Mercury
Mercury is a chemical element with symbol Hg and atomic number 80. It is commonly known as quicksilver and was formerly named hydrargyrum (/haɪˈdrɑːrdʒərəm/). A heavy, silvery d-block element, mercury is the only metallic element that is liquid at standard conditions for temperature and pressure; the only other element that is liquid under these conditions is bromine, though metals such as caesium, gallium, and rubidium melt just above room temperature.
At a glance
- Atomic number
- 80
- Atomic mass
- 200.5923 u
- Phase
- Liquid
- Density
- 13.534 g/cm³
- Melting point
- 234.321 K
- Boiling point
- 629.88 K
- First ionization energy
- 1,007.1 kJ/mol
- Electronegativity
- 2
- Electron affinity
- -48 kJ/mol
- Molar heat capacity
- 27.983 J/(mol·K)
- Period
- 6
- Appearance
- silvery
Conditions and isotopes affect measured properties. Some properties of short-lived elements are predicted. Electronegativity uses the Pauling scale.
Mercury’s orbitals use a hydrogen-like approximation. Every orbital of each visible subshell is shown: in Shapes as the surface holding half its probability, with light and dark shades for opposite signs of the wavefunction; in Cloud as dots where its electrons are likely to be. Sizes are stepped by shell, like the Shell model.
54 is the [Xe] core total across five shells.
Preparing the orbital view…
80 protons122 neutrons
Mercury-202: its most common form in nature, or its longest-lived if it has none. The nucleus is drawn far too big: it’s about 100,000 times smaller than the atom.
Turn up the heat
A step of 1 K is the same size as 1 °C, so the two scales are always 273.15 apart. Fahrenheit is different: its degrees are smaller and it starts elsewhere, so water freezes at 273.15 K, 0 °C and 32 °F.25 °C · 77 °FLiquid
At this temperature, mercury is a liquid.
At normal atmospheric pressure (1 atm). The temperature scale is logarithmic. The particle box is schematic: real samples hold vastly more atoms, and spacing and speeds are not to scale.
Pull the electrons off
HgNeutral atom · no charge
A neutral mercury atom. Removing its first electron takes 1,007 kJ/mol.
Mercury’s outer shell holds 2 electrons. Electron 3 is the first from an inner shell: it sits closer to the nucleus with less shielding, so removing it takes 1.8× as much energy as the one before. Each dashed line on the chart marks another jump, into a shell even closer to the nucleus.
What does this tell us?
- Within a shell the steps rise gently. Each electron removed leaves fewer electrons pushing the others away, while the nucleus pulls just as hard, so the next one is held a little more tightly.
Show the values as a table
| Electron | Shell | Energy (kJ/mol) | × previous | Value |
|---|---|---|---|---|
| 1 | 6 | 1,007 | – | Measured |
| 2 | 6 | 1,810 | 1.8 | Measured |
| 3 | 5 | 3,328 | 1.8 | Measured |
| 4 | 5 | 4,684 | 1.4 | Measured |
| 5 | 5 | 5,905 | 1.3 | Measured |
| 6 | 5 | 7,391 | 1.3 | Measured |
| 7 | 5 | 8,973 | 1.2 | Measured |
| 8 | 5 | 10,990 | 1.2 | Calculated |
| 9 | 5 | 12,929 | 1.2 | Calculated |
| 10 | 5 | 14,762 | 1.1 | Calculated |
| 11 | 5 | 16,692 | 1.1 | Calculated |
| 12 | 5 | 18,593 | 1.1 | Estimated |
| 13 | 5 | 26,717 | 1.4 | Estimated |
