4.71 A block of mass \(20.0 \mathrm{~kg}\) supported by a vertical massless cable is initially at rest. The block is then pulled upward with a constant acceleration of \(2.32 \mathrm{~m} / \mathrm{s}^{2}\). a) What is the tension in the cable? b) What is the net force acting on the mass? c) What is the speed of the block after it has traveled \(2.00 \mathrm{m?}\)

Short Answer

Expert verified
Answer: The tension in the cable is 242.6 N, the net force acting on the mass is 46.4 N, and the speed of the block after it has traveled 2.00m is 3.05 m/s.

Step by step solution

01

Write down Newton's second law of motion for the block in the vertical direction.

Newton's second law states that the net force acting on an object is equal to the mass of the object times its acceleration: \(F_{net} = m \times a\). Since the block is moving vertically upward, its weight (\(m \times g\)) will be acting downward. The tension (T) in the cable will be acting upward to support the weight and to provide the required acceleration. So, the net force acting on the block is: \(F_{net} = T - m \times g\). Now, we can use Newton's second law to find the tension in the cable.
02

Calculation of Tension in the Cable.

Plug in the known values to the equation \(F_{net} = T - m \times g\), then solve for T. Given: \(m = 20.0 \mathrm{~kg}\) \(a = 2.32 \mathrm{~m} / \mathrm{s}^{2}\) \(g = 9.81 \mathrm{~m} / \mathrm{s}^{2}\) (gravitational acceleration) \(F_{net} = m \times a = (20.0 \mathrm{~kg}) \times (2.32 \mathrm{~m} / \mathrm{s}^{2}) = 46.4 \mathrm{~N}\) \(T = F_{net} + m \times g = (46.4 \mathrm{~N}) + (20.0 \mathrm{~kg}) \times (9.81 \mathrm{~m} / \mathrm{s}^{2}) = 46.4 \mathrm{~N} + 196.2 \mathrm{~N} = 242.6 \mathrm{~N}\). The tension in the cable is \(242.6 \mathrm{~N}\). #b) What is the net force acting on the mass?# We have already found the net force acting on the mass in the previous calculation of tension as \(F_{net} = 46.4 \mathrm{~N}\). #c) What is the speed of the block after it has traveled \(2.00 \mathrm{m?}\)#
03

Write down the relevant kinematic equation.

The kinematic equation that allows us to find the final velocity (v) of the block after traveling a certain distance (d) with a constant acceleration starting from rest is: \(v^2 = u^2 + 2 \times a \times d\), where u is the initial velocity, which is 0 in this case.
04

Calculation of the Final Velocity of the Block after traveling 2.00m.

Plug in the known values to the kinematic equation and solve for v. Given: \(u = 0 \mathrm{~m} / \mathrm{s}\) \(a = 2.32 \mathrm{~m} / \mathrm{s}^{2}\) \(d = 2.00 \mathrm{~m}\) \(v^2 = 0 + 2 \times (2.32 \mathrm{~m} / \mathrm{s}^{2}) \times (2.00 \mathrm{~m}) = 9.28 \mathrm{~m^2} / \mathrm{s^2}\) Taking the square root of both sides, we get the final velocity: \(v = \sqrt{9.28 \mathrm{~m^2}/\mathrm{s^2}} = 3.05 \mathrm{~m} / \mathrm{s}\). The speed of the block after it has traveled \(2.00 \mathrm{m}\) is \(3.05 \mathrm{~m} / \mathrm{s}\). In summary, a) The tension in the cable is \(242.6 \mathrm{~N}\). b) The net force acting on the mass is \(46.4 \mathrm{~N}\). c) The speed of the block after it has traveled \(2.00 \mathrm{m}\) is \(3.05 \mathrm{~m} / \mathrm{s}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Tension in a Cable
Understanding the concept of tension in a cable is essential when dealing with mechanical systems that involve pulling or supporting masses. Tension can be thought of as the force conducted along the length of a cable or rope, acting in a direction that pulls on objects the cable is attached to. The tension in the cable must be sufficient to both support the weight of the mass and provide any additional force to accelerate the mass, if necessary.

When a block is suspended and accelerated upwards, the tension in the cable not only has to counteract the force of gravity but to also accelerate the block upwards. This can be mathematically expressed as:
\( T = m \times g + m \times a\), where \(T\) is the tension, \(m\) the mass of the block, \(g\) the acceleration due to gravity, and \(a\) the acceleration of the block. Here, it's critical to ensure the mass is properly accounted for when both gravity and acceleration are involved in the net force calculation.
Net Force Calculation
The net force calculation is a fundamental aspect of Newton's second law, which states that the net force acting on an object is equal to its mass times its acceleration (\(F_{net} = m \times a\)). To visualize this, imagine the conflicting forces acting on an object: in one direction, you have weight due to gravity, and in another, you might have tension or some other applied force.

