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A typical neutron star may have a mass equal to that of the Sun but a radius of only \(10.0 \mathrm{~km} .(a)\) What is the gravitational acceleration at the surface of such a star? \((b)\) How fast would an object be moving if it fell from rest through a distance of \(1.20 \mathrm{~m}\) on such a star?

Short Answer

Expert verified
The gravitational acceleration at the surface of the star is approximately \(1.32 \times 10^{12} \mathrm{ms^{-2}}\) and the speed of the object after falling a distance of 1.2m on the star from rest is approximately \(4.8 \times 10^{6} \mathrm{ms^{-1}}\).

Step by step solution

01

Identify Given Parameters

Let's denote the mass of the star (M) as the mass of the Sun which is approximately \(1.98 \times 10^{30} \mathrm{~kg}\). The radius (r) of the star is given as \(10.0 \mathrm{~km}\), which is \(1.0 \times 10^{4} \mathrm{~m}\). The gravitational constant (G) is \(6.67 \times 10^{-11} \mathrm{Nm^2kg^{-2}}\).
02

Calculate Gravitational Acceleration (Part A)

The formula for the gravitational acceleration at the surface of an object is \(g = \frac{GM}{r^2}\). Substituting the known values, we get \(g = \frac{(6.67 \times 10^{-11})(1.98 \times 10^{30})}{(1.0 \times 10^{4})^2}\) which simplifies to approximately \(1.32 \times 10^{12} \mathrm{ms^{-2}}\).
03

Calculate Speed of Falling Object (Part B)

Utilize the equation of motion which is \(v^2 = u^2 + 2gs\), where v is the final velocity, u is the initial velocity, g is the acceleration due to gravity, and s is the distance. Given that the initial velocity (u) of the object is 0 (since it starts from rest), distance (s) = 1.2m and g = \(1.32 \times 10^{12} \mathrm{ms^{-2}}\), substituting these values will give \(v^2 = 0 + 2(1.32 \times 10^{12})(1.2)\). The final velocity (v) will be approximately \(4.8 \times 10^{6} \mathrm{ms^{-1}}\) when calculated.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Neutron Star Mass
Neutron stars are the remnants of massive stars that have ended their lives in supernova explosions. Despite having a mass that can be comparable to that of our Sun, neutron stars are incredibly dense, resulting in a radius of only about 10 kilometers. This is because their composition is primarily neutron-rich matter; the intense gravity of the star's core having crushed the atomic structure to the point where protons and electrons combine to form neutrons. Understanding the mass of neutron stars is crucial because it affects their gravitational pull, which in turn influences their surroundings in space, including binary star systems and the emission of gravitational waves.
Gravitational Constant
The gravitational constant, denoted by the symbol G, is a key player in the universal law of gravitation. It is the proportionality constant used in Newton's law of universal gravitation, and it appears in other important physics equations, such as those applied in gravimetric measurements and celestial mechanics. The value of the gravitational constant is approximately \(6.67 \times 10^{-11} \mathrm{Nm^2kg^{-2}}\), which indicates the strength of gravity in a specific measurement system. It's crucial to apply the correct value of G when performing calculations related to gravitational force or acceleration, as it ensures the accuracy of the results. When considering objects such as neutron stars, the gravitational constant enables us to calculate extreme gravitational accelerations, demonstrating the vast differences between gravitational forces in space compared to those we experience on Earth.
Equation of Motion
The equation of motion for an object under the influence of gravity provides a relationship between initial velocity, final velocity, acceleration, and distance covered. Specifically, the equation \(v^2 = u^2 + 2gs\) is a useful kinematic equation, with 'v' representing final velocity, 'u' the initial velocity, 'g' the acceleration due to gravity, and 's' the distance traveled by the object. When applying this equation to a falling object on a neutron star, we input the immense gravitational acceleration already calculated and the fact that the object started from rest, meaning its initial velocity is zero. Using these values, the equation allows us to determine the final velocity of the object after it has fallen through a certain distance. This showcases how the fundamental principles of motion provide a window into understanding extreme scenarios like objects falling on the surface of a neutron star.

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Most popular questions from this chapter

Assume that a geosynchronous communications satellite is in orbit at the longitude of Chicago. You are in Chicago and want to pick up its signals. In what direction should you point the axis of your parabolic antenna? The latitude of Chicago is \(47.5^{\circ} \mathrm{N}\)

Two particles of mass \(m\) and \(M\) are initially at rest an infinite distance apart. Show that at any instant their relative velocity of approach attributable to gravitational attraction is \(\sqrt{2 G(M+m) / d}\), where \(d\) is their separation at that instant.

Two point-like particles, each of mass \(m\), are originally separated by a distance \(d\) and moving in opposite directions each with a speed of \(v\). What is the maximum value for \(v\) so that the particles will eventually move back together under the influence of the mutual gravitational attraction?

It is conjectured that a "burned-out" star could collapse to a "gravitational radius," defined as the radius for which the work needed to remove an object of mass \(m\) from the star's surface to infinity equals the rest energy \(m c^{2}\) of the object. Show that the gravitational radius of the Sun is \(G M_{\mathrm{S}} / c^{2}\) and determine its value in terms of the Sun's present radius. (For a review of this phenomenon see "Black Holes: New Horizons in Gravitational Theory," by Philip C. Peters, American Scientist, September- October \(1974, \mathrm{p} .575 .)\)

The asteroid Eros, one of the many minor planets that orbit the Sun in the region between Mars and Jupiter, has a radius of \(7.0 \mathrm{~km}\) and a mass of \(5.0 \times 10^{15} \mathrm{~kg} .(a)\) If you were standing on Eros, could you lift a \(2000-\mathrm{kg}\) pickup truck? \((b)\) Could you run fast enough to put yourself into orbit? Ignore effects due to the rotation of the asteroid. (Note: The Olympic records for the \(400-\mathrm{m}\) run correspond to speeds of \(9.1 \mathrm{~m} / \mathrm{s}\) for men and \(8.2 \mathrm{~m} / \mathrm{s}\) for women.)

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