/*! 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 109 DATA In your physics lab, a bloc... [FREE SOLUTION] | 91Ó°ÊÓ

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DATA In your physics lab, a block of mass m is at rest on a horizontal surface. You attach a light cord to the block and apply a horizontal force to the free end of the cord. You find that the block remains at rest until the tension \(T\) in the cord exceeds \(20.0 \mathrm{~N}\). For \(T>20.0 \mathrm{~N},\) you measure the acceleration of the block when \(T\) is maintained at a constant value, and you plot the results (Fig. \(\mathrm{P} 5.109)\). The equation for the straight line that best fits your data is \(a=\left[0.182 \mathrm{~m} /\left(\mathrm{N} \cdot \mathrm{s}^{2}\right)\right] T-2.842 \mathrm{~m} / \mathrm{s}^{2}\) For this block and surface, what are (a) the coefficient of static friction and (b) the coefficient of kinetic friction? (c) If the experiment were done on the earth's moon, where \(g\) is much smaller than on the earth, would the graph of \(a\) versus \(T\) still be fit well by a straight line? If so, how would the slope and intercept of the line differ from the values in Fig. \(\mathrm{P} 5.109 ?\) Or, would each of them be the same?

Short Answer

Expert verified
The coefficient of static friction (\(\mu_s\)) is approximately 0.225 and the coefficient of kinetic friction (\(\mu_k\)) is about 0.141. If this experiment were conducted on the moon, the graph of \(a\) versus \(T\) would still be a straight line, but with a smaller intercept, while the slope would remain unchanged.

Step by step solution

01

Understanding the Problem

When the block is at rest, i.e., not moving, the static friction is acting on it and balanced by the tension. Once the block starts moving, the kinetic friction comes into play. The static friction is given by \(\mu_s \cdot m \cdot g\) and kinetic friction \(\mu_k \cdot m \cdot g\). Here, \(m\) is the mass of the block, \(g\) is acceleration due to gravity and \(\mu_s\) and \(\mu_k\) are static and kinetic friction coefficients respectively. The tension needed to overcome static friction is \(20.0 N\). After the block starts moving, it's acceleration is given by \(a=[0.182(m/N\cdot s^2)]T - 2.842m/s^2\). We need to use these relationships to find the coefficients of static and kinetic friction.
02

Find the Static Friction Coefficient

When the block is on the verge of moving, net force is zero, thus \(T - \mu_s \cdot m \cdot g = 0\), which gives \(\mu_s \cdot m \cdot g = 20 N\). Since \(\mu_s\) and \(m\) are positive, we have \(\mu_s = 20/mg\). We need to find the value of \(m\) to calculate \(\mu_s\).
03

Find the Mass of the Block

When the block is moving, net force is \(ma\), which gives \(T - \mu_k \cdot m \cdot g = m \cdot a\), i.e., \(T = m \cdot (a + \mu_k \cdot g)\). Comparing this with given \(a=[0.182(m/N\cdot s^2)]T - 2.842m/s^2\), we have \(m = 1 / 0.182 kg\). Substituting back into the equation for \(\mu_s\), we get the value of \(\mu_s\)
04

Find the Kinetic Friction Coefficient

Substitute the calculated mass into the equation and solve for \(\mu_k\). The term \(-2.842m/s^2\) can be written as \( - \mu_k \cdot g\), from which \(\mu_k\) is obtained.
05

Analyzing the Effect on the Moon

On the moon, value of \(g\) would be lesser than on Earth. However, since both the static and kinetic friction involve \(g\) and the tension also decreases due to lesser gravitational force, it would still be represented well by a straight line. The intercept would decrease due to smaller \(g\) but the slope would remain the same as the mass of the block remains unchanged.

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Key Concepts

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

Static Friction
In physics, static friction is the force that holds back a stationary object relative to the surface it's on, preventing motion despite applied forces. It exists between two surfaces not currently in motion relative to each other and acts in the opposite direction to the potential movement. To initiate movement, an external force greater than the maximum static frictional force must be applied. In the given problem, the static frictional force is overcome when the tension in the cord exceeds 20.0 N. This is the threshold force at which the block begins to move. The static friction coefficient, \( \mu_s \), is a dimensionless number representing the ratio of the maximum static frictional force to the normal force exerted by the weight of the object. The equilibrium equation, where the force needed to overcome static friction equals the tension (20.0 N), is used to calculate \( \mu_s \).

To make the process clearer to students, we calculate \( \mu_s \), by rearranging the equation \( \mu_s \cdot m \cdot g = T \) to solve for \( \mu_s \) and then substituting known values, where \( m \) is the block's mass and \( g \) is the acceleration due to gravity.
Kinetic Friction
Kinetic friction, also known as dynamic friction, is the force that opposes the relative motion of two surfaces that are in contact and moving past each other. It is typically less than static friction, explaining why it's easier to keep an object moving than to start the motion. The kinetic friction coefficient, \( \mu_k \), is calculated from the equation of motion once the object has started moving and is subject to a constant force. In this scenario, the equation \( a = [0.182 (m/N \cdot s^2)]T - 2.842 m/s^2 \) is provided, where \( a \) represents the acceleration of the block, and \( T \) the tension in the cord. The term \( -2.842 m/s^2 \) is crucial as it correlates directly to \( \mu_k \cdot g \) once the object is in motion.

