/*! 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 6 A metal bar is in the \(x y\) -p... [FREE SOLUTION] | 91Ó°ÊÓ

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A metal bar is in the \(x y\) -plane with one end of the bar at the origin. A force \(\overrightarrow{\boldsymbol{F}}=(7.00 \mathrm{~N}) \hat{\imath}+(-3.00 \mathrm{~N}) \hat{\jmath}\) is applied to the bar at the point \(x=3.00 \mathrm{~m}, y=4.00 \mathrm{~m} .\) (a) In terms of unit vectors \(\hat{\imath}\) and \(\hat{\jmath},\) what is the position vector \(\vec{r}\) for the point where the force is applied? (b) What are the magnitude and direction of the torque with respect to the origin produced by \(\overrightarrow{\boldsymbol{F}} ?\)

Short Answer

Expert verified
(a) \( \vec{r} = (3.00 \, \text{m}) \hat{\imath} + (4.00 \, \text{m}) \hat{\jmath} \). (b) Magnitude: 37.00 Nâ‹…m, Direction: into the plane.

Step by step solution

01

Find the Position Vector

The position vector \( \vec{r} \) is given by the coordinates of the point where the force is applied, \( x = 3.00 \, \text{m} \) and \( y = 4.00 \, \text{m} \). Therefore, the position vector in terms of the unit vectors \( \hat{\imath} \) and \( \hat{\jmath} \) is \( \vec{r} = (3.00 \, \text{m}) \hat{\imath} + (4.00 \, \text{m}) \hat{\jmath} \).
02

Calculate the Torque

Torque \( \vec{\tau} \) is given by the cross product of the position vector \( \vec{r} \) and the force vector \( \vec{F} \). The cross product in two dimensions is calculated as follows: \( \vec{\tau} = \vec{r} \times \vec{F} = |\begin{array}{cc} 3.00 \, \text{m} & 4.00 \, \text{m} \ 7.00 \, \text{N} & -3.00 \, \text{N} \end{array}| \). This results in \( \vec{\tau} = (3.00)(-3.00) - (4.00)(7.00) \).
03

Evaluate the Determinant

Calculate the determinant to find the torque: \( \vec{\tau} = (3.00)(-3.00) - (4.00)(7.00) = -9.00 - 28.00 = -37.00 \, \text{N}\cdot\text{m} \).
04

Determine Direction of Torque

In the 2-dimensional problem, the direction of torque can be inferred as perpendicular to the plane, along the \( \hat{k} \) direction. Since the torque \( \vec{\tau} \) is negative, this indicates the direction is into the plane (negative \( \hat{k} \)).

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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 an essential tool in physics and engineering, especially for calculating torque. It involves determining the product of two vectors, resulting in a third vector that is perpendicular to the plane containing the initial vectors.
In this exercise, we calculate the cross product of a position vector \( \vec{r} \) and a force vector \( \vec{F} \) to find the torque \( \vec{\tau} \). The cross product is typically defined in a three-dimensional space, but it simplifies in two dimensions where results are along the \( \hat{k} \) direction, indicating the torque's perpendicular nature to the xy-plane.
The cross product in two dimensions is represented by the determinant \( | \begin{array}{cc} x & y \ f_x & f_y \end{array} | \), which simplifies to express a scalar value indicating the magnitude of the torque.
Position Vector
The position vector is crucial when calculating torque, as it defines the point of application of force relative to the origin or another reference point.
In our problem, the position vector \( \vec{r} \) represents the coordinates of the force's point of application in the xy-plane, given by \( \vec{r} = (3.00 \, \text{m}) \hat{\imath} + (4.00 \, \text{m}) \hat{\jmath} \). This vector quantifies the position of the force relative to the origin (0,0), providing a way to determine how effectively a force can induce rotational motion.
The position vector plays a critical role when we calculate torque, as it determines the lever arm which directly influences the torque's magnitude.
Force Vector
The force vector shows the direction and magnitude of the given force applied to an object. In this exercise, the force vector \( \vec{F} \) is \( (7.00 \, \text{N}) \hat{\imath} + (-3.00 \, \text{N}) \hat{\jmath} \).
This vector indicates that:
  • \(7.00 \, \text{N}\) of force is acting in the positive x-direction.
  • \(-3.00 \, \text{N}\) points in the negative y-direction.
Understanding the components of a force vector is imperative for calculating resulting effects like torque, where different vector components interact to produce rotation.
By manipulating force vectors, we can predict and analyze the impact they will have on an object or a system.
Determinants
Determinants provide us with a mathematical function to extract useful scalar information from a matrix, often used to solve systems of linear equations and calculate vector products like the cross product.
In torque calculations, the determinant simplifies finding the cross product in two dimensions. By organizing the components of our position and force vectors into a 2x2 matrix, we can quickly evaluate the determinant which corresponds to the magnitude of the torque.
In our exercise, the cross product and hence the determinant \( | \begin{array}{cc} 3.00 \, \text{m} & 4.00 \, \text{m} \ 7.00 \, \text{N} & -3.00 \, \text{N} \end{array} | \) is calculated as \( -37.00 \, \text{N}\cdot\text{m} \), indicating both the torque's magnitude and its sense of rotation. Understanding how to evaluate determinants is key in applications like these, ensuring accurate calculations and analyses.

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Most popular questions from this chapter

A doubling of the torque produces a greater angular acceleration. Which of the following would do this, assuming that the tension in the rope doesn't change? (a) Increasing the pulley diameter by a factor of \(\sqrt{ 2 }\); (b) increasing the pulley diameter by a factor of 2; (c) increasing the pulley diameter by a factor of 4; (d) decreasing the pulley diameter by a factor of \(\sqrt{ 2 }\).

We can roughly model a gymnastic tumbler as a uniform solid cylinder of mass 75 kg and diameter 1.0 m. If this tumbler rolls forward at 0.50 rev/s, (a) how much total kinetic energy does he have, and (b) what percent of his total kinetic energy is rotational?

The moment of inertia of the empty turntable is \(1.5 \mathrm{~kg} \mathrm{~m}^{2}\). With a constant torque of \(2.5 \mathrm{~N} \cdot \mathrm{m},\) the turntable-person system takes \(3.0 \mathrm{~s}\) to spin from rest to an angular speed of \(1.0 \mathrm{rad} / \mathrm{s}\). What is the person's moment of inertia about an axis through her center of mass? Ignore friction in the turntable axle. (a) \(2.5 \mathrm{~kg} \cdot \mathrm{m}^{2}\) (b) \(6.0 \mathrm{~kg} \cdot \mathrm{m}^{2}\) (c) \(7.5 \mathrm{~kg} \cdot \mathrm{m}^{2}\) (d) \(9.0 \mathrm{~kg} \cdot \mathrm{m}^{2}\).

A 5.00-kg ball is dropped from a height of 12.0 m above one end of a uniform bar that pivots at its center. The bar has mass 8.00 kg and is 4.00 m in length. At the other end of the bar sits another 5.00-kg ball, unattached to the bar. The dropped ball sticks to the bar after the collision. How high will the other ball go after the collision?

A solid ball is released from rest and slides down a hillside that slopes downward at 65.0\(^\circ\) from the horizontal. (a) What minimum value must the coefficient of static friction between the hill and ball surfaces have for no slipping to occur? (b) Would the coefficient of friction calculated in part (a) be sufficient to prevent a hollow ball (such as a soccer ball) from slipping? Justify your answer. (c) In part (a), why did we use the coefficient of static friction and not the coefficient of kinetic friction?

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