Periodic Trends in Physical Properties

Slide a finger across period 3 of the periodic table — sodium, magnesium, aluminium, silicon — and the atoms quietly shrink, hold their electrons tighter, and get harder to ionise, step by step. Slide down a group instead and the opposite happens: atoms swell, electrons loosen, and ionisation gets easier. Nothing mysterious is going on. Every one of these physical properties — atomic radius, ionic radius, ionisation enthalpy, electron gain enthalpy, electronegativity — is the same tug-of-war between the nucleus's pull and the electron cloud's shielding, replayed with different numbers. Learn the tug-of-war once and the whole periodic table becomes predictable instead of memorised.

The core insight

Every periodic trend in atomic size, ionisation enthalpy, electron gain enthalpy and electronegativity is governed by how effective nuclear charge and electron shielding change across a period and down a group.

The core idea

Effective nuclear charge does the driving. A valence electron never feels the full pull of all ZZ protons — inner-shell electrons sit between it and the nucleus and cancel part of that pull. The net charge actually felt is

Zeff=Z−σ,Z_{eff} = Z - \sigma,

where: ZZ is the atomic number (total protons), σ\sigma is the shielding constant contributed by inner, filled shells, and ZeffZ_{eff} is the effective nuclear charge felt by an outer electron. Across a period, ZZ climbs by one unit at a time while electrons keep filling the same outer shell, so shielding barely changes and ZeffZ_{eff} rises steadily. Down a group, a brand-new outer shell opens up each time, so the extra inner shells shield far more effectively — ZeffZ_{eff} stays roughly similar even as ZZ climbs, but the outer electron now sits in a shell of larger radius nn.

Atomic and ionic radius follow directly. Across a period, rising ZeffZ_{eff} pulls the same-shell electron cloud inward, so atomic radius shrinks left to right. Down a group, the new outer shell dominates over the modest rise in ZeffZ_{eff}, so radius grows. Ions obey the same logic adjusted for charge: a cation is smaller than its parent atom (one fewer electron, same nuclear pull), an anion is larger (one more electron, more electron-electron repulsion), and within an isoelectronic series — same electron count, different ZZ — radius shrinks as ZZ rises, because every electron now feels a bigger ZeffZ_{eff}.

Ionisation enthalpy, electron gain enthalpy and electronegativity all track ZeffZ_{eff} in the same direction. Ionisation enthalpy (energy to remove the outermost electron, in kJ mol−1\text{kJ mol}^{-1}) generally rises across a period and falls down a group, because a tightly held, close-in electron is harder to pull away. Electron gain enthalpy (energy change on adding an electron to a neutral atom) generally becomes more negative across a period and less negative down a group, for the same reason — a higher ZeffZ_{eff} welcomes the extra electron more strongly. Electronegativity, the pull an atom in a molecule exerts on a shared bonding pair, rises across a period and falls down a group. All four properties are really one story told four ways.

Figure
Effective nuclear charge rising across a period and roughly constant down a group, shown as arrows of increasing thickness across a row and equal thickness down a column of the periodic table
Zeff rises across a period, stays similar down a group Na Mg Al Si Zeff increases left to right — radius shrinks, ionisation enthalpy rises Li Na Down a group Zeff stays roughly the same, but a new outer shell means radius grows
Derivation ARanking isoelectronic ions by effective nuclear charge

The goal is to show, using only the definition Zeff=Z−σZ_{eff} = Z - \sigma and the fact that an isoelectronic series shares one fixed electron count, why increasing atomic number inside that fixed set of electrons must shrink the ionic radius, and to use that reasoning to order four real ions with 10 electrons each without needing any measured radius values as a starting point.

Step 1. Fix the electron count. Take the isoelectronic series O2−\text{O}^{2-}, F−\text{F}^-, Na+\text{Na}^+, Mg2+\text{Mg}^{2+}: every one of these species has exactly 10 electrons in the configuration 1s22s22p61s^2 2s^2 2p^6, identical to neon. Because the electron arrangement — and hence the shielding pattern σ\sigma contributed by those electrons on one another — is the same in all four species, σ\sigma is essentially constant across the series.

Step 2. Vary only ZZ. The four species differ only in nuclear charge: Z(O)=8Z(\text{O}) = 8, Z(F)=9Z(\text{F}) = 9, Z(Na)=11Z(\text{Na}) = 11, Z(Mg)=12Z(\text{Mg}) = 12. Since Zeff=Z−σZ_{eff} = Z - \sigma and σ\sigma is fixed, ZeffZ_{eff} must increase in exactly the same order as ZZ: oxide feels the smallest pull, magnesium ion the largest.

Step 3. Connect ZeffZ_{eff} to radius. A larger ZeffZ_{eff} pulls the same fixed cloud of 10 electrons inward more strongly, contracting the electron cloud and shrinking the ionic radius. So radius must fall as ZZ rises across the series — the ion with the smallest ZZ is the largest, and the ion with the largest ZZ is the smallest.

