sciencebriefs
13:00in productionCh. 1 · The race toward absolute zero/ 13:00 · ceiling 15 min
Physics

Superconductivity

Three years after liquefying helium itself, Heike Kamerlingh Onnes watched mercury's electrical resistance vanish outright rather than merely fall, opening a phenomenon still not fully explained for its high-temperature cousins.

Heike Kamerlingh Onnes built his career at Leiden University around reaching ever lower temperatures, a pursuit that culminated in 1908 when he became the first to liquefy helium, reaching roughly 1.5 kelvin, the coldest temperature achieved anywhere at the time. That capability let him test how metals behaved near absolute zero, and on 8 April 1911 he found that solid mercury's electrical resistance did not simply keep falling as it cooled but disappeared abruptly below about 4.2 kelvin, a genuinely new state of matter rather than an extension of ordinary conduction. He received the 1913 Nobel Prize in Physics for his low-temperature work generally, including the helium liquefaction that made the discovery possible. The effect, later named superconductivity, was not given a full microscopic explanation until BCS theory in 1957, and it now underpins technologies from MRI magnets to maglev trains.

Chapters & takeaways6
  1. 0:08
    The race toward absolute zero

    Onnes built his laboratory's reputation on pushing temperatures as low as the equipment of the day allowed.

  2. 2:10
    Liquefying helium in 1908

    Onnes became the first to liquefy helium, reaching about 1.5 kelvin and unlocking a new range of achievable cold.

  3. 4:20
    Resistance that vanishes, not fades

    On 8 April 1911, mercury's resistance dropped to nothing below roughly 4.2 kelvin, rather than continuing a gradual decline.

  4. 6:30
    A Nobel for the cold, not just the effect

    Onnes's 1913 Nobel Prize recognised his broader low-temperature research programme, of which the mercury result was one outcome.

  5. 8:40
    Decades before an explanation

    A microscopic theory explaining why superconductivity happens, BCS theory, did not arrive until 1957, well after Onnes's death.

  6. 10:50
    From a lab curiosity to MRI magnets

    Zero-resistance conduction and the associated expulsion of magnetic fields now power medical imaging, accelerators, and maglev transport.

Worth your time?

Yes. Study the whole thing.

4/ 5
What works
  • it shows discovery and instrument-building as inseparable, since the helium liquefaction and the superconductivity finding are really one continuous project
  • the multi-decade gap before BCS theory explained the effect is stated plainly rather than skipped over
  • practical modern applications are named specifically enough to feel concrete rather than a generic list
What does not
  • it does not resolve the minor discrepancy in exactly what temperature mercury's transition occurs at, only that it is close to 4 kelvin
  • the Meissner effect, discovered decades after Onnes's original finding, is introduced without much explanation of how it differs from zero resistance itself
Study it if
  • anyone who wants the origin story behind MRI and maglev technology
  • readers interested in how instrument-building itself can be the scientific breakthrough
  • people curious how long a gap can sit between discovering an effect and explaining it
Skip it if
  • readers wanting the BCS theory mechanism explained in technical depth
  • anyone mainly interested in modern high-temperature superconductors rather than the original discovery
The written brief3 min read

The race toward absolute zero

Heike Kamerlingh Onnes spent much of his career at Leiden University pursuing a single technical goal: reaching temperatures colder than anyone had achieved before, and building the equipment needed to study matter once it got there. That pursuit reached a major milestone on 10 July 1908, when he became the first person to liquefy helium, using a sequence of pre-cooling stages, and by further reducing the pressure on the liquid he reached roughly 1.5 kelvin, the lowest temperature recorded anywhere at the time. The achievement mattered beyond the record itself, because liquid helium gave Onnes a coolant capable of holding other materials at temperatures no prior apparatus could sustain, which is what let him ask a new kind of question about how ordinary metals behave that close to absolute zero.

Liquefying helium in 1908

Using his helium-cooling apparatus, Onnes measured the electrical resistance of solid mercury as he cooled it further and further. On 8 April 1911 he observed something that did not fit the expected pattern of resistance gradually declining as temperature fell: below a temperature close to 4.2 kelvin, the mercury’s resistance did not taper off but vanished essentially completely, dropping so sharply that it looked less like an extension of ordinary cooling behaviour and more like a distinct transition into a new state. This abrupt disappearance, rather than a gradual fade, is what marked the discovery as something genuinely new rather than simply very cold, very good conduction.

Resistance that vanishes, not fades

The core observation has held up entirely: what Onnes found in mercury in 1911 is recognised as the first documented instance of superconductivity, and the phenomenon has since been confirmed in a wide range of other materials, each with its own characteristic critical temperature below which the same abrupt loss of resistance occurs. His broader low-temperature research programme, including the helium liquefaction that made the mercury measurement possible in the first place, was recognised with the 1913 Nobel Prize in Physics, awarded for his investigations of matter’s properties at low temperatures generally rather than for the superconductivity finding narrowly, reflecting that the discovery and the instrument that enabled it were treated as one body of work.

A Nobel for the cold, not just the effect

What Onnes’s original experiment did not, and could not, supply was any explanation of why the effect happened. The mechanism remained unexplained for decades; even the Meissner effect, the finding that superconductors actively expel magnetic fields rather than merely allowing current to flow without resistance, was not observed until 1933, more than two decades after Onnes’s original result, and added a further layer to what needed accounting for. A workable microscopic theory, describing electrons forming pairs that move through the material without scattering, did not arrive until 1957, when John Bardeen, Leon Cooper, and John Robert Schrieffer proposed what became known as BCS theory, itself later recognised with a Nobel Prize in 1972, well after Onnes had died.

Decades before an explanation

The practical reach of Onnes’s discovery took even longer to unfold, but has become substantial. Superconducting magnets, exploiting exactly the zero-resistance property Onnes first observed, now generate the powerful, stable magnetic fields used in MRI scanners and in particle accelerators, while the Meissner effect’s expulsion of magnetic fields underlies magnetic levitation technology used in some train systems. None of that infrastructure existed in any form close to Onnes’s lifetime; it depended on later work extending superconductivity to materials with higher critical temperatures and on decades of engineering to make superconducting components practical outside a physics laboratory, but all of it traces back to the mercury wire he cooled in liquid helium in April 1911.

From a lab curiosity to MRI magnets

This is a strong use of an hour because it captures something true about how physics often actually proceeds: an instrument built for one purpose, reaching colder temperatures than anyone before, opens up an entirely unanticipated phenomenon, which then takes generations to explain and even longer to put to use. The story rewards attention precisely because the gaps matter, between liquefying helium and finding superconductivity, and between finding it and explaining it with BCS theory nearly half a century later. Readers wanting the deeper physics of Cooper pairs or the specifics of Type I versus Type II superconductors will need to go further, but as an account of how a single low-temperature measurement in 1911 turned into a century-long research programme, it holds together well.

Same field · Physics4 of 183
Up next in Science

High-temperature superconductivity

· 13:00

A ceramic that theory said should not superconduct at all did so at 35 kelvin in 1986, and the mechanism behind it is still not fully explained nearly four decades later.

13:00