/*! 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 24 The star Lalande 21185 was found... [FREE SOLUTION] | 91Ó°ÊÓ

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The star Lalande 21185 was found in 1996 to have two planets in roughly circular orbits, with periods of 6 and 30 years. What is the ratio of the two planets' orbital radii?

Short Answer

Expert verified
The ratio of the orbital radii is approximately 1:2.924.

Step by step solution

01

Understanding Kepler's Third Law

According to Kepler's Third Law of Planetary Motion, the square of the orbital period of a planet is directly proportional to the cube of the semi-major axis of its orbit. Mathematically, this can be expressed as \(T^2 \propto a^3\), where \(T\) is the orbital period and \(a\) is the semi-major axis (radius for circular orbits).
02

Calculating the Ratio of Period Squared

Given the periods of the planets are 6 years and 30 years, we first calculate the ratio of their periods squared: \(\left(\frac{T_1}{T_2}\right)^2 = \left(\frac{6}{30}\right)^2 = \left(\frac{1}{5}\right)^2 = \frac{1}{25}\).
03

Relating Period Ratio to Orbital Radius Ratio

Since \(T^2 \propto a^3\), it follows that \(\left(\frac{T_1}{T_2}\right)^2 = \left(\frac{a_1}{a_2}\right)^3\). Therefore, \(\frac{1}{25} = \left(\frac{a_1}{a_2}\right)^3\).
04

Solving for Orbital Radius Ratio

To find the ratio \(\frac{a_1}{a_2}\), take the cube root of \(\frac{1}{25}\): \(\frac{a_1}{a_2} = \left(\frac{1}{25}\right)^{1/3} \approx \frac{1}{2.924}\).
05

Simplifying the Ratio

Rounding to a simple ratio for clarity, \(\frac{1}{2.924}\) is approximately 0.342, which can be expressed as \(a_1 : a_2 = 1 : 2.924\).

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Key Concepts

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

Planetary Motion
Planetary motion refers to the movement of planets around a star. This is a fundamental principle observed by Johannes Kepler in the 17th century and is described through his three laws of planetary motion. These laws help us understand how planets, such as those in our Solar System or around other stars, interact with the gravitational forces exerted by the star they orbit. The path taken by a planet is typically elliptical, with the star at one of the two foci, though circular orbits can be approximated as well. Understanding planetary motion allows scientists to predict the position of a planet at any given time, crucial for everything from sending spacecraft across the solar system to understanding the potential for life on other planets. This forms the foundation of much of modern astronomy and space exploration.
Orbital Period
The orbital period of a planet is the time it takes to complete one full orbit around its star. This is a key concept in understanding planetary motion. The length of this period can vary widely, depending on the distances involved and the gravitational forces at play. In the case of the Lalande 21185 star system, one planet has an orbital period of 6 years, while another takes 30 years. This period reflects how the gravitational pull from the star balances with the planet's velocity to maintain its orbit. For astronomers, determining the orbital period is essential for characterizing the dynamics of planetary systems and for predicting future positions of the planets. This helps in planning missions and understanding the conditions that might exist on those planets.
Semi-Major Axis
The semi-major axis is a measure used in astronomy to describe the size of an elliptical orbit. It is essentially the average distance from the planet to the star, which for nearly circular orbits like the planets of Lalande 21185, can also be referred to as the orbital radius. This axis plays a key role in determining the orbital period of a planet. According to Kepler's Third Law, the square of the orbital period is proportional to the cube of the semi-major axis. Therefore, knowing the semi-major axis helps astronomers calculate and predict the orbital characteristics of celestial bodies. This is particularly important in determining the habitability of exoplanets, as the semi-major axis affects the planet's climate and potential to support life.
Orbital Radius
The orbital radius, often used interchangeably with the semi-major axis for circular or nearly circular orbits, represents the distance from the center of the planet's orbit to the star. In our context, understanding this radius is crucial, as it helps determine other planetary characteristics like speed and gravitational relationship with the host star. For Lalande 21185's planets, we used the orbital radius in the context of Kepler's Third Law to find the relative sizes of the orbits. Scientists use this concept to measure how far away a planet is from its star, affecting everything from surface temperatures to potential atmospheric conditions. Accurately measuring the orbital radius is important for understanding both planetary climates and the challenges of space exploration.
Mathematical Proportionality
Mathematical proportionality in the context of Kepler's laws is significant for understanding relationships in planetary motion. Kepler's Third Law tells us that there is a proportional relationship between a planet's orbital period squared and its semi-major axis cubed. This is expressed mathematically as \(T^2 \propto a^3\), highlighting how periods and distances relate in a predictable manner. For the planets in the Lalande 21185 system, this relationship allowed us to compare their orbital radii based on their orbital periods. By knowing two of these variables, the third can be deduced, showcasing how mathematics is integral in interpreting astronomical phenomena. This proportionality is foundational in fields ranging from astrophysics to celestial mechanics, providing a framework to understand how space systems operate.

