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In 1993 the spacecraft Galileo sent an image (Fig. \(13-48)\) of asteroid 243 Ida and a tiny orbiting moon (now known as Dactyl), the first confirmed example of an asteroid-moon system. In the image, the moon, which is \(1.5 \mathrm{~km}\) wide, is \(100 \mathrm{~km}\) from the center of the asteroid, which is \(55 \mathrm{~km}\) long. Assume the moon's orbit is circular with a period of \(27 \mathrm{~h}\). (a) What is the mass of the asteroid? (b) The volume of the asteroid, measured from the Galileo images, is \(14100 \mathrm{~km}^{3}\). What is the density (mass per unit volume) of the asteroid?

Short Answer

Expert verified
The mass of the asteroid is approximately \(4.2 \times 10^{16}\) kg. Its density is \(2.98 \times 10^{12}\) kg/m³.

Step by step solution

01

Identify Given Values

The exercise provides specific measurements: the moon is 1.5 km wide and 100 km from the center of the asteroid. The asteroid, Ida, is 55 km long, and the orbital period of the moon is 27 hours. The volume of the asteroid is given as 14100 km³.
02

Calculate Orbital Velocity

Convert the orbital period of the moon from hours to seconds: 27 hours = 27 × 3600 = 97200 seconds. The radius of the orbit, r, is 100 km, which is 100,000 meters. The orbital velocity, v, of the moon is given by the formula \( v = \frac{2\pi r}{T} \). Calculate v:\[ v = \frac{2 \cdot \pi \cdot 100,000}{97200} \approx 6.47 \, \text{m/s} \]
03

Apply Gravitational Formula

Use the formula for gravitational force to solve for the mass of the asteroid. The gravitational force providing the centripetal force is given by \( F = \frac{mv^2}{r} = G\frac{Mm}{r^2} \), where M is the mass of the asteroid, m is the mass of the moon (which cancels out), G is the gravitational constant (\(6.674 \times 10^{-11} \, \text{Nm}^2/\text{kg}^2\)), and r is the orbit radius. Rearrange to solve for M:\[ M = \frac{v^2 r}{G} \]Substitute known values:\[ M = \frac{(6.47)^2 \cdot 100,000}{6.674 \times 10^{-11}} \approx 4.2 \times 10^{16} \, \text{kg} \]
04

Calculate Density

Density, \( \rho \), is calculated using the formula \( \rho = \frac{M}{V} \), where M is the mass of the asteroid and V is its volume. Substitute the mass and volume:\[ \rho = \frac{4.2 \times 10^{16}}{1.41 \times 10^{4}} \approx 2.98 \times 10^{12} \, \text{kg/m}^3 \]

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Key Concepts

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

Asteroid-Moon System
In the vastness of space, not only do planets have moons, but so do some asteroids. An asteroid-moon system occurs when a small moon, often just a minor rock in comparison to larger bodies, orbits an asteroid. The first confirmed asteroid with its own moon was discovered in 1993 when Galileo spacecraft captured an image of Asteroid 243 Ida and its moon, Dactyl.

This discovery brought a new understanding of how celestial bodies can interact in space. The system is quite similar to the Earth-Moon system, but on a much smaller scale. Similar principles of gravitational force and orbital mechanics apply. Scientists study these systems to understand more about the formation and behavior of asteroids, which can differ from more extensive planetary systems.

Understanding asteroid-moon systems can help us learn more about asteroid compositions, positing that some moons might form from debris following collisions. Additionally, such systems can provide crucial insights into the history and evolution of our solar system.
Orbital Mechanics
Orbital mechanics is the study of the motion of celestial bodies subject to gravitational forces. It's a branch of physics that helps explain how objects, like the moon Dactyl, orbit around an asteroid.

An essential aspect of orbital mechanics is understanding how gravitational forces create the centripetal force that keeps a moon in orbit. The circular path of an orbiting body results from a constant balance between its velocity and the gravitational pull of the more massive body it's orbiting. In our example, the asteroid Ida's gravitational force is responsible for keeping its moon, Dactyl, in a stable orbit.

Calculations involving orbital mechanics often use Kepler's laws and Newton's law of universal gravitation to determine things like orbital period, velocity, and forces involved. For instance, when calculating the mass of an asteroid based on its moon's orbit, you'll use the formula: \[ M = \frac{v^2 r}{G} \] where \( v \) is the velocity, \( r \) is the orbit's radius, and \( G \) is the gravitational constant. This allows scientists to estimate the mass of the asteroid without landing on it. As you can see, orbital mechanics is both a challenging and fascinating field of study.
Density Calculation
Density plays a crucial role in understanding the physical characteristics of celestial bodies. In simple terms, density is the mass of an object divided by its volume. It's a fundamental property that tells us about the material composition of a body.

For instance, knowing the asteroid Ida's density helps determine if it's made of metal, rock, or a combination. To find density, you use the equation:\[ \rho = \frac{M}{V} \]where \( \rho \) represents density, \( M \) is mass, and \( V \) is volume.

For the asteroid 243 Ida, the mass is calculated using data from its moon's orbit, and the volume is determined from Galileo's images. By substituting these values into the density equation, you can estimate the density of the asteroid.

This estimation helps scientists infer the asteroid's composition and internal structure. High-density values may indicate a metallic composition, while lower densities could suggest rock-and-dust mixtures. These inferences are crucial for planning space missions, especially if mining asteroids for resources becomes a future option.

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