| 14 | 5 | 29,621 | 1.1 | Calculated |
| 15 | 5 | 32,033 | 1.1 | Calculated |
| 16 | 5 | 34,445 | 1.1 | Calculated |
| 17 | 5 | 38,787 | 1.1 | Calculated |
| 18 | 5 | 41,392 | 1.1 | Calculated |
| 19 | 5 | 46,024 | 1.1 | Calculated |
| 20 | 5 | 51,137 | 1.1 | Calculated |
| 21 | 4 | 54,032 | 1.1 | Calculated |
| 22 | 4 | 56,926 | 1.1 | Calculated |
| 23 | 4 | 62,715 | 1.1 | Calculated |
| 24 | 4 | 68,505 | 1.1 | Calculated |
| 25 | 4 | 73,329 | 1.1 | Calculated |
| 26 | 4 | 79,118 | 1.1 | Calculated |
| 27 | 4 | 84,907 | 1.1 | Calculated |
| 28 | 4 | 89,731 | 1.1 | Calculated |
| 29 | 4 | 95,520 | 1.1 | Calculated |
| 30 | 4 | 101,310 | 1.1 | Calculated |
| 31 | 4 | 107,099 | 1.1 | Calculated |
| 32 | 4 | 111,923 | 1 | Calculated |
| 33 | 4 | 117,712 | 1.1 | Calculated |
| 34 | 4 | 123,501 | 1 | Calculated |
| 35 | 4 | 149,456 | 1.2 | Calculated |
| 36 | 4 | 154,666 | 1 | Calculated |
| 37 | 4 | 160,262 | 1 | Calculated |
| 38 | 4 | 166,244 | 1 | Calculated |
| 39 | 4 | 171,744 | 1 | Calculated |
| 40 | 4 | 177,437 | 1 | Calculated |
| 41 | 4 | 186,024 | 1 | Calculated |
| 42 | 4 | 191,909 | 1 | Calculated |
| 43 | 4 | 197,988 | 1 | Calculated |
| 44 | 4 | 203,874 | 1 | Calculated |
| 45 | 4 | 227,126 | 1.1 | Calculated |
| 46 | 4 | 232,723 | 1 | Calculated |
| 47 | 4 | 239,091 | 1 | Calculated |
| 48 | 4 | 244,976 | 1 | Calculated |
| 49 | 4 | 264,852 | 1.1 | Calculated |
| 50 | 4 | 271,606 | 1 | Calculated |
| 51 | 4 | 287,623 | 1.1 | Calculated |
| 52 | 4 | 294,271 | 1 | Estimated |
| 53 | 3 | 487,733 | 1.7 | Calculated |
| 54 | 3 | 500,855 | 1 | Calculated |
| 55 | 3 | 514,749 | 1 | Calculated |
| 56 | 3 | 529,704 | 1 | Calculated |
| 57 | 3 | 543,791 | 1 | Calculated |
| 58 | 3 | 557,685 | 1 | Calculated |
| 59 | 3 | 582,868 | 1 | Calculated |
| 60 | 3 | 597,437 | 1 | Calculated |
| 61 | 3 | 613,261 | 1 | Calculated |
| 62 | 3 | 627,927 | 1 | Calculated |
| 63 | 3 | 668,933 | 1.1 | Calculated |
| 64 | 3 | 681,765 | 1 | Calculated |
| 65 | 3 | 695,756 | 1 | Calculated |
| 66 | 3 | 709,167 | 1 | Calculated |
| 67 | 3 | 772,848 | 1.1 | Calculated |
| 68 | 3 | 787,320 | 1 | Calculated |
| 69 | 3 | 817,231 | 1 | Calculated |
| 70 | 3 | 831,704 | 1 | Calculated |
| 71 | 2 | 1,789,803 | 2.2 | Calculated |
| 72 | 2 | 1,824,538 | 1 | Calculated |
| 73 | 2 | 1,863,132 | 1 | Calculated |
| 74 | 2 | 1,898,831 | 1 | Calculated |
| 75 | 2 | 2,134,256 | 1.1 | Calculated |
| 76 | 2 | 2,178,639 | 1 | Calculated |
| 77 | 2 | 2,235,565 | 1 | Calculated |
| 78 | 2 | 2,271,660 | 1 | Calculated |
| 79 | 1 | 9,081,653 | 4 | Calculated |
| 80 | 1 | 9,252,769 | 1 | Calculated |
Successive ionization energies of gas-phase atoms and ions from the NIST Atomic Spectra Database. Solid bars are measured; hatched bars were estimated from nearby measurements or calculated from quantum theory, as is usual for highly charged ions. Electrons are taken from the outermost shell first, a simplification: electrons in different subshells of the same shell also differ in energy. On the log scale each gridline is 10 times the one below.
A fingerprint made of light
Mercury’s violet, blue and green lines, and its strong ultraviolet ones, light fluorescent lamps: a coating inside the tube turns the ultraviolet into visible light.
