Isotopen van mendelevium

Het chemisch element mendelevium (Md), met een atoommassa van ongeveer 258 u, bezit geen stabiele isotopen en wordt dus geclassificeerd als radioactief element. De 17 radio-isotopen zijn onstabiel en hebben een relatief korte halfwaardetijd (de meeste minder dan een uur).

In de natuur komt geen mendelevium voor: alle isotopen zijn synthetisch bereid in een laboratorium. De eerste synthetische isotoop was 256Md, in 1955.

De kortstlevende isotoop van mendelevium is 245Md, met een halfwaardetijd van ongeveer 0,9 milliseconden. De langstlevende is 258Md, met een halfwaardetijd van 51,5 dagen.

Overzicht

Nuclide Z (p) N (n) Isotopische massa (u) Halveringstijd Radioactief verval Kernspin
Excitatie-energie
245Md 101 144 245,08083(35) 0,90(25) ms SS (1/2)
Md 101 245 Es 99 241 + 2 4 α {\displaystyle {\ce {{^{245}_{101}Md}->{^{241}_{99}Es}+\,_{2}^{4}\alpha }}} (zelden)
245mMd 200(100) keV 400(200) ms Md 101 245 m Es 99 241 + 2 4 α {\displaystyle {\ce {{^{245m}_{101}Md}->{^{241}_{99}Es}+\,_{2}^{4}\alpha }}} (7/2+)
Md 101 245 Fm 100 245 + e + + ν e {\displaystyle {\ce {{^{245}_{101}Md}->{^{245}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (zelden)
246Md 101 145 246,08189(35) 1,0(4) s Md 101 246 Es 99 242 + 2 4 α {\displaystyle {\ce {{^{246}_{101}Md}->{^{242}_{99}Es}+\,_{2}^{4}\alpha }}}
Md 101 246 Fm 100 246 + e + + ν e {\displaystyle {\ce {{^{246}_{101}Md}->{^{246}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (zelden)
247Md 101 146 247,08164(35) 1,12(22) s SS 1/2
Md 101 247 Es 99 243 + 2 4 α {\displaystyle {\ce {{^{247}_{101}Md}->{^{243}_{99}Es}+\,_{2}^{4}\alpha }}} (zelden)
247mMd ± 0,2 s Md 101 247 m Es 99 243 + 2 4 α {\displaystyle {\ce {{^{247m}_{101}Md}->{^{243}_{99}Es}+\,_{2}^{4}\alpha }}} (99,99%)
SS (10−4%)
248Md 101 147 248,08282(26) 7(3) s Md 101 248 Fm 100 248 + e + + ν e {\displaystyle {\ce {{^{248}_{101}Md}->{^{248}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (80%)
Md 101 248 Es 99 244 + 2 4 α {\displaystyle {\ce {{^{248}_{101}Md}->{^{244}_{99}Es}+\,_{2}^{4}\alpha }}} (20%)
SS (0,05%)
249Md 101 148 249,08301(24) 24(4) s Md 101 249 Es 99 245 + 2 4 α {\displaystyle {\ce {{^{249}_{101}Md}->{^{245}_{99}Es}+\,_{2}^{4}\alpha }}} (60%) (7/2)
Md 101 249 Fm 100 249 + e + + ν e {\displaystyle {\ce {{^{249}_{101}Md}->{^{249}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (40%)
249mMd 100(100) keV 1,9(9) s (1/2)
250Md 101 149 250,08442(32) 52(6) s Md 101 250 Fm 100 250 + e + + ν e {\displaystyle {\ce {{^{250}_{101}Md}->{^{250}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (93%)
Md 101 250 Es 99 246 + 2 4 α {\displaystyle {\ce {{^{250}_{101}Md}->{^{246}_{99}Es}+\,_{2}^{4}\alpha }}} (7%)
SS (0,02%)
251Md 101 150 251,08484(22) 4,0(5) min Md 101 251 Fm 100 251 + e + + ν e {\displaystyle {\ce {{^{251}_{101}Md}->{^{251}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (90%) 7/2
Md 101 251 Es 99 247 + 2 4 α {\displaystyle {\ce {{^{251}_{101}Md}->{^{247}_{99}Es}+\,_{2}^{4}\alpha }}} (10%)
252Md 101 151 252,08656(21) 2,3(8) min Md 101 252 Fm 100 252 + e + + ν e {\displaystyle {\ce {{^{252}_{101}Md}->{^{252}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (50%)
Md 101 252 Es 99 248 + 2 4 α {\displaystyle {\ce {{^{252}_{101}Md}->{^{248}_{99}Es}+\,_{2}^{4}\alpha }}} (50%)
