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Science Astronomy Atmosphere

Vol. Science · Astronomy · The spin

Pulsars
and the spin-down

A radio pulsar is a neutron star whose beam sweeps past Earth. Two measured numbers carry the dipole story: the spin period P and how fast that period is growing, Ṗ. For magnetic-dipole braking the index is n = 3, so the characteristic age is τ = P / (2 Ṗ). The surface dipole field in the catalogue convention is B = 3.2×10¹⁹ √(P Ṗ) gauss, with a moment of inertia I = 10⁴⁵ g cm² (10³⁸ kg m²) and a radius of 10 km. The spin-down luminosity is Ė = 4π² I Ṗ / P³. The light cylinder, where a co-rotating field would move at the speed of light, is Rlc = c P / (2π). c = 299,792,458 m/s exactly. The four buttons are P0 and P1 printed by the ATNF Pulsar Catalogue version 2.9.0 (Manchester, Hobbs, Teoh, and Hobbs 2005). The Crab’s catalogue age is 1,257 yr. The supernova of 1054 is 972 years before 2026. A heavy star’s path to a neutron star is the stellar lifetime desk. A horizon, if the remnant is heavier, is the black holes desk.

Educational calculator. Idealized magnetic dipole. Braking index fixed at 3. Moment of inertia fixed at 10⁴⁵ g cm². Radius fixed at 10 km. True ages and true fields differ. The Crab’s true age is the supernova of 1054, 972 years by a count of calendar years to 2026, not the characteristic age. Catalogue periods are at the printed epoch, not a live ephemeris. Not a timing model.

Interactive · Period and derivative

Log period across · log period derivative up · short and fast-slowing is the upper left

  • This point
  • Cited preset
  • Constant age
  • Constant B
  • 10¹² V sketch

Catalogue presets · P0 and P1, ATNF v2.9.0

Period

Period derivative · logarithmic · dimensionless

Opens on the Crab, B0531+21, catalogue epoch MJD 48442.5. Lines of constant age slope up to the right. Lines of constant dipole field slope down. The dashed line is a 10¹² V polar-cap sketch, not a fitted death line. Only the four cited pulsars are marked.

ATNF v2.9.0 presets · dipole formulas on the printed P0 and P1
Pulsar P Ṗ Epoch τ B Ė Rlc
Crab B0531+2133.3924123 ms4.20972×10⁻¹³MJD 48442.51,257 yr3.794×10¹² G4.463×10³¹ W1,593.3 km
Vela B0833−4589.328385024 ms1.25008×10⁻¹³MJD 51559.31911.32 kyr3.382×10¹² G6.924×10²⁹ W4,262.2 km
J0437−47155.757451941593412 ms5.729220×10⁻²⁰MJD 554861.592 Gyr5.812×10⁸ G1.185×10²⁷ W274.71 km
B1919+211.3373021601895 s1.348207×10⁻¹⁵MJD 48999.015.72 Myr1.359×10¹² G2.226×10²⁴ W63,807 km

What the numbers are

Two numbers, and the beam. A pulsar is a neutron star, seen when the beam swings past Earth. The catalogue period is the time for one turn. The period derivative is how much that time grows each second. It is tiny, and it is dimensionless. The Crab’s catalogue period is 33.3924123 ms and its derivative is 4.20972×10⁻¹³. J0437−4715 turns in 5.757451941593412 ms. B1919+21 takes 1.3373021601895 s.

The age is an assumption. Characteristic age is the period divided by twice the derivative. Braking index 3 is the dipole. The Crab’s catalogue numbers give 1,257 yr. The guest star of 1054, the supernova tied to the Crab Nebula, is 972 years before 2026. The characteristic age is longer because the star was not born at a standstill, and because the braking index does not have to stay at 3. Vela’s catalogue age is 11.32 kyr. B1919+21’s is 15.72 Myr. J0437−4715’s is 1.592 Gyr, a recycling age, not the age of the star.