Heated or electrified, mercury gives off light only at the exact wavelengths below. Each one comes from an electron falling between two energy levels, so the pattern is unique to the element, like a fingerprint.
Click a line to see where it comes from.
404.7 nmviolet
An electron falls from the 7s level down to the 6p level. It loses 3.06 eV of energyAn electronvolt (eV) is a tiny unit of energy used for atoms: the energy one electron gains crossing 1 volt. A particle of visible light carries between about 1.7 eV (red) and 3.3 eV (violet). and gives it off as one particle of violet light. Bigger drops give bluer light.
The strongest visible lines of neutral mercury from the NIST Atomic Spectra Database. Line brightness follows NIST’s relative intensities, which only compare lines of the same element. Colours are approximate, and lamp colours are as they look to the eye.
Why is mercury liquid? Blame Einstein
Mercury is the only metal that’s liquid at room temperature. The reason is surprising: Einstein’s theory of relativity. Its 80 protons pull its electrons so hard that the innermost ones race at over half the speed of light, and that changes how the whole atom behaves.
The real mercury atom
- Innermost electrons
- Race at about 58% of the speed of light (orange)
- At that speed
- They act about 23% heavier, so they huddle about 19% closer
- Outer electrons
- Pulled in too, held tightly, and hard to share (blue)
- Melts at
- −39 °C (measured)
Metal atoms stick together by sharing their outer electrons. Mercury keeps its two held so tightly that its atoms barely stick, so a little warmth lets them slide apart: it melts at −39 °C.
E = mc², at speed
Einstein’s E = mc² says that even a resting electron carries energy: 511 keV. The full version, E = γmc², adds a factor γ that grows with speed. The more protons an atom has, the faster its innermost electrons race, and the more γ matters. Slide through the elements to see it.
E = mc² at rest = 511 keV
γ = 1 ÷ √(1 − v²/c²) = 1 ÷ √(1 − 0.584²) = 1.232
E = γmc² = 1.232 × 511 keV = 629 keV
γ barely moves at everyday speeds, even at the speed of a rocket. It only takes off as you get close to the speed of light, which is why only heavy atoms, with lots of protons pulling hard, feel it.
Try it at different temperatures
20 °C, relativity onLiquid
The odd one out in its family
Zinc, cadmium and mercury sit in the same column of the table. Going down a column, atoms get bigger and usually let go of their outer electrons more easily. Mercury breaks the pattern: it grips them hardest of all, and melts hundreds of degrees lower.
- ZincMelts at 420 °CGrip on its outer electrons: 906.4 kJ/mol
- CadmiumMelts at 321 °CGrip on its outer electrons: 867.8 kJ/mol
- MercuryMelts at −39 °CGrip on its outer electrons: 1,007.1 kJ/mol
The electron speed (about Z/137 of light speed for the innermost electrons), γ and size change are rough estimates from a simple model of the atom; the electron’s rest energy, 511 keV, is the measured (CODATA) value. The effect on the melting point comes from computer simulations by Calvo, Pahl, Wormit and Schwerdtfeger (Angewandte Chemie, 2013). “Grip” is the first ionization energy, the energy needed to pull off one outer electron (NIST).
How does it compare?
Density
13.5 g/cm³14th highest of 99
Melting point
234 K11th lowest of 96
Boiling point
630 K16th lowest of 97
Electronegativity
231st highest of 96
First ionization energy
1,007 kJ/mol16th highest of 99
Elements 1–99 from the reference data; heavier elements are left out because only a few atoms have ever been made, so their bulk properties are predictions. First ionization energies come from NIST. Density uses a logarithmic scale, because gases are around a thousand times less dense than solids; gas densities are at 0 °C and 1 atm. Melting and boiling points are at normal pressure. Everyday temperatures and light sources in the pictures are approximate. Hover over a dot to see the element, or click it to compare.
Keep exploring
Explore the stories, imagery, and reference data in more depth. Properties with no value in the reference are marked unavailable.
- MercuryRoyal Society of Chemistry
- MercuryWikipedia
- Quantum numbers and electron configurationsPurdue
- Hydrogenic wavefunctionsNIST
- Ionization energiesNIST Atomic Spectra Database
- Spectral linesNIST Atomic Spectra Database