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A \(2.00 \mathrm{~kg}\) object is subjected to three forces that give it an acceleration \(\vec{a}=-\left(8.00 \mathrm{~m} / \mathrm{s}^{2}\right) \hat{\mathrm{i}}+\left(6.00 \mathrm{~m} / \mathrm{s}^{2}\right) \hat{\mathrm{j}} . \quad\) If two of the three forces are \(\vec{F}_{1}=(30.0 \mathrm{~N}) \hat{\mathrm{i}}+(16.0 \mathrm{~N}) \hat{\mathrm{j}}\) and \(\vec{F}_{2}=\) \(-(12.0 \mathrm{~N}) \hat{\mathrm{i}}+(8.00 \mathrm{~N}) \hat{\mathrm{j}},\) find the third force.

Short Answer

Expert verified
The third force is \((-34.0 \text{ N}) \hat{i} + (-12.0 \text{ N}) \hat{j}\).

Step by step solution

01

Understand the Net Force Equation

The net force acting on the object is given by Newton's second law of motion: \( \vec{F}_{net} = m \cdot \vec{a} \), where \( m \) is the mass and \( \vec{a} \) is the acceleration.
02

Calculate the Net Force

Substitute the given values into the formula: \( \vec{F}_{net} = 2.00 \text{ kg} \times \left( -8.00 \text{ m/s}^2 \hat{i} + 6.00 \text{ m/s}^2 \hat{j} \right) = (-16.0 \text{ N}) \hat{i} + (12.0 \text{ N}) \hat{j} \).
03

Set Up the Equation for the Third Force

The net force is also the sum of the three forces: \( \vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2} + \vec{F}_{3} \). We need to solve this equation for \( \vec{F}_{3} \).
04

Solve for the Third Force

Using the equation \( \vec{F}_{3} = \vec{F}_{net} - \vec{F}_{1} - \vec{F}_{2} \), substitute the known values: \( \vec{F}_{3} = [(-16.0 \text{ N}) \hat{i} + (12.0 \text{ N}) \hat{j}] - [(30.0 \text{ N}) \hat{i} + (16.0 \text{ N}) \hat{j}] - [(-12.0 \text{ N}) \hat{i} + (8.0 \text{ N}) \hat{j}] \).
05

Compute the Components of the Third Force

Calculate the individual components: \(\\ \vec{F}_{3_x} = -16.0 \text{ N} - 30.0 \text{ N} + 12.0 \text{ N} = -34.0 \text{ N} \ \vec{F}_{3_y} = 12.0 \text{ N} - 16.0 \text{ N} - 8.0 \text{ N} = -12.0 \text{ N} \\).
06

Write Down the Third Force

The third force is therefore: \( \vec{F}_{3} = (-34.0 \text{ N}) \hat{i} + (-12.0 \text{ N}) \hat{j} \).

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Key Concepts

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

Net Force
When studying forces acting on an object, it's essential to understand the concept of net force. Net force is the overall force resulting from the combination of all individual forces acting on an object. According to Newton's Second Law, it is described by the equation \( \vec{F}_{net} = m \cdot \vec{a} \), where \( m \) is the mass of the object, and \( \vec{a} \) is its acceleration.

To find the net force, you need to account for all the forces involved. Begin by identifying all the forces acting on the object. Once the individual forces are identified, their vector components are added together to yield the net force.

In the given exercise, a 2.00 kg object is subjected to an acceleration of \((-8.00 \, \text{m/s}^2) \hat{i} + (6.00 \, \text{m/s}^2) \hat{j}\). The net force on the object can be found using the equation:

\[ \vec{F}_{net} = 2.00 \, \text{kg} \times \left( (-8.00 \, \text{m/s}^2) \hat{i} + (6.00 \, \text{m/s}^2) \hat{j} \right) = (-16.0 \, \text{N}) \hat{i} + (12.0 \, \text{N}) \hat{j}.\]
Vector Components
The forces in this exercise are presented as vectors, expressed with both magnitude and direction. In vector notation, individual components in different directions can be represented separately using unit vectors—\(\hat{i}\) for the x-direction and \(\hat{j}\) for the y-direction.

Understanding vector components allows us to work with each direction individually. For instance, if you have a force \( \vec{F}_{1} = (30.0 \, \text{N}) \hat{i} + (16.0 \, \text{N}) \hat{j} \), the vector components are:

  • \(30.0 \, \text{N}\) along the x-axis (\(\hat{i}\)).
  • \(16.0 \, \text{N}\) along the y-axis (\(\hat{j}\)).
Every force can be dissected similarly, focusing on its impact in each dimension separately, thereby simplifying the calculations as you sum or subtract these components individually to determine the net force.
Force Calculation
Force calculation involves understanding how individual forces work together or against each other, impacting the motion of an object. Using the information from net force and vector components, you can determine unknown forces by rearranging known equations.