Field, power, and the light cylinder. The surface dipole field on this page is 3.2×10¹⁹ √(P Ṗ) gauss. That is the ATNF BSURF convention, with I = 10⁴⁵ g cm² and R = 10 km. The Crab computes 3.794×10¹² G, order 10¹² G. J0437−4715 computes 5.812×10⁸ G. The polar field in Harding’s equation (5) is twice this, 6.4×10¹⁹ √(P Ṗ), because a dipole is stronger at the pole. Spin-down luminosity is 4π² I Ṗ / P³. The Crab’s is 4.463×10³¹ W, which is 4.463×10³⁸ erg/s. The ATNF EDOT column prints that power in erg/s, rounded. The light cylinder is c P / (2π). Inside it, a co-rotating field would still be slower than light. The Crab’s is 1,593.3 km.

Literacy · the words on the readout

Period
P, the barycentric spin period, in seconds. The millisecond buttons are the same number times 1,000. One turn of the Crab’s catalogue period is 33.3924123 ms, which is 29.947 Hz.
Period derivative
Ṗ, how many seconds the period grows in one second. Dimensionless. The slider is logarithmic, from 10⁻²² to 10⁻⁹. A negative derivative, a glitch, or a measured Shklovskii term is outside this page.
Characteristic age
τ = P / (2 Ṗ). The 2 is the dipole, braking index n = 3, because τ = P / ((n − 1) Ṗ). It counts from a birth spin much faster than today’s. A year here is 365.25 × 86,400 seconds.
Dipole field
B = 3.2×10¹⁹ √(P Ṗ) gauss. Canonical I = 10⁴⁵ g cm² and R = 10 km. The 3.2 has two figures. This is the ATNF BSURF column, the equatorial convention. Harding’s polar field is twice it.
Spin-down luminosity
Ė = 4π² I Ṗ / P³. With I = 10³⁸ kg m² the result is watts. Multiply by 10⁷ for erg/s, which is how the catalogue prints EDOT, rounded. It is the rotational power, not a measured flux at Earth.
Light cylinder and the diagram
Rlc = c P / (2π), with c = 299,792,458 m/s. On the log-log diagram, constant age is a line of slope +1 and constant B is a line of slope −1. Millisecond pulsars sit at short P and tiny Ṗ. The dashed line is Harding’s equation (1) at a polar-cap potential of 10¹² V, the round value Xia Zhou holds fixed in IAU Symposium 337. Chen and Ruderman call the real radio boundary a death valley, not this one line. The shaded side is that sketch. No other pulsars are plotted.

Sources · the periods and the formulas

Cited, not invented

Classroom dipole. P and Ṗ for the four buttons are ATNF Pulsar Catalogue v2.9.0, not invented and not a later ephemeris. τ = P/(2 Ṗ). B = 3.2×10¹⁹ √(P Ṗ) G. Ė = 4π² I Ṗ / P³. Rlc = c P / (2π). The Crab’s characteristic age is 1,257 yr. The supernova of 1054 is 972 years before 2026. The dashed line is a 10¹² V sketch. Not a timing model. Earthrise preview: NASA / Bill Anders (public domain).

Keep going

The path

Stellar lifetime

Mass, a mass–luminosity fit, and t ≈ 10 Gyr × M/L. A neutron star is one rough end for a heavy star. The spin clock is this page.

The horizon

Black holes

Schwarzschild radius, photon sphere, and ISCO. The nominal solar mass is 2.953 km. A heavier remnant does not pulse.

The chirp

Gravitational waves

A compact binary’s leading-order sweep. 36 and 29 solar masses compute a chirp mass of 28.10. Not a waveform model.

Diagram

HR diagram

Another log-log picture. Temperature across, luminosity up. This page’s axes are period and its derivative.

Map

Solar map

The neighborhood. Neutron stars are not on that orrery. The formulas are here.