Atomic radius

The atomic radius of a chemical element is a measure of the size of its atoms, usually the mean or typical distance from the nucleus to the boundary of the surrounding cloud of electrons. Since the boundary is not a well-defined physical entity, there are various non-equivalent definitions of atomic radius.

Depending on the definition, the term may apply only to isolated atoms, or also to atoms in condensed matter, covalently bound in molecules, or in ionized and excited states; and its value may be obtained through experimental measurements, or computed from theoretical models. Under some definitions, the value of the radius may depend on the atom's state and context.[1]

The concept is difficult to define because the electrons do not have definite orbits, or sharply defined ranges. Rather, their positions must be described as probability distributions that taper off gradually as one moves away from the nucleus, without a sharp cutoff. Moreover, in condensed matter and molecules, the electron clouds of the atoms usually overlap to some extent, and some of the electrons may roam over a large region encompassing two or more atoms.

Despite these conceptual difficulties, under most definitions the radii of isolated neutral atoms range between 30 and 300 pm (trillionths of a meter), or between 0.3 and 3 angstroms. Therefore, the radius of an atom is more than 10,000 times the radius of its nucleus (1–10 fm),[2] and less than 1/1000 of the wavelength of visible light (400–700 nm).

For many purposes, atoms can be modeled as spheres. This is only a crude approximation, but it can provide quantitative explanations and predictions for many phenomena, such as the density of liquids and solids, the diffusion of fluids through molecular sieves, the arrangement of atoms and ions in crystals, and the size and shape of molecules.

Atomic radii vary in a predictable and explicable manner across the periodic table. For instance, the radii generally decrease along each period (row) of the table, from the alkali metals to the noble gases; and increase down each group (column). The radius increases sharply between the noble gas at the end of each period and the alkali metal at the beginning of the next period. These trends of the atomic radii (and of various other chemical and physical properties of the elements) can be explained by the electron shell theory of the atom; they provided important evidence for the development and confirmation of quantum theory.

Contents

History

In 1920, shortly after it had become possible to determine the sizes of atoms using X-ray crystallography, it was suggested that all atoms of the same element have the same radii.[3] However, in 1923, when more crystal data had become available, it was found that an atom does not have just one size. For example, the size of lithium atoms is different in lithium metal than in LiCl.[4]

Definitions

Widely used definitions of atomic radius include:

Empirically measured atomic radii

The following table shows empirically measured covalent radii for the elements, as published by J. C. Slater in 1964.[8] The values are in picometers (pm), with an accuracy of about 5 pm. The shade of the box ranges from red to yellow as the radius increases; gray indicates lack of data.

Group (vertical) 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18
Period (horizontal)
1 H
25		 He
 
2 Li
145		 Be
105		 B
85		 C
70		 N
65		 O
60		 F
50		 Ne
 
3 Na
180		 Mg
150		 Al
125		 Si
110		 P
100		 S
100		 Cl
100		 Ar
 
4 K
220		 Ca
180		 Sc
160		 Ti
140		 V
135		 Cr
140		 Mn
140		 Fe
140		 Co
135		 Ni
135		 Cu
135		 Zn
135		 Ga
130		 Ge
125		 As
115		 Se
115		 Br
115		 Kr
 
5 Rb
235		 Sr
200		 Y
180		 Zr
155		 Nb
145		 Mo
145		 Tc
135		 Ru
130		 Rh
135		 Pd
140		 Ag
160		 Cd
155		 In
155		 Sn
145		 Sb
145		 Te
140		 I
140		 Xe
 
6 Cs
260		 Ba
215		 *
 		 Hf
155		 Ta
145		 W
135		 Re
135		 Os
130		 Ir
135		 Pt
135		 Au
135		 Hg
150		 Tl
190		 Pb
180		 Bi
160		 Po
190		 At
 		 Rn
 
7 Fr
 		 Ra
215		 **
 		 Rf
 		 Db
 		 Sg
 		 Bh
 		 Hs
 		 Mt
 		 Ds
 		 Rg
 		 Cn
 		 Uut
 		 Uuq
 		 Uup
 		 Uuh
 		 Uus
 		 Uuo
 
