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 256 Md, in 1955.
De kortstlevende isotoop van mendelevium is 245 Md, met een halfwaardetijd van ongeveer 0,9 milliseconden . De langstlevende is 258 Md, met een halfwaardetijd van 51,5 dagen .
Overzicht
Nuclide
Z (p )
N (n )
Isotopische massa (u)
Halveringstijd
Radioactief verval
Kernspin
Excitatie-energie
245 Md
101
144
245,08083(35)
0,90(25) ms
SS
(1/2− )
Md
101
245
⟶ ⟶ -->
Es
99
241
+
2
4
α α -->
{\displaystyle {\ce {{^{245}_{101}Md}->{^{241}_{99}Es}+\,_{2}^{4}\alpha }}}
(zelden)
245m Md
200(100) keV
400(200) ms
Md
101
245
m
⟶ ⟶ -->
Es
99
241
+
2
4
α α -->
{\displaystyle {\ce {{^{245m}_{101}Md}->{^{241}_{99}Es}+\,_{2}^{4}\alpha }}}
(7/2+ )
Md
101
245
⟶ ⟶ -->
Fm
100
245
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{245}_{101}Md}->{^{245}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(zelden)
246 Md
101
145
246,08189(35)
1,0(4) s
Md
101
246
⟶ ⟶ -->
Es
99
242
+
2
4
α α -->
{\displaystyle {\ce {{^{246}_{101}Md}->{^{242}_{99}Es}+\,_{2}^{4}\alpha }}}
Md
101
246
⟶ ⟶ -->
Fm
100
246
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{246}_{101}Md}->{^{246}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(zelden)
247 Md
101
146
247,08164(35)
1,12(22) s
SS
1/2−
Md
101
247
⟶ ⟶ -->
Es
99
243
+
2
4
α α -->
{\displaystyle {\ce {{^{247}_{101}Md}->{^{243}_{99}Es}+\,_{2}^{4}\alpha }}}
(zelden)
247m Md
± 0,2 s
Md
101
247
m
⟶ ⟶ -->
Es
99
243
+
2
4
α α -->
{\displaystyle {\ce {{^{247m}_{101}Md}->{^{243}_{99}Es}+\,_{2}^{4}\alpha }}}
(99,99%)
SS (10−4 %)
248 Md
101
147
248,08282(26)
7(3) s
Md
101
248
⟶ ⟶ -->
Fm
100
248
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{248}_{101}Md}->{^{248}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(80%)
Md
101
248
⟶ ⟶ -->
Es
99
244
+
2
4
α α -->
{\displaystyle {\ce {{^{248}_{101}Md}->{^{244}_{99}Es}+\,_{2}^{4}\alpha }}}
(20%)
SS (0,05%)
249 Md
101
148
249,08301(24)
24(4) s
Md
101
249
⟶ ⟶ -->
Es
99
245
+
2
4
α α -->
{\displaystyle {\ce {{^{249}_{101}Md}->{^{245}_{99}Es}+\,_{2}^{4}\alpha }}}
(60%)
(7/2− )
Md
101
249
⟶ ⟶ -->
Fm
100
249
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{249}_{101}Md}->{^{249}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(40%)
249m Md
100(100) keV
1,9(9) s
(1/2− )
250 Md
101
149
250,08442(32)
52(6) s
Md
101
250
⟶ ⟶ -->
Fm
100
250
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{250}_{101}Md}->{^{250}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(93%)
Md
101
250
⟶ ⟶ -->
Es
99
246
+
2
4
α α -->
{\displaystyle {\ce {{^{250}_{101}Md}->{^{246}_{99}Es}+\,_{2}^{4}\alpha }}}
(7%)
SS (0,02%)
251 Md
101
150
251,08484(22)
4,0(5) min
Md
101
251
⟶ ⟶ -->
Fm
100
251
+
e
+
+
ν 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 α -->
{\displaystyle {\ce {{^{251}_{101}Md}->{^{247}_{99}Es}+\,_{2}^{4}\alpha }}}
(10%)
252 Md
101
151
252,08656(21)
2,3(8) min
Md
101
252
⟶ ⟶ -->
Fm
100
252
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{252}_{101}Md}->{^{252}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(50%)
Md
101
252
⟶ ⟶ -->
Es
99
248
+
2
4
α α -->
{\displaystyle {\ce {{^{252}_{101}Md}->{^{248}_{99}Es}+\,_{2}^{4}\alpha }}}
(50%)
253 Md
101
152
253,08728(22)
12(8) min
Md
101
253
⟶ ⟶ -->
Fm
100
253
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{253}_{101}Md}->{^{253}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
