Problem 66
Question
A 6.00 -kg box sits on a ramp that is inclined at \(37.0^{\circ}\) above the horizontal. The coefficient of kinetic friction between the box and the ramp is \(\mu_{k}=0.30 .\) What horizontal force is required to move the box up the incline with a constant acceleration of 4.20 \(\mathrm{m} / \mathrm{s}^{2}\) ?
Step-by-Step Solution
Verified Answer
The horizontal force required is approximately 61.2 N.
1Step 1: Determine the Components of Gravity
First, we need to decompose the gravitational force acting on the box into components parallel and perpendicular to the inclined plane. The gravitational force can be calculated as \( F_g = mg \) where \( m = 6.00 \text{ kg} \) and \( g = 9.81 \text{ m/s}^2 \). The component along the ramp is \( F_{g, \, parallel} = mg \sin(\theta) \) and the component perpendicular to the ramp is \( F_{g, \, perpendicular} = mg \cos(\theta) \).
2Step 2: Calculate the Frictional Force
Using the component of gravity perpendicular to the incline, calculate the normal force since there is no vertical movement. Therefore, \( N = F_{g, \, perpendicular} = mg \cos(\theta) \). The frictional force \( f_k \) is then \( \mu_k N \).
3Step 3: Sum Forces Along the Incline
Applying Newton's second law along the ramp, the net force \( F_{net} \) required to achieve the acceleration of \( 4.20 \text{ m/s}^2 \) is given by \( F_{net} = ma = F_{applied} - F_{g, \, parallel} - f_k \), where \( F_{applied} \) is the component of the horizontal force along the ramp.
4Step 4: Relate Horizontal Force to Applied Force
The horizontal force \( F_h \) must be expressed in terms of its component along the incline. Since the ramp is inclined at \( 37.0^{\circ} \), \( F_{applied} = F_h \cos(\theta) \). Substitute into the equation from the previous step.
5Step 5: Solve for the Horizontal Force
Rearrange the equation from the previous step to solve for the horizontal force \( F_h \): \( F_h = \frac{ma + mg\sin(\theta) + f_k}{\cos(\theta)} \). Insert the values for each parameter: mass, gravity, friction coefficient, angle, and desired acceleration.
Key Concepts
Newton's Second LawInclined PlaneKinetic FrictionGravitational Force Decomposition
Newton's Second Law
Newton's Second Law is a foundational principle in physics that describes how the motion of an object changes when it is subjected to external forces. According to the law, the acceleration of an object depends on two variables: the net force acting upon the object and its mass. The law is typically expressed with the equation:
When dealing with objects on inclined planes, like the box in the problem, Newton's Second Law helps us determine the necessary force to achieve a specific acceleration. The net force will be a combination of the applied horizontal force, gravitational force, and frictional force acting on the box.
By calculating the net force required, students can find the necessary horizontal force which when applied, controls the box’s motion on the ramp.
- \( F_{net} = ma \)
When dealing with objects on inclined planes, like the box in the problem, Newton's Second Law helps us determine the necessary force to achieve a specific acceleration. The net force will be a combination of the applied horizontal force, gravitational force, and frictional force acting on the box.
By calculating the net force required, students can find the necessary horizontal force which when applied, controls the box’s motion on the ramp.
Inclined Plane
An inclined plane, or ramp, is a flat surface tilted at an angle to the horizontal. It serves as a simple machine making it easier to raise objects to higher heights. The angle of inclination affects how forces need to be calculated and applied. For our problem, the ramp is inclined at \( 37.0^{\circ} \).
The important forces to consider on an inclined plane include:
The important forces to consider on an inclined plane include:
- The gravitational force pulls the object downward.
- Perpendicular (normal) force acts at a right angle to the plane.
- Frictional force opposes the motion and acts along the plane.
Kinetic Friction
Kinetic friction is the resisting force that occurs when two surfaces move against each other. It plays a significant role in determining the amount of force required to move the box along the inclined plane. In our problem, the coefficient of kinetic friction \( \mu_k \) between the box and the ramp is given as \( 0.30 \).
The frictional force can be calculated using the formula:
Kinetic friction always acts in the opposite direction of the movement, so when you apply additional force to move the box up the plane, the friction will oppose it, requiring even more force.
The frictional force can be calculated using the formula:
- \( f_k = \mu_k N \)
Kinetic friction always acts in the opposite direction of the movement, so when you apply additional force to move the box up the plane, the friction will oppose it, requiring even more force.
Gravitational Force Decomposition
Gravitational force decomposition is a method used to simplify the analysis of motion on inclined planes. Instead of dealing with the gravitational force as a whole, it is broken down into components parallel and perpendicular to the plane. This decomposition helps us understand how much of the gravitational force contributes to downward motion and how much acts as a normal force.
For an inclined plane at an angle \( \theta \), the formulas are:
For an inclined plane at an angle \( \theta \), the formulas are:
- Parallel component: \( F_{g, \, parallel} = mg \sin(\theta) \)
- Perpendicular component: \( F_{g, \, perpendicular} = mg \cos(\theta) \)
Other exercises in this chapter
Problem 64
A 5.00 -kg box sits at rest at the bottom of a ramp that is 8.00 \(\mathrm{m}\) long and that is inclined at \(30.0^{\circ}\) above the horizontal. The coeffici
View solution Problem 65
Two boxes connected by a light horizontal rope are on a horizontal surface, as shown in Fig. P5.35. The coefficient of kinetic friction between each box and the
View solution Problem 69
Two bicycle tires are set rolling with the same initial speed of 3.50 \(\mathrm{m} / \mathrm{s}\) on a long, straight road, and the distance each travels before
View solution Problem 70
A block with mass \(M\) is attached to the lower end of a vertical, uniform rope with mass \(m\) and length \(L\) A constant upward force \(\vec{\boldsymbol{F}}
View solution