Problem 10
Question
Force of attraction When a particle of mass \(m\) is at \((x, 0),\) it is attracted toward the origin with a force whose magnitude is \(k / x^{2}\) . If the particle starts from rest at \(x=b\) and is acted on by no other forces, find the work done on it by the time it reaches \(x=a\) , \(0 < a < b\) .
Step-by-Step Solution
Verified Answer
The work done is \( W = k \left( \frac{1}{b} - \frac{1}{a} \right) \).
1Step 1: Identify the Force Acting on the Particle
The force acting on the particle due to the attraction towards the origin is given by the formula: \( F(x) = \frac{k}{x^2} \), where \( k \) is a constant. This force is directed towards the origin along the x-axis.
2Step 2: Set Up the Integral for Work
Work done by a force is calculated by integrating the force over the displacement. Hence, the work done, \( W \), on the particle as it moves from \( x = b \) to \( x = a \) is given by: \( W = \int_{b}^{a} F(x) \, dx = \int_{b}^{a} \frac{k}{x^2} \, dx \).
3Step 3: Evaluate the Integral
To find the work done, evaluate the integral: \( \int_{b}^{a} \frac{k}{x^2} \, dx = k \int_{b}^{a} x^{-2} \, dx \). Integrating, we have: \( \int x^{-2} \, dx = -x^{-1} \), so the result is: \( k[-x^{-1}] \bigg|_{b}^{a} \).
4Step 4: Compute the Definite Integral
Substitute the limits \( x = b \) and \( x = a \) into the antiderivative: \( W = k \left( -\frac{1}{a} + \frac{1}{b} \right) \). Thus, \( W = k \left( \frac{1}{b} - \frac{1}{a} \right) \).
5Step 5: Finalize the Work Done Expression
The work done on the particle by the time it reaches \( x = a \) is given by the expression: \( W = k \left( \frac{1}{b} - \frac{1}{a} \right) \). Since \( b > a \), this result is positive, confirming that work was indeed done on the particle as it moved towards the origin.
Key Concepts
Force of AttractionIntegral CalculusMechanicsDefinite Integral
Force of Attraction
The concept of force of attraction is quite fascinating. It describes how objects are pulled towards each other due to various factors like mass and distance. In this exercise, the force of attraction is directed towards the origin. Specifically, for a particle of mass, the force magnitude is given by the formula:
The essence of forces like gravity follow this inverse square law, meaning they become weaker with the square of the distance.
- \( F(x) = \frac{k}{x^2} \)
The essence of forces like gravity follow this inverse square law, meaning they become weaker with the square of the distance.
Integral Calculus
Integral calculus is used to find quantities such as areas, volumes, and in this context, work done by a force. When a force acts along a path, integral calculus helps in calculating the total work done over that path.
It’s like adding up all the tiny pieces of work done along its journey.
- The process involves setting up an integral, which is a mathematical description of summing up an infinite number of infinitesimally small quantities.
It’s like adding up all the tiny pieces of work done along its journey.
Mechanics
Mechanics is a branch of physics that deals with motion and the forces that cause it. This exercise falls under the branch of classical mechanics, where the motion of particles is analyzed under the influence of forces.
- The particle in this problem starts at rest, meaning its initial velocity is zero.
- The only force acting on it is the attractive force towards the origin, given by \( F(x) = \frac{k}{x^2} \).
- This force gets translated into work done as the particle moves along the x-axis.
Definite Integral
The definite integral plays a crucial role in calculating the work done in this problem. Unlike an indefinite integral, which gives a general antiderivative, a definite integral computes the net value over an interval.
The result being positive indicates that work was done by the force of attraction to move the particle closer to the origin.
- The definite integral here is expressed as:
The result being positive indicates that work was done by the force of attraction to move the particle closer to the origin.
Other exercises in this chapter
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