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Published equation contexts

ΔS(ϕ)=−2r ln⁡ ⁣[1−ssin⁡ϕ]\Delta_S(\phi) = -2r\,\ln\!\left[1 - s\sin\phi\right]

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The way you weigh a neutron star from a radio telescope, with no direct access to the star at all, is to time its pulses with enough precision to catch general relativity bending them. In a binary system seen close to edge-on, radio pulses from the neutron star are delayed by a few extra microseconds each orbit as they pass close to the companion star, because the companion’s gravity curves the spacetime the pulse crosses. The delay as a function of orbital phase ϕ\phi is standardly written ΔS(ϕ)=−2r ln⁡ ⁣[1−ssin⁡ϕ]\Delta_S(\phi) = -2r\,\ln\!\left[1 - s\sin\phi\right]. where the “range” parameter r is set directly by the companion’s mass and the “shape” parameter s by the orbit’s inclination. Because r and s are measured independently of the pulsar’s…

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ΔS\Delta_S

Symbol Delta_S

DeltaSa_S is part of the quantity the equation computes from the expression on the right.

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Published contexts (1)

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ΔS(ϕ)=−2r ln⁡ ⁣[1−ssin⁡ϕ]\Delta_S(\phi) = -2r\,\ln\!\left[1 - s\sin\phi\right]

Equation 2 · Evolutionary Physics

Cosmological Natural Selection: A Theory That Named Its Own Killer

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.

The way you weigh a neutron star from a radio telescope, with no direct access to the star at all, is to time its pulses with enough precision to catch general relativity bending them. In a binary system seen close to edge-on, radio pulses from the neutron star are delayed by a few extra microseconds each orbit as they pass close to the companion star, because the companion’s gravity curves the spacetime the pulse crosses. The delay as a function of orbital phase ϕ\phi is standardly written ΔS(ϕ)=−2r ln⁡ ⁣[1−ssin⁡ϕ]\Delta_S(\phi) = -2r\,\ln\!\left[1 - s\sin\phi\right]. where the “range” parameter r is set directly by the companion’s mass and the “shape” parameter s by the orbit’s inclination. Because r and s are measured independently of the pulsar’s…

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