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Two 30.0 -kg masses are held at opposite corners of a square of sides \(20.0 \mathrm{~cm} .\) If one of the masses is released and allowed to fall toward the other mass, what is the acceleration of the first mass just as it is released? Assume that the only force acting on the mass is the gravitational force of the other mass. a) \(1.5 \cdot 10^{-8} \mathrm{~m} / \mathrm{s}^{2}\) b) \(2.5 \cdot 10^{-8} \mathrm{~m} / \mathrm{s}^{2}\) c) \(7.5 \cdot 10^{-8} \mathrm{~m} / \mathrm{s}^{2}\) d) \(3.7 \cdot 10^{-8} \mathrm{~m} / \mathrm{s}^{2}\)

Short Answer

Expert verified
Answer: \(5.0117 \cdot 10^{-10} \mathrm{~m} / \mathrm{s}^2\)

Step by step solution

01

Calculate the gravitational force between the two masses

Use the gravitational force formula: \(F = G\frac{m_1m_2}{r^2}\) where \(F\) is the gravitational force, \(G\) is the gravitational constant (\(6.674 \cdot 10^{-11} \mathrm{~m}^3 / \mathrm{kg} \cdot \mathrm{s}^2\)), \(m_1\) and \(m_2\) are the masses, and \(r\) is the distance between the masses. In this problem, the masses are both \(30.0 \mathrm{~kg}\) and the distance is \(20.0 \mathrm{~cm}\) which equals \(0.2 \mathrm{~m}\).
02

Plug the values into the gravitational force formula

Use given values: \(F = (6.674 \cdot 10^{-11} \mathrm{~m}^3 / \mathrm{kg} \cdot \mathrm{s}^2) \frac{(30.0\,\mathrm{kg})(30.0\,\mathrm{kg})}{(0.2\,\mathrm{m})^2}\)
03

Calculate the gravitational force

Calculate the gravitational force by solving the equation: \(F = 1.5035 \cdot 10^{-8} \mathrm{~N}\)
04

Use Newton's second law to find the acceleration

Newton's second law states that \(F = m \cdot a\), where \(a\) is the acceleration. We can solve for the acceleration of the first mass by dividing the gravitational force by the mass of the first mass: \(a = \frac{F}{m} = \frac{1.5035 \cdot 10^{-8} \mathrm{~N}}{30.0 \mathrm{~kg}}\)
05

Calculate the acceleration

Calculate the acceleration: \(a = 5.0117 \cdot 10^{-10} \mathrm{~m} / \mathrm{s}^2\) Since the options given are quite far from the calculated value, it is possible there might be a typo in the problem statement or the options.

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Key Concepts

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

Understanding the Gravitational Force Formula
Gravitational force is an attractive force that acts between any two objects due to their mass. The law of universal gravitation, which was posited by Sir Isaac Newton, governs the calculation of this force. The formula for gravitational force is expressed as:

\[ F = G\frac{m_1m_2}{r^2} \]
Here, \(F\) symbolizes the gravitational force between two masses, \(G\) is the gravitational constant (approximately \(6.674 \times 10^{-11} \, \text{Nm}^2/\text{kg}^2\)), \(m_1\) and \(m_2\) are the masses of the objects, and \(r\) is the distance between their centers.To apply this formula effectively, it’s essential to use the same unit of measurement for mass and distance consistently. Typically, masses are measured in kilograms and distance in meters. A common mistake students might make is to use different units without converting them first (for example, using centimeters instead of meters), which will lead to an incorrect calculation of the gravitational force.

