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Force \(\vec{F}=(-8.0 \mathrm{~N}) \hat{\mathrm{i}}+(6.0 \mathrm{~N}) \hat{\mathrm{j}}\) acts on a particle with position vector \(\vec{r}=(3.0 \mathrm{~m}) \hat{\mathrm{i}}+(4.0 \mathrm{~m}) \mathrm{j} .\) What are (a) the torque on the particle about the origin and (b) the angle between the directions of \(\vec{r}\) and \(\vec{F} ?\)

Short Answer

Expert verified
Torque is \( 50.0 \ \mathrm{mN} \ \hat{\mathrm{k}} \) and angle is \( 90^\circ \ \).

Step by step solution

01

Write Down Given Vectors

Force vector: \( \vec{F} = (-8.0 \ \mathrm{N}) \ \hat{\mathrm{i}} + (6.0 \ \mathrm{N}) \ \hat{\mathrm{j}} \)Position vector: \( \ \vec{r} = (3.0 \ \mathrm{m}) \ \hat{\mathrm{i}} + (4.0 \ \mathrm{m}) \ \hat{\mathrm{j}} \)
02

Calculate the Torque

The torque \( \vec{\tau} \) is given by the cross product of \( \vec{r} \) and \( \vec{F} \). \( \vec{\tau} = \vec{r} \ \times \ \vec{F} \) Calculate each component: \[ avigator.com{\tau} = (3.0 \ \mathrm{m}) \ \times (6.0 \ \mathrm{N}) - (4.0 \ \mathrm{m}) \ \times (-8.0 \ \mathrm{N}) \] \[ \vec{\tau} = (18.0 - (-32.0)) \ \hat{\mathrm{k}} \] \[ \vec{\tau} = 50.0 \ \mathrm{mN} \ \hat{\mathrm{k}} \]
03

Determine the Dot Product for the Angle Calculation

Find the dot product of \( \vec{r} \) and \( \vec{F} \).\( \ \vec{r} \ \cdot \ \vec{F} \):\[ \vec{r} \ \cdot \vec{F} = (3.0 \ \mathrm{m}) \ \cdot (-8.0 \ \mathrm{N}) + (4.0 \ \mathrm{m}) \ \cdot (6.0 \ \mathrm{N}) \]\[ \vec{r} \cdot \ \vec{F} = -24.0 + 24.0 \ = 0 \]
04

Calculate Magnitudes of Vectors

Find the magnitudes of \( \vec{r} \) and \( \vec{F} \).\( \|\vec{r}\| = \sqrt{(3.0 \ \mathrm{m})^{2} + (4.0 \ \mathrm{m})^{2}} = 5.0 \ \mathrm{m} \)\( \|\vec{F}\| = \sqrt{(-8.0 \ \mathrm{N})^{2} + (6.0 \ \mathrm{N})^{2}} = 10.0 \ \mathrm{N} \)
05

Use Dot Product to Find Angle

Since, \[ \vec{r} \ \cdot \ \vec{F} = \|\vec{r}\| \ \|\vec{F}\| \ \cdot \ \cos \theta = 0 \]Using \(\cos \theta \ = \ 0 \): \( \theta = 90^\circ \)

