2.2
0.8
0.2
-7.31
eV
216.4
pm
2.2
0.8
0.2
-7.31
eV
216.4
pm
The Effective Nuclear Charge Calculator computes Z_eff, the net positive charge experienced by a specific electron in a multi-electron atom after accounting for electron shielding. In any atom beyond hydrogen, inner electrons partially shield outer electrons from the full nuclear charge, reducing the effective attraction between the nucleus and the valence electrons. This concept, quantified by Slater's rules or more sophisticated methods, is fundamental to understanding periodic trends including atomic radius, ionization energy, electron affinity, and electronegativity. The effective nuclear charge Z_eff equals the actual nuclear charge Z minus the shielding constant S: Z_eff = Z - S. This calculator also estimates the orbital energy using the hydrogen-like model and the approximate orbital radius, providing a comprehensive picture of how shielding affects electron behavior in multi-electron atoms.
The central equation is:
Z_eff = Z - S
Where Z is the atomic number (nuclear charge) and S is the shielding constant representing the screening effect of other electrons. The shielding constant S is calculated using Slater's rules:
The orbital energy is estimated from the hydrogen-like formula: E = -13.6 x Z_eff² / n² eV. The orbital radius is estimated as r = a0 x n² / Z_eff, where a0 = 52.9 pm (Bohr radius). The penetration ratio Z_eff/Z indicates what fraction of the nuclear charge the electron effectively experiences.
A higher Z_eff means the electron is more tightly bound to the nucleus, resulting in lower (more negative) orbital energy and smaller orbital radius. The penetration ratio shows the shielding effectiveness: values close to 1 indicate poor shielding (the electron feels nearly the full nuclear charge), while small values indicate strong shielding. Across a period, Z_eff increases because electrons are added to the same shell (poor shielding of each other), explaining why atoms get smaller and ionization energies increase from left to right. Down a group, despite increasing Z, the distance effect dominates, and the outermost electron is less tightly held.
Inputs
Results
Sodium's 3s valence electron has Z_eff = 2.2 (Slater's: 2 electrons in 1s contribute 2x1.00=2.0, 8 in 2s2p contribute 8x0.85=6.8, S=8.8). The effective charge is only 20% of the nuclear charge, showing strong shielding by 10 inner electrons. The estimated orbital radius of 216 pm is close to sodium's actual atomic radius of 186 pm.
Inputs
Results
Oxygen's 2p electron has Z_eff = 3.45 (Slater's: 2 in 1s contribute 2x0.85=1.70, 5 in same group contribute 5x0.35=1.75, inner contribute 2x0.85, S=4.55). The higher Z_eff compared to sodium explains why oxygen is smaller and harder to ionize than expected for its group position.
Slater's rules provide a simple empirical method to estimate the shielding constant S. Electrons are grouped by shell and type, and each group's contribution to shielding depends on its position relative to the electron of interest. Same-shell electrons contribute 0.35, (n-1) shell electrons contribute 0.85, and deeper shells contribute 1.00. While approximate, Slater's rules give useful Z_eff values for understanding periodic trends.
Across a period (left to right), Z increases by 1 per element but shielding increases by only about 0.35 (same-shell electrons shield poorly). So Z_eff increases, making atoms smaller with higher ionization energies. Down a group, although Z increases significantly, n also increases, and the larger orbital radius dominates, making atoms larger with lower ionization energies.
No. Slater's rules are an empirical approximation developed in 1930. More accurate values come from Hartree-Fock self-consistent field calculations or Clementi-Raimondi values (published in 1963), which use variational methods. For example, Slater gives Z_eff = 2.20 for Na 3s, while Clementi-Raimondi gives 2.51. Slater's rules are useful for qualitative understanding and quick estimates.
s electrons have nonzero probability density at the nucleus (they penetrate closer to the nucleus), giving them greater shielding effectiveness. p electrons have a node at the nucleus and penetrate less. The shielding order is s > p > d > f, which is why s electrons in an inner shell contribute more shielding than d or f electrons at similar distances.
Penetration describes how much of an electron's probability density is found close to the nucleus. Electrons with high penetration experience more nuclear charge and are more tightly bound. For the same shell, s orbitals penetrate most, followed by p, d, and f. This explains the subshell energy ordering (s < p < d < f within the same shell) in multi-electron atoms.
Higher Z_eff leads to stronger attraction for electrons, increasing electronegativity and making the atom better at attracting shared electrons in covalent bonds. It also increases ionization energy (harder to remove electrons) and decreases atomic radius. These effects determine bond polarity, molecular geometry, and overall chemical reactivity patterns.
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