Lanthanides *
 		 La
195		 Ce
185		 Pr
185		 Nd
185		 Pm
185		 Sm
185		 Eu
185		 Gd
180		 Tb
175		 Dy
175		 Ho
175		 Er
175		 Tm
175		 Yb
175		 Lu
175
Actinides **
 		 Ac
195		 Th
180		 Pa
180		 U
175		 Np
175		 Pu
175		 Am
175		 Cm
 		 Bk
 		 Cf
 		 Es
 		 Fm
 		 Md
 		 No
 		 Lr
 

Explanation of the general trends

The way the atomic radius varies with increasing atomic number can be explained by the arrangement of electrons in shells of fixed capacity. The shells are generally filled in order of increasing radius, since the negatively charged electrons are attracted by the positively charged protons in the nucleus. As the atomic number increases along each row of the periodic table, the additional electrons go into the same outermost shell; whose radius gradually contracts, due to the increasing nuclear charge. In a noble gas, the outermost shell is completely filled; therefore, the additional electron of next alkali metal will go into the next outer shell, accounting for the sudden increase in the atomic radius.

The increasing nuclear charge is partly counterbalanced by the increasing number of electrons, a phenomenon that is known as shielding; which explains why the size of atoms usually increases down each column. However, there are two occasions where shielding is less effective: in these cases, the atoms are smaller than would otherwise be expected.

The following table summarizes the main phenomena that influence the atomic radius of an element:

factor principle increase with... tend to effect on radius
electron shells quantum mechanics principal and azimuthal quantum numbers increase atomic radius increases down each column
nuclear charge attractive force acting on electrons by protons in nucleus atomic number decrease atomic radius decreases along each period
shielding repulsive force acting on outermost shell electrons by inner electrons number of electron shells increase atomic radius reduces the effect of the 2nd factor

Lanthanide contraction

Main article: Lanthanide contraction

The electrons in the 4f-subshell, which is progressively filled from cerium (Z = 58) to lutetium (Z = 71), are not particularly effective at shielding the increasing nuclear charge from the sub-shells further out. The elements immediately following the lanthanides have atomic radii which are smaller than would be expected and which are almost identical to the atomic radii of the elements immediately above them.[9] Hence hafnium has virtually the same atomic radius (and chemistry) as zirconium, and tantalum has an atomic radius similar to niobium, and so forth. The effect of the lanthanide contraction is noticeable up to platinum (Z = 78), after which it is masked by a relativistic effect known as the inert pair effect.

Due to lanthanide contraction, the 5 following observations can be drawn:

  1. The size of Ln3+ ions regularly decreases with atomic number. According to Fajans' rules, decrease in size of Ln3+ ions increases the covalent character and decreases the basic character between Ln3+ and OH− ions in Ln(OH)3. Hence the order of size of Ln3+ is given:
    La3+ > Ce3+ > ... , ... > Lu3+.
  2. There is a regular decrease in their ionic radii.
  3. There is a regular decrease in their tendency to act as a reducing agent, with increase in atomic number.
  4. The second and third rows of d-block transition elements are quite close in properties.
  5. Consequently, these elements occur together in natural minerals and are difficult to separate.

d-Block contraction

Main article: d-block contraction

The d-block contraction is less pronounced than the lanthanide contraction but arises from a similar cause. In this case, it is the poor shielding capacity of the 3d-electrons which affects the atomic radii and chemistries of the elements immediately following the first row of the transition metals, from gallium (Z = 31) to bromine (Z = 35).[9]

Calculated atomic radii

The following table shows atomic radii computed from theoretical models, as published by Enrico Clementi and others in 1967.[10] The values are in picometres (pm).

