/*! 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 92 Our Sun is \(2.3 \times 10^{4}\)... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Our Sun is \(2.3 \times 10^{4}\) ly (light-years) from the center of our Milky Way galaxy and is moving in a circle around that center at a speed of \(250 \mathrm{~km} / \mathrm{s}\). (a) How long does it take the Sun to make one revolution about the galactic center? (b) How many revolutions has the Sun completed since it was formed about \(4.5 \times 10^{9}\) years ago?

Short Answer

Expert verified
(a) Approximately 1.733 x 10^8 years for one revolution. (b) The Sun has completed about 26 revolutions since formation.

Step by step solution

01

Convert Light-years to Kilometers

First, we need to convert the distance from light-years to kilometers for consistency. We know that:\[ 1 \text{ light-year (ly)} = 9.461 \times 10^{12} \text{ km} \]Therefore, the distance of the Sun from the galactic center is:\[ 2.3 \times 10^{4} \text{ ly} \times 9.461 \times 10^{12} \frac{\text{km}}{\text{ly}} = 2.17603 \times 10^{17} \text{ km} \]
02

Calculate the Circumference of the Sun's Orbit

Since the Sun moves in a circular path around the center of the Milky Way, we can calculate the circumference \(C\) of its orbit using the formula for the circumference of a circle:\[ C = 2 \pi \times \text{radius} \]Thus,\[ C = 2 \pi \times 2.17603 \times 10^{17} \text{ km} \approx 1.36743 \times 10^{18} \text{ km} \]
03

Find the Time for One Revolution

The time \(T\) it takes for the Sun to complete one revolution can be found using the formula \(T = \frac{\text{circumference}}{\text{speed}}\):\[ T = \frac{1.36743 \times 10^{18} \text{ km}}{250 \text{ km/s}} \approx 5.46972 \times 10^{15} \text{ s} \]
04

Convert Time to Years

Convert the time from seconds to years. We know there are \(3600 \times 24 \times 365.25\) seconds in a year (considering leap years as well), so:\[ T = \frac{5.46972 \times 10^{15} \text{ s}}{3600 \times 24 \times 365.25} \approx 1.733 \times 10^{8} \text{ years} \]
05

Calculate Number of Revolutions

With the Sun having been formed approximately \(4.5 \times 10^{9}\) years ago, the number of revolutions \(N\) it has completed is:\[ N = \frac{4.5 \times 10^{9} \text{ years}}{1.733 \times 10^{8} \text{ years/revolution}} \approx 25.96 \]
06

Rounding to Find a Suitable Answer

Since the number of revolutions is a practical concept, we round it to the nearest whole number. Therefore, the Sun has completed approximately 26 revolutions around the galactic center.

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 91Ó°ÊÓ!

Key Concepts

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

Orbital Motion
Understanding orbital motion is fundamental when discussing the dynamics of galaxies. Our Sun's orbit around the Milky Way is similar to how Earth orbits the Sun, but on a much larger scale. In this scenario, the Sun moves in a nearly circular orbit, maintained by the gravitational pull of the massive galactic center.
As the Sun travels along this path, it maintains a consistent speed, known as its orbital speed, which is given as 250 km/s. This constant speed suggests a stable orbit devoid of significant external disturbances.
This concept of orbital motion helps us compute how long the Sun takes to make one complete trip around the galaxy by considering the extensive distance of its path, known as the orbital circumference.
Light-year Conversion
A light-year is a unit of astronomical distance used to express how far light travels in one year. To evaluate the Sun's galactic journey, it's crucial to convert light-years into kilometers, a more familiar unit of distance. One can accomplish this using the conversion factor: \(1 \text{ ly} = 9.461 \times 10^{12} \text{ km}\).
For this problem, we start with the Sun being 23,000 light-years away from the galaxy's center. By multiplying this figure by the conversion factor, you can calculate the Sun's distance in kilometers, resulting in approximately \(2.17603 \times 10^{17} \text{ km}\).
This conversion allows for further calculations involving speeds in km/s and ultimately in determining the time it takes for the Sun to orbit the Milky Way.
Circumference Calculation
To find out how long it takes the Sun to orbit the center of the Milky Way, we need to know the complete path or circumference of this orbit. The formula for the circumference of a circle \(C = 2 \pi \times \text{radius}\) helps us with this computation.
Given that the orbital radius is the distance from the Sun to the galactic center, which we have calculated to be approximately \(2.17603 \times 10^{17} \text{ km}\), inserting this into the formula gives us the circumference:
\[ C = 2 \pi \times 2.17603 \times 10^{17} \approx 1.36743 \times 10^{18} \text{ km} \]
This calculation signifies the total distance over which the Sun travels in one full orbit, a crucial figure for determining orbital period.
Time Conversion to Years
Once the distance and speed are known, the next step is finding the time it takes for the Sun to complete one orbit. The formula \(T = \frac{\text{circumference}}{\text{speed}}\) gives us the time in seconds.
Inserting the values, we find the time is approximately \(5.46972 \times 10^{15} \text{ seconds}\).
However, seconds are not very practical for expressing such vast time spans, so a conversion to years is needed.
We know a year has approximately 31,557,600 seconds on average, accounting for leap years. Hence, when these seconds are converted into years, we find:
\[ T = \frac{5.46972 \times 10^{15} \text{ s}}{31,557,600} \approx 1.733 \times 10^{8} \text{ years} \]
Thus, it takes roughly 173 million years for the Sun to circle the galactic center once.

