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Physics Book A \(4.0 \mathrm{~kg}\) physics book and a \(6.0 \mathrm{~kg}\) calculus book, connected by a spring, are stationary on a horizontal frictionless surface. The spring constant is \(8000 \mathrm{~N} / \mathrm{m}\). The books are pushed together, compressing the spring, and then they are released from rest. When the spring has returned to its unstretched length, the speed of the calculus book is \(4.0 \mathrm{~m} / \mathrm{s}\). How much energy is stored in the spring at the instant the books are released?

Short Answer

Expert verified
The energy stored in the spring at the instant the books are released is \(120 \mathrm{~J}\).

Step by step solution

01

Identify given data

Here is the information given in the problem: - Mass of the physics book, \(m_1 = 4.0 \mathrm{~kg}\) - Mass of the calculus book, \(m_2 = 6.0 \mathrm{~kg}\) - Spring constant, \(k = 8000 \mathrm{~N} / \mathrm{m}\) - Speed of the calculus book, \(v_2 = 4.0 \mathrm{~m} / \mathrm{s}\)
02

Use conservation of momentum

Since the system is isolated and there are no external forces, the momentum before and after the release is conserved. Initially, the total momentum is zero: \( p_{\text{initial}} = 0 \) At the unstretched length of the spring, the total momentum will be: \[p_{\text{final}} = m_1 v_1 + m_2 v_2 = 0\] Solving for the velocity of the physics book \(v_1\): \[4.0 \mathrm{~kg} \cdot v_1 + 6.0 \mathrm{~kg} \cdot 4.0 \mathrm{~m/s} = 0\] \[4.0 \mathrm{~kg} \cdot v_1 = -24.0 \mathrm{~kg \cdot m/s}\] \[v_1 = -6.0 \mathrm{~m/s}\]
03

Calculate the kinetic energy

The kinetic energy of the system is the sum of the kinetic energies of both books. The kinetic energy \(K\) of an object is given by: \[K = \frac{1}{2}mv^2\] Hence, the total kinetic energy at the point when the spring is unstretched is: \[K = \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2\] Substituting the values: \[K = \frac{1}{2} (4.0 \mathrm{~kg})(-6.0 \mathrm{~m/s})^2 + \frac{1}{2} (6.0 \mathrm{~kg})(4.0 \mathrm{~m/s})^2\] \[K = \frac{1}{2} (4.0 \mathrm{~kg}) (36 \mathrm{~m^2 / s^2}) + \frac{1}{2} (6.0 \mathrm{~kg}) (16 \mathrm{~m^2 / s^2})\] \[K = 72 \mathrm{~J} + 48 \mathrm{~J} = 120 \mathrm{~J}\]
04

Determine the energy stored in the spring

The total kinetic energy at the point when the spring is unstretched is equal to the potential energy stored in the spring at the moment the books were released. So the energy stored in the spring is: \[ E_{\text{spring}} = 120 \mathrm{~J} \]

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Key Concepts

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

conservation of momentum
When studying physics, especially in spring systems, one essential concept you need to grasp is the conservation of momentum. Momentum is a measure of the motion of an object and is calculated by multiplying the object's mass and its velocity. Conservation of momentum states that in a closed system without external forces, the total momentum before and after an event remains constant.

In our exercise, two books are connected by a spring and initially stationary, meaning their total momentum is zero. When the books are released, although they start moving, the system's total momentum must still sum to zero. This conservation lets us set up the equation:

\( m_1 v_1 + m_2 v_2 = 0 \)

With this, we solve for the unknown velocity, in this case, of the physics book (because we know the speed of the calculus book). For calculations:
\[ \begin{align*} 4.0 \, kg \, v_1 + 6.0 \, kg \, \cdot \, 4.0 \, m/s &= 0 \ 4.0 \, kg \, \cdot \ v_1 &= -24.0 \, kg \, \cdot \, m/s \ v_1 &= -6.0 \, m/s \end{align*} \]

Thus, the velocity of the physics book is \( -6.0 \, m/s \).
kinetic energy
Kinetic energy (KE) is the energy an object has due to its motion. Calculation of kinetic energy involves the mass of the object and the square of its velocity, as per the equation:
\[ K = \frac{1}{2} \, mv^2 \]