253Md 101 152 253,08728(22) 12(8) min Md 101 253 Fm 100 253 + e + + ν e {\displaystyle {\ce {{^{253}_{101}Md}->{^{253}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} 7/2
Md 101 253 Es 99 249 + 2 4 α {\displaystyle {\ce {{^{253}_{101}Md}->{^{249}_{99}Es}+\,_{2}^{4}\alpha }}}
254Md 101 153 254,08966(11) 10(3) min Md 101 254 Fm 100 254 + e + + ν e {\displaystyle {\ce {{^{254}_{101}Md}->{^{254}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (0)
Md 101 254 Es 99 250 + 2 4 α {\displaystyle {\ce {{^{254}_{101}Md}->{^{250}_{99}Es}+\,_{2}^{4}\alpha }}} (zelden)
254mMd 50(100) keV 28(8) min Md 101 254 Fm 100 254 + e + + ν e {\displaystyle {\ce {{^{254}_{101}Md}->{^{254}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (3)
Md 101 254 Es 99 250 + 2 4 α {\displaystyle {\ce {{^{254}_{101}Md}->{^{250}_{99}Es}+\,_{2}^{4}\alpha }}} (zelden)
255Md 101 154 255,091083(7) 27(2) min Md 101 255 Fm 100 255 + e + + ν e {\displaystyle {\ce {{^{255}_{101}Md}->{^{255}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (92%) (7/2)
Md 101 255 Es 99 251 + 2 4 α {\displaystyle {\ce {{^{255}_{101}Md}->{^{251}_{99}Es}+\,_{2}^{4}\alpha }}} (8%)
SS (0,15%)
256Md 101 155 256,09406(6) 77(2) min Md 101 256 Fm 100 256 + e + + ν e {\displaystyle {\ce {{^{256}_{101}Md}->{^{256}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (89%) (1)
Md 101 256 Es 99 252 + 2 4 α {\displaystyle {\ce {{^{256}_{101}Md}->{^{252}_{99}Es}+\,_{2}^{4}\alpha }}} (11%)
257Md 101 156 257,095541(3) 5,52(5) uur Md 101 257 + e Fm 100 257 + ν e {\displaystyle {\ce {{^{257}_{101}Md}+{e^{-}}->{^{257}_{100}Fm}+{\nu }_{e}}}} (84,8%) (7/2)
Md 101 257 Es 99 253 + 2 4 α {\displaystyle {\ce {{^{257}_{101}Md}->{^{253}_{99}Es}+\,_{2}^{4}\alpha }}} (15,2%)
SS (1%)
258Md 101 157 258,098431(5) 51,5(3) dagen Md 101 258 Es 99 254 + 2 4 α {\displaystyle {\ce {{^{258}_{101}Md}->{^{254}_{99}Es}+\,_{2}^{4}\alpha }}} (99,99%) (8)
Md 101 258 No 102 258 + e + ν ¯ e {\displaystyle {\ce {{^{258}_{101}Md}->{^{258}_{102}No}+{e^{-}}+{\bar {\nu }}_{e}}}} (0,0015%)
Md 101 258 Fm 100 258 + e + + ν e {\displaystyle {\ce {{^{258}_{101}Md}->{^{258}_{100}Fm}+{e^{+}}+{\nu }_{e}}}} (0,0015%)
258mMd 0(200) keV 57,0(9) min Md 101 258 + e Fm 100 258 + ν e {\displaystyle {\ce {{^{258}_{101}Md}+{e^{-}}->{^{258}_{100}Fm}+{\nu }_{e}}}} (70%) 1
SS (20%)
Md 101 258 No 102 258 + e + ν ¯ e {\displaystyle {\ce {{^{258}_{101}Md}->{^{258}_{102}No}+{e^{-}}+{\bar {\nu }}_{e}}}} (10%)
Md 101 258 Es 99 254 + 2 4 α {\displaystyle {\ce {{^{258}_{101}Md}->{^{254}_{99}Es}+\,_{2}^{4}\alpha }}} (1,2%)
259Md 101 158 259,10051(22) 1,60(6) uur SS (98,7%) 7/2
Md 101 259 Es 99 255 + 2 4 α {\displaystyle {\ce {{^{259}_{101}Md}->{^{255}_{99}Es}+\,_{2}^{4}\alpha }}} (1,3%)
260Md 101 159 260,10365(34) 27,8(8) dagen SS (85%)
Md 101 260 Es 99 256 + 2 4 α {\displaystyle {\ce {{^{260}_{101}Md}->{^{256}_{99}Es}+\,_{2}^{4}\alpha }}} (5%)
Md 101 260 + e Fm 100 260 + ν e {\displaystyle {\ce {{^{260}_{101}Md}+{e^{-}}->{^{260}_{100}Fm}+{\nu }_{e}}}} (5%)
Md 101 260 No 102 260 + e + ν ¯ e {\displaystyle {\ce {{^{260}_{101}Md}->{^{260}_{102}No}+{e^{-}}+{\bar {\nu }}_{e}}}} (3,5%)
261Md 101 160 261,10572(70) 40 min 7/2
262Md 101 161 262,10887(63) 3 min

