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A neutron star is a stellar object whose density is about that of nuclear matter, \(2 \times 10^{17} \mathrm{~kg} / \mathrm{m}^{3}\). Suppose that the Sun were to collapse and become such a star without losing any of its present mass. What would be its radius?

Short Answer

Expert verified
The radius of the neutron star would be approximately 10.4 km.

Step by step solution

01

Identify the Given Values

We know that the density of the neutron star is \( \rho = 2 \times 10^{17} \text{ kg/m}^3 \). The mass of the Sun \( M \) is approximately \( 1.989 \times 10^{30} \text{ kg} \). We need to find the radius \( R \) of the neutron star.
02

Use the Density Formula

The formula to find the volume \( V \) of an object using density \( \rho \) and mass \( M \) is \( \rho = \frac{M}{V} \). Rearranging this, we find \( V = \frac{M}{\rho} \).
03

Calculate the Volume

Substitute the known values into the volume formula: \[ V = \frac{1.989 \times 10^{30} \text{ kg}}{2 \times 10^{17} \text{ kg/m}^3} = 9.945 \times 10^{12} \text{ m}^3 \]
04

Relate Volume to Radius

The volume of a sphere is given by \( V = \frac{4}{3} \pi R^3 \). We need to solve for \( R \). Reorganize the formula to find \( R \):\[ R^3 = \frac{3V}{4\pi} \]
05

Calculate the Radius

Substitute the calculated volume into the rearranged formula:\[ R^3 = \frac{3 \times 9.945 \times 10^{12}}{4 \pi} \]Solve for \( R \):\[ R = \left(\frac{3 \times 9.945 \times 10^{12}}{4 \pi}\right)^{1/3} \approx 10400 \text{ m} \]
06

Convert the Radius to Kilometers

Convert the radius from meters to kilometers for a more intuitive understanding: \( R \approx 10.4 \text{ km} \).

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Key Concepts

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

Understanding Density
Density is a measure of how much mass is contained in a given volume. It helps describe how tightly or loosely matter is packed together within an object. For example, a neutron star is incredibly dense, with its density being about the same as that of nuclear matter, which is an extraordinary value of \(2 \times 10^{17} \, \text{kg/m}^3\).

To understand density better, imagine trying to press a large amount of mass into a compact volume. This is exactly what happens in a neutron star, where gravity compresses huge masses into tiny spaces.
  • High density means lots of mass in a small space.
  • Low density means a small amount of mass spread over a large space.

For practical purposes, when calculating other properties of objects like a neutron star, density serves as an essential bridge between mass and volume.
Calculating Mass
Mass is a fundamental property of matter representing the amount of matter within an object. In the universe of astrophysics, understanding mass is crucial, especially when dealing with such massive objects as stars.

The mass of the Sun, for example, is approximately \(1.989 \times 10^{30} \, \text{kg}\). This mass would not change even if the Sun were to transform into a neutron star. Despite the Sun's transformation into a neutron star, the huge amount of mass remains constant.
  • Mass is constant regardless of the object's state.
  • It is a key factor in the gravitational pull of objects.
  • Mass can be calculated in different states or forms, maintaining its value.

Mass plays a critical role in calculating other physical properties, beginning with its measurement and proceeding to how it relates to density and volume.
Volume and Its Calculation
Volume measures the amount of space an object occupies. When a massive object like the Sun becomes a neutron star, understanding how much space it takes up is crucial for determining its new size.

To find the volume of a neutron star, we use the formula for density: \(\rho = \frac{M}{V}\), which can be rearranged to give \(V = \frac{M}{\rho}\). Using the Sun's mass \( (1.989 \times 10^{30} \, \text{kg}) \) and the neutron star's density \( (2 \times 10^{17} \, \text{kg/m}^3) \), we calculate the volume to be approximately \(9.945 \times 10^{12} \, \text{m}^3\).
  • Volume is a measure of space occupied.
  • The volume changes as a star's state changes, even if mass remains the same.

This calculated volume gives insight into just how compact a neutron star becomes, despite retaining the full mass of the Sun.
Radius Calculation
The radius of a spherical object like a neutron star can be derived from its volume through geometry. Once we know the volume, finding the radius is essential for visualizing the actual size of the object.

The formula for the volume of a sphere is \(V = \frac{4}{3} \pi R^3\). By rearranging to solve for the radius \(R\), we get \(R^3 = \frac{3V}{4\pi}\). By substituting our volume \((9.945 \times 10^{12} \, \text{m}^3)\) into this equation, we find that \(R\) is approximately \(10400 \, \text{m}\) or \(10.4 \, \text{km}\).
  • Radius provides a sense of scale for spherical objects.
  • Calculating radius from volume involves geometric formulas.

Knowing the radius gives us a tangible measurement, making it easier to comprehend just how compact and dense a neutron star really is.