For our spring system, we know the velocities of the books obtained via momentum conservation. To find total kinetic energy, we sum the kinetic energies of both books. Here's how it's computed:
\[ \begin{align*} K_{total} &= \frac{1}{2} m_1 v_1^2 + \frac{1}{2} m_2 v_2^2 \ &= \frac{1}{2} (4.0 \, kg)(-6.0 \, m/s)^2 + \frac{1}{2} (6.0 \, kg)(4.0 \, m/s)^2 \ &= \frac{1}{2} (4.0 \, kg) (36 \, m^2 / s^2) + \frac{1}{2} (6.0 \, kg) (16 \, m^2 / s^2) \ &= 72 \, J + 48 \, J = 120 \, J \end{align*} \]

So, total kinetic energy when the spring is unstretched is 120 Joules.
potential energy
Potential energy (PE) is the stored energy of an object due to its position or state. For spring systems, this involves the compression or elongation of the spring. The potential energy stored in a spring follows Hooke's Law and is calculated using the formula:
\[ E_{\text{spring}} = \frac{1}{2} k x^2 \]

However, direct calculation isn't always necessary. In our system, at the moment the spring returns to its unstretched length, all stored potential energy is converted into kinetic energy (as found in the previous section). Hence, we equate the total kinetic energy directly to the spring's potential energy:
\[ E_{\text{spring}} = K_{total} = 120 \, J \]

This tells us that 120 Joules of energy were initially stored in the spring, which was released and converted into the kinetic energy of both books. Understanding this conversion helps you grasp energy conservation principles in mechanical systems.

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Most popular questions from this chapter

A small block of mass \(m\) can slide along the frictionless loop-the-loop. The block is released from rest at point \(P\), at height \(h=5 R\) above the bottom of the loop. How much work does the gravitational force do on the block as the block travels from point \(P\) to (a) point \(Q\) and \((\mathrm{b})\) the top of the loop? If the gravitational potential energy of the block-Earth system is taken to be zero at the bottom of the loop, what is that potential energy when the block is (c) at point \(P,(\mathrm{~d})\) at point \(Q\), and \((\mathrm{e})\) at the top of the loop? (f) If, instead of being released, the block is given some initial speed downward along the track, do the answers to (a) through (e) increase, decrease, or remain the same?

Cable Breaks The cable of the 1800 \(\mathrm{kg}\) elevator cab in Fig. \(10-54\) snaps when the cab is at rest at the first floor, where the cab bottom is a distance \(d=3.7 \mathrm{~m}\) above a cushioning spring whose spring constant is \(k=0.15 \mathrm{MN} / \mathrm{m}\). A safety device clamps the cab against guide rails so that a constant frictional force of \(4.4 \mathrm{kN}\) opposes the cab's motion. (a) Find the speed of the cab just before it hits the spring. (b) Find the maximum distance \(x\) that the spring is compressed (the frictional force still acts during this compression). (c) Find the distance that the cab will bounce back up the shaft. (d) Using conservation of energy, find the approximate total distance that the cab will move before coming to rest. (Assume that the frictional force on the cab is negligible when the cab is stationary.)

Block Dropped on a Spring A \(250 \mathrm{~g}\) block is dropped onto a relaxed vertical spring that has a spring constant of \(k=\) 2.5 N/cm (Fig. 10-32). The block becomes attached to the spring and compresses the spring \(12 \mathrm{~cm}\) before momentarily stopping. While the spring is being compressed, what work is done on the block by (a) the gravitational force on it and (b) the spring force? (c) What is the speed of the block just before it hits the spring? (Assume that friction is negligible.) (d) If the speed at impact is doubled, what is the maximum compression of the spring?

Block Dropped on a Spring Two A \(2.0 \mathrm{~kg}\) block is dropped from a height of \(40 \mathrm{~cm}\) onto a spring of spring constant \(k=1960 \mathrm{~N} / \mathrm{m}\) (Fig. 10-39). Find the maximum distance the spring is compressed.

You drop a \(2.00\) kg textbook to a friend who stands on the ground \(10.0 \mathrm{~m}\) below the textbook with outstretched hands \(1.50 \mathrm{~m}\) above the ground (Fig. \(10-26\) ). (a) How much work \(W^{\text {grav }}\) is done on the textbook by the gravitational force as it drops to your friend's hands? (b) What is the change \(\Delta U\) in the gravitational potential energy of the textbook-Earth system during the drop? If the gravitational potential energy \(U\) of that system is taken to be zero at ground level, what is \(U\) when the textbook (c) is released and (d) reaches the hands? Now take \(U\) to be \(100 \mathrm{~J}\) at ground level and again find (e) \(W\) grav (f) \(\Delta U,(\mathrm{~g}) U\) at the release point, and (h) \(U\) at the hands.

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