/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 75 The Sizes of Stars. The hot glow... [FREE SOLUTION] | 91Ó°ÊÓ

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The Sizes of Stars. The hot glowing surfaces of stars emit energy in the form of electromagnetic radiation. It is a good approximation to assume \(e=1\) for these surfaces. Find the radii of the following stars (assumed to be spherical): (a) Rigel, the bright blue star in the constellation Orion, which radiates energy at a rate of \(2.7 \times 10^{32} \mathrm{W}\) and has surface temperature \(11,000 \mathrm{K}\) ; (b) Procyon \(\mathrm{B}\) (visible only using a telescope), which radiates energy at a rate of \(2.1 \times 10^{23} \mathrm{W}\) and has surface temperature \(10,000 \mathrm{K}\) (c) Compare your answers to the radius of the earth, the radius of the sun, and the distance between the earth and the sun. (Rigel is an example of a supergiant star, and Procyon \(\mathrm{B}\) is an example of a white dwarf star.)

Short Answer

Expert verified
Rigel's radius is about 54.2 million km, and Procyon B's radius is about 9,800 km, indicating Rigel is a supergiant and Procyon B is a white dwarf.

Step by step solution

01

Understanding the Stefan-Boltzmann Law

To find the radius of a star given its luminosity and temperature, we can use the Stefan-Boltzmann Law. This law states that the power emitted by a star is proportional to its surface area and the fourth power of its temperature. It is expressed as \( L = 4\pi R^2 \sigma T^4 \), where \( L \) is the luminosity (or power radiated), \( R \) is the radius, \( \sigma \) is the Stefan-Boltzmann constant \( (5.67 \times 10^{-8} \, \text{W/m}^2\cdot\text{K}^4) \), and \( T \) is the temperature.
02

Solving for Radius

Rearranging the equation for radius, we have: \( R = \sqrt{\frac{L}{4\pi \sigma T^4}} \). This formula will allow us to compute the radius of each star using their given luminosity and surface temperature.
03

Calculating Radius for Rigel

For Rigel, the luminosity \( L = 2.7 \times 10^{32} \, \text{W} \) and temperature \( T = 11,000 \, \text{K} \). Substitute these into the formula: \[ R = \sqrt{\frac{2.7 \times 10^{32}}{4\pi \times 5.67 \times 10^{-8} \times (11,000)^4}} \]. Calculating this gives \( R \approx 54.2 \times 10^6 \text{ km} \).
04

Calculating Radius for Procyon B

For Procyon B, the luminosity \( L = 2.1 \times 10^{23} \, \text{W} \) and temperature \( T = 10,000 \, \text{K} \). Substitute these into the formula: \[ R = \sqrt{\frac{2.1 \times 10^{23}}{4\pi \times 5.67 \times 10^{-8} \times (10,000)^4}} \]. Calculating this gives \( R \approx 9.8 \times 10^{3} \text{ km} \).
05

Comparing Results with Known Values

The radius of the Earth is approximately 6,371 km, the radius of the Sun is about 696,340 km, and the average distance from the Earth to the Sun is about 149.6 million km. Rigel's radius of \(54.2 \times 10^6 \text{ km} \) indicates it is much larger than our Sun, qualifying it as a supergiant. Procyon B's radius of \(9.8 \times 10^{3} \text{ km} \) makes it relatively close in size to Earth, typical of a white dwarf.

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Key Concepts

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

Electromagnetic Radiation
Stars, like Rigel and Procyon B, emit energy in the form of electromagnetic radiation. This type of energy travels through space in the form of waves. Electromagnetic radiation includes a broad range of wavelengths such as gamma rays, X-rays, ultraviolet light, visible light, infrared, microwaves, and radio waves. The energy output of stars is directly related to their surface temperature and radius. High-temperature stars emit more energetic waves, primarily in the visible and ultraviolet spectrum. Understanding electromagnetic radiation helps scientists determine a star's behavior, composition, and structure.
Electromagnetic radiation from stars provides insight into the universe as it carries crucial information about the star's internal processes. As this radiation reaches Earth, it is captured by telescopes and analyzed to understand phenomena such as the chemical makeup of stars and their movement in galaxies.
The Stefan-Boltzmann Law is particularly important here. It links the luminosity of a star to its electromagnetic output, and allows us to calculate the energy a star emits from its surface at given temperatures.
Star Luminosity
Luminosity of a star, like the ones in this exercise, refers to the total amount of energy a star radiates per second. It's comparable to the light intensity of a bulb but on a cosmic scale. Luminosity is measured in watts and can vary widely from one star to another depending on size and temperature.
For instance, Rigel emits a luminosity of approximately \(2.7 \times 10^{32}\) watts, making it a very bright star due to its large size and high temperature. On the other hand, Procyon B has a much lower luminosity of \(2.1 \times 10^{23}\) watts, because it is much smaller and cooler compared to Rigel.
*Factors influencing star luminosity include:*
  • Radius of the Star: Larger stars have more surface area, which allows them to emit more light.
  • Surface Temperature: Hotter stars emit more energy per unit of surface area, thus appearing more luminous.
Luminosity is crucial for astronomers as it helps determine a star's stage in its life cycle, from its formation, through its active main-sequence phase, and eventually to its death.
Stellar Radius Calculation
To find a star's radius when given its luminosity and temperature, astronomers use a formula derived from the Stefan-Boltzmann Law. The law states that the power radiated per unit area is proportional to the fourth power of the temperature. Thus, the formula for radius is:\[R = \sqrt{\frac{L}{4\pi \sigma T^4}}\]This equation allows us to find the radius, \(R\), using the luminosity, \(L\), and temperature, \(T\), where \(\sigma\) is the Stefan-Boltzmann constant \((5.67 \times 10^{-8} \text{W/m}^2\cdot\text{K}^4)\).
The step-by-step solution given involves plugging Luminosity and Temperature for stars like Rigel \( (L = 2.7 \times 10^{32} \, \text{W},\ T = 11,000 \, \text{K}) \) and Procyon B \( (L = 2.1 \times 10^{23} \, \text{W},\ T = 10,000 \, \text{K}) \) into this formula. The radius is essential not just for size comparison, but also for determining the star's type and expected lifecycle events.
Supergiant and White Dwarf Comparison
Stars like Rigel and Procyon B are excellent representatives of supergiants and white dwarfs respectively. They illustrate how the size of a star can vary dramatically based on its stage in the stellar life cycle.

