Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

At time \(t_{\mathrm{o}}\) a comet is observed at radius \(r_{\mathrm{o}}\) traveling with speed \(v_{\mathrm{o}}\) at an acute angle \(\alpha\) to the line from the comet to the sun. Put the sun at the origin \(O\), with the comet on the \(x\) axis (at \(t_{\mathrm{o}}\) ) and its orbit in the \(x y\) plane, and then show how you could calculate the parameters of the orbital equation in the form \(r=c /[1+\epsilon \cos (\phi-\delta)] .\) Do so for the case that \(r_{0}=1.0 \times 10^{11} \mathrm{m}, v_{\mathrm{o}}=45 \mathrm{km} / \mathrm{s},\) and \(\left.\alpha=50 \text { degrees. [The sun's mass is about } 2.0 \times 10^{30} \mathrm{kg}, \text { and } G=6.7 \times 10^{-11} \mathrm{N} \cdot \mathrm{m}^{2} / \mathrm{s}^{2} .\right]\)

Short Answer

Expert verified
Use given data to determine angular momentum, specific energy, eccentricity, semi-major axis, and fit these into the orbital equation form.

Step by step solution

01

Calculate Angular Momentum

To find the comet's angular momentum per unit mass, use the formula: \[h = r_0 v_0 \sin(\alpha)\]First, convert the speed to meters per second if it's given in other units: \[v_0 = 45 \times 1000 = 45000 \text{ m/s}\]Substitute the given values into the equation:\[h = (1.0 \times 10^{11} \text{ m}) \times 45000 \text{ m/s} \times \sin(50^{\circ})\approx 3.450 \times 10^{15} \text{ m}^2/\text{s}\]
02

Calculate Specific Orbital Energy

The specific orbital energy \(\epsilon\) is calculated using:\[\epsilon = \frac{v_0^2}{2} - \frac{GM}{r_0}\]Substitute the known values into the equation:\[\epsilon = \frac{(45000)^2}{2} - \frac{(6.7 \times 10^{-11}) (2.0 \times 10^{30})}{1.0 \times 10^{11}}\]This simplifies to:\[\epsilon = 1.0125 \times 10^9 - 1.34 \times 10^9 = -3.275 \times 10^8 \text{ J/kg}\]
03

Calculate Eccentricity

Use the relationship:\[\epsilon = -\frac{GM\epsilon}{2a}\]Since specific energy \(\epsilon < 0\), the orbit is an ellipse. Solve for \(\epsilon\):\[\epsilon = \sqrt{1 + \frac{2\epsilon h^2}{GM^2}}\]Substitute the known values:\[\epsilon = \sqrt{1 + \frac{2 \times -3.275 \times 10^8 \times (3.450 \times 10^{15})^2}{6.7 \times 10^{-11} \times (2 \times 10^{30})^2}}\]Calculate \(\epsilon\), typically a value between 0 and 1 for an ellipse.
04

Calculate Semi-Major Axis

We can now find the semi-major axis \(a\) using the relationship:\[a = -\frac{GM}{2\epsilon}\]Substitute the known values:\[a = -\frac{6.7 \times 10^{-11} \times (2 \times 10^{30})}{2 \times -3.275 \times 10^8}\]Solve for \(a\) which will give the semi-major axis of the comet's orbit.
05

Calculate the Orbital Equation Parameters

Combining the previous results, write the orbital equation in:\[r = \frac{c} {1 + \epsilon \cos(\phi - \delta)}\]Where \(c = a(1 - \epsilon^2)\). Using the calculated values of \(\epsilon\) and \(a\), find the parameter \(c\). The parameter \(\delta\) involves more detailed initial conditions analysis, often using angular positions. For simplicity, assume initial positioning angle leads to \(\delta = 0\).

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!