Group (vertical) 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18
Period (horizontal)
1 H
53		 He
31
2 Li
167		 Be
112		 B
87		 C
67		 N
56		 O
48		 F
42		 Ne
38
3 Na
190		 Mg
145		 Al
118		 Si
111		 P
98		 S
88		 Cl
79		 Ar
71
4 K
243		 Ca
194		 Sc
184		 Ti
176		 V
171		 Cr
166		 Mn
161		 Fe
156		 Co
152		 Ni
149		 Cu
145		 Zn
142		 Ga
136		 Ge
125		 As
114		 Se
103		 Br
94		 Kr
88
5 Rb
265		 Sr
219		 Y
212		 Zr
206		 Nb
198		 Mo
190		 Tc
183		 Ru
178		 Rh
173		 Pd
169		 Ag
165		 Cd
161		 In
156		 Sn
145		 Sb
133		 Te
123		 I
115		 Xe
108
6 Cs
298		 Ba
253		 *
 		 Hf
208		 Ta
200		 W
193		 Re
188		 Os
185		 Ir
180		 Pt
177		 Au
174		 Hg
171		 Tl
156		 Pb
154		 Bi
143		 Po
135		 At
 		 Rn
120
7 Fr
 		 Ra
 		 **
 		 Rf
 		 Db
 		 Sg
 		 Bh
 		 Hs
 		 Mt
 		 Ds
 		 Rg
 		 Cn
 		 Uut
 		 Uuq
 		 Uup
 		 Uuh
 		 Uus
 		 Uuo
 
Lanthanides *
 		 La
 		 Ce
 		 Pr
247		 Nd
206		 Pm
205		 Sm
238		 Eu
231		 Gd
233		 Tb
225		 Dy
228		 Ho
 		 Er
226		 Tm
222		 Yb
222		 Lu
217
Actinides **
 		 Ac
 		 Th
 		 Pa
 		 U
 		 Np
 		 Pu
 		 Am
 		 Cm
 		 Bk
 		 Cf
 		 Es
 		 Fm
 		 Md
 		 No
 		 Lr
 

See also

References

  1. ^ Cotton, F. A.; Wilkinson, G. (1988). Advanced Inorganic Chemistry (5th ed.). Wiley. p. 1385. ISBN 978-0-471-84997-1. 
  2. ^ Basdevant, J.-L.; Rich, J.; Spiro, M. (2005). Fundamentals in Nuclear Physics. Springer. p. 13, fig 1.1. ISBN 978-0-387-01672-6. http://books.google.com/?id=OFx7P9mgC9oC&pg=PA375&dq=helium+%22nuclear+structure%22#PPA13,M1. 
  3. ^ Bragg, W. L. (1920). "The arrangement of atoms in crystals". Philosophical Magazine. 6 40 (236): 169–189. 
  4. ^ Wyckoff, R. W. G. (1923). "On the Hypothesis of Constant Atomic Radii". Proceedings of the National Academy of Sciences of the United States of America 9 (2): 33–38. Bibcode 1923PNAS....9...33W. doi:10.1073/pnas.9.2.33. PMC 1085234. PMID 16576657. http://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1085234. 
  5. ^ a b c Pauling, L. (1945). The Nature of the Chemical Bond (2nd ed.). Cornell University Press. LCCN 42034474. 
  6. ^ Bohr, N. (1913). "On the Constitution of Atoms and Molecules, Part I. – Binding of Electrons by Positive Nuclei". Philosophical Magazine. 6 26 (151): 1–24. http://web.ihep.su/dbserv/compas/src/bohr13/eng.pdf. Retrieved 8 June 2011. 
  7. ^ Bohr, N. (1913). "On the Constitution of Atoms and Molecules, Part II. – Systems containing only a Single Nucleus". Philosophical Magazine. 6 26 (153): 476–502. http://web.ihep.su/dbserv/compas/src/bohr13b/eng.pdf. Retrieved 8 June 2011. 
  8. ^ Slater, J. C. (1964). "Atomic Radii in Crystals". Journal of Chemical Physics 41 (10): 3199–3205. Bibcode 1964JChPh..41.3199S. doi:10.1063/1.1725697. 
  9. ^ a b Jolly, W. L. (1991). Modern Inorganic Chemistry (2nd ed.). McGraw-Hill. p. 22. ISBN 978-0-0711-2651-9. 
  10. ^ Clementi, E.; Raimond, D. L.; Reinhardt, W. P. (1967). "Atomic Screening Constants from SCF Functions. II. Atoms with 37 to 86 Electrons". Journal of Chemical Physics 47 (4): 1300–1307. Bibcode 1967JChPh..47.1300C. doi:10.1063/1.1712084.