/*! 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 61 (a) How high a hill can a car co... [FREE SOLUTION] | 91Ó°ÊÓ

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(a) How high a hill can a car coast up (engines disengaged) if work done by friction is negligible and its initial speed is \(110 \mathrm{km} / \mathrm{h}\) ? (b) If, in actuality, a \(750-\mathrm{kg}\) car with an initial speed of \(110 \mathrm{km} / \mathrm{h}\) is observed to coast up a hill to a height \(22.0 \mathrm{m}\) above its starting point, how much thermal energy was generated by friction? (c) What is the average force of friction if the hill has a slope of \(2.5^{\circ}\) above the horizontal?

Short Answer

Expert verified
(a) The height the car can coast up without friction is 47.63 m. (b) The thermal energy generated by friction is 261720 J. (c) The average force of friction is 517.62 N, opposing the car's motion up the hill.

Step by step solution

01

Part (a): Height without friction

We can use the conservation of mechanical energy principle. The initial kinetic energy of the car will be converted into potential energy as it goes up the hill. We have the initial kinetic energy: \(K_{i} = \frac{1}{2}mv_{i}^2\) and the final potential energy: \(U_{f} = mgh\) Since there is no friction, we have: \(K_{i} = U_{f}\) Now we need to find the initial speed in meters per second, and then we can find the height: \(v_{i} = 110 \frac{\mathrm{km}}{\mathrm{h}} \times \frac{1000 \mathrm{m}}{\mathrm{km}} \times \frac{1 \mathrm{h}}{3600 \mathrm{s}} = 30.56 \frac{\mathrm{m}}{\mathrm{s}}\) Write the equation to find the height the car can coast up: \(h = \frac{1}{2}\frac{v_{i}^2}{g}\)
02

Calculate the height

Now, we plug in the initial speed of the car and the acceleration due to gravity (\(g = 9.81 \frac{\mathrm{m}}{\mathrm{s}^2}\)): \(h = \frac{1}{2}\frac{(30.56 \frac{\mathrm{m}}{\mathrm{s}})^2}{9.81 \frac{\mathrm{m}}{\mathrm{s}^2}}\) \(h = 47.63 \mathrm{m}\) The height the car can coast up without friction is 47.63 m.
03

Part (b): Thermal energy generated by friction

We need to find the thermal energy generated by friction. First, we'll calculate the initial and final mechanical energies, and use work-energy principle: \(W_{nc} = E_f - E_i\) Where \(W_{nc}\) represents the work done by non-conservative forces (friction), and \(E_i\) and \(E_f\) are the initial and final mechanical energies, respectively. The initial mechanical energy is the initial kinetic energy: \(E_i = K_{i} = \frac{1}{2}mv_{i}^2\) The final mechanical energy is the final potential energy (when the car is at the height of 22.0 m): \(E_f = U_{f} = mgh_f\) Now, plug in the mass, initial speed, acceleration due to gravity, and the final height: \(W_{nc} = (750\mathrm{kg})(9.81\frac{\mathrm{m}}{\mathrm{s}^2})(22.0\mathrm{m}) - \frac{1}{2}(750\mathrm{kg})(30.56\frac{\mathrm{m}}{\mathrm{s}})^2\) \(W_{nc} = -261720 \mathrm{J}\) The negative sign indicates that this work was done against the car's motion. The energy generated by friction is 261720 J.
04

Part (c): Average friction force

To find the average friction force, we need to find the distance the car traveled up the slope and then use the work done by friction: \(F_{avg} = \frac{W_{nc}}{d}\) We can use trigonometry to find the distance: \(d = \frac{h_f}{\sin(\theta)}\) Plug in the final height and the slope angle (converted to radians): \(d = \frac{22.0\mathrm{m}}{\sin(2.5^{\circ})}\) \(d = 505.44 \mathrm{m}\) Now, we can find the average friction force: \(F_{avg} = \frac{-261720 \mathrm{J}}{505.44 \mathrm{m}}\) \(F_{avg} = -517.62 \mathrm{N}\) The average force of friction is 517.62 N, opposing the car's motion up the hill.

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Key Concepts

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

Kinetic Energy
Kinetic energy is the energy of an object in motion. This type of energy is determined by both the mass and the speed of the object. The equation for kinetic energy is given by \[K = \frac{1}{2}mv^2\] where:
  • m is the mass of the object
  • v is the velocity of the object
In the context of our problem, the car's initial speed is crucial because its kinetic energy will determine how high the car can ascend the hill without the engine's help. When the engines are disengaged, this kinetic energy transforms as the car climbs, converting into potential energy until the car can no longer move upwards.
Potential Energy
Potential energy is the energy stored within an object due to its position relative to other objects, often in the context of gravity. The potential energy of an object lifted up against gravity is calculated as:\[U = mgh\]where:
  • m is mass of the object
  • g is acceleration due to gravity
  • h is the height above a reference point
In our exercise, as the car climbs the hill, its kinetic energy is gradually converted into potential energy. Once the kinetic energy is fully transformed, the height reached corresponds directly to the car's potential energy. The balance of these energies reflects the fundamental law of conservation of energy, showing how energy shifts form but not quantity.
Friction
Friction is the force that opposes motion between two surfaces in contact. It acts against the movement of the car as it ascends the hill, causing some of the mechanical energy to turn into thermal energy. Friction can be seen as an energy killer, transforming kinetic to thermal energy and therefore requiring more initial energy for the same task. In calculations where friction cannot be ignored, it alters the net work done on the car. Here, it resulted in thermal energy, reducing how high the car could ascend compared to a frictionless scenario. Evaluating friction's impact involves considering both its force and the distance over which it acts.
Non-Conservative Forces
Non-conservative forces, such as friction, result in energy transformation or loss from a mechanical system. Unlike conservative forces, which store potential energy (such as gravity), non-conservative forces like friction lead to energy dissipation.In our example, friction performs non-conservative work against the car's motion, converting some kinetic energy into thermal energy, which is not recoverable for mechanical use. This irreversible transformation is critical to understanding real-world mechanics where perfect conservation rarely occurs.An equation often used to evaluate this transformation is:\[W_{nc} = E_f - E_i\]Where \(W_{nc}\) is the work done by non-conservative forces, reflecting the energy balance shift. In our case, this calculation shows the energy loss due to friction, affecting the height achieved by the car on the hill.

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