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11.7 A \(15-\mathrm{kg}\) child sits on a playground seesaw, \(2.0 \mathrm{~m}\) from the pivot. A second child located \(1.0 \mathrm{~m}\) on the other side of the pivot would have to have a mass of _________ to lift the first child off the ground. a) greater than \(30 \mathrm{~kg} \quad\) c) equal to \(30 \mathrm{~kg}\) b) less than \(30 \mathrm{~kg}\)

Short Answer

Expert verified
Answer: The mass of the second child required to lift the first child off the ground is 30 kg.

Step by step solution

01

Identifying the given variables

The given variables in this problem are: 1. Mass of first child = \(15~kg\) 2. Distance of the first child from the pivot = \(2.0~m\) 3. Distance of the second child from the pivot = \(1.0~m\) Our goal is to find the mass of the second child so that the first child is lifted off the ground.
02

Balancing the Torque

In order to balance the torque, we follow the equation: \(τ_1 = τ_2\) where \(τ_1\) is the torque created by the first child and \(τ_2\) is the torque created by the second child. Torque can be calculated as: \(τ = (force) * (distance~to~pivot)\) Force is the product of mass and gravitational acceleration, \(F = mg\). Therefore, \(τ = (mg) * (distance~to~pivot)\)
03

Applying the Torque equation

Now, we need to balance the torque created by both children: \((m_1g)d_1 = (m_2g)d_2\) Where \(m_1 = 15~kg\), \(d_1 = 2.0~m\), \(d_2 = 1.0~m\) and we need to find \(m_2\). Gravitational acceleration \(g\) will be the same for both children and cancels out when equating torques. \((15~kg)(2.0~m) = (m_2)(1.0~m)\)
04

Solve for the mass of the second child

To find the mass of the second child, we can rearrange the equation: \(m_2 = \frac{(15~kg)(2.0~m)}{1.0~m}\) \(m_2 = 30~kg\) The mass of the second child required to lift the first child off the ground is equal to \(30~kg\). So, the correct answer is c) equal to \(30~kg\).

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Key Concepts

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

Seesaw balancing
Seesaws are a fantastic way to learn about balance and physics in a fun, real-world setting. A seesaw is a long, plank-like object that rests on a central point called a pivot or fulcrum. When you place different weights at varying distances from the pivot, you can achieve balance, or seesaw equilibrium. Imagine two children of different weights sitting on opposite sides of a seesaw: to balance it, their distances from the pivot must be adjusted according to their weights. This principle is what makes seesaw physics intriguing and educational. By understanding and applying the concept of balance, you can predict how changes in weight and distance affect the overall equilibrium of the seesaw.
Rotational equilibrium
Rotational equilibrium is a key concept in physics that describes an object that is balanced so that it does not rotate around its axis. For a seesaw to be in rotational equilibrium, the torques on either side of the pivot must be equal. Torque is the rotational equivalent of force and is calculated by multiplying the force applied by the distance from the pivot: \[\tau = F \times \text{distance to pivot}\]In the seesaw problem, each child generates torque based on their weight and distance from the pivot. To achieve equilibrium, the torques they create must be equal. If one side has more torque, the seesaw will tip towards that side. Understanding rotational equilibrium allows us to solve problems relating to balance and stability effectively.
Physics problem-solving
Physics problems often require a step-by-step approach to break down concepts into manageable parts, especially with topics like balance and torque. In solving the seesaw balance problem, we start by identifying known values like the mass of the children and their distances from the pivot. We then apply important formulas, such as the torque equation, to understand how various factors affect balance. Using the equation \((m_1g)d_1 = (m_2g)d_2\),we can determine the necessary mass of the second child by ensuring both torques are equal, simplifying the problem to an algebraic expression. Lastly, always check the solution to ensure it makes sense within the physical context of the problem, like assessing if the calculated mass is reasonable.
Child mass calculation
Calculating the mass needed for balance on a seesaw is a valuable example of applying physics in real life. To balance a seesaw where one child weighs 15 kg and sits 2 meters from the pivot, the second child’s mass can be found using the torque equilibrium equation: \[m_2 = \frac{(m_1 \times d_1)}{d_2}\]Substitute the given values: \((15\, \text{kg}) \times (2\, \text{m}) = m_2 \times (1\, \text{m})\)So, \[m_2 = \frac{30}{1} = 30\, \text{kg}\]This calculation shows that the second child must weigh 30 kg to achieve balance, showcasing how theoretical physics concepts are used to solve practical problems. Knowing how to manipulate and solve using formulas helps demystify real-world applications like seesaw mechanics.

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Most popular questions from this chapter

The angular displacement of a torsional spring is proportional to the applied torque; that is \(\tau=\kappa \theta,\) where \(\kappa\) is a constant. Suppose that such a spring is mounted to an arm that moves in a vertical plane. The mass of the arm is \(45.0 \mathrm{~g}\), and it is \(12.0 \mathrm{~cm}\) long. The arm-spring system is at equilibrium with the arm at an angular displacement of \(17.0^{\circ}\) with respect to the horizontal. If a mass of \(0.420 \mathrm{~kg}\) is hung from the arm \(9.00 \mathrm{~cm}\) from the axle, what will be the angular displacement in the new equilibrium position (relative to that with the unloaded spring)?

A 2.00 -m-long diving board of mass \(12.0 \mathrm{~kg}\) is \(3.00 \mathrm{~m}\) above the water. It has two attachments holding it in place. One is located at the very back end of the board, and the other is \(25.0 \mathrm{~cm}\) away from that end. a) Assuming that the board has uniform density, find the forces acting on each attachment (take the downward direction to be positive). b) If a diver of mass \(65.0 \mathrm{~kg}\) is standing on the front end, what are the forces acting on the two attachments?

A trapdoor on a stage has a mass of \(19.2 \mathrm{~kg}\) and a width of \(1.50 \mathrm{~m}\) (hinge side to handle side). The door can be treated as having uniform thickness and density. A small handle on the door is \(1.41 \mathrm{~m}\) away from the hinge side. \(\mathrm{A}\) rope is tied to the handle and used to raise the door. At one instant, the rope is horizontal, and the trapdoor has been partly opened so that the handle is \(1.13 \mathrm{~m}\) above the floor. What is the tension, \(T,\) in the rope at this time?

Two uniform planks, each of mass \(m\) and length \(L,\) are connected by a hinge at the top and by a chain of negligible mass attached at their centers, as shown in the figure. The assembly will stand upright, in the shape of an \(A,\) on a frictionless surface without collapsing. As a function of the length of the chain, find each of the following: a) the tension in the chain, b) the force on the hinge of each plank, and c) the force of the ground on each plank.

A \(1000-\mathrm{N}\) crate rests on a horizontal floor. It is being pulled up by two vertical ropes. The left rope has a tension of \(400 \mathrm{~N}\). Assuming the crate does not leave the floor, what can you say about the tension in the right rope?

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