Step 4. Read off the order. Ranking by increasing ZZ gives decreasing radius: O2− (Z=8)>F− (Z=9)>Na+ (Z=11)>Mg2+ (Z=12)\text{O}^{2-}\,(Z=8) > \text{F}^-\,(Z=9) > \text{Na}^+\,(Z=11) > \text{Mg}^{2+}\,(Z=12). This single argument — fixed electron count, rising ZeffZ_{eff} with rising ZZ, shrinking radius — is the general rule for ranking any isoelectronic series, and it needs no memorised radius table at all.

Worked example

Question: Arrange Na, Mg, Al, Si (period 3) in order of increasing first ionisation enthalpy, explaining any exception to the general period trend, and state what this predicts about their atomic radii.

Step 1. Write the outer configurations: Na is 3s13s^1, Mg is 3s23s^2, Al is 3s23p13s^2 3p^1, Si is 3s23p23s^2 3p^2.

Step 2. Apply the plain period trend first. ZeffZ_{eff} rises steadily from Na to Si, so the naive prediction — ignore subshell stability for a moment — is a smooth increase: Na less than Mg less than Al less than Si.

Step 3. Check for the stability exception. Mg has a completely filled 3s23s^2 subshell, which is extra stable and resists losing an electron more than the naive ZeffZ_{eff} trend suggests. Al's outermost electron instead comes from the higher-energy, less-penetrating 3p13p^1 orbital, which is comparatively easy to remove even though Al has a higher ZeffZ_{eff} than Mg. Net effect: Al's first ionisation enthalpy drops below Mg's.

Step 4. State the corrected order and the radius consequence. The corrected ionisation-enthalpy order is Na < Al < Mg < Si. Since ionisation enthalpy broadly tracks the same rising ZeffZ_{eff} that shrinks atomic radius, the radius order across the same four atoms runs the opposite way, largest to smallest: Na > Mg > Al > Si (radius has no subshell-stability exception the way ionisation enthalpy does, since it depends only on where the outermost shell sits, not on which subshell the last electron left).

Answer: ionisation enthalpy order Na < Al < Mg < Si, with radius shrinking steadily Na > Mg > Al > Si.

Common traps

  • Assuming atomic radius drops on every single step across a period with no exception — the big drop from a noble gas to the next period's alkali metal is a jump between periods, not part of the same monotonic run.
  • Mixing up ionisation enthalpy (removing an electron, always needs energy, always positive) with electron gain enthalpy (adding an electron, often releases energy, often negative) — they are opposite-direction processes with opposite typical signs.
  • Forgetting the half-filled and fully-filled subshell exceptions (Group 2 above Group 13, Group 15 above Group 16 in ionisation enthalpy) and predicting a perfectly smooth period-wide increase.
  • Treating electronegativity as a fixed, isolated-atom number like ionisation enthalpy — it is a relative, scale-dependent measure of pull on a shared bonding pair within a molecule, not a standalone atomic property.

Ask the tutor: want to practice ranking a fresh set of atoms or ions by radius, ionisation enthalpy, or electronegativity, or walk through another isoelectronic-series example step by step?

Why does effective nuclear charge rise across a period but not much down a group?

Across a period every new electron is added to the same outer shell while the nuclear charge climbs by one each time, so there is nothing new to shield the extra proton and ZeffZ_{eff} rises steadily. Down a group, each new element adds a whole new inner shell before the next valence electron, and that entire extra shell sits between the nucleus and the new outer electron, shielding it almost as effectively as the rising ZZ pulls it in. The two effects roughly cancel down a group, so ZeffZ_{eff} stays similar even though ZZ itself keeps growing.

Is it true that ionisation enthalpy always increases across a period with no exceptions?

No, and this trips up a lot of students. The general direction is an increase, driven by rising ZeffZ_{eff}, but two stable-subshell exceptions break the smooth climb: a filled subshell like 3s23s^2 in magnesium or 3p63p^6 resists losing an electron more than expected, and a half-filled subshell like 3p33p^3 in phosphorus does the same. That is why Mg sits above Al, and Group 15 sits above Group 16, even though both pairs go against the raw ZeffZ_{eff} prediction. Always check for filled or half-filled subshells before assuming a smooth trend.

How is electron gain enthalpy different from electronegativity if both describe attracting electrons?

Electron gain enthalpy is a measured energy change, in kJ mol−1\text{kJ mol}^{-1}, for a specific process — adding one electron to an isolated gaseous atom to form an anion. Electronegativity is not a measured energy at all; it is a relative number on a scale (like the Pauling scale) describing how strongly an atom pulls a bonding electron pair toward itself while already bonded in a molecule. Both increase across a period and decrease down a group for the same ZeffZ_{eff} reason, but one is a standalone-atom energy and the other only makes sense for an atom sitting inside a bond.

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