Chapter 7: Problem 18
A particle of mass \(0.2 \mathrm{~kg}\) is moving in one dimension under a force that delivers a constant power \(0.5 W\) to the particle. If the initial speed (in \(m s^{-1}\) ) of the particle is zero, the speed (in \(m s^{-1}\) ) after \(5 s\) is _____ .
Short Answer
Expert verified
\(v = \sqrt{25} = 5 \, m s^{-1}\)
Step by step solution
01
Understanding the Problem
We are given the constant power delivered to a particle, its mass, and the time duration during which the power is delivered. We need to find the final speed of the particle after 5 seconds assuming it started from rest.
02
Relating Power to Work and Energy
Power is the rate at which work is done. The work done on the particle equals the change in kinetic energy. Since the initial speed is zero, the work done will equal the final kinetic energy of the particle.
03
Using the Work-Energy Principle
Use the work-energy principle, which states that the work done on an object is equal to the change in kinetic energy. Since the initial kinetic energy is zero, the work done (Power × Time) will be equal to the final kinetic energy (\(\frac{1}{2}mv^2\)).
04
Calculating Final Kinetic Energy
Calculate the final kinetic energy using the power and time: Work Done = Power × Time = 0.5 W × 5 s = 2.5 J.
05
Computing the Final Speed
Final Kinetic Energy = \(\frac{1}{2}mv^2\). Solve for velocity v: \(v = \sqrt{\frac{2\times \text{Final Kinetic Energy}}{m}} = \sqrt{\frac{2\times 2.5}{0.2}}\).
06
Final Calculation
Perform the final calculation to find the speed after 5 seconds: \(v = \sqrt{\frac{5}{0.2}}\).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Understanding the Work-Energy Principle
The work-energy principle is a crucial concept in physics that connects force, motion, and energy. It essentially tells us that the work done by forces acting on an object results in a change in the object's kinetic energy.
Putting this into practice, if we apply a constant force to move an object in one dimension, the work done by that force is equal to the change in the object's kinetic energy. For a particle starting from rest, like in our exercise, this means that all the work done on it by external forces (in this case, due to the power being delivered) transforms into kinetic energy, causing the particle to accelerate.
Putting this into practice, if we apply a constant force to move an object in one dimension, the work done by that force is equal to the change in the object's kinetic energy. For a particle starting from rest, like in our exercise, this means that all the work done on it by external forces (in this case, due to the power being delivered) transforms into kinetic energy, causing the particle to accelerate.
- Work Done (W) = Change in Kinetic Energy (∆KE)
- W = Force (F) × Displacement (s) = Power (P) × Time (t)
Calculating Kinetic Energy
Kinetic energy represents the energy an object possesses due to its motion. It can be calculated using the mass of the object and its speed. The formula to determine the kinetic energy (KE) of an object is:
\[KE = \frac{1}{2}mv^2\]
where:
\[KE = \frac{1}{2}mv^2\]
where:
- \(m\) is the mass of the object,
- \(v\) is the velocity of the object.
Relationship Between Power and Speed
Power in physics is defined as the rate at which work is done or energy is transferred. It can be expressed as:
\[P = \frac{W}{t} = Fv\]
where:
\[P = \frac{W}{t} = Fv\]
where:
- \(P\) stands for power,
- \(W\) is work done,
- \(t\) is time,
- \(F\) is force, and
- \(v\) is the velocity or speed of the object.
Force and Motion in One Dimension
When dealing with force and motion in one dimension, we use Newton's second law of motion which states that the force exerted on an object is equal to the mass of the object multiplied by its acceleration (F = ma).
In scenarios where objects move along a straight line, such as the particle in our textbook problem, analyzing the motion becomes simpler. We equate the rate of change of kinetic energy to the work done by the force (because work is defined as the force times displacement). Here, power delivering a constant force results in a constant acceleration and uniform change in speed over time. This direct relationship makes it easier to translate the power delivered into a final speed, as demonstrated in the problem where the speed after 5 seconds is solely based on the constant power applied to the particle.
In scenarios where objects move along a straight line, such as the particle in our textbook problem, analyzing the motion becomes simpler. We equate the rate of change of kinetic energy to the work done by the force (because work is defined as the force times displacement). Here, power delivering a constant force results in a constant acceleration and uniform change in speed over time. This direct relationship makes it easier to translate the power delivered into a final speed, as demonstrated in the problem where the speed after 5 seconds is solely based on the constant power applied to the particle.