Problem 32
Question
Show that the work \(W\) required to launch a rocket of mass \(m\) from the ground vertically upward to a height \(h\) is given by the formula $$ W=\frac{m g R h}{R+h} $$ Hint: Use Newton's Law of Gravitation given in Exercise 31 and follow these steps: (i) Let \(m\) and \(M\) denote the mass of the rocket and the earth, respectively, so that \(F=G m M / r^{2}\), where \(R \leq r \leq R+h\). At \(r=R\) the force will be the weight of the rocket, that is, \(m g=G m M / R^{2} .\) Therefore, \(G=g R^{2} / M\), so \(F=m g R^{2} / r^{2}\). (ii) \(W=\int_{R}^{R+h} F d r\). where \(R\) is the radius of the earth.
Step-by-Step Solution
Verified Answer
To find the work required to launch a rocket of mass \(m\) vertically upward to a height \(h\), we first derive an expression for the gravitational force acting on the rocket as a function of its distance from the center of the Earth, \(F(r)=\frac{mgR^2}{r^2}\). Then, we integrate this force expression between the Earth's surface (\(r=R\)) and the desired height (\(r=R+h\)), giving us the work \(W=\int_{R}^{R+h} F(r) dr\). After evaluating the integral and simplifying the expression, we find that the work required to launch the rocket is given by the formula: \(W=\frac{mgRh}{R+h}\).
1Step 1: (i) Force expression for the rocket
First, we need to find the expression for the gravitational force acting on the rocket. The rocket has mass \(m\) and the earth has mass \(M\). The gravitational force acting on the rocket at a distance \(r\) from the center of the earth is given by:
$$
F = \frac{GmM}{r^2}
$$
At the surface of the Earth, \(r=R\), the force will be equal to the weight of the rocket, \(mg\):
$$
m g = \frac{GmM}{R^2} \implies G = \frac{gR^2}{M}
$$
Now, we can rewrite the force acting on the rocket as a function of \(r\):
$$
F(r) = \frac{mgR^2}{r^2}
$$
2Step 2: (ii) Calculate the work \(W\)
To find the total work required to take the rocket from the ground to a height \(h\), we need to integrate the force expression over the distance traveled:
$$
W = \int_{R}^{R+h} F(r) dr
$$
Now, substitute the force expression into the integral:
$$
W = \int_{R}^{R+h} \frac{mgR^2}{r^2} dr
$$
To integrate this expression, we can apply the integral of the form:
$$
\int \frac{1}{r^2} dr = -\frac{1}{r}
$$
So, by following the integration, we get:
$$
W = mgR^2 \Biggl(-\frac{1}{r} \Biggr|_{R}^{R+h}
$$
Now, evaluate the integral expression between the limits:
$$
W = mgR^2 \left( -\frac{1}{R+h} + \frac{1}{R} \right)
$$
Finally, simplify the expression to find the work required to launch the rocket to a height \(h\):
$$
W = \frac{mgRh}{R+h}
$$
Key Concepts
Gravitational ForceNewton's Law of GravitationIntegration in CalculusPhysics Problem Solving
Gravitational Force
Gravitational force is a fundamental interaction in nature, attracting two bodies towards each other. This force is what keeps planets in orbit around the sun and what causes an apple to fall to the ground. It's directly proportional to the product of the two masses involved and inversely proportional to the square of the distance between their centers.
Gravitational force can be expressed using the formula:
Gravitational force can be expressed using the formula:
- \( F = \frac{GmM}{r^2} \)
- \( F \) is the gravitational force.
- \( G \) is the gravitational constant (\( 6.674 \times 10^{-11} \) m\(^3\) kg\(^{-1}\) s\(^{-2}\)).
- \( m \) and \( M \) are the masses of the objects.
- \( r \) is the distance between the centers of the two masses.
Newton's Law of Gravitation
Sir Isaac Newton's formulation of the law of gravitation was groundbreaking and forms the foundation of classical physics. According to Newton's Law of Gravitation, every point mass attracts every other point mass in the universe with a force that is proportional to the product of their masses and inversely proportional to the square of the distance between the two points.
Newton’s Law can be expressed as:
Newton’s Law can be expressed as:
- \( F = \frac{GmM}{r^2} \)
- The force decreases with increasing distance between masses (\( r \)).
- A larger mass (\( m \) or \( M \)) results in a greater force.
Integration in Calculus
Integration is an essential concept in calculus that helps in finding quantities like area under a curve, total accumulation, and work done by a force over a distance. In physics problems, particularly those involving variable forces such as gravitational force, integration provides the method to calculate total work done when the force varies over the distance moved.
To find the work done \( W \) when moving an object within a gravitational field, we use the integral of the force over the path taken:
To find the work done \( W \) when moving an object within a gravitational field, we use the integral of the force over the path taken:
- \( W = \int_{R}^{R+h} F(r) dr \)
- Use \( -\frac{1}{r} \) as the integral of \( \frac{1}{r^2} \).
- Evaluate over bounds to find the total work, resulting in an expression like \( \frac{mgRh}{R+h} \).
Physics Problem Solving
Approaching a physics problem requires a structured method to break down complex interactions into manageable calculations. Physics problem solving involves understanding the problem, identifying principles involved, deriving equations, performing calculations, and interpreting results. Let's consider a standard approach:
- **Identify Key Concepts:** Recognize the principles and laws at play, such as gravity in the case of launching a rocket.
- **Translate the Problem:** Convert the physical situation into mathematical expressions using related formulas, as we do using \( F = \frac{GmM}{r^2} \) for gravity.
- **Perform Calculations:** Use mathematical techniques such as integration to compute quantities of interest, such as work done, carefully managing constants and limits.
- **Analyze Results:** Interpret the solution in the context of the problem, checking plausibility and consistency with physical laws.
Other exercises in this chapter
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