Place the main-sequence lifetimes of the following stars in order from shortest to longest. a. the Sun: mass \(1 M_{\text {sun }}\), luminosity \(1 L_{\text {sun }}\) b. Capella Aa: mass 3 \(M_{\text {sun }}\), luminosity 76 \(L_{\text {Sun }}\) c. Rigel: mass \(24 M_{\text {sun }}\), luminosity \(85,000 L_{\text {sun }}\) d. Sirius A: mass 2 \(M_{\text {sun }}\), luminosity 25 \(L_{\text {sun }}\) e. Canopus: mass \(8.5 M_{\text {sun }}\), luminosity \(13,600 L_{\text {sun }}\) f. Achernar: mass \(7 M_{\text {sun }}\), luminosity \(3,150 L_{\text {sun }}\)

Short Answer

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Rigel, Canopus, Achernar, Capella Aa, Sirius A, the Sun

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01

Understand the Main-Sequence Lifetime Formula

The main-sequence lifetime of a star can be approximated by the formula: \[ t = \frac{10^{10} \text{ years}}{\frac{M}{L}} \] where \(t\) is the lifetime, \(M\) is the mass of the star in solar masses \(M_{\text{sun}}\), and \(L\) is the luminosity of the star in solar luminosities \(L_{\text{sun}}\).
02

Calculate the Main-Sequence Lifetimes

For each star, use the above formula to calculate the main-sequence lifetime.1. **The Sun**: \[ t_{\text{Sun}} = \frac{10^{10} \text{ years}}{\frac{1}{1}} = 10^{10} \text{ years} \]2. **Capella Aa**: \[ t_{\text{Capella Aa}} = \frac{10^{10} \text{ years}}{\frac{3}{76}} = \frac{10^{10} \text{ years} \times 76}{3} \text{ years} \]\[ t_{\text{Capella Aa}} \approx 2.53 \times 10^9 \text{ years} \]3. **Rigel**: \[ t_{\text{Rigel}} = \frac{10^{10} \text{ years}}{\frac{24}{85,000}} = \frac{10^{10} \text{ years} \times 85,000}{24} \text{ years} \]\[ t_{\text{Rigel}} \approx 3.54 \times 10^5 \text{ years} \]4. **Sirius A**: \[ t_{\text{Sirius A}} = \frac{10^{10} \text{ years}}{\frac{2}{25}} = \frac{10^{10} \text{ years} \times 25}{2} \text{ years} \]\[ t_{\text{Sirius A}} \approx 1.25 \times 10^9 \text{ years} \]5. **Canopus**: \[ t_{\text{Canopus}} = \frac{10^{10} \text{ years}}{\frac{8.5}{13,600}} = \frac{10^{10} \text{ years} \times 13,600}{8.5} \text{ years} \]\[ t_{\text{Canopus}} \approx 1.60 \times 10^8 \text{ years} \]6. **Achernar**: \[ t_{\text{Achernar}} = \frac{10^{10} \text{ years}}{\frac{7}{3,150}} = \frac{10^{10} \text{ years} \times 3,150}{7} \text{ years} \]\[ t_{\text{Achernar}} \approx 4.50 \times 10^8 \text{ years} \]
03

Order the Lifetimes from Shortest to Longest

Arrange the calculated lifetimes in ascending order:1. **Rigel**: \(3.54 \times 10^5\) years2. **Canopus**: \(1.60 \times 10^8\) years3. **Achernar**: \(4.50 \times 10^8\) years4. **Capella Aa**: \(2.53 \times 10^9\) years5. **Sirius A**: \(1.25 \times 10^9\) years6. **The Sun**: \(10^{10}\) years