Overzicht van isotopen per element

1 18
1 H 2 Periodiek systeem 13 14 15 16 17 He
2 Li Be De links verwijzen naar isotopen per element B C N O F Ne
3 Na Mg 3 4 5 6 7 8 9 10 11 12 Al Si P S Cl Ar
4 K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr
5 Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe
6 Cs Ba Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn
7 Fr Ra ↓↓ Rf Db Sg Bh Hs Mt Ds Rg Cn Nh Fl Mc Lv Ts Og
 
Lanthaniden La Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu
Actiniden Ac Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr
Bronnen
  • (en) R.B. Firestone, S.Y. Frank Chu & C.M. Baglin (1999) - Table of Isotopes (online versie van de cd-rom)
  • (en) G. Audi, A.H. Wapstra, C. Thibault, J. Blachot & O. Bersillon (2003) - The NUBASE evaluation of nuclear and decay properties, Nuclear Physics A, 729, pp. 3-128
  • (en) J.R. de Laeter, J.K. Böhlke, P. De Bièvre, H. Hidaka, H.S. Peiser, K.J.R. Rosman & P.D.P. Taylor (2003) - Atomic weights of the elements. Review 2000 (IUPAC Technical Report), Pure and Applied Chemistry, 75 (6), pp. 683–800
  • (en) M.E. Wieser (2006) - Atomic weights of the elements 2005 (IUPAC Technical Report), Pure and Applied Chemistry, 78 (11), pp. 2051–2066
  • (en) David R. Lide (2004) - CRC Handbook of Chemistry and Physics (85th ed.), hoofdstuk 11, CRC Press - ISBN 978-0849304859
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Isotopen van mendelevium (Md)

245Md · 245mMd · 246Md · 247Md · 247mMd · 248Md · 249Md · 249mMd · 250Md · 251Md · 252Md · 253Md · 254Md · 254mMd · 255Md · 256Md · 257Md · 258Md · 258mMd · 259Md · 260Md · 261Md · 262Md