The net force is effectively the vector sum of all these forces acting on an object. If the mass is stationary, the net force is zero, implying a state of equilibrium. However, if the object is accelerating, the net force will be non-zero and in the direction of the acceleration. In the context of the given exercise, the upward tension and downward gravitational force were considered to find the net force acting on the block.
Kinematic Equations
The kinematic equations are a set of four equations that describe the motion of objects under constant acceleration. These equations connect the five kinematic variables: displacement, initial velocity, final velocity, acceleration, and time.

For situations like our exercise, where an object starts from rest and is subject to a consistent acceleration, one of the key equations we use is \( v^2 = u^2 + 2 \times a \times d \), where \( v \) is the final velocity, \( u \) the initial velocity (zero in cases starting from rest), \( a \) the acceleration, and \( d \) the displacement. Understanding these kinematic equations is crucial for problems involving motion, as they provide a reliable method to calculate various motion parameters from known values.
Constant Acceleration
An object experiences constant acceleration when it speeds up or slows down at a steady rate over time. In physics, this implies that the object's acceleration stays the same in magnitude and direction.

When solving physics problems, constant acceleration can simplify calculations because it allows us to use the kinematic equations confidently. For instance, in the provided exercise, knowing that the block is pulled upward with a constant acceleration ensures that we can predict its movement accurately over any given distance or time interval. This property is particularly useful as it makes the system's behavior more predictable and thus easier to study and understand.
Final Velocity
The final velocity of an object is the speed and direction it has after undergoing acceleration over a distance or period. It can be computed using kinematic equations, and in scenarios with constant acceleration, the calculation is straightforward.

In our case, the block's final velocity after traveling a certain distance was determined using the equation \( v^2 = u^2 + 2 \times a \times d \). Key takeaways include that if an object starts from rest, the initial velocity (\(u\)) is zero, making the equation simpler. Moreover, the square root must be taken after plugging in the values to solve for \(v\). Understanding how to calculate final velocity is critical in predicting future positions and speeds of objects in motion.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Which of the following observations about the friction force is (are) incorrect? a) The magnitude of the kinetic friction force is always proportional to the normal force b) The magnitude of the static friction force is always proportional to the normal force. c) The magnitude of the static friction force is always proportional to the external applied force. d) The direction of the kinetic friction force is always opposite the direction of the relative motion of the object writh respect to the surface the object moves on. e) The direction of the static friction force is always opposite that of the impending motion of the object relative to the surface it rests on f) All of the above are correct.

A box of books is initially at rest a distance \(D=0.540 \mathrm{~m}\) from the end of a wooden board. The coefficient of static friction between the box and the board is \(\mu_{s}=0.320\), and the coefficient of kinetic friction is \(\mu_{k}=0.250 .\) The angle of the board is increased slowly, until the box just begins to slide; then the board is held at this angle. Find the speed of the box as it reaches the end of the board. -4.55 A block of mass \(M_{1}=0.640 \mathrm{~kg}\) is initially at rest on a cart of mass \(M_{2}=0.320 \mathrm{~kg}\) with the cart initially at rest on a level air track. The coefficient of static friction between the block and the cart is \(\mu_{s}=0.620\), but there is essentially no friction between the air track and the cart. The cart is accelerated by a force of magnitude \(F\) parallel to the air track. Find the maximum value of \(F\) that allows the block to accelerate with the cart, without sliding on top of the cart.

A block of mass \(M_{1}=0.640 \mathrm{~kg}\) is initially at rest on a cart of mass \(M_{2}=0.320 \mathrm{~kg}\) with the cart initially at rest on a level air track. The coefficient of static friction between the block and the cart is \(\mu_{s}=0.620\), but there is essentially no friction between the air track and the cart. The cart is accelerated by a force of magnitude \(F\) parallel to the air track. Find the maximum value of \(F\) that allows the block to accelerate with the cart, without sliding on top of the cart.

You are at the shoe store to buy a pair of basketball shoes that have the greatest traction on a specific type of hardwood. To determine the coefficient of static friction. \(\mu\), you place each shoe on a plank of the wood and tilt the plank to an angle \(\theta\), at which the shoe just starts to slide. Obtain an expression for \(\mu\) as a function of \(\theta\).

In a physics class, a 2.70 - g ping pong ball was suspended from a massless string. The string makes an angle of \(\theta=15.0^{\circ}\) with the vertical when air is blown horizontally at the ball at a speed of \(20.5 \mathrm{~m} / \mathrm{s}\). Assume that the friction force is proportional to the squared speed of the air stream. a) What is the proportionality constant in this experiment? b) What is the tension in the string?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free