Physics

Physics · mechanics

Problem

a - Calculate the flattening factor, given that the gravitational constant is 6.67×10−116.67 \times 10^{-11} N.m ⋅kg−2\cdot \mathrm{kg}^{-2}. Given constants: The rotating neutron star. A 'millisecond pulsar' is a source of radiation in the universe that emits very short pulses with a period of one to several milliseconds. This radiation is in the radio range of wavelengths; and a suitable radio receiver can be used to detect the separate pulses and thereby to measure the period with great accuracy. These radio pulses originate from the surface of a particular sort of star, the so-called neutron star. These stars are very compact: they have a mass of the same order of magnitude as that of the sun, but their radius is only a few tens of kilometers. They spin very quickly. Because of the fast rotation, a neutron star is slightly flattened (oblate). Assume the axial cross-section of the surface to be an ellipse with almost equal axes. Let rpr_{p} be the polar and rer_{e} the equatorial radii; and let us define the flattening factor by: ϵ=(re−rp)rp\epsilon=\frac{\left(r_{e}-r_{p}\right)}{r_{p}}
a mass of2.0⋅1030 kg2.0 \cdot 10^{30} \mathrm{~kg},
an average radius of1.0⋅104 m1.0 \cdot 10^{4} \mathrm{~m},
and a rotation period of2.0⋅10−2 s2.0 \cdot 10^{-2} \mathrm{~s}.

Browse the problem library