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Key Concepts

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

Cross Product
The cross product is a mathematical operation used to find a vector that is perpendicular to two given vectors. It is denoted by the symbol \( \times \).
In physics, torque (\( \vec{\tau} \)) can be calculated with the cross product of the position vector (\( \vec{r} \)) and the force vector (\( \vec{F} \)).
The formula for the cross product is:
\[ \vec{\tau} = \vec{r} \times \vec{F} \]When applied to our problem:
Force vector: \( \vec{F} = (-8.0 \mathrm{~N}) \hat{\mathrm{i}} + (6.0 \mathrm{~N}) \hat{\mathrm{j}} \)
Position vector: \( \vec{r} = (3.0 \mathrm{~m}) \hat{\mathrm{i}} + (4.0 \mathrm{~m}) \hat{\mathrm{j}} \)These vectors are used to find the torque.
The calculation with respective components gives:
\[ \vec{\tau} = (3.0 \mathrm{~m}) \times (6.0 \mathrm{~N}) - (4.0 \mathrm{~m}) \times (-8.0 \mathrm{~N}) \]
\[ \vec{\tau} = 50.0 \mathrm{~mN} \hat{\mathrm{k}} \] This result shows the torque around the origin.
Dot Product
The dot product is another mathematical operation, signifying the product of two vectors' magnitudes and the cosine of the angle between them. It is symbolized by \( \cdot \) and given by:
\[ \vec{A} \cdot \vec{B} = |\vec{A}| |\vec{B}| \cos \theta \]In our problem, it's used to find the angle between the force vector and the position vector.
The force vector: \( \vec{F} \)
The position vector: \( \vec{r} \)
The dot product calculates as:
\[ \vec{r} \cdot \vec{F} = (3.0 \mathrm{~m}) \cdot (-8.0 \mathrm{~N}) + (4.0 \mathrm{~m}) \cdot (6.0 \mathrm{~N}) = 0 \]
Since the dot product is zero, the cosine of the angle is zero. Therefore, the angle between them is 90 degrees.
Vector Magnitudes
The magnitude of a vector is its length or size and can be calculated using the Pythagorean theorem.
For any vector \( \vec{V} = a \hat{\mathrm{i}} + b \hat{\mathrm{j}} \),
The magnitude \( |\vec{V}| \) is given by:
\[ |\vec{V}| = \sqrt{a^2 + b^2} \] For the position vector \( \vec{r} \):
\[ |\vec{r}| = \sqrt{(3.0 \mathrm{~m})^2 + (4.0 \mathrm{~m})^2} = 5.0 \mathrm{~m} \]
For the force vector \( \vec{F} \):
\[ |\vec{F}| = \sqrt{(-8.0 \mathrm{~N})^2 + (6.0 \mathrm{~N})^2} = 10.0 \mathrm{~N} \]
The magnitude thus provides information about the size of these vectors.
Force Vector
A force vector represents a force applied in a specific direction and has both magnitude and direction.
In mathematical terms, it is expressed as:
\[ \vec{F} = F_x \hat{\mathrm{i}} + F_y \hat{\mathrm{j}} \]
For our problem, the force vector is:
\( \vec{F} = (-8.0 \mathrm{~N}) \hat{\mathrm{i}} + (6.0 \mathrm{~N}) \hat{\mathrm{j}} \)
This identifies 8.0 N in the negative x-direction and 6.0 N in the positive y-direction.
Force vectors are significant in torque calculations because they show how force applied can cause rotational motion.
Position Vector
The position vector indicates a specific point in space relative to an origin. It also has both magnitude and direction.
It is expressed as:
\[ \vec{r} = r_x \hat{\mathrm{i}} + r_y \hat{\mathrm{j}} \] In our problem, the position vector is:
\( \vec{r} = (3.0 \mathrm{~m}) \hat{\mathrm{i}} + (4.0 \mathrm{~m}) \hat{\mathrm{j}} \)
This denotes a point 3.0 meters along the x-axis and 4.0 meters along the y-axis.
You use this vector during cross product calculations to compute torque as it shows the point of force application relative to the origin.

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Most popular questions from this chapter

A horizontal vinyl record of mass \(0.10 \mathrm{~kg}\) and radius \(0.10 \mathrm{~m}\) rotates freely about a vertical axis through its center with a rotational speed of \(4.7 \mathrm{rad} / \mathrm{s}\). The rotational inertia of the record about its axis of rotation is \(5.0 \times 10^{-4} \mathrm{~kg} \cdot \mathrm{m}^{2} .\) A wad of wet putty of mass \(0.020 \mathrm{~kg}\) drops vertically onto the record from above and sticks to the edge of the record. What is the rotational speed of the record immediately after the putty sticks to it?

Two disks are mounted on low-friction bearings on the same axle and can be brought together so that they couple and rotate as one unit. (a) The first disk, with rotational inertia \(3.3 \mathrm{~kg} \cdot \mathrm{m}^{2}\) about its central axis, is set spinning at 450 rev/min. The second disk, with rotational inertia \(6.6 \mathrm{~kg} \cdot \mathrm{m}^{2}\) about its central axis, is set spinning at 900 rev/min in the same direction as the first. They then couple together. What is their rotational speed after coupling? (b) If instead the second disk is set spinning at 900 rev/min in the direction opposite the first disk's rotation, what is their rotational speed and direction of rotation after coupling?

A refrigerator has separate shelves on the door for storing bottles. Thin plastic straps keep the bottles from falling off the door. Someone in the house slams the door with a bit too much vigor and a heavy bottle breaks the strap. Do you think the bottle would be more likely to break the plastic strap if it is close to the hinge? Close to the handle? Or doesn't it matter? Explain your answer in terms of the physics we have learned.

What is the torque about the origin on a jar of jalapeño peppers located at coordinates \((3.0 \mathrm{~m},-2.0 \mathrm{~m}, 4.0 \mathrm{~m})\) due to (a) force \(\vec{F}_{A}=(3.0 \mathrm{~N}) \hat{\mathrm{i}}-(4.0 \mathrm{~N}) \hat{\mathrm{j}}+(5.0 \mathrm{~N}) \hat{\mathrm{k}},(\mathrm{b})\) force \(\vec{F}_{B}=\) \((-3.0 \mathrm{~N}) \hat{\mathrm{i}}-(4.0 \mathrm{~N}) \hat{\mathrm{j}}-(5.0 \mathrm{~N}) \hat{\mathrm{k}}\), and \((\mathrm{c})\) the vector sum of \(\vec{F}_{A}\) and \(\vec{F}_{B} ?\) (d) Repeat part (c) about a point with coordinates \((3.0 \mathrm{~m},\), \(2.0 \mathrm{~m}, 4.0 \mathrm{~m}\) ) instead of about the origin.

Two particles, each of mass \(m\) and speed \(v\), travel in opposite directions along parallel lines separated by a distance \(d\). (a) In terms of \(m, v\), and \(d\), find an expression for the magnitude \(L\) of the rotational momentum of the two-particle system around a point midway between the two lines. (b) Does the expression change if the point about which \(L\) is calculated is not midway between the lines? (c) Now reverse the direction of travel for one of the particles and repeat (a) and (b).

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