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Certain neutron stars (extremely dense stars) are believed to be rotating at about 1 rev \(/ \mathrm{s}\). If such a star has a radius of \(20 \mathrm{~km},\) what must be its minimum mass so that material on its surface remains in place during the rapid rotation?

Short Answer

Expert verified
The minimum mass is approximately \(1.85 \times 10^{27} \mathrm{kg}\).

Step by step solution

01

Understanding the Problem

We need to calculate the minimum mass of a neutron star so that the gravitational force can keep material on its surface in place despite the rapid rotation. We can relate this problem to the concept of centripetal force and gravitational force balancing each other.
02

Identify Known Quantities

We know the radius of the neutron star is \( r = 20 \, \mathrm{km} = 20000 \, \mathrm{m} \) and its rotation rate is \( \omega = 1 \, \mathrm{rev/s} = 2\pi \, \mathrm{rad/s} \).
03

Centripetal Force Requirement

For a mass \( m \) on the surface of the star, the required centripetal force to keep it in circular motion is given by \( F_c = m \omega^2 r \).
04

Gravitational Force acting on the mass

The gravitational force acting on the mass \( m \) is \( F_g = \frac{GMm}{r^2} \), where \( M \) is the mass of the neutron star and \( G \) is the gravitational constant \( 6.674 \times 10^{-11} \, \mathrm{N} \cdot \mathrm{m}^2/\mathrm{kg}^2 \).
05

Balance the Forces

To keep the material in place, the centripetal force \( F_c \) must equal the gravitational force \( F_g \). Set the equation \( m \omega^2 r = \frac{GMm}{r^2} \) and cancel \( m \).
06

Solve for Minimum Mass

Rearrange and solve for \( M \): \[ M = \frac{\omega^2 r^3}{G} \]. Substitute the known values: \[ M = \frac{(2\pi)^2 \times (20000)^3}{6.674 \times 10^{-11}} \].
07

Calculate the Result

Calculate the expression: \[ M \approx \frac{39.4784 \times 8 \times 10^{12}}{6.674 \times 10^{-11}} \] which results in \[ M \approx 1.85 \times 10^{27} \, \mathrm{kg} \].

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Key Concepts

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

Neutron Stars
Neutron stars are remnants of massive stars that have exploded in supernovae. They are incredibly dense and small. Imagine something so dense that just a teaspoon of its material could weigh as much as a mountain found on Earth. These stars pack almost all of their mass into a small sphere with a diameter of about 20 kilometers.
This small size makes neutron stars very interesting objects to study in astrophysics. In the context of our exercise, we consider a neutron star rotating very quickly, completing one full rotation every second. This rapid rotation helps us explore forces that act around the star, especially those that keep matter attached to such a swiftly spinning object.
Centripetal Force
Centripetal force is a crucial concept when studying objects moving in a circular path. The term 'centripetal' refers to "center-seeking" force. It's the force that keeps an object moving in that circular path rather than flying off in a straight tangent. For anything spinning in a circle, like the material on the surface of a rotating neutron star, there needs to be a force pulling it toward the center.
In our exercise, this force is the centripetal force caused by gravity pulling the material back toward the center of the star. The formula used to calculate this is:
  • For any mass, the centripetal force required for circular motion is given as:\( F_c = m \omega^2 r \)
  • Where \( \omega \) is the angular velocity in radians per second, \( r \) is the radius, and \( m \) is the mass of the object.

Understanding centripetal force helps us see how gravity and motion work together on the material on the neutron star's surface.
Physics Problems
Physics problems often involve translating complex phenomena into mathematical models. Problems like determining the minimum mass of a neutron star require a step-by-step approach.
Here's how:
  • **Identify what you know** - Gather known values like radius and rotational speed.
  • **Set up equations** - Use physics equations, like gravitational and centripetal force equations, that describe the conditions of the problem.
  • **Balance forces** - Equate the equations to solve for the unknown, ensuring forces balance for stable motion.
  • **Calculate the result** - Substitute known values into the equations and solve.

This structured approach helps transform abstract questions into manageable calculations.
Rotational Motion
Rotational motion involves objects spinning around an axis, much like our neutron star example. The irregular rotation of celestial bodies can create fascinating challenges in physics, such as determining forces acting upon them.
For our problem of finding the neutron star's minimum mass, understanding rotational motion is crucial. The faster an object spins, the more centripetal force is needed to keep objects at its surface from flying off due to inertia.
Understanding rotational motion involves:
  • **Angular velocity** \( \omega \) - This measures how quickly an object rotates, expressed in radians per second. In our case, the neutron star rotates at \( 2\pi \) radians per second.
  • **Radius of rotation** \( r \) - The distance from the rotation axis to the rotating object.

These elements combine to help us solve the equation that balances gravitational and centripetal forces, ultimately finding the minimum mass needed to keep the neutron star stable.

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