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According to the manual of a certain car, a maximum torque of magnitude \(65.0 \mathrm{~N} \cdot \mathrm{m}\) should be applied when tightening the lug nuts on the vehicle. If you use a wrench of length \(0.330 \mathrm{~m}\) and you apply the force at the end of the wrench at an angle of \(75.0^{\circ}\) with respect to a line going from the lug nut through the end of the handle, what is the magnitude of the maximum force you can exert on the handle without exceeding the recommendation?

Short Answer

Expert verified
The maximum force that can be exerted on the handle without exceeding the recommendation is \( 226.29 \) N.

Step by step solution

01

Convert the angle from degrees to radians

The angle (\( \theta \)) is given in degrees, but trigonometric functions typically assume the angle is in radians, so the angle needs to be converted into radians using the formula \( \theta_{rad} = \theta_{deg} \times \frac{\pi}{180} \). Here, \( \theta_{deg} = 75.0 \) degrees, therefore \( \theta_{rad} = 75.0 \times \frac{\pi}{180} = 1.31 \) radians.
02

Rearrange the torque formula to solve for Force

Next, rearrange the formula for torque (\( \tau = rFsin\theta \)) to solve for force (F). Doing this gives \( F = \frac{\tau}{rsin\theta} \).
03

Substitute the values into the formulated equation

Substitute the given values into the equation: \( F = \frac{65.0}{0.330 \times sin(1.31)} \)
04

Simplify to get the magnitude of the force

After substituting, simplify to find the magnitude of the force. This gives \( F = 226.29 \) N or Newtons as the maximum force that can be exerted without exceeding the recommended maximum torque.

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Key Concepts

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

Force calculation
Calculating force is essential when you're dealing with different physical applications, such as tightening a lug nut on a vehicle. In this exercise, we've encountered a situation where we need to adhere to a maximum torque, which is a measure of the force causing an object to rotate. Torque is represented by the formula:
  • \( \tau = r \times F \times \sin(\theta) \)
Here, \( r \) is the length of the wrench (the lever arm), \( F \) is the force applied at the end of the wrench, and \( \theta \) is the angle at which force is applied relative to the lever arm.
To calculate the force exerted without exceeding the torque limit, we rearrange the torque formula to solve for force (\( F \)) as follows:
  • \( F = \frac{\tau}{r \times \sin(\theta)} \)
By substituting the values like torque, the length of the wrench, and the appropriate angle, you can compute the specific force that can be safely applied. In this exercise, the calculated force turned out to be \( 226.29 \) N.
Radians conversion
Angles are often presented in degrees, but most trigonometric functions in physics use radians. Therefore, converting degrees to radians is a common step in these calculations.
The conversion between degrees and radians uses the formula:
  • \( \theta_{rad} = \theta_{deg} \times \frac{\pi}{180} \)
In this exercise, the angle given was \( 75.0^{\circ} \), which you converted to radians by multiplying by \( \frac{\pi}{180} \). This results in an angle of approximately \( 1.31 \) radians.
Remembering this conversion factor is quite handy since many scientific calculators will require angle inputs in radians when performing trigonometric calculations.
Trigonometric functions
Understanding trigonometric functions is essential to solving problems involving angles. These functions, such as sine (\( \sin \)), cosine (\( \cos \)), and tangent (\( \tan \)), help describe the relationship between the angles and sides of a triangle.
In torque problems, the sine function is particularly important. When a force is applied at an angle, it's only the component of the force that acts perpendicular to the lever arm which contributes to torque. This is why the torque formula uses \( \sin(\theta) \).
  • \( \sin(\theta) \) represents the ratio of the opposite side over the hypotenuse in a right-angle triangle
By applying \( \sin(1.31) \) in the exercise, we find the effective force component that influences torque, allowing us to solve for the correct force magnitude without exceeding the limit. Always ensure angle measures are properly converted and applied in these calculations for accurate results.

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Most popular questions from this chapter

A rope of negligible mass is wrapped around a 225-kg solid cylinder of radius \(0.400 \mathrm{~m}\). The cylinder is suspended several meters off the ground with its axis oriented horizontally, and turns on that axis without friction. (a) If a \(75.0\) -kg man takes hold of the free end of the rope and falls under the force of gravity, what is his acceleration? (b) What is the angular acceleration of the cylinder? (c) If the mass of the rope were not neglected, what would happen to the angular acceleration of the cylinder as the man falls?

Consider the following mass distribution, where \(x\) - and \(y\) -coordinates are given in meters: \(5.0 \mathrm{~kg}\) at \((0.0,0.0) \mathrm{m}\) \(3.0 \mathrm{~kg}\) at \((0.0,4.0) \mathrm{m}\), and \(4.0 \mathrm{~kg}\) at \((3.0,0.0) \mathrm{m} .\) Where should a fourth object of \(8.0 \mathrm{~kg}\) be placed so that the center of gravity of the four-object arrangement will be at \((0.0,0.0) \mathrm{m} ?\)

Each of the following objects has a radius of \(0.180 \mathrm{~m}\) and a mass of \(2.40 \mathrm{~kg}\), and each rotates about an axis through its center (as in Table 8.1) with an angular speed of \(35.0 \mathrm{rad} / \mathrm{s}\). Find the magnitude of the angular momentum of cach object. (a) a hoop (b) a solid cylinder (c) a solid sphere (d) a hollow spherical shell

A solid uniform sphere of mass \(m\) and radius \(R\) rolls without slipping down an incline of height \(h\). (a) What forms of mechanical energy are associated with the sphere at any point along the incline when its angular speed is \(\omega\) ? Answer in words and symbolically in terms of the quantities \(m, g, y, I, \omega\), and \(u\) (b) What force acting on the sphere causes it to roll rather than slip down the incline? (c) Determine the ratio of the sphere's rotational kinetic energy to its total kinetic energy at any instant.

A student sits on a rotating stool holding two \(3.0-\mathrm{kg}\) objects. When his arms are extended horizontally, the objects are \(1.0 \mathrm{~m}\) from the axis of rotation and he rotates with an angular speed of \(0.75 \mathrm{rad} / \mathrm{s}\). The moment of incrtia of the student plus stool is \(3.0 \mathrm{~kg} \cdot \mathrm{m}^{2}\) and is assumed to be constant. The student then pulls in the objects horizontally to \(0.30 \mathrm{~m}\) from the rotation axis. (a) Find the new angular speed of the student. (b) Find the kinetic energy of the student before and after the objects are pulled in.

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