In the exercise, you want to find the third unknown force, \(\vec{F}_{3}\). The relationship given by Newton's law is:\[ \vec{F}_{net} = \vec{F}_{1} + \vec{F}_{2} + \vec{F}_{3}. \]
To solve for \(\vec{F}_{3}\), you rearrange this equation to:

\( \vec{F}_{3} = \vec{F}_{net} - \vec{F}_{1} - \vec{F}_{2}.\)

By substituting the values, \(\vec{F}_{net} = (-16.0 \, \text{N}) \hat{i} + (12.0 \, \text{N}) \hat{j}, \vec{F}_{1} = (30.0 \, \text{N}) \hat{i} + (16.0 \, \text{N}) \hat{j}, \) and \(\vec{F}_{2} = (-12.0 \, \text{N}) \hat{i} + (8.00 \, \text{N}) \hat{j},\) you can compute:

  • For the x-component: \[-16.0 \, \text{N} - (30.0 \, \text{N}) + (-12.0 \, \text{N}) = -34.0 \, \text{N}\]
  • For the y-component: \[12.0 \, \text{N} - (16.0 \, \text{N}) - (8.0 \, \text{N}) = -12.0 \, \text{N}\]
Thus, the third force \(\vec{F}_{3} = (-34.0 \, \text{N}) \hat{i} + (-12.0 \, \text{N}) \hat{j}.\) By decomposing and calculating forces this way, you gain a clear understanding of how different forces act on an object to produce motion.

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Most popular questions from this chapter

An interstellar ship has a mass of \(1.20 \times 10^{6} \mathrm{~kg}\) and is initially at rest relative to a star system. (a) What constant acceleration is needed to bring the ship up to a speed of \(0.10 c\) (where \(c\) is the speed of light, \(\left.3.0 \times 10^{8} \mathrm{~m} / \mathrm{s}\right)\) relative to the star system in 3.0 days? (b) What is that acceleration in \(g\) units? (c) What force is required for the acceleration? (d) If the engines are shut down when \(0.10 c\) is reached (the speed then remains constant), how long does the ship take (start to finish) to journey 5.0 light-months, the distance that light travels in 5.0 months?

A car that weighs \(1.30 \times 10^{4} \mathrm{~N}\) is initially moving at \(40 \mathrm{~km} / \mathrm{h}\) when the brakes are applied and the car is brought to a stop in \(15 \mathrm{~m} .\) Assuming the force that stops the car is constant, find (a) the magnitude of that force and (b) the time required for the change in speed. If the initial speed is doubled, and the car experiences the same force during the braking, by what factors are (c) the stopping distance and (d) the stopping time multiplied? (There could be a lesson here about the danger of driving at high speeds.)

While two forces act on it, a particle is to move at the constant velocity \(\vec{v}=(3 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{i}}-(4 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{j}}\). One of the forces is \(\vec{F}_{1}=(2 \mathrm{~N}) \hat{\mathrm{i}}+\) \((-6 \mathrm{~N}) \hat{\mathrm{j}} .\) What is the other force?

A customer sits in an amusement park ride in which the compartment is to be pulled downward in the negative direction of a \(y\) axis with an acceleration magnitude of \(1.24 g,\) with \(g=9.80 \mathrm{~m} / \mathrm{s}^{2}\). A \(0.567 \mathrm{~g}\) coin rests on the customer's knee. Once the motion begins and in unit-vector notation, what is the coin's acceleration relative to (a) the ground and (b) the customer? (c) How long does the coin take to reach the compartment ceiling, \(2.20 \mathrm{~m}\) above the knee? In unit-vector notation, what are (d) the actual force on the coin and (e) the apparent force according to the customer's measure of the coin's acceleration?

If the 1 kg standard body is accelerated by only \(\vec{F}_{1}=(3.0 \mathrm{~N}) \hat{\mathrm{i}}+(4.0 \mathrm{~N}) \hat{\mathrm{j}}\) and \(\vec{F}_{2}=(-2.0 \mathrm{~N}) \hat{\mathrm{i}}+(-6.0 \mathrm{~N}) \hat{\mathrm{j}},\) then what is \(\vec{F}_{\text {net }}\) (a) in unit-vector notation and as (b) a magnitude and (c) an angle relative to the positive \(x\) direction? What are the (d) magnitude and (e) angle of \(\vec{a}\) ?

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