Effective Nuclear Charge Calculator – Slater's Rules, Shielding and Trends
An electron in a many-electron atom never feels the full charge of the nucleus. The other electrons get in the way and cancel part of it. The charge that is left is the effective nuclear charge, Z_eff = Z − σ, where σ is the shielding constant. This effective nuclear charge calculator applies Slater's rules to any element or ion, shows which electrons do the shielding, and plots how Zeff changes across the periodic table.
Shielding and penetration
Electrons in inner shells sit between the nucleus and an outer electron almost all the time, so they cancel nearly one unit of charge each. Electrons in the same shell spread over the same region and cancel much less, because an outer electron is often closer to the nucleus than they are. How far an orbital reaches inside the core is called penetration. An s orbital penetrates more than a p orbital of the same shell, and a p more than a d. A more penetrating electron feels a larger effective charge and is held more tightly.
Slater's rules step by step
Write the configuration in Slater groups, in this order: (1s) (2s,2p) (3s,3p) (3d) (4s,4p) (4d) (4f) (5s,5p) (5d) (5f) (6s,6p) …. Then add up what every other electron contributes:
Electron in Same group n − 1 n − 2 or lower To its right
(ns, np) 0.35 (1s: 0.30) 0.85 each, any l 1.00 each 0
(nd), (nf) 0.35 1.00 each: every group to the left 0Nitrogen 2p. N is (1s)² (2s,2p)⁵. The other four n = 2 electrons give 4 × 0.35 = 1.40 and the two 1s electrons give 2 × 0.85 = 1.70. So σ = 3.10 and Zeff = 7 − 3.10 = 3.90.
Zinc 3d and 4s. Zn is [Ar] 3d¹⁰ 4s². For a 4s electron: the other 4s electron gives 0.35, the eighteen n = 3 electrons (3s, 3p and 3d) give 18 × 0.85 = 15.30, and the ten inner electrons give 10.00. σ = 25.65, so Zeff = 4.35. For a 3d electron, the 4s pair is to the right and does not count. The other nine 3d electrons give 9 × 0.35 = 3.15 and the eighteen electrons to the left give 18.00. σ = 21.15, so Zeff = 8.85. The 3d electrons feel twice the charge of the 4s ones.
Periodic trends in effective nuclear charge
Across a period, each step adds one proton and one same-shell electron that shields only 0.35. Zeff on the valence electrons rises by 0.65 per element (Li 1.30 to Ne 5.85). That rising charge pulls the shell inward, which is why atomic radius falls and ionization energy rises across a period. Down a group, a new shell starts and Zeff collapses (Ne 5.85 to Na 2.20). The outer electron is also much farther out, so the atom gets bigger.
Across the lanthanides the 6s value stays flat at 2.85 or 3.00. Slater counts each new 4f electron as a full 1.00 shield of the 6s electron, cancelling the new proton exactly. Real 4f electrons shield poorly, so the outer electrons do feel a slowly rising charge. That is the cause of the lanthanide contraction, which Slater's rules cannot show.
Potassium: 4s or 3d?
Potassium's 19th electron could go into 4s or 3d. With an argon core, a 4s electron feels Zeff = 2.20: the eight n = 3 electrons shield 0.85 each. A 3d electron feels only 1.00, because all eighteen core electrons shield it fully. The 4s electron is bound more tightly, so the ground state is [Ar] 4s¹. Try both in the Custom configuration tab, together with excited states of your own.
Limitations and SCF comparison
Slater's rules were made for quick hand calculation. They treat ns and np alike, give every alkali metal from sodium down the same 2.20, and use fixed numbers for every element. Self-consistent-field (SCF) values from Clementi and Raimondi (1963) are shown beside them where available. They agree well for chlorine 3p (Slater 6.10, SCF 6.116) but not for sodium 3s (2.20 against 2.507) or potassium 4s (2.20 against 3.495). The SCF values also split boron's 2s (2.576) from its 2p (2.421), which Slater cannot do.