Mars has a mass of about \(6.42 \times 10^{23} \mathrm{kg} .\) The length of a day on Mars is \(24 \mathrm{h}\) and 37 min, a little longer than the length of a day on Earth. Your task is to put a satellite into a circular orbit around Mars so that it stays above one spot on the surface, orbiting Mars once each Mars day. At what distance from the center of the planet should you place the satellite?

Short Answer

Expert verified
Answer: The satellite should be placed approximately 20,430,000 meters (20,430 km) from the center of Mars.

Step by step solution

01

Gravitational force formula

The gravitational force between two objects is given by Newton's law of gravitation. The formula for this force is: \(F = G \frac{m_1 m_2}{r^2}\) where \(F\) is the force, \(G\) is the gravitational constant \(6.674 \times 10^{-11}\,\text{N}\,\text{m}^2\,\text{kg}^{-2}\), \(m_1\) and \(m_2\) are the masses of the two objects (in this case Mars and the satellite), and \(r\) is the distance between their centers.
02

Centripetal force formula

The centripetal force acting on the satellite is given by the formula: \(F_c = m\,a = m\,\frac{v^2}{r}\) Where \(m\) is the mass of the satellite, \(a\) is the centripetal acceleration, and \(v\) is the orbital velocity.
03

Equate gravitational force and centripetal force

The gravitational force is the only force acting on the satellite, so it must be equal to the centripetal force: \(F = F_c\) \(G \frac{m_1 m_2}{r^2} = m\,\frac{v^2}{r}\)
04

Express orbital velocity in terms of the orbital period

To find the orbital velocity, we use the formula for the circumference of the orbit divided by the orbital period: \(v = \frac{2 \pi r}{T}\) Where \(T\) is the orbital period, which is equal to the length of a Mars day (24 hours and 37 minutes). We want the orbital period to be the same as a day on Mars, so we need to convert the hours and minutes into seconds: \(T = (24 * 3600) + (37 * 60) \approx 88740\,s\) Now we substitute this expression for \(v\) back into the equation from Step 3: \(G \frac{m_1 m_2}{r^2} = m\,\frac{(2 \pi r / T)^2}{r}\)
05

Solve for the distance from the center of Mars

Now we can simplify the equation and solve for \(r\): \(G \frac{m_1 m_2}{r^2} = m\,\frac{(4 \pi^2 r^2) / T^2}{r}\) Notice that the mass of the satellite \(m\) cancels out, so we're left with: \(G \,m_1 = \frac{4 \pi^2 r^3}{T^2 r}\) Now we can solve for the distance \(r\): \(r^3=\frac{G\, m_1\, T^2}{4\,\pi^2}\) \(r=\sqrt[3]{\frac{G\, m_1\, T^2}{4\,\pi^2}}\) Plugging in the values for Mars mass, \(G\), and \(T\): \(r=\sqrt[3]{\frac{6.674 \times 10^{-11}\,\text{N}\,\text{m}^2\,\text{kg}^{-2} \times 6.42 \times 10^{23}\,\text{kg} \times (88740\,s)^2}{4\,\pi^2}}\) Evaluating this expression gives: \(r \approx 20430000\,\text{m}\) So the satellite should be placed approximately 20,430,000 meters from the center of Mars to have a circular orbit with a period equal to one Mars day.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Verify that all three expressions for radial acceleration $\left(v \omega, v^{2} / r, \text { and } \omega^{2} r\right)$ have the correct dimensions for an acceleration.
Objects that are at rest relative to the Earth's surface are in circular motion due to Earth's rotation. (a) What is the radial acceleration of an object at the equator? (b) Is the object's apparent weight greater or less than its weight? Explain. (c) By what percentage does the apparent weight differ from the weight at the equator? (d) Is there any place on Earth where a bathroom scale reading is equal to your true weight? Explain.
A carnival swing is fixed on the end of an 8.0 -m-long beam. If the swing and beam sweep through an angle of \(120^{\circ},\) what is the distance through which the riders move?
A person rides a Ferris wheel that turns with constant angular velocity. Her weight is \(520.0 \mathrm{N}\). At the top of the ride her apparent weight is \(1.5 \mathrm{N}\) different from her true weight. (a) Is her apparent weight at the top \(521.5 \mathrm{N}\) or \(518.5 \mathrm{N} ?\) Why? (b) What is her apparent weight at the bottom of the ride? (c) If the angular speed of the Ferris wheel is \(0.025 \mathrm{rad} / \mathrm{s},\) what is its radius?
In a Beams ultracentrifuge, the rotor is suspended magnetically in a vacuum. Since there is no mechanical connection to the rotor, the only friction is the air resistance due to the few air molecules in the vacuum. If the rotor is spinning with an angular speed of $5.0 \times 10^{5} \mathrm{rad} / \mathrm{s}$ and the driving force is turned off, its spinning slows down at an angular rate of \(0.40 \mathrm{rad} / \mathrm{s}^{2} .\) (a) How long does the rotor spin before coming to rest? (b) During this time, through how many revolutions does the rotor spin?
See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free