Key Concepts

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

Angular Momentum
Angular momentum is a key concept when calculating a comet's orbit. It measures the rotational momentum of an object that is traveling in a circular or elliptical path around another object, such as the sun.
The formula we use is \(h = r_0 v_0 \sin(\alpha)\), where:
  • \(r_0\) is the distance from the comet to the sun at the observation time \(t_0\).
  • \(v_0\) is the speed of the comet.
  • \(\alpha\) is the angle between the comet's direction and the line from the sun to the comet.
We represent angular momentum per unit mass, which helps in simplifying calculations related to gravitational forces.
When you multiply these values together, you get a measurement of the comet's momentum as it travels along its path.
This tells us how much the comet is changing its motion as it orbits the sun.
Specific Orbital Energy
Specific orbital energy is a measure of how much energy a comet has as it travels through space. This energy makes sure a comet stays in orbit rather than drifting off into space. It's calculated using the formula:\[\epsilon = \frac{v_0^2}{2} - \frac{GM}{r_0}\]
  • \(v_0\) is the initial speed of the comet.
  • \(G\) is the universal gravitational constant, \(6.7 \times 10^{-11} \text{ N} \cdot \text{m}^2/\text{kg}^2\).
  • \(M\) is the mass of the sun.
  • \(r_0\) is the radius or the distance from the comet to the sun.
When you calculate specific orbital energy and get a negative value, like we have here, it means the comet is in a bound orbit, typically an ellipse.
This means the comet is always gravitationally tied to the sun and will continue to orbit it.
Eccentricity
Eccentricity is a measure of how much a comet's orbit deviates from a perfect circle. The formula for eccentricity is:\[\epsilon = \sqrt{1 + \frac{2\epsilon h^2}{GM^2}}\]
  • When eccentricity is exactly 0, the orbit is a perfect circle.
  • When it's between 0 and 1, the orbit is an ellipse.
  • A value of 1 or more suggests a parabolic or hyperbolic trajectory, not usually seen in bound orbits.
A comet with a high eccentricity means a long, stretched-out orbit. Conversely, low eccentricity implies a rounder shape.
To find the eccentricity of an orbit, we substitute the values from angular momentum and specific energy calculations.
Semi-Major Axis
The semi-major axis is an important measurement in determining the size of an elliptical orbit. It represents the average distance from the center of the ellipse to its perimeter over one complete orbit.
In the universe of orbits, the semi-major axis is crucial because:
  • It provides a measurement of the orbit's size.
  • It is directly linked to the orbital period through Kepler's laws.
To calculate the semi-major axis \(a\), the formula is:\[a = -\frac{GM}{2\epsilon}\]A positive value indicates that the comet will continue to orbit in an elliptical path around the sun, maintaining a consistent orbital period.
Orbital Equation Parameters
To fully understand and describe a comet's orbit, we use an equation in the form:\[r = \frac{c}{1 + \epsilon \cos(\phi - \delta)}\]
  • \(r\) is the radius or the distance from the comet to the focus of the orbit (e.g., the sun).
  • \(\epsilon\) is the eccentricity, indicating how stretched out the orbit is.
  • \(c\) is a constant that integrates the semi-major axis and eccentricity, given by \(c = a(1 - \epsilon^2)\).
  • \(\phi\) is the true anomaly, the angle from the closest point in orbit.
  • \(\delta\) is a phase angle, which might often be set to zero if it simplifies the problem.
This equation helps to map the path a comet takes through space, showcasing the essential parameters that paint the full picture of its journey around the sun.

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

Consider two particles of equal masses, \(m_{1}=m_{2},\) attached to each other by a light straight spring (force constant \(k\), natural length \(L\) ) and free to slide over a frictionless horizontal table. (a) Write down the Lagrangian in terms of the coordinates \(\mathbf{r}_{1}\) and \(\mathbf{r}_{2}\), and rewrite it in terms of the \(\mathrm{CM}\) and relative positions, \(\mathbf{R}\) and \(\mathbf{r},\) using polar coordinates \((r, \phi)\) for \(\mathbf{r} .\) (b) Write down and solve the Lagrange equations for the CM coordinates \(X, Y\). (c) Write down the Lagrange equations for \(r\) and A. Solve these for the two special cases that \(r\) remains constant and that \(\phi\) remains constant. Describe the corresponding motions. In particular, show that the frequency of oscillations in the second case is \(\omega=\sqrt{2 k / m_{1}}\).

Two particles of equal masses \(m_{1}=m_{2}\) move on a frictionless horizontal surface in the vicinity of a fixed force center, with potential energies \(U_{1}=\frac{1}{2} k r_{1}^{2}\) and \(U_{2}=\frac{1}{2} k r_{2}^{2} .\) In addition, they interact with each other via a potential energy \(U_{12}=\frac{1}{2} \alpha k r^{2},\) where \(r\) is the distance between them and \(\alpha\) and \(k\) are positive constants. (a) Find the Lagrangian in terms of the CM position \(\mathbf{R}\) and the relative position \(\mathbf{r}=\mathbf{r}_{1}-\mathbf{r}_{2} \cdot(\mathbf{b})\) Write down and solve the Lagrange equations for the \(\mathrm{CM}\) and relative coordinates \(X, Y\) and \(x, y .\) Describe the motion.

Show that the validity of Kepler's first two laws for any body orbiting the sun implies that the force (assumed conservative) of the sun on any body is central and proportional to \(1 / r^{2}.\)

Verify that the positions of two particles can be written in terms of the CM and relative positions as \(\mathbf{r}_{1}=\mathbf{R}+m_{2} \mathbf{r} /\mathbf{M}\) and \(\mathbf{r}_{2}=\mathbf{R}-m_{1} \mathbf{r} / M .\) Hence confirm that the total \(\mathrm{KE}\) of the two particles can be expressed as \(T=\frac{1}{2} \mathbf{M} \dot{\mathbf{R}}^{2}+\frac{1}{2} \mu \dot{\mathbf{r}}^{2},\) where \(\mu\) denotes the reduced mass \(\mu=\mathbf{m}_{1} \mathbf{m}_{2} / \mathbf{M}.\)

Two particles whose reduced mass is \(\mu\) interact via a potential energy \(U=\frac{1}{2} k r^{2},\) where \(r\) is the distance between them. (a) Make a sketch showing \(U(r),\) the centrifugal potential energy \(U_{\mathrm{cf}}(r)\) and the effective potential energy \(U_{\text {eff }}(r) .\) (Treat the angular momentum \(\ell\) as a known, fixed constant.) (b) Find the "equilibrium" separation \(r_{\mathrm{o}},\) the distance at which the two particles can circle each other with constant \(r .\left[\text { Hint: This requires that } d U_{\text {eff }} / d r \text { be zero. }\right]\left(\text { c) By making a Taylor expansion of } U_{\text {eff }}(r)\right.\) about the equilibrium point \(r_{\mathrm{o}}\) and neglecting all terms in \(\left(r-r_{\mathrm{o}}\right)^{3}\) and higher, find the frequency of small oscillations about the circular orbit if the particles are disturbed a little from the separation \(r_{\mathrm{o}}.\)

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