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Halley's comet moves about the Sun in an elliptical orbit, with its closest approach to the Sun being \(0.59 \mathrm{~A} . \mathrm{U} .\) and its greatest distance being \(35 \mathrm{~A} . \mathrm{U}\). ( \(1 \mathrm{~A} . \mathrm{U}\). is the Earth-Sun distance). If the comet's speed at closest approach is \(54 \mathrm{~km} / \mathrm{s}\), what is its speed when it is farthest from the Sun? You may neglect any change in the comet's mass and assume that its angular momentum about the Sun is conserved.

Short Answer

Expert verified
The speed of Halley's comet when it is farthest from the Sun is given by \(v_2 = (54\,km/s \cdot 0.59\, A.U.) / 35\, A.U.\).

Step by step solution

01

Write down the conservation of angular momentum equation

Given that angular momentum \(L = m \cdot v \cdot r\) is conserved we can express this as: \(m_1 \cdot v_1 \cdot r_1 = m_2 \cdot v_2 \cdot r_2\). Where the subscripts 1 and 2 refer to the closest and farthest distances and speeds, respectively. In this problem, the mass of Halley's comet is constant so \(m_1\) equals \(m_2\), and the equation can be simplified further to: \(v_1 \cdot r_1 = v_2 \cdot r_2\).
02

Substitute known values into the equation

Now substitute the given values into this equation with \(v_1=54 \, km/s, r_1=0.59 \, A.U.\) and \(r_2=35 \, A.U.\) to get: \(54\,km/s \cdot 0.59\, A.U. = v_2 \cdot 35\, A.U.\). We need to solve this equation for \(v_2\), the speed of Halley's comet when it's farthest from the sun.
03

Solve for \(v_2\)

To do this, divide both sides of the equation by 35 A.U., this will isolate \(v_2\) on one side of the equation: \(v_2 = (54\,km/s \cdot 0.59\, A.U.) / 35\, A.U.\). Lastly, compute the right hand side which gives the numerical value of \(v_2\).

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Key Concepts

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

Halley's Comet Orbit
Halley's Comet, a well-known comet that visits the inner part of our solar system approximately every 76 years, is famous not only for its predictability but also for its highly elliptical orbit. This means the path it follows around the Sun is elongated, like an oval, rather than circular. In its dance with our star, the comet reaches a point nearest to the Sun, called perihelion, and a point farthest from the Sun, known as aphelion. These points are crucial when considering the speed of the comet; it travels fastest when it is closest to the Sun due to the stronger gravitational pull and slows down when it is farther away.

The Earth-Sun distance, which is about 149.6 million kilometers, is used as a standard unit of measurement in astronomy and is referred to as an Astronomical Unit (A.U.). Halley's Comet swings from a cozy 0.59 A.U. at perihelion to a distant 35 A.U. at aphelion. Understanding the comet's orbit enriches our grasp of celestial mechanics and helps in teaching us about the historical and predictive modeling of these fascinating celestial bodies.
Elliptical Orbit Physics
The physics of elliptical orbits is governed by the laws of celestial mechanics, particularly by Kepler's laws and the law of conservation of angular momentum. Unlike circular orbits where the orbital speed is constant, in an elliptical orbit, an object's speed varies depending on its distance from the focal point, in this case, the Sun.

When a comet is closest to the Sun (perihelion), it experiences the greatest gravitational force, causing it to move at its maximum speed. As it travels to the point farthest from the Sun (aphelion), the gravitational force weakens, hence the comet slows down. This speed change is a direct consequence of the conservation of angular momentum, a fundamental principle indicating that if no external torques act on a system, the total angular momentum remains constant. In simple terms, as Halley's Comet moves further from the Sun, it covers a greater distance but does so more slowly to maintain a balance in angular momentum.
Celestial Mechanics
Celestial mechanics is the branch of astronomy that deals with the motions and gravitational forces of celestial bodies. It lays the groundwork for understanding the orbits of planets, moons, comets, and other astronomical objects. Underpinning celestial mechanics are the conservation laws of motion, particularly the conservation of angular momentum, which is crucial in explaining why planets and comets orbit in the way that they do.

In our example involving Halley's Comet, we apply the principle of angular momentum conservation to find the comet’s speed at its farthest point from the Sun. Given that the angular momentum is the product of an object's mass, velocity, and the distance to the point about which it is rotating (in this case the Sun), a comet traveling a wider, more extended path at aphelion must move slower to ensure that the product of its mass, speed, and distance from the Sun remains consistent.

Without delving into complex calculations, these principles enable us to predict the movements of celestial objects with remarkable accuracy. Halley's comet, like clockwork, has allowed generations to witness its journey across our skies, all thanks to the unchanging laws of celestial mechanics.

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Most popular questions from this chapter

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