7/2−
Md
101
253
⟶ ⟶ -->
Es
99
249
+
2
4
α α -->
{\displaystyle {\ce {{^{253}_{101}Md}->{^{249}_{99}Es}+\,_{2}^{4}\alpha }}}
254 Md
101
153
254,08966(11)
10(3) min
Md
101
254
⟶ ⟶ -->
Fm
100
254
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{254}_{101}Md}->{^{254}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(0− )
Md
101
254
⟶ ⟶ -->
Es
99
250
+
2
4
α α -->
{\displaystyle {\ce {{^{254}_{101}Md}->{^{250}_{99}Es}+\,_{2}^{4}\alpha }}}
(zelden)
254m Md
50(100) keV
28(8) min
Md
101
254
⟶ ⟶ -->
Fm
100
254
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{254}_{101}Md}->{^{254}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(3− )
Md
101
254
⟶ ⟶ -->
Es
99
250
+
2
4
α α -->
{\displaystyle {\ce {{^{254}_{101}Md}->{^{250}_{99}Es}+\,_{2}^{4}\alpha }}}
(zelden)
255 Md
101
154
255,091083(7)
27(2) min
Md
101
255
⟶ ⟶ -->
Fm
100
255
+
e
+
+
ν 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 α -->
{\displaystyle {\ce {{^{255}_{101}Md}->{^{251}_{99}Es}+\,_{2}^{4}\alpha }}}
(8%)
SS (0,15%)
256 Md
101
155
256,09406(6)
77(2) min
Md
101
256
⟶ ⟶ -->
Fm
100
256
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{256}_{101}Md}->{^{256}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(89%)
(1− )
Md
101
256
⟶ ⟶ -->
Es
99
252
+
2
4
α α -->
{\displaystyle {\ce {{^{256}_{101}Md}->{^{252}_{99}Es}+\,_{2}^{4}\alpha }}}
(11%)
257 Md
101
156
257,095541(3)
5,52(5) uur
Md
101
257
+
e
− − -->
⟶ ⟶ -->
Fm
100
257
+
ν 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 α -->
{\displaystyle {\ce {{^{257}_{101}Md}->{^{253}_{99}Es}+\,_{2}^{4}\alpha }}}
(15,2%)
SS (1%)
258 Md
101
157
258,098431(5)
51,5(3) dagen
Md
101
258
⟶ ⟶ -->
Es
99
254
+
2
4
α α -->
{\displaystyle {\ce {{^{258}_{101}Md}->{^{254}_{99}Es}+\,_{2}^{4}\alpha }}}
(99,99%)
(8− )
Md
101
258
⟶ ⟶ -->
No
102
258
+
e
− − -->
+
ν ν -->
¯ ¯ -->
e
{\displaystyle {\ce {{^{258}_{101}Md}->{^{258}_{102}No}+{e^{-}}+{\bar {\nu }}_{e}}}}
(0,0015%)
Md
101
258
⟶ ⟶ -->
Fm
100
258
+
e
+
+
ν ν -->
e
{\displaystyle {\ce {{^{258}_{101}Md}->{^{258}_{100}Fm}+{e^{+}}+{\nu }_{e}}}}
(0,0015%)
258m Md
0(200) keV
57,0(9) min
Md
101
258
+
e
− − -->
⟶ ⟶ -->
Fm
100
258
+
ν 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 ν -->
¯ ¯ -->
e
{\displaystyle {\ce {{^{258}_{101}Md}->{^{258}_{102}No}+{e^{-}}+{\bar {\nu }}_{e}}}}
(10%)
Md
101
258
⟶ ⟶ -->
Es
99
254
+
2
4
α α -->
{\displaystyle {\ce {{^{258}_{101}Md}->{^{254}_{99}Es}+\,_{2}^{4}\alpha }}}
(1,2%)
259 Md
101
158
259,10051(22)
1,60(6) uur
SS (98,7%)
7/2−
Md
101
259
⟶ ⟶ -->
Es
99
255
+
2
4
α α -->
{\displaystyle {\ce {{^{259}_{101}Md}->{^{255}_{99}Es}+\,_{2}^{4}\alpha }}}
(1,3%)
260 Md
101
159
260,10365(34)
27,8(8) dagen
SS (85%)
Md
101
260
⟶ ⟶ -->
Es
99
256
+
2
4
α α -->
{\displaystyle {\ce {{^{260}_{101}Md}->{^{256}_{99}Es}+\,_{2}^{4}\alpha }}}
(5%)
Md
101
260
+
e
− − -->
⟶ ⟶ -->
Fm
100
260
+
ν ν -->
e
{\displaystyle {\ce {{^{260}_{101}Md}+{e^{-}}->{^{260}_{100}Fm}+{\nu }_{e}}}}
(5%)
Md
101
260
⟶ ⟶ -->
No
102
260
+
e
− − -->
+
ν ν -->
¯ ¯ -->
e
{\displaystyle {\ce {{^{260}_{101}Md}->{^{260}_{102}No}+{e^{-}}+{\bar {\nu }}_{e}}}}
(3,5%)
261 Md
101
160
261,10572(70)
40 min
7/2−
262 Md
101
161
262,10887(63)
3 min
Overzicht van isotopen per element
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