/*! 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 EP A 10.0 -kg microwave oven is ... [FREE SOLUTION] | 91Ó°ÊÓ

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EP A 10.0 -kg microwave oven is pushed 8.00 m up the sloping surface of a loading ramp inclined at an angle of \(36.9^{\circ}\) above the horizontal, by a constant force \(\vec{\boldsymbol{F}}\) with a magnitude 110 \(\mathrm{N}\) and acting parallel to the ramp. The coefficient of kinetic friction between the oven and the ramp is 0.250 . (a) What is the work done on the oven by the force \(F ?\) (b) What is the work done on the oven by the friction force? (c) Compute the increase in potential energy for the oven. (d) Use your answers to parts (a), (b), and (c) to calculate the increase in the oven's kinetic energy. (e) Use \(\Sigma \vec{F}=m \vec{a}\) to calculate the acceleration of the oven. Assuming that the oven is initially at rest, use the acceleration to calculate the oven's speed after traveling 8.00 \(\mathrm{m}\) . From this, compute the increase in the oven's kinetic energy, and compare it to the answer you got in part (d).

Short Answer

Expert verified
(a) 880 J; (b) -156.96 J; (c) 470.40 J; (d) 252.64 J; (e) 10.06 m/s² and 12.69 m/s final speed, \( \Delta KE = 250.43 J \).

Step by step solution

01

Work Done by Force F

The work done by a force is given by the formula \( W = F \cdot d \cdot \cos(\theta) \). Since the force \( F \) is acting parallel to the ramp, the angle \( \theta \) is 0 degrees. Hence, \( \cos(\theta) = 1 \). Thus, the work done by the force \( F \) is:\[W_F = 110 \text{ N} \times 8.00 \text{ m} \times 1 = 880 \text{ J}.\]
02

Work Done by Friction Force

The friction force can be calculated using \( f_k = \mu_k \cdot N \), where \( \mu_k = 0.250 \) and \( N = mg \cdot \cos(\alpha) \) is the normal force. The normal force \( N \) does not act along the ramp, so we use the incline angle \( \alpha = 36.9^{\circ} \):\[ N = 10 \text{ kg} \cdot 9.8 \text{ m/s}^2 \cdot \cos(36.9^{\circ}) = 78.48 \text{ N}. \]Thus, the friction force is:\[ f_k = 0.250 \cdot 78.48 \text{ N} = 19.62 \text{ N}. \]The work done by this force over 8 meters is:\[ W_f = 19.62 \text{ N} \cdot 8.00 \text{ m} \cdot \cos(180^{\circ}) = -156.96 \text{ J}. \]
03

Increase in Potential Energy

The increase in potential energy \( \Delta U \) is given by \( \Delta U = mgh \), where \( h \) is the height gained. Using the inclined angle:\[ h = 8.00 \text{ m} \cdot \sin(36.9^{\circ}) = 4.80 \text{ m}. \]Thus, the potential energy increase is:\[ \Delta U = 10 \text{ kg} \cdot 9.8 \text{ m/s}^2 \cdot 4.80 \text{ m} = 470.40 \text{ J}. \]
04

Increase in Kinetic Energy

The total work-energy principle gives us that the increase in kinetic energy (\( \Delta KE \)) is equal to the total work done on the object:\[ \Delta KE = W_F + W_f - \Delta U. \]Substituting the known values:\[ \Delta KE = 880 \text{ J} - 156.96 \text{ J} - 470.40 \text{ J} = 252.64 \text{ J}. \]
05

Calculate the Acceleration

Using Newton's Second Law \( \Sigma F = ma \), where the net force \( \Sigma F \) is the sum of the force \( F \), gravitational component along the ramp, and friction:\[ \Sigma F = F - mg \sin(\alpha) - f_k. \]Substitute known values:\[ \Sigma F = 110 \text{ N} - 10 \text{ kg} \cdot 9.8 \text{ m/s}^2 \cdot \sin(36.9^{\circ}) - 19.62 \text{ N} = 100.6 \text{ N}. \]\[ a = \frac{\Sigma F}{m} = \frac{100.6 \text{ N}}{10 \text{ kg}} = 10.06 \text{ m/s}^2. \]
06

Calculate Final Speed and Kinetic Energy

Using the kinematic equation \( v^2 = u^2 + 2as \), where initial speed \( u = 0 \), \( a \) is acceleration, \( s = 8.00 \text{ m} \):\[ v^2 = 0 + 2 \times 10.06 \text{ m/s}^2 \times 8.00 \text{ m}. \]\[ v = \sqrt{161.0} \approx 12.69 \text{ m/s}. \]The kinetic energy increase \( \Delta KE = \frac{1}{2}mv^2 \):\[ \Delta KE = \frac{1}{2} \cdot 10 \text{ kg} \cdot (12.69 \text{ m/s})^2 = 250.43 \text{ J}. \]The calculated \( \Delta KE \) (250.43 J) is close to our previous result (252.64 J) within potential calculation or rounding inaccuracies.

