/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 13 Block \(A\) has a weight of 8 lb... [FREE SOLUTION] | 91Ó°ÊÓ

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Block \(A\) has a weight of 8 lb and block \(B\) has a weight of 6 lb. They rest on a surface for which the coefficient of kinetic friction is \(\mu_{k}=0.2 .\) If the spring has a stiffness of \(k=20\) lb/ft, and it is compressed \(0.2 \mathrm{ft}\), determine the acceleration of each block just after they are released.

Short Answer

Expert verified
The acceleration of block \(A\) just after being released is \(9.34 \, ft/s^2\) and the acceleration of block \(B\) is \(14.01 \, ft/s^2\).

Step by step solution

01

Determine the Spring Force

Use Hooke's law which states that the force exerted by a spring is directly proportional to the displacement of the spring. The formula used is \(F_{s} = k \cdot d\), where \(F_{s}\) is the force exerted by the spring, \(k\) is the spring constant and \(d\) is the displacement. Plugging in the provided values, we get \(F_{s} = 20 \cdot 0.2 = 4 \, lb\).
02

Find the Force Due to Friction

The kinetic friction force \(F_{f}\) is given by \(F_{f} = \mu_{k} \cdot N\), where \(\mu_{k}\) is the coefficient of kinetic friction and \(N\) is the normal force. Since there's no vertical acceleration, the normal force equals the weight. For block \(A\), \(F_{fA} = 0.2 \cdot 8 = 1.6 \, lb\). Similarly, for block \(B\), \(F_{fB} = 0.2 \cdot 6 = 1.2 \, lb\).
03

Determine the Net Force

Using Newton's second law, the net force is given by \(F_{net} = m \cdot a\), where \(m\) is the mass and \(a\) is acceleration. The net forces acting on block \(A\) and \(B\) help us set up the following equations: For Block \(A\): \(F_{net}^{A} = F_{s} - F_{fA} = m_{A} \cdot a_{A}\)For Block \(B\): \(F_{net}^{B} = F_{s} - F_{fB} = m_{B} \cdot a_{B}\)Note that we take weight as mass as \(1 \, lb\) in weight is equal to \(1/32.2 \, ft/s^2\) acceleration.
04

Calculate Acceleration

Solving the first equation: \(4 \, lb - 1.6 \, lb = (8/32.2) \, ft/s^2 \cdot a_{A}\). Simplifying, we find \(a_{A} = 9.34 \, ft/s^2\).Solving the second equation: \(4 \, lb - 1.2 \, lb = (6/32.2) \, ft/s^2 \cdot a_{B}\). Simplifying, we get \(a_{B} = 14.01 \, ft/s^2\). These are the accelerations of the blocks just after they are released.

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Key Concepts

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

Spring Force and Hooke's Law
When dealing with springs, understanding Hooke's Law is key. It provides the basis for calculating the force exerted by a spring when it is compressed or stretched. Hooke's Law is expressed as:
  • \( F_{s} = k \cdot d \)
This formula indicates that the spring force, \( F_{s} \), is directly proportional to the displacement, \( d \), and the spring constant, \( k \).
In the given problem, the spring constant is 20 lb/ft and the spring is compressed by 0.2 ft. By substituting these values into the formula, we find that the spring exerts a force of:
  • \( F_{s} = 20 \cdot 0.2 = 4 \, \text{lb} \)
This force acts against the friction and is critical in moving the blocks once they are released.
Kinetic Friction
Friction plays a significant role when an object moves across a surface. Kinetic friction is the force that opposes this movement. It is calculated using the equation:
  • \( F_{f} = \mu_{k} \cdot N \)
Here, \( F_{f} \) is the force of friction, \( \mu_{k} \) is the coefficient of kinetic friction, and \( N \) is the normal force.
For both blocks in this exercise, the normal force equals the weight, since there is no vertical movement. This makes the calculation straightforward:
For block A:
  • \( F_{fA} = 0.2 \cdot 8 = 1.6 \, \text{lb} \)
For block B:
  • \( F_{fB} = 0.2 \cdot 6 = 1.2 \, \text{lb} \)
These values help us understand how much force is needed to overcome friction and initiate the movement of the blocks.
Block Acceleration Calculation
Understanding Newton’s Second Law is essential for calculating acceleration. It links the concepts of force, mass, and acceleration through the equation:
  • \( F_{net} = m \cdot a \)
Where \( F_{net} \) is the net force acting on the object, \( m \) is the mass, and \( a \) is the acceleration.
For block A, the net force is calculated by subtracting the frictional force from the spring force:
  • \( F_{net}^A = 4 \, \text{lb} - 1.6 \, \text{lb} = 2.4 \, \text{lb} \)
The mass of block A can be derived from its weight, taking the weight divided by gravitational acceleration (\( 32.2 \, \text{ft/s}^2 \), where 1 lb equals \( 1 \, \text{lb}/{32.2 \, \text{ft/s}^2} \)). Thus, the acceleration \( a_A \) is calculated as:
  • \( a_A = \frac{2.4}{8/32.2} \approx 9.34 \, \text{ft/s}^2 \)
Similarly, for block B:
  • \( F_{net}^B = 4 \, \text{lb} - 1.2 \, \text{lb} = 2.8 \, \text{lb} \)
  • \( a_B = \frac{2.8}{6/32.2} \approx 14.01 \, \text{ft/s}^2 \)
These calculations provide the acceleration values that define how quickly each block will start moving once released.

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Most popular questions from this chapter

Block \(A\) has a mass \(m_{A}\) and is attached to a spring having a stiffness \(k\) and unstretched length \(l_{0} .\) If another block \(B,\) having a mass \(m_{B},\) is pressed against \(A\) so that the spring deforms a distance \(d\), determine the distance both blocks slide on the smooth surface before they begin to separate. What is their velocity at this instant?

The rocket is in circular orbit about the earth at an altitude of \(20 \mathrm{Mm}\). Determine the minimum increment in speed it must have in order to escape the earth's gravitational field.

The forked rod is used to move the smooth 2-lb particle around the horizontal path in the shape of a limaçon, \(r=(2+\cos \theta)\) ft. If \(\theta=\left(0.5 t^{2}\right)\) rad, where \(t\) is in seconds, determine the force which the rod exerts on the particle at the instant \(t=1\) s. The fork and path contact the particle on only one side.

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The collar has a mass of \(2 \mathrm{kg}\) and travels along the smooth horizontal rod defined by the equiangular spiral \(r=\left(e^{\theta}\right) \mathrm{m},\) where \(\theta\) is in radians. Determine the tangential force \(F\) and the normal force \(N\) acting on the collar when \(\theta=45^{\circ},\) if the force \(F\) maintains a constant angular motion \(\dot{\theta}=2 \operatorname{rad} / \mathrm{s}.\)

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