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Key Concepts

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

Stellar Evolution
Stellar evolution refers to the life cycle of a star from its formation to its eventual death. Stars form from clouds of gas and dust known as nebulas. As gravity pulls these materials together, they form a protostar. When the core temperature becomes high enough, nuclear fusion ignites, turning the protostar into a main-sequence star.
In the main-sequence phase, a star fuses hydrogen into helium in its core, generating energy and light. The main-sequence phase is the longest and most stable period in a star's life.
Stars leave the main sequence when they exhaust their hydrogen fuel, leading them to become red giants, white dwarfs, neutron stars, or black holes, depending on their initial mass.
Luminosity
Luminosity is the measure of the total amount of energy a star emits per second. It's a key property in understanding a star's structure and behavior. The luminosity of a star is often compared to our Sun’s luminosity, denoted as \(L_{\text{sun}}\).
Factors affecting a star's luminosity include its size and surface temperature. Larger and hotter stars tend to have higher luminosities. For example, Rigel, with a mass of 24 solar masses and a luminosity of 85,000 solar luminosities, is significantly more luminous than the Sun.
The luminosity of a star can be used to estimate its energy output and, indirectly, its life expectancy, as highly luminous stars consume their fuel more rapidly.
Mass-Luminosity Relationship
The mass-luminosity relationship is a key principle in stellar astrophysics. It states that a star's luminosity is proportional to its mass raised to a power ranging between 3 and 4. Mathematically, it is represented as:
\[ L \propto M^{3.5} \] This means that even small increases in a star's mass can lead to significant increases in its luminosity. For instance, a star with twice the mass of the Sun is roughly 11 times more luminous.
This relationship is crucial in predicting how long a star will remain in the main sequence. More massive stars have higher luminosities and therefore shorter lifetimes because they burn through their nuclear fuel more quickly.
Main-Sequence Lifetime Formula
To estimate a star's main-sequence lifetime, a crucial formula is used:
\[ t = \frac{10^{10} \text{ years}}{\frac{M}{L}} \] Here, \(t\) is the lifetime, \(M\) is the mass of the star in solar masses, and \(L\) is the luminosity in solar luminosities. This formula demonstrates that a star's lifetime is inversely proportional to its mass-to-luminosity ratio.
For example, Rigel, with a mass of 24 solar masses and a luminosity of 85,000 solar luminosities, has a much shorter main-sequence lifetime (\(3.54 \times 10^5\) years) compared to the Sun, which has a lifetime of \(10^{10}\) years.
This formula allows us to predict the duration for which a star will remain stable in its main-sequence phase, an essential part of understanding stellar evolution.

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Most popular questions from this chapter

Go to the Hubble Space Telescope's planetary nebula gallery (http://hubblesite.org/gallery/album/nebula/planetary). For each of the three types of symmetry, find an example of a nebula that shows clearly the type of symmetry: spherical (being symmetric in every direction, like a circle), bipolar (having an axis about which they are symmetric, like a person's face, and point-symmetric (being symmetric about a point, like the letter \(S\) ). Print each of the three images you chose, and label the type of symmetry each one represents. For all three nebulae, identify the location of the central star. For bipolar symmetry, draw a line that shows the axis about which the nebula is symmetric. For point symmetry, identify several features that are symmetric across the location of the central star.

Place the following steps in the evolution of a low-mass star in order. a. main-sequence star b. planetary nebula ejection c. horizontal branch d. helium flash e. red giant branch f. asymptotic giant branch g. white dwarf

A white dwarf has a density of approximately \(10^{9}\) kilograms per cubic meter \(\left(\mathrm{kg} / \mathrm{m}^{3}\right)\). Earth has an average density of \(5,500 \mathrm{kg} / \mathrm{m}^{3}\) and a diameter of \(12,700 \mathrm{km} .\) If Earth were compressed to the same density as a white dwarf, what would its radius be?

If a main-sequence star suddenly started burning hydrogen at a faster rate in its core, it would become a. larger, hotter, and more luminous. b. larger, cooler, and more luminous. c. smaller, hotter, and more luminous. d. smaller, cooler, and more luminous.

What will the escape velocity be when the Sun becomes an AGB star with a radius 200 times greater and a mass only 0.7 times that of today? How will these changes in escape velocity affect mass loss from the surface of the Sun as an AGB star?

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