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Mass on a plane \(\mathrm{A}\) 100-kg object rests on an inclined plane at an angle of \(30^{\circ}\) to the floor. Find the components of the force perpendicular to and parallel to the plane. (The vertical component of the force exerted by an object of mass \(m\) is its weight, which is \(m g\) where \(g=9.8 \mathrm{m} / \mathrm{s}^{2}\) is the acceleration due to gravity.)

Short Answer

Expert verified
The components of the force perpendicular to and parallel to the inclined plane are approximately 848.28 N and 490 N, respectively.

Step by step solution

01

Calculate the Weight of the Object

To find the vertical component of the force exerted by the object, we need to calculate its weight. The weight of the object can be found using the formula: Weight = mass × gravitational acceleration. Given, mass (m) = 100 kg gravitational acceleration (g) = 9.8 m/s² Weight = m × g = 100 kg × 9.8 m/s² = 980 N (Newtons)
02

Find the Components of the Force

Now, we need to find the components of the force, which are perpendicular to and parallel to the inclined plane. To do that, we can use the following trigonometric relationships: 1. Perpendicular component of the force (F⊥) = Weight × cos(θ) 2. Parallel component of the force (F∥) = Weight × sin(θ) Given, θ = 30°
03

Calculate the Perpendicular Component of the Force

To find the perpendicular component of the force, we can apply the first trigonometric relationship: F⊥ = Weight × cos(θ) = 980 N × cos(30°) Use a calculator to find the cosine of 30°: cos(30°) ≈ 0.866 F⊥ ≈ 980 N × 0.866 ≈ 848.28 N The perpendicular component of the force is approximately 848.28 N.
04

Calculate the Parallel Component of the Force

To find the parallel component of the force, we can apply the second trigonometric relationship: F∥ = Weight × sin(θ) = 980 N × sin(30°) Use a calculator to find the sine of 30°: sin(30°) ≈ 0.5 F∥ ≈ 980 N × 0.5 ≈ 490 N The parallel component of the force is approximately 490 N. To summarize, the components of the force perpendicular to and parallel to the inclined plane are approximately 848.28 N and 490 N, respectively.

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Key Concepts

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

Force Components
When an object is placed on an inclined plane, its weight force can be split into two parts: perpendicular to the plane and parallel to the plane. Understanding these components is crucial to solving problems related to inclined planes.
  • The perpendicular component is responsible for the object's normal force, which is the force pressing it into the surface.
  • The parallel component causes the object to slide down the plane if unopposed by friction or other forces.
Breaking down the weight force into these components helps us analyze the object's behavior. This is particularly important in physics and engineering, where analyzing how forces act in different directions allows us to make precise calculations.
Trigonometric Relationships
To accurately find the force components on an inclined plane, we use trigonometric relationships. These relationships are central to decomposing the force of gravity acting on the object. For an incline at angle
  • The perpendicular component is calculated using the cosine function: \[F_\perp = \text{Weight} \times \cos(\theta)\]
  • The parallel component uses the sine function: \[F_{\parallel} = \text{Weight} \times \sin(\theta)\]
Here, \(\theta\) is the angle of the inclined plane, and using these functions allows us to separate the weight into its respective components accurately. These calculations help predict how the object will move or remain stationary on the incline.
Gravity Force
Gravity is the force that pulls objects downward towards Earth. On an inclined plane, gravity acts on the object to create its weight force, which can be calculated by multiplying its mass by the gravitational acceleration (\(g = 9.8 \, \text{m/s}^2\)). Gravity always acts vertically downward, but when dealing with an inclined plane, we need to consider how this vertical force splits into two components due to the angle of the incline.
  • The weight of the object on the inclined plane is given by: \[\text{Weight} = m \times g = 100 \, \text{kg} \times 9.8 \, \text{m/s}^2 = 980 \, \text{N}\]
This weight is then used to find the force components, enabling us to understand how gravity influences the object's behavior on the slope. These calculations are essential in physics to predict movement and ensure stability in practical situations.

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Most popular questions from this chapter

Given a fixed vector \(\mathbf{v},\) there is an infinite set of vectors \(\mathbf{u}\) with the same value of proj\(_{\mathbf{v}} \mathbf{u}\). Let \(\mathbf{v}=\langle 0,0,1\rangle .\) Give a description of all position vectors \(\mathbf{u}\) such that \(\operatorname{proj}_{\mathbf{v}} \mathbf{u}=\operatorname{proj}_{\mathbf{v}}\langle 1,2,3\rangle\).

Zero curvature Prove that the curve $$ \mathbf{r}(t)=\left\langle a+b t^{p}, c+d t^{p}, e+f t^{p}\right\rangle $$ where \(a, b, c, d, e,\) and \(f\) are real numbers and \(p\) is a positive integer, has zero curvature. Give an explanation.

An object on an inclined plane does not slide provided the component of the object's weight parallel to the plane \(\left|\mathbf{W}_{\text {par }}\right|\) is less than or equal to the magnitude of the opposing frictional force \(\left|\mathbf{F}_{\mathrm{f}}\right|\). The magnitude of the frictional force, in turn, is proportional to the component of the object's weight perpendicular to the plane \(\left|\mathbf{W}_{\text {perp }}\right|\) (see figure). The constant of proportionality is the coefficient of static friction, \(\mu\) a. Suppose a 100 -lb block rests on a plane that is tilted at an angle of \(\theta=20^{\circ}\) to the horizontal. Find \(\left|\mathbf{W}_{\text {parl }}\right|\) and \(\left|\mathbf{W}_{\text {perp }}\right|\) b. The condition for the block not sliding is \(\left|\mathbf{W}_{\mathrm{par}}\right| \leq \mu\left|\mathbf{W}_{\text {perp }}\right| .\) If \(\mu=0.65,\) does the block slide? c. What is the critical angle above which the block slides with \(\mu=0.65 ?\)

Let \(D\) be a solid heat-conducting cube formed by the planes \(x=0, x=1, y=0, y=1, z=0,\) and \(z=1 .\) The heat flow at every point of \(D\) is given by the constant vector \(\mathbf{Q}=\langle 0,2,1\rangle\) a. Through which faces of \(D\) does \(Q\) point into \(D ?\) b. Through which faces of \(D\) does \(\mathbf{Q}\) point out of \(D ?\) c. On which faces of \(D\) is \(Q\) tangential to \(D\) (pointing neither in nor out of \(D\) )? d. Find the scalar component of \(\mathbf{Q}\) normal to the face \(x=0\). e. Find the scalar component of \(\mathbf{Q}\) normal to the face \(z=1\). f. Find the scalar component of \(\mathbf{Q}\) normal to the face \(y=0\).

Practical formula for \(\mathbf{N}\) Show that the definition of the principal unit normal vector $\mathbf{N}=\frac{d \mathbf{T} / d s}{|d \mathbf{T} / d s|}\( implies the practical formula \)\mathbf{N}=\frac{d \mathbf{T} / d t}{|d \mathbf{T} / d t|} .\( Use the Chain Rule and Note that \)|\mathbf{v}|=d s / d t>0.$

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