For clarity, you calculate \( \mu_k \) by recognizing that the force of kinetic friction equals the product of \( \mu_k \) and the normal force. This is derived from Newton's second law, with \( T - \mu_k \cdot m \cdot g = m \cdot a \) after the block moves, identifying \( \mu_k \) from the provided equation for acceleration.
Newton's Laws of Motion
Newton’s laws of motion are three principles that describe the relationship between an object and the forces acting upon it, and its motion in response to those forces. The first law, also known as the law of inertia, states that an object at rest stays at rest and an object in motion remains in motion at a constant velocity unless acted upon by a net external force. The second law provides the details on how force, mass, and acceleration are related. It tells us that the acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass (\( F = m \cdot a \)). The third law states that for every action, there's an equal and opposite reaction.

This concept underpins our exercise, especially the second law, which is critical for understanding the interaction between tension, friction, mass, and acceleration. The law can be used to explain how finding the block’s mass allows us to calculate the friction coefficients, and it plays a critical role in graph analysis, connecting force to acceleration.
Force and Acceleration Graph Analysis
Graph analysis is a critical component of understanding the relationship between force and acceleration in physics. A force vs. acceleration graph can demonstrate how the force applied to an object affects its movement. When represented on a graph, Newton's second law (\( F = m \cdot a \) ) indicates that force and acceleration are directly proportional, showing a linear relationship if the mass of the object remains constant.

In the problem presented, the equation of the straight line from the graph provides the acceleration for varying tensions. By analyzing the slope and the y-intercept of this line, we can decipher the block's physical behavior. The slope \( [0.182 m/(N \cdot s^2)] \) gives the relationship between the tension force and acceleration, which aids in calculating the block's mass. The y-intercept corresponds to the point where the force of kinetic friction equals the tension, offering insight into the coefficient of kinetic friction. Graph analysis makes these connections visible, conveying the magnitude and direction of forces involved in motion.

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Most popular questions from this chapter

Two \(25.0 \mathrm{~N}\) weights are suspended at opposite ends of a rope that passes over a light, friction less pulley. The pulley is attached to a chain from the ceiling. (a) What is the tension in the rope? (b) What is the tension in the chain?

Friction and Climbing Shoes. Shoes made for the sports of bouldering and rock climbing are designed to provide a great deal of friction between the foot and the surface of the ground. Such shoes on smooth rock might have a coefficient of static friction of 1.2 and a coefficient of kinetic friction of 0.90 . For a person wearing these shoes, what's the maximum angle (with respect to the horizontal) of a smooth rock that can be walked on without slipping? (a) \(42^{\circ} ;\) (b) \(50^{\circ} ;\) (c) \(64^{\circ} ;\) (d) larger than \(90^{\circ}\).

Stopping Distance. (a) If the coefficient of kinetic friction between tires and dry pavement is \(0.80,\) what is the shortest distance in which you can stop a car by locking the brakes when the car is traveling at \(28.7 \mathrm{~m} / \mathrm{s}\) (about \(65 \mathrm{mi} / \mathrm{h}) ?\) (b) On wet pavement the coefficient of kinetic friction may be only \(0.25 .\) How fast should you drive on wet pavement to be able to stop in the same distance as in part (a)? (Note: Locking the brakes is not the safest way to stop. \()\)

A physics major is working to pay her college tuition by performing in a traveling carnival. She rides a motorcycle inside a hollow, transparent plastic sphere. After gaining sufficient speed, she travels in a vertical circle with radius \(13.0 \mathrm{~m}\). She has mass \(70.0 \mathrm{~kg},\) and her motorcycle has mass \(40.0 \mathrm{~kg} .\) (a) What minimum speed must she have at the top of the circle for the motorcycle tires to remain in contact with the sphere? (b) At the bottom of the circle, her speed is twice the value calculated in part (a). What is the magnitude of the normal force exerted on the motorcycle by the sphere at this point?

Two blocks, with masses \(4.00 \mathrm{~kg}\) and \(8.00 \mathrm{~kg},\) are connected by a string and slide down a \(30.0^{\circ}\) inclined plane (Fig. \(\mathbf{P 5 . 9 6}\) ). The coefficient of kinetic friction between the \(4.00 \mathrm{~kg}\) block and the plane is \(0.25 ;\) that between the \(8.00 \mathrm{~kg}\) block and the plane is \(0.35 .\) Calculate (a) the acceleration of each block and (b) the tension in the string. (c) What happens if the positions of the blocks are reversed, so that the \(4.00 \mathrm{~kg}\) block is uphill from the \(8.00 \mathrm{~kg}\) block?

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