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The only force acting on a \(2.0 \mathrm{~kg}\) canister that is moving in an \(x y\) plane has a magnitude of \(5.0 \mathrm{~N}\). The canister initially has a velocity of \(4.0 \mathrm{~m} / \mathrm{s}\) in the positive \(x\) direction and some time later has a velocity of \(6.0 \mathrm{~m} / \mathrm{s}\) in the positive \(y\) direction. How much work is done on the canister by the \(5.0 \mathrm{~N}\) force during this time?

Short Answer

Expert verified
The work done on the canister is 20.0 J.

Step by step solution

01

Identify the initial and final velocities

The problem states the canister initially has a velocity of \(4.0 \, \mathrm{m/s}\) in the positive \(x\) direction and later a velocity of \(6.0 \, \mathrm{m/s}\) in the positive \(y\) direction. We can represent these velocities as vectors: \(\mathbf{v_i} = (4.0 \, \mathrm{m/s}, 0)\) and \(\mathbf{v_f} = (0, 6.0 \, \mathrm{m/s})\).
02

Calculate initial kinetic energy

The kinetic energy \(K\) is given by \(K = \frac{1}{2} mv^2\). For the initial velocity, \(v_i = 4.0 \, \mathrm{m/s}\).\[K_i = \frac{1}{2} \times 2.0 \, \mathrm{kg} \times (4.0 \, \mathrm{m/s})^2 = 16.0 \, \mathrm{J}\]
03

Calculate final kinetic energy

Now calculate the kinetic energy with the final velocity \(v_f = 6.0 \, \mathrm{m/s}\).\[K_f = \frac{1}{2} \times 2.0 \, \mathrm{kg} \times (6.0 \, \mathrm{m/s})^2 = 36.0 \, \mathrm{J}\]
04

Apply work-energy theorem

The work-energy theorem states that the work done on an object is the change in its kinetic energy: \( W = K_f - K_i \).Substitute the calculated kinetic energies:\[ W = 36.0 \, \mathrm{J} - 16.0 \, \mathrm{J} = 20.0 \, \mathrm{J} \]

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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 a form of energy that an object possesses due to its motion. Imagine it as the energy that is required to accelerate an object from rest to its current velocity. The more massive an object is and the faster it moves, the more kinetic energy it has. It is calculated using the formula:
  • \( K = \frac{1}{2} mv^2 \)
where \( K \) is the kinetic energy, \( m \) is the mass of the object, and \( v \) is the velocity of the object.
In this exercise, the canister experienced a change in kinetic energy as it changed its velocity due to the applied force. Initially, when it was moving at \(4.0 \, \mathrm{m/s}\), the canister had an initial kinetic energy \(K_i = 16.0 \, \mathrm{J}\). After speeding up to \(6.0 \, \mathrm{m/s}\) in another direction, its kinetic energy increased to \(K_f = 36.0 \, \mathrm{J}\).
This change signifies the amount of work done on the canister by the force acting on it.
Velocity Vectors
Velocity vectors help us understand the direction and magnitude of an object's velocity. In physics, velocity is not just about how fast something moves, but also the direction in which it moves. Hence, we represent it as a vector, which contains information about both speed and direction.
In the problem, the canister's initial and final velocities can be described using velocity vectors:
  • Initial Velocity Vector \( \mathbf{v_i} = (4.0 \, \mathrm{m/s}, 0) \)
  • Final Velocity Vector \( \mathbf{v_f} = (0, 6.0 \, \mathrm{m/s}) \)
These vectors indicate a change in direction and speed, rooted in the concept of vectors in mathematics. Initially, the object moves straight along the x-axis, while later, it shifts to move along the y-axis. This alteration in motion is vectorially significant and impacts how we calculate changes in kinetic energy.
Force in Physics
In simple terms, force in physics is an interaction that changes the motion of an object. It is what causes an object to start moving, stop moving, or alter its motion. Forces have both magnitude and direction, making them vector quantities closely linked to velocity vectors.
In our scenario, a force of magnitude \(5.0 \, \mathrm{N}\) is the external influence altering the canister’s velocity. This force causes the canister to change direction and speed over time, which in turn impacts its kinetic energy. Applying the work-energy theorem, the work done by this force is equal to the change in the object’s kinetic energy:
  • \( W = K_f - K_i \)
Where \( W \) is the work done by the force, deriving from the measurable shift in kinetic energy from \(16.0 \, \mathrm{J}\) to \(36.0 \, \mathrm{J}\), resulting in \( W = 20.0 \, \mathrm{J}\). Understanding this, we see the profound connection between forces, work done, and kinetic energy changes.

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Most popular questions from this chapter

The force on a particle is directed along an \(x\) axis and given by \(F=F_{0}\left(x / x_{0}-1\right)\). Find the work done by the force in moving the particle from \(x=0\) to \(x=2 x_{0}\) by (a) plotting \(F(x)\) and measuring the work from the graph and (b) integrating \(F(x)\).

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