","status":"publish","type":"post","link":"https:\/\/wissen.science-and-fun.de\/chemistry\/2013\/11\/18\/dysprosium\/","title":{"rendered":"Dysprosium"},"content":{"rendered":"

NMR- Data<\/h2>\n\n\n\n\n\n\n\n\n\n\n\n\n\n
Isotope<\/td>\n\u00a0161<\/sup>Dy<\/td>\nSpin<\/td>\n\u00a05\/2<\/td>\n<\/tr>\n
Natural abundance (%)<\/td>\n\u00a018.91<\/td>\nMagnetic moment \u03bc\/\u03bcN<\/sub><\/td>\n\u00a0-0.5683<\/td>\n<\/tr>\n
Magnetogyric ratio
\n\u03b3\/107<\/sup>rad s-1<\/sup>T-1<\/sup><\/td>\n		\u00a0-0.9201<\/td>\nQuadrupole moment
\nQ\/fm2<\/sup><\/td>\n		\u00a0250.7<\/td>\n<\/tr>\n
Frequency ratio
\n\u039e\/%<\/td>\n		\u00a0(3.44)<\/td>\n<\/td>\n<\/td>\n<\/tr>\n
Larmor Frequenzies (MHz) vs. Bruker Field Strengths (Tesla<\/span>)<\/th>\n<\/tr>\n
7.04925<\/td>\n9.39798<\/td>\n11.7467<\/td>\n14.0954<\/td>\n<\/tr>\n
\u00a010.32<\/td>\n\u00a013.75<\/td>\n\u00a017.19<\/td>\n\u00a020.63<\/td>\n<\/tr>\n
16.4442<\/td>\n17.6185<\/td>\n18.7929<\/td>\n19.9673<\/td>\n<\/tr>\n
\u00a024.07<\/td>\n\u00a025.78<\/td>\n\u00a027.50<\/td>\n\u00a029.22<\/td>\n<\/tr>\n
21.1416<\/td>\n22.3160<\/td>\n23.4904<\/td>\n<\/td>\n<\/tr>\n
\u00a030.94<\/td>\n\u00a032.66<\/td>\n\u00a034.38<\/td>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n
\n\n\n\n\n\n\n\n\n\n\n\n\n\n
Isotope<\/td>\n\u00a0163<\/sup>Dy<\/td>\nSpin<\/td>\n\u00a05\/2<\/td>\n<\/tr>\n
Natural abundance (%)<\/td>\n\u00a024.90<\/td>\nMagnetic moment \u03bc\/\u03bcN<\/sub><\/td>\n\u00a00.7958<\/td>\n<\/tr>\n
Magnetogyric ratio
\n\u03b3\/107<\/sup>rad s-1<\/sup>T-1<\/sup><\/td>\n		\u00a01.289<\/td>\nQuadrupole moment
\nQ\/fm2<\/sup><\/td>\n		\u00a0264.8<\/td>\n<\/tr>\n
Frequency ratio
\n\u039e\/%<\/td>\n		\u00a0(4.82)<\/td>\n<\/td>\n<\/td>\n<\/tr>\n
Larmor Frequenzies (MHz) vs. Bruker Field Strengths (Tesla<\/span>)<\/th>\n<\/tr>\n
7.04925<\/td>\n9.39798<\/td>\n11.7467<\/td>\n14.0954<\/td>\n<\/tr>\n
\u00a014.46<\/td>\n\u00a019.28<\/td>\n\u00a024.10<\/td>\n\u00a028.92<\/td>\n<\/tr>\n
16.4442<\/td>\n17.6185<\/td>\n18.7929<\/td>\n19.9673<\/td>\n<\/tr>\n
\u00a033.74<\/td>\n\u00a036.15<\/td>\n\u00a038.56<\/td>\n\u00a040.97<\/td>\n<\/tr>\n
21.1416<\/td>\n22.3160<\/td>\n23.4904<\/td>\n<\/td>\n<\/tr>\n
\u00a043.38<\/td>\n\u00a045.79<\/td>\n\u00a048.20<\/td>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"

NMR- Data Isotope \u00a0161Dy Spin \u00a05\/2 Natural abundance (%) \u00a018.91 Magnetic moment \u03bc\/\u03bcN \u00a0-0.5683 Magnetogyric ratio \u03b3\/107rad s-1T-1 \u00a0-0.9201 Quadrupole moment Q\/fm2 \u00a0250.7 Frequency ratio \u039e\/% \u00a0(3.44) Larmor Frequenzies (MHz) vs. Bruker Field Strengths (Tesla) 7.04925 9.39798 11.7467 14.0954 \u00a010.32 \u00a013.75 \u00a017.19 \u00a020.63 16.4442 17.6185 18.7929 19.9673 \u00a024.07 \u00a025.78 \u00a027.50 \u00a029.22 21.1416 22.3160 23.4904 \u00a030.94 … <\/p>\n

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