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Most popular questions from this chapter

Explain in terms of conservation of energy why sweating cools your body, even though the sweat is at the same temperature as your body. Describe the forms of energy involved in this energy transformation. Why don't you get the same cooling effect if you wipe the sweat off with a towel? Hint: The sweat is evaporating.

(a) A circular hoop of mass \(m\) and radius \(r\) spins like a wheel while its center remains at rest. Let \(\omega\) (Greek letter omega) be the number of radians it covers per unit time, i.e., \(\omega=2 \pi / T\), where the period, \(T\), is the time for one revolution. Show that its kinetic energy equals \((1 / 2) m \omega^{2} r^{2}\) (b) Show that the answer to part a has the right units. (Note that radians aren't really units, since the definition of a radian is a unitless ratio of two lengths.) (c) If such a hoop rolls with its center moving at velocity \(v\), its kinetic energy equals \((1 / 2) m v^{2}\), plus the amount of kinetic energy found in part a. Show that a hoop rolls down an inclined plane with half the acceleration that a frictionless sliding block would have.

The following table gives the amount of energy required in order to heat, melt, or boil a gram of water. $$\begin{array}{ll}\hline \text { heat } 1 \mathrm{~g} \text { of ice by } 1^{\circ} \mathrm{C} & 2.05 \mathrm{~J} \\ \text { melt } 1 \mathrm{~g} \text { of ice } & 333 \mathrm{~J} \\ \text { heat } 1 \mathrm{~g} \text { of liquid by } 1^{\circ} \mathrm{C} & 4.19 \mathrm{~J} \\ \text { boil } 1 \mathrm{~g} \text { of water } & 2500 \mathrm{~J} \\ \text { heat } 1 \mathrm{~g} \text { of steam by } 1^{\circ} \mathrm{C} & 2.01 \mathrm{~J} \\ \hline\end{array}$$ (a) How much energy is required in order to convert \(1.00 \mathrm{~g}\) of ice at \(-20^{\circ} \mathrm{C}\) into steam at \(137^{\circ} \mathrm{C}\) ? (answer check available at lightandmatter.com) (b) What is the minimum amount of hot water that could melt \(1.00 \mathrm{~g}\) of ice? (answer check available at lightandmatter.com)

(a) You release a magnet on a tabletop near a big piece of iron, and the magnet leaps across the table to the iron. Does the magnetic energy increase, or decrease? Explain. (b) Suppose instead that you have two repelling magnets. You give them an initial push towards each other, so they decelerate while approaching each other. Does the magnetic energy increase, or decrease? Explain.

Object A has a kinetic energy of \(13.4\) J. Object B has a mass that is greater by a factor of \(3.77\), but is moving more slowly by a factor of \(2.34\). What is object B's kinetic energy? (solution in the pdf version of the book)

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