Chapter 6: Problem 696
If the radius of earth is \(\mathrm{R}\) then height \({ }^{\prime} \mathrm{h}\) ' at which value of ' \(\mathrm{g}\) ' becomes one-fourth is (A) \(\mathrm{R} / 4\) (B) \(3 \mathrm{R} / 4\) (C) \(\mathrm{R}\) (D) \(\mathrm{R} / 8\)
Short Answer
Expert verified
The height at which the gravitational acceleration (g) becomes one-fourth of its value on Earth's surface is \(h = R\). So, the correct option is (C).
Step by step solution
01
1. Formula for gravitational force
We know that the formula for gravitational force is given by:
\[F = G \frac{m \cdot M}{r^2}\]
Where:
* F is the gravitational force
* G is the gravitational constant
* m and M are the two masses
* r is the distance between the centers of masses
02
2. Calculate gravitational acceleration on Earth's surface
The acceleration due to gravity on the Earth's surface, g, is related to the gravitational force by:
\( F = m \cdot g\)
Using the formula from the first step, we can find the gravitational acceleration on Earth's surface:
\(g = \frac{GM_\oplus}{R^2}\)
Here, Mâ‚‘ represents the mass of Earth.
03
3. Find the value of g which is one-fourth
Given that the value of g becomes one-fourth at height h, the new value of g can be represented as:
\(g_{new} = \frac{1}{4} \cdot g = \frac{1}{4}\frac{GM_\oplus}{R^2}\)
04
4. Calculate g at height h
We need to find the value of g at height h. The formula for g at height h can be given by:
\(g_{h} = \frac{GM_\oplus}{(R+h)^2}\)
05
5. Equate g_new with g_h and solve for h
Now, equate g_new with g_h:
\(\frac{1}{4}\frac{GM_\oplus}{R^2} = \frac{GM_\oplus}{(R+h)^2}\)
Solve for h:
\(\frac{1}{4}R^2 = (R+h)^2\)
\(R^2 = 4(R+h)^2\)
\(R^2 = 4R^2 + 8Rh + 4h^2\)
\(-3R^2 = 8Rh + 4h^2\)
\(-\frac{3}{4}R^2 = 2h^2 + 4Rh\)
\(-\frac{3}{8}R^2 = h^2 + 2Rh\)
Now, we have a quadratic equation in terms of h:
\(h^2 + 2Rh -\frac{3}{8}R^2 = 0\)
06
6. Solve the quadratic equation
Now, solve this quadratic equation for h using the quadratic formula:
\(h = \frac{-b\pm\sqrt{b^2 - 4ac}}{2a}\)
In this case, we have \(a = 1\), \(b = 2R\), and \(c = -\frac{3}{8}R^2\).
Plug in the values and solve for h:
\(h = \frac{-2R\pm\sqrt{(2R)^2 - 4(\frac{3}{8}R^2)}}{2}\)
\(h = -R\pm\sqrt{R^2}\)
One solution is \(h = -R\), but the height cannot be negative, so we can discard this solution.
The other solution is \(h = R\).
07
Conclusion
Therefore, the height at which the gravitational acceleration (g) becomes one-fourth of its value on Earth's surface is \(h = R\). So, the correct option is (C).
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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 the attractive force acting between two masses due to their mass. The basic formula governing this force is expressed as:
\[F = G \frac{m \cdot M}{r^2}\]
Here,
\[F = G \frac{m \cdot M}{r^2}\]
Here,
- \(F\) stands for the gravitational force between two objects.
- \(G\) is the gravitational constant, which remains the same throughout the universe.
- \(m\) and \(M\) are the masses of the two objects, respectively.
- \(r\) is the distance between the centers of the two masses.
Quadratic Equation
A quadratic equation is a polynomial equation of degree two, and it takes the general form:
\[ax^2 + bx + c = 0\]
In the context of the exercise, we encountered a quadratic equation while calculating the height at which gravitational acceleration becomes one-fourth of its value at Earth's surface. The specific equation derived was:
\[h^2 + 2Rh -\frac{3}{8}R^2 = 0\]
To solve this equation, the quadratic formula is used:
\[h = \frac{-b\pm\sqrt{b^2 - 4ac}}{2a}\]
\[ax^2 + bx + c = 0\]
In the context of the exercise, we encountered a quadratic equation while calculating the height at which gravitational acceleration becomes one-fourth of its value at Earth's surface. The specific equation derived was:
\[h^2 + 2Rh -\frac{3}{8}R^2 = 0\]
To solve this equation, the quadratic formula is used:
\[h = \frac{-b\pm\sqrt{b^2 - 4ac}}{2a}\]
- \(a\) represents the coefficient of \(h^2\).
- \(b\) is the coefficient of \(h\).
- \(c\) is the constant term.
Earth's Radius
The Earth's radius is a fundamental value when performing calculations involving gravitational force and acceleration. It is approximately 6,371 kilometers or about 3,959 miles. In our exercise, the Earth's radius is noted as \(R\), which serves as a reference point for both the surface level gravitational acceleration and calculations involving height above the surface.
Understanding Earth's radius is important because:
Understanding Earth's radius is important because:
- It helps determine the surface gravity \(g\), which can be calculated using the formula \(g = \frac{GM_\oplus}{R^2}\).
- It acts as a benchmark for evaluating changes in gravity as you move away from the Earth's surface. For example, moving to a height \(h\) above the surface changes the effective distance to \((R+h)\).
- It assists in calculating geophysical and astronomical phenomena, such as the Earth's orbit and satellite positioning.
Acceleration Due to Gravity
Acceleration due to gravity, often denoted as \(g\), is the rate at which an object accelerates when falling freely towards the Earth, under the influence of the Earth's gravitational force. At sea level, this acceleration is approximately 9.81 meters per second squared (m/s²).
It's represented by the equation:
\[g = \frac{GM_\oplus}{R^2}\]
This equation shows that:
\[g_{h} = \frac{GM_\oplus}{(R+h)^2}\]
As \(h\) increases, \(g\) decreases due to the greater distance from the Earth's centre. Understanding acceleration due to gravity is vital in many fields, such as engineering, physics, and astrophysics, as it affects everything from falling objects to orbits of satellites.
It's represented by the equation:
\[g = \frac{GM_\oplus}{R^2}\]
This equation shows that:
- \(G\) is the gravitational constant.
- \(M_\oplus\) is the mass of the Earth.
- \(R\) is the Earth’s radius.
\[g_{h} = \frac{GM_\oplus}{(R+h)^2}\]
As \(h\) increases, \(g\) decreases due to the greater distance from the Earth's centre. Understanding acceleration due to gravity is vital in many fields, such as engineering, physics, and astrophysics, as it affects everything from falling objects to orbits of satellites.