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

Attached to each end of a thin steel rod of length \(1.20 \mathrm{~m}\) and mass \(6.40 \mathrm{~kg}\) is a small ball of mass \(1.06 \mathrm{~kg} .\) The rod is constrained to rotate in a horizontal plane about a vertical axis through its midpoint. At a certain instant, it is rotating at \(39.0 \mathrm{rev} / \mathrm{s}\). Because of friction, it slows to a stop in \(32.0\) s Assuming a constant retarding torque due to friction, compute (a) the angular acceleration, (b) the retarding torque, (c) the total energy transferred from mechanical energy to thermal energy by friction, and (d) the number of revolutions rotated during the \(32.0 \mathrm{~s}\) (e) Now suppose that the retarding torque is known not to be constant. If any of the quantities (a), (b), (c), and (d) can still be computed without additional information, give its value.

A diver makes \(2.5\) revolutions on the way from a \(10-\mathrm{m}\) -high platform to the water. Assuming zero initial vertical velocity, find the average angular velocity during the dive.

(a) Show that the rotational inertia of a solid cylinder of mass \(M\) and radius \(R\) about its central axis is equal to the rotational inertia of a thin hoop of mass \(M\) and radius \(R / \sqrt{2}\) about its central axis. (b) Show that the rotational inertia \(I\) of any given body of mass \(M\) about any given axis is equal to the rotational inertia of an equivalent hoop about that axis, if the hoop has the same mass \(M\) and a radius \(k\) given by $$ k=\sqrt{\frac{I}{M}} $$ The radius \(k\) of the equivalent hoop is called the radius of gyration of the given body.

In Fig. 10-31, wheel \(A\) of radius \(r_{A}=10 \mathrm{~cm}\) is coupled by belt \(B\) to wheel \(C\) of radius \(r_{C}=25 \mathrm{~cm}\). The angular speed of wheel \(A\) is increased from rest at a constant rate of \(1.6 \mathrm{rad} / \mathrm{s}^{2}\). Find the time needed for wheel \(C\) to reach an angular speed of 100 rev/min, assuming the belt does not slip. (Hint: If the belt does not slip, the linear speeds at the two rims must be equal.)

The masses and coordinates of four particles are as follows: \(50 \mathrm{~g}, x=2.0 \mathrm{~cm}, y=2.0 \mathrm{~cm} ; 25 \mathrm{~g}, x=0, y=4.0 \mathrm{~cm} ; 25 \mathrm{~g}\), \(x=-3.0 \mathrm{~cm}, y=-3.0 \mathrm{~cm} ; 30 \mathrm{~g}, x=-2.0 \mathrm{~cm}, y=4.0 \mathrm{~cm} .\) What are the rotational inertias of this collection about the (a) \(x\), (b) \(y\), and (c) \(z\) axes? (d) Suppose that we symbolize the answers to (a) and (b) as \(A\) and \(B\), respectively. Then what is the answer to (c) in terms of \(A\) and \(B ?\)

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.