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Key Concepts

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

Kinetic Friction
Kinetic friction occurs when two surfaces slide against each other. It plays a crucial role in energy problems because it opposes motion. Imagine pushing a cart up a slope; the surface of the slope exerts a frictional force opposing the cart's movement.
  • The amount of kinetic friction depends on two factors: the normal force (the component of weight perpendicular to the movement) and the coefficient of kinetic friction (\( \mu_k \)).
  • The formula for kinetic friction is given by \( f_k = \mu_k \cdot N \), where \( N \) is the normal force.
Kinetic friction never acts in the direction of motion. Instead, it resists the movement, doing negative work. This means it takes energy away from the system, seen in the negative value of the work done by friction. Understanding kinetic friction helps in calculating the total work involved in moving objects along surfaces.
Potential Energy
Potential energy is the energy stored in an object due to its position. When dealing with an inclined plane, potential energy is often discussed in terms of height above a reference point, like the bottom of a ramp.
  • Potential energy due to gravity is calculated by \( PE = mgh \), where \( m \) is mass, \( g \) is gravitational acceleration, and \( h \) is the height.
  • In inclined plane problems, the height \( h \) can be found using the length of the slope and trigonometric functions, \( h = d \cdot \sin(\alpha) \), with \( \alpha \) being the incline angle.
When an object is moved up a ramp, it gains potential energy. This is because it is moved against the gravitational force, accumulating energy that could be converted into motion if released. This concept ties closely with kinetic energy, as potential energy can transform into kinetic energy and vice versa.
Kinetic Energy
Kinetic energy is the energy an object has due to its motion. It's crucial when understanding how forces and energy affect moving objects.
  • The formula for kinetic energy is \( KE = \frac{1}{2} mv^2 \), where \( m \) is the mass and \( v \) is the velocity.
  • When forces do work on an object, the kinetic energy changes, which can be calculated using the work-energy principle \( \Delta KE = \text{Total Work} \).
In the context of an inclined plane, kinetic energy helps to determine how fast an object moves up or down the slope. When an object is pushed up a ramp, the work done by the force increases its kinetic energy, while friction and gravitational forces decrease it. Calculating kinetic energy changes helps to understand an object's speed at different points, such as when it reaches the end of a ramp.

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Most popular questions from this chapter

A slingshot will shoot a 10 -g pebble 22.0 \(\mathrm{m}\) straight up. (a) How much potential energy is stored in the slingshot's rubberband? (b) With the same potential energy stored in the rubber band, how high can the slingshot shoot a \(25-\) g pebble? (c) What physical effects did you ignore in solving this problem?

A 1500 -kg rocket is to be launched with an initial upward speed of 50.0 \(\mathrm{m} / \mathrm{s}\) . In order to assist its engines, the engineers will start it from rest on a ramp that rises \(53^{\circ}\) above the horizontal (Fig. \(\mathrm{P7.56} )\) . At the bottom, the ramp turns upward and launches the rocket vertically. The engines provide a constant forward thrust of \(2000 \mathrm{N},\) and friction with the ramp surface is a constant 500 \(\mathrm{N}\) . How far from the base of the ramp should the rocket start, as measured along the surface of the ramp?

BIO Bone Fractures. The maximum energy that a bone can absorb without breaking depends on its characteristics, such as its cross-sectional area and its elasticity. For healthy human leg bones of approximately 6.0 \(\mathrm{cm}^{2}\) cross-sectional area, this energy has been experimentally measured to be about 200 \(\mathrm{J}\) . (a) From approximately what maximum height could a 60 -kg person jump and land rigidly upright on both feet without breaking his legs? (b) You are probably surprised at how small the answer to part (a) is. People obviously jump from much greater heights without breaking their legs. How can that be? What else absorbs the energy when they jump from greater heights? (Hint: How did the person in part (a) land? How do people normally land when they jump from greater heights? (c) In light of your answers to parts (a) and (b), what might be some of the reasons that older people are much more prone than younger ones to bone fractures from simple falls (such as a fall in the shower)?

Two blocks with different masses are attached to either end of a light rope that passes over a light, frictionless pulley suspended from the ceiling. The masses are released from rest, and the more massive one starts to descend. After this block has descended \(1.20 \mathrm{m},\) its speed is 3.00 \(\mathrm{m} / \mathrm{s} .\) If the total mass of the two blocks is 15.0 \(\mathrm{kg},\) what is the mass of each block?

A 2.00 -kg block is pushed against a spring with negligible mass and force constant \(k=400 \mathrm{N} / \mathrm{m},\) compressing it 0.220 \(\mathrm{m}\) . When the block is released, it moves along a frictionless, horizontal surface and then up a frictionless incline with slope 37.0" (Fig. \(\mathrm{P7} .42\) ). (a) What is the speed of the block as it slides along the horizontal surface after having left the spring? (b) How far does the block travel up the incline before starting to slide back down?

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