Chapter 4: Problem 21
Verify that the gravitational force \(-G M m \hat{\mathbf{r}} / r^{2}\) on a point mass \(m\) at \(\mathbf{r},\) due to a fixed point mass \(M\) at the origin, is conservative and calculate the corresponding potential energy.
Short Answer
Expert verified
The gravitational force is conservative; potential energy is \( V(r) = -\frac{GMm}{r} \).
Step by step solution
01
Identify the Gravitational Force
The gravitational force on a point mass \( m \) at position \( \mathbf{r} \) due to another fixed point mass \( M \) at the origin is given by: \( \mathbf{F} = -\frac{GMm}{r^2} \hat{\mathbf{r}} \), where \( G \) is the gravitational constant, and \( \hat{\mathbf{r}} \) is the unit vector in the direction of \( \mathbf{r} \).
02
Check for Conservatism of the Force
A force field is conservative if the curl of the force field is zero. For a central force like gravity, \( \mathbf{F} = -abla V \), where \( V \) is the potential energy. We express the curl condition: \( abla \times \mathbf{F} = 0 \). In Cartesian coordinates, the curl of a radial force field like this is always zero, confirming the force is conservative.
03
Determine the Potential Energy
For a conservative force, potential energy \( V \) is found by integrating the force with respect to \( r \). Using the relation: \( \mathbf{F} = -abla V \), integrate \( F \) with respect to \( r \): \( V = - \int \mathbf{F} \cdot d\mathbf{r} = - \int -\frac{GMm}{r^2} dr = -\left[-\frac{GMm}{r}\right] + C \), where \( C \) is a constant of integration.
04
Finalize the Potential Energy Expression
It's common to set the potential energy at infinity to zero, \( V(\infty) = 0 \). Thus, \( C = 0 \), and we have the gravitational potential energy as: \( V(r) = -\frac{GMm}{r} \).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Gravitational Force
Gravitational force is a fundamental interaction that pulls objects with mass towards each other. In the formula for gravitational force between two masses, \[ \mathbf{F} = -\frac{GMm}{r^2} \hat{\mathbf{r}} \]
Understanding gravitational force gives insight into fields like astronomy and physics, explaining phenomena from apple falling to planetary orbits.
- \( G \) is the gravitational constant, a value that represents the strength of gravity universally.
- \( M \) and \( m \) are the masses of the two objects involved.
- \( r \) is the distance between the centers of these two masses.
- \( \hat{\mathbf{r}} \) is a unit vector pointing from the mass \( M \) to the mass \( m \).
Understanding gravitational force gives insight into fields like astronomy and physics, explaining phenomena from apple falling to planetary orbits.
Potential Energy
Potential energy represents the stored energy of an object due to its position relative to other objects. In the context of gravitational force, we often calculate it by finding the work done against or by gravitational forces. The potential energy \( V \) due to gravity is given by:\[ V(r) = -\frac{GMm}{r} \]
Recognizing how potential energy operates allows prediction and mapping of motion under gravity, essential for many real-world applications.
- This form arises because the gravitational force is conservative, meaning the work done around any closed path is zero.
- Potential energy is defined up to an arbitrary constant, which often is chosen such that \( V(\infty) = 0 \), leading to no constant in our final expression.
Recognizing how potential energy operates allows prediction and mapping of motion under gravity, essential for many real-world applications.
Integral Calculus
Integral calculus is a mathematical branch used to calculate quantities like areas under curves, among other applications. When dealing with forces and energies, integration helps in determining quantities such as potential energy.
\[ V = - \int \mathbf{F} \cdot d\mathbf{r} \]This integral signifies accumulation over the path from infinity to a distance \( r \), effectively measuring the total effect of the force over that distance.
Calculating Potential Energy
In our context, we used integration to find the potential energy due to a gravitational force. Specifically, the relationship between force \( \mathbf{F} \) and potential energy \( V \) can be expressed as:\[ V = - \int \mathbf{F} \cdot d\mathbf{r} \]This integral signifies accumulation over the path from infinity to a distance \( r \), effectively measuring the total effect of the force over that distance.
The Importance of the Integrals
- The process of integration helps translate local force interactions into global energy levels.
- Especially for conservative forces, such as gravity, it ensures that energy is conserved and allows for predictions in movement and energy requirements.