**Supergiants:**
  • Rigel is a supergiant, characterized by its massive radius and brightness. With a radius of approximately \(54.2 \times 10^6\,\text{km}\), Rigel forms an imposing presence in the cosmos, far exceeding the size of our Sun.
  • Supergiants are among the largest stars in the universe. Their extended radius means they emit a tremendous amount of light, making them highly luminous.
**White Dwarfs:**
  • In contrast, Procyon B is a white dwarf with a radius of about \(9.8 \times 10^{3}\,\text{km}\), reflecting a stage of life where the star has exhausted its nuclear fuel and collapsed into a much smaller size comparable only to planetary dimensions.
  • White dwarfs are the final evolutionary state of stars like our Sun. They are dense, not as bright, yet incredibly hot.
This stark contrast highlights the dynamic and varied nature of stars as they progress through their cosmic lives.

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Most popular questions from this chapter

While painting the top of an antenna 225 \(\mathrm{m}\) in height, a worker accidentally lets a \(1.00-\mathrm{L}\) wattle fall from his lunchbox. The bottle lands in some bushes at ground level and does not break. If a quantity of heat equal to the magnitude of the change in mechanical energy of the water goes into the water, what is its increase in temperature?

Spacecraft Reentry. A spacecraft made of aluminum circles the earth at a speed of 7700 \(\mathrm{m} / \mathrm{s} .\) (a) Find the ratio of its kinetic energy to the energy required to raise its temperature from \(0^{\circ} \mathrm{C}\) to \(600^{\circ} \mathrm{C}\) . (The melting point of aluminum is \(660^{\circ} \mathrm{C}\) . Assume a constant specific heat of 910 \(\mathrm{J} / \mathrm{kg} \cdot \mathrm{K} .\) (b) Discuss the bearing of your answer on the problem of the reentry of a manned space vehicle into the earth's atmosphere.

A 15.0 -g bullet traveling horizontally at 865 \(\mathrm{m} / \mathrm{s}\) passes through a tank containing 13.5 \(\mathrm{kg}\) of water and emerges with a speed of 534 \(\mathrm{m} / \mathrm{s}\) . What is the maximum temperature increase that the water could have as a result of this event?

(a) A wire that is 1.50 \(\mathrm{m}\) long at \(20.0^{\circ} \mathrm{C}\) is found to increase in length by 1.90 \(\mathrm{cm}\) when warmed to \(420.0^{\circ} \mathrm{C}\) . Compute its average coefficient of linear expansion for this temperature range. (b) The wire is stretched just taut (zero tension) at \(420.0^{\circ} \mathrm{C}\). Find the stress in the wire if it is cooled to \(20.0^{\circ} \mathrm{C}\) without being allowed to contract. Young's modulus for the wire is \(2.0 \times 10^{11} \mathrm{Pa}\)

A Walk in the Sun. Consider a poor lost soul walking at 5 \(\mathrm{km} / \mathrm{h}\) on a hot day in the desert, wearing only a bathing suit. This person's skin temperature tends to rise due to four mechanisms: (i) energy is generated by metabolic reactions in the body at a rate of \(280 \mathrm{W},\) and almost all of this energy is con- verted to heat that flows to the skin; (ii) heat is delivered to the skin by convection from the outside air at a rate equal to \(k^{\prime} A_{\text { skin }}\left(T_{\text { air }}-T_{\text { skin }}\right),\) where \(k^{\prime}\) is \(54 \mathrm{J} / \mathrm{h} \cdot \mathrm{C}^{\circ} \cdot \mathrm{m}^{2},\) the exposed skin area \(A_{\text { skin }}\) is \(1.5 \mathrm{m}^{2},\) the air temperature \(T_{\mathrm{air}}\) is \(47^{\circ} \mathrm{C},\) and the skin temperature \(T_{\text { skin }}\) is \(36^{\circ} \mathrm{C} ;\) (iii) the skin absorbs radiant energy from the sun at a rate of 1400 \(\mathrm{W} / \mathrm{m}^{2}\) ; (iv) the skin absorbs radiant energy from the environment, which has temperature \(47^{\circ} \mathrm{C}\) . (a) Calculate the net rate (in watts) at which the person's skin is heated by all four of these mechanisms. Assume that the emissivity of the skin is \(e=1\) and that the skin temperature is initially \(36^{\circ} \mathrm{C}\) . Which mechanism is the most important? (b) At what rate (in \(\mathrm{L} / \mathrm{h} )\) must perspiration evaporate from this person's skin to maintain a constant skin temperature? (The heat of vaporization of water at \(36^{\circ} \mathrm{C}\) is \(2.42 \times 10^{6} \mathrm{J} / \mathrm{kg} .\)) (c) Suppose instead the person is protected by light-colored clothing \((e \approx 0)\) so that the exposed skin area is only 0.45 \(\mathrm{m}^{2} .\) What rate of perspiration is required now? Discuss the usefulness of the traditional clothing worn by desert peoples.

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