Lesson 13 of 15

Gravitational Wave Strain

Gravitational Wave Strain

The gravitational wave strain hh is a dimensionless number that measures the fractional stretching of space. If a detector of length LL is stretched by δL\delta L, then h=2δL/Lh = 2\delta L/L. LIGO measures strains of order 102110^{-21} — one part in a billion billion billion.

For a compact binary at luminosity distance dd, with chirp mass Mc\mathcal{M}_c and instantaneous GW frequency ff, the strain amplitude from the leading-order quadrupole formula is:

h=4dGMcc2(πGMcfc3)2/3h = \frac{4}{d} \cdot \frac{G\mathcal{M}_c}{c^2} \cdot \left(\frac{\pi G \mathcal{M}_c f}{c^3}\right)^{2/3}

This grows during the inspiral as ff increases, reaching its peak at the ISCO frequency.

GW150914 Numbers

ParameterValue
m1m2m_1 \approx m_230M\sim 30\,M_\odot
dd410\sim 410 Mpc
fISCOf_{\rm ISCO}73\sim 73 Hz
Peak strain1021\sim 10^{-21}

Distance Conversion

One megaparsec (Mpc): 1 Mpc=3.0857×10221\text{ Mpc} = 3.0857 \times 10^{22} m.

Constants (define inside each function)

  • G=6.674×1011G = 6.674 \times 10^{-11} m³ kg⁻¹ s⁻²
  • c=299792458c = 299792458 m/s

Your Task

Implement the three functions below. The chirp mass and ISCO frequency formulae from previous lessons may be computed inline inside gw_strain_at_isco.

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