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Most popular questions from this chapter

A certain radionuclide is being manufactured in a cyclotron at a constant rate \(R\). It is also decaying with disintegration constant \(\lambda\). Assume that the production process has been going on for a time that is much longer than the half-life of the radionuclide. (a) Show that the number of radioactive nuclei present after such time remains constant and is given by \(N=R / \lambda\). (b) Now show that this result holds no matter how many radioactive nuclei were present initially. The nuclide is said to be in secular equilibrium with its source; in this state its decay rate is just equal to its production rate.

Plutonium isotope \({ }^{239} \mathrm{Pu}\) decays by alpha decay with a half- life of \(24100 \mathrm{y}\). How many milligrams of helium are produced by an initially pure \(10.0 \mathrm{~g}\) sample of \({ }^{239} \mathrm{Pu}\) at the end of \(20000 \mathrm{y}\) ? is emitted by a nucleus, along with a neutrino. The emitted particles share the available disintegration energy. The electrons and positrons emitted in beta decay have a continuous spectrum of energies from near zero up to a limit \(K_{\max }\left(=Q=-\Delta m c^{2}\right)\). Radioactive Dating Naturally occurring radioactive nuclides provide a means for estimating the dates of historic and prehistoric events. For example, the ages of organic materials can often be found by measuring their \({ }^{14} \mathrm{C}\) content; rock samples can be dated using the radioactive isotope \({ }^{40} \mathrm{~K}\). Radiation Dosage Three units are used to describe exposure to ionizing radiation. The becquerel ( \(1 \mathrm{~Bq}=1\) decay per second) measures the activity of a source. The amount of energy actually absorbed is measured in grays, with 1 Gy corresponding to \(1 \mathrm{~J} / \mathrm{kg}\). The estimated biological effect of the absorbed energy is measured in sieverts; a dose equivalent of 1 Sv causes the same biological effect regardless of the radiation type by which it was acquired. Nuclear Models The collective model of nuclear structure assumes that nucleons collide constantly with one another and that relatively long-lived compound nuclei are formed when a projectile is captured. The formation and eventual decay of a compound nucleus are totally independent events. The independent particle model of nuclear structure assumes that each nucleon moves, essentially without collisions, in a quantized state within the nucleus. The model predicts nucleon levels and magic nucleon numbers \((2,8,20,28,50,82\), and 126) associated with closed shells of nucleons; nuclides with any of these numbers of neutrons or protons are particularly stable. The combined model, in which extra nucleons occupy quantized states outside a central core of closed shells, is highly successful in predicting many nuclear properties.

Large radionuclides emit an alpha particle rather than other combinations of nucleons because the alpha particle has such a stable, tightly bound structure. To confirm this statement, calculate the disintegration energies for these hypothetical decay processes and discuss the meaning of your findings: (a) \({ }^{235} \mathrm{U} \rightarrow{ }^{232} \mathrm{Th}+{ }^{3} \mathrm{He}, \quad\) (b) \({ }^{235} \mathrm{U} \rightarrow{ }^{231} \mathrm{Th}+{ }^{4} \mathrm{He}\), (c) \({ }^{235} \mathrm{U} \rightarrow{ }^{230} \mathrm{Th}+{ }^{5} \mathrm{He}\). The needed atomic masses are \(\begin{array}{llll}{ }^{232} \mathrm{Th} & 232.0381 \mathrm{u} & { }^{3} \mathrm{He} & 3.0160 \mathrm{u} \\ { }^{21} \mathrm{Th} & 231.0363 \mathrm{u} & { }^{4} \mathrm{He} & 4.0026 \mathrm{u} \\ { }^{230} \mathrm{Th} & 230.0331 \mathrm{u} & { }^{5} \mathrm{He} & 5.0122 \mathrm{u} \\ { }^{235} \mathrm{U} & 235.0429 \mathrm{u} & & \end{array}\)

An \(\alpha\) particle ( \({ }^{4} \mathrm{He}\) nucleus) is to be taken apart in the following steps. Give the energy (work) required for each step: (a) remove a proton, (b) remove a neutron, and (c) separate the remaining proton and neutron. For an \(\alpha\) particle, what are (d) the total binding energy and (e) the binding energy per nucleon? (f) Does either match an answer to (a), (b), or (c)? Here are some atomic masses and the neutron mass. \(\begin{array}{llll}{ }^{4} \mathrm{He} & 4.00260 \mathrm{u} & { }^{2} \mathrm{H} & 2.01410 \mathrm{u} \\ { }^{3} \mathrm{H} & 3.01605 \mathrm{u} & { }^{1} \mathrm{H} & 1.00783 \mathrm{u} \\ \mathrm{n} & 1.00867 \mathrm{u} & & \end{array}\)

The half-life of a radioactive isotope is \(120 \mathrm{~d}\). How many days would it take for the decay rate of a sample of this isotope to fall to one- fourth of its initial value?

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