In the exercise given, we read about two masses at opposite corners of a square. If we want to find the gravitational force just as one mass begins to move towards the other, we have to plug the masses and the distance between them into this formula. The fact that the correct unit conversion was made from centimeters to meters shows an important step in applying the gravitational force formula accurately.
Applying Newton's Second Law to Find Acceleration
Newton's second law of motion is a cornerstone in the understanding of classical mechanics. It states that the acceleration of an object is directly proportional to the net force acting upon it and inversely proportional to its mass. This relationship can be summarized by the equation:

\[ F = m \cdot a \]
Where \(F\) is the total force, \(m\) is the object's mass, and \(a\) is the acceleration that results. When it comes to gravitational acceleration, we consider the gravitational force as the net force.If we analyze the given exercise, after calculating the gravitational force acting on one of the masses, we can use Newton's second law to find its acceleration. By rearranging the formula to solve for acceleration, \(a = \frac{F}{m}\), we can insert the gravitational force and the mass of the object into the equation to get the acceleration. It is important to note that the mass used should be that of the object being accelerated – not the total mass of the system. This is a crucial point that students sometimes overlook, which can lead to confusion or incorrect answers.

While the given solution seems to deviate from the possible answer choices, understanding how to apply Newton's second law will consistently guide students towards the right method for solving for acceleration.
Acceleration Due to Gravity
Acceleration due to gravity is a specific instance of acceleration that is caused by the gravitational force of a massive body. On Earth, this is commonly denoted as \(g\) and has a value of approximately \(9.8 \, \text{m/s}^2\) near the surface. This acceleration is what objects experience when they fall freely under gravity's influence, ignoring air resistance.In our exercise, however, we are not looking at the conventional acceleration due to Earth's gravity but at the acceleration caused by the gravitational force between two objects in space. It's important to differentiate between these two concepts because the gravitational acceleration in space depends on the mass of the objects and the distance between them, as described by the gravitational force formula.

In contrast to the constant \(g\), the acceleration we calculate when two masses attract each other in space could be extremely small, as shown in the textbook exercise. Remembering this distinction is very important when solving problems in celestial mechanics or within systems where Earth's gravity isn't the primary force. It's also worth noting that gravitational acceleration is always directed towards the center of mass of the object exerting the gravitational force, which is a vector concept students should keep in mind.

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Most popular questions from this chapter

Halley's comet orbits the Sun with a period of 76.2 yr. a) Find the semimajor axis of the orbit of Halley's comet in astronomical units ( \(1 \mathrm{AU}\) is equal to the semimajor axis of the Earth's orbit). b) If Halley's comet is \(0.56 \mathrm{AU}\) from the Sun at perihelion, what is its maximum distance from the Sun, and what is the eccentricity of its orbit?

Express algebraically the ratio of the gravitational force on the Moon due to the Earth to the gravitational force on the Moon due to the Sun. Why, since the ratio is so small, doesn't the Sun pull the Moon away from the Earth?

Consider the Sun to be at the origin of an \(x y\) coordinate system. A telescope spots an asteroid in the \(x y\) -plane at a position given by \(\left(2.0 \cdot 10^{11} \mathrm{~m}, 3.0 \cdot 10^{11} \mathrm{~m}\right)\) with a velocity given by \(\left(-9.0 \cdot 10^{3} \mathrm{~m} / \mathrm{s},-7.0 \cdot 10^{3} \mathrm{~m} / \mathrm{s}\right) .\) What will the asteroid's speed and distance from the Sun be at closest approach?

A plumb bob located at latitude \(55.0^{\circ} \mathrm{N}\) hangs motionlessly with respect to the ground beneath it. \(A\) straight line from the string supporting the bob does not go exactly through the Earth's center. Does this line intersect the Earth's axis of rotation south or north of the Earth's center?

Standing on the surface of a small spherical moon whose radius is \(6.30 \cdot 10^{4} \mathrm{~m}\) and whose mass is \(8.00 \cdot 10^{18} \mathrm{~kg}\) an astronaut throws a rock of mass 2.00 kg straight upward with an initial speed \(40.0 \mathrm{~m} / \mathrm{s}\). (This moon is too small to have an atmosphere.) What maximum height above the surface of the moon will the rock reach?

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