/*! 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 7 Two people carry a heavy clectri... [FREE SOLUTION] | 91Ó°ÊÓ

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Two people carry a heavy clectric motor by placing it on a light board 2.00 \(\mathrm{m}\) long. One person lifts at one end with a force of \(400 \mathrm{N},\) and the other lifts the opposite end with a force of 600 \(\mathrm{N}\) . (a) What is the weight of the motor, and where along the board is its center of gravity located? (b) Suppose the board is not light bnt weighs 200 \(\mathrm{N}\) , with its center of gravity at its center, and the two people each exert the same forces as before. What is the weight of the motor in this case, and where is its center of gravity located?

Short Answer

Expert verified
(a) The motor weighs 1000 N and is 1.20 m from the 400 N end. (b) The motor weighs 800 N and its center is 1.75 m from the 400 N end.

Step by step solution

01

Understanding Force Balance

In order for the board to remain in equilibrium, the sum of the upward forces must equal the sum of the downward forces. Therefore, the total weight supported by the two people (400 N and 600 N) is equal to the weight of the motor. This means that the motor's weight is the sum of the lifting forces: 400 N + 600 N = 1000 N.
02

Finding Center of Gravity Position

To locate the motor's center of gravity, consider the torques about one end of the board. If we take the torque about the end where the 400 N force is applied, the torque for equilibrium is given by: \(400 \times 0 = 0 + 600 \times 2.00 - W \times x = 0\), where x is the distance of the motor's center of gravity from the 400 N end. Solving for x gives us \(600 \times 2.00 = 1000 \times x\), so \(x = 1.20\ m\).
03

Considering the Board's Weight

Now, including the weight of the board, the total weight supported must be equal to the sum of the forces: 400 N + 600 N = 1000 N. However, part of this is the weight of the board (200 N), so the motor's weight (W) is now 1000 N - 200 N = 800 N.
04

Finding New Center of Gravity

Incorporating the board's weight, the new center of gravity for the motor is found by balancing torques. Let the center of gravity of the board at 1.00 m contribute to the torques: \( (400)(0) + (200)(1) + (600)(2) = W \cdot x\). Solving for x with W = 800 N gives \(800x = 200 + 1200\), so \(x = 1.75\ m\) from the 400 N end.

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Key Concepts

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

Center of Gravity
The center of gravity is the point where the total weight of an object or system can be considered to act. It is crucial for understanding how objects balance. In the context of this exercise, the center of gravity for the motor is initially determined by considering just the forces applied by the two people. This is because to find where the motor "balances" on the board, we need to know where its weight effectively pulls down.

For instance, when the motor is supported by these forces alone, its center of gravity is not at the midpoint of the board but rather at 1.20 m from the end where the lesser force is applied (400 N). This uneven distribution arises because different force magnitudes affect how the weight is spread along the board.

When the board's own weight is considered, the entire system's center of gravity changes. Now the board's weight distribution also factors into the balance, shifting the motor's center of gravity to a new point. This shows how additional weights and their placements can alter balance dynamics.
Torque Calculation
Torque is the measure of how much a force acting on an object causes it to rotate. Mathematically, it's calculated as the product of the force and the distance from the pivot point (torque arm). The equation for torque, \( \tau = F \cdot d \), highlights this relationship.

In this problem, to find the motor's center of gravity, we calculate the torques applied by the lifting forces. Taking torques about the board's end with the 400 N force, we set the following equilibrium condition \( 0 = 400 \times 0 + 600 \times 2.00 - W \times x \). Solving for \( x \) (the motor's center of gravity) shows how far from the pivot the motor 's center acts.

With the board added in the second part, the calculation shifts. The board's own weight introduces new torque, hence balancing torques now includes contributions from both the motor and board: \( 800x = 200 + 1200 \). Each element's position and weight adjusts how the system achieves equilibrium.
Force Balance
Force balance ensures that an object in equilibrium doesn't accelerate. This means the total forces pushing and pulling on it must cancel each other out. In this exercise, the forces from both people (400 N and 600 N) should sum up to match the downward force of the motor's weight. When they add up to 1000 N, it perfectly balances the motor against gravity.

When the board's weight of 200 N is factored in, it changes the force distribution without changing the total force applied by the lifters. This effectively means the motor's weight must adjust to 800 N so that the total weight, considering the board, still aligns with the overall lifting efforts. This principle is fundamental in physics for understanding balance and rotation.
Weight of Objects
The concept of weight is straightforward—it's simply the force of gravity acting on an object. However, understanding how this plays into equilibrium problems can be less intuitive.

In the problem given, the motor's weight is initially what balances the forces exerted by the two people. This direct calculation equates the sum of these forces (400 N + 600 N = 1000 N) to the motor's weight.

Adding the weight of the board (200 N) changes the scenario. Now, the combined weight of the motor and board still needs to be 1000 N to maintain balance given unchanged exertion by the carriers. Therefore, the motor's adjusted weight becomes 800 N to preserve this balance. This shift illustrates how distributions affect overall systems, an important concept in physics.

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Most popular questions from this chapter

Minimizing the Tension. A heavy horizontal girder of length \(L\) has several objects suspended from it. It is supported by a frictionless pivot at its left end and a cable of negligible weight that is attached to an I-beam at a point a distance \(h\) directly above the girder's center. Where should the other end of the cable be attached to the girder so that the cable's tension is a minimum? (Hint: In evaluating and presenting your answer, don't forget that the maximum distance of the point of attachment from the pivot is the length \(L\) of the beam.)

A \(15,000-N\) crane pivots around a friction-free axle at its base and is supported by a cable making a \(25^{\circ}\) angle with the crane (Fig. 11.29 ). The crane is 16 \(\mathrm{m}\) long and is not uniform, its center of gravity being 7.0 \(\mathrm{m}\) from the axle as measured along the crane. The cable is attached 3.0 \(\mathrm{m}\) from the upper end of the crane. When the crane is raised to \(55^{\circ}\) above the horizontal holding an \(11,000-N\) pallet of bricks by a 2.2 -in very light cord, find (a) the tension in the cable, and \((b)\) the horizontal and vertical components of the force that the axle exerts on the crane. Start with a free-body diagram of the crane.

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Flying Buttress. (a) A symmetric building has a roof sloping upward at \(35.0^{\circ}\) above the horizontal on each side. If each side of the uniform roof weighs \(10,000 \mathrm{N}\) , find the horizontal force that this roof exerts at the top of the wall, which tends to push out the walls. Which type of building would be more in danger of collapsing: one with tall walls or one with short walls? Explain. (b) As you saw in part (a), tall walls are in danger of collapsing from the weight of the roof. This problem plagued the ancient builders of large structures. A solution used in the great Gothic cathedrals during the 1200 s was the flying buttress, a stone support running between the walls and the ground that helped to hold in the walls. A Gothic church has a uniform roof weighing a total of \(20,000 \mathrm{N}\) and rising at \(40^{\circ}\) above the horizontal at each wall. The walls are 40 \(\mathrm{m}\) tall, and a flying buttress meets each wall 10 \(\mathrm{m}\) below the base of the roof. What horizontal force must this flying buttress apply to the wall?

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