Rubidium-85
Properties and data of the isotope 85Rb.
Rubidium-85 is a stable isotope of the chemical element rubidium, which has 48 neutrons in its atomic nucleus in addition to the element-specific 37 protons; the sum of the number of these atomic nucleus building blocks results in a mass number of 85. Rb-85 accounts for 72,17 % of natural terrestrial rubidium deposits.
The discovery of Rubidium-85 using a Cavendish mass spectrograph was reported in 1921 [1].
See also: List of individual Rubidium isotopes (and general data sources).
General data
Name of the isotope:Rubidium-85; Rb-85Symbol:85Rb or 8537RbMass number A:85 (= number of nucleons)Atomic number Z:37 (= number of protons)Neutrons N:48Nucleon pairing (Z - N):odd - evenNuclear ratio (N/Z ratio):1.2972972972973 (= neutron-proton ratio)Neutron excess (N-Z):11Isotopic mass:84.911789736(5) u (atomic weight of Rubidium-85)Nuclide mass:84.8914931 u (calculated nuclear mass without electrons)Mass excess:-82.16733 MeVMass defect:0.793652416 u (per nucleus)Nuclear binding energy:739.28246359 MeV (per nucleus)
8.69744075 MeV (average binding energy per nucleon)Separation energy:SN = 10.4797(22) MeV (first neutron)
SP = 7.016966(6) MeV (first proton)Half-life:stableSpin and parity:
(nuclear angular momentum)5/2-Magnetic dipole moment:μ(μN) = +1.35306(4)Charge radius:4.2036(23) femtometer fmYear of discovery:1921
Parent Nuclides
Direct parent isotopes are: 85Kr, 85Sr.
Occurrence
Comparison of the natural Rubidium isotopes including isotopic abundance (mole fraction of the isotope mixture in percent):
| | Atomic Mass ma | Quantity | Half-life | Spin |
|---|
Rubidium Isotopic mixture | 85.4678 u | 100 % | | |
| Isotope 85Rb | 84.911789736(5) u | 72.17(2) % | stable | 5/2- |
| Isotope 87Rb | 86.909180529(6) u | 27.83(2) % | 4.97(3) × 1010 a | 3/2- |
NMR data
Nuclear magnetic properties and parameters of the NMR active Nuclide 85Rb
Isotope:85Rb-NMRQuantity:72.17(2) %Spin:5/2-Nuclearmagnetic moment
μ/μN:+1.35306(4)Gyromagnetic ratio γ:2.5923 · 107 rad T-1 s-1
4.12577 MHz T-1Nuclear g-factor:gl = 0.541224Quadrupole moment Q:+0.276(1) barn (100 fm2)Line width parameter (factor):l = 243.76 fm4Resonance frequency:v0 = 4.1253 MHz at 1 TRelative Sensitivity:[related to 1H = 1.000]:
0.01061 (H0 = const.)
1.1304 (v0 = const.)
0.00767 (at natural abundance)
relative receptivity as compared to 13C:
45.0 (at natural abundance)
62.4 (enriched)Reference compound:
(conditions)In 85Rb-NMR, a solution of 0.01M rubidium chloride (RbCl) in deuterium oxide> (D2O) is used for calibration.Frequency ratio:Ξ(85Rb) = 9.654943 % [based on the reference substance]Chemical shift range:ca. 110 ppm [-80 to +30]
Nuclear Isomers
Nuclear isomers or excited states with the activation energy in keV related to the ground state.
| Nuclear Isomer | Excitation Energy | Half-life | Spin |
|---|
| 85mRb | 514.0065(22) keV | 1.015 μs | 9/2+ |
Isotones and Isobars
The following table shows the atomic nuclei that are isotonic (same neutron number N = 48) and isobaric (same nucleon number A = 85) with Rubidium-85. Naturally occurring isotopes are marked in green; light green = naturally occurring radionuclides.
| Z | Isotone N = 48 | Isobar A = 85 |
| 26 | 74Fe | |
| 27 | 75Co | |
| 28 | 76Ni | |
| 29 | 77Cu | |
| 30 | 78Zn | 85Zn |
| 31 | 79Ga | 85Ga |
| 32 | 80Ge | 85Ge |
| 33 | 81As | 85As |
| 34 | 82Se | 85Se |
| 35 | 83Br | 85Br |
| 36 | 84Kr | 85Kr |
| 37 | 85Rb | 85Rb |
| 38 | 86Sr | 85Sr |
| 39 | 87Y | 85Y |
| 40 | 88Zr | 85Zr |
| 41 | 89Nb | 85Nb |
| 42 | 90Mo | 85Mo |
| 43 | 91Tc | 85Tc |
| 44 | 92Ru | 85Ru |
| 45 | 93Rh | |
| 46 | 94Pd | |
| 47 | 95Ag | |
| 48 | 96Cd | |
| 49 | 97In | |
| 50 | 98Sn | |
External data and identifiers
Literature and References
[1] - F. W. ASTON:
The Constitution of the Alkali Metals.
In: Nature, 107, 72, (1921), DOI 10.1038/107072b0.
[2] - Yu. I. Neronov, A. N. Pronin:
Study of NMR Signals of Rubidium in Aqueous Solutions and Determination of the Magnetic Moments of Rb-85 and Rb-87 Nuclei.
In: Technical Physics, 68(3), (2023), DOI 10.1134/S106378422390070X.
Last update: 2026-01-24
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