Problem 25
Question
(II) A small block of mass \(m\) is given an initial speed \(v_{0}\) up a ramp inclined at angle \(\theta\) to the horizontal. It travels a distance \(d\) up the ramp and comes to rest. ( \(a\) ) Determine a formula for the coefficient of kinetic friction between block and ramp. (b) What can you say about the value of the coefficient of static friction?
Step-by-Step Solution
Verified Answer
(a) \( \mu_k = \frac{\frac{1}{2} mv_0^2 - mgd \sin \theta}{mgd \cos \theta} \); (b) \( \mu_s > \mu_k \).
1Step 1: Understand the forces involved
When the block moves up the ramp, there are several forces acting on it: gravitational force, normal force, and frictional force. The frictional force is what opposes the motion of the block as it goes up the ramp.
2Step 2: Write the force equations
The block travels until it comes to rest, meaning the net work done on it is zero. The work done by the friction force and gravity is equal to the initial kinetic energy. The component of gravitational force along the plane is given by \(mg \sin \theta\) and the friction force is \( \mu_k N\), where \( \mu_k \) is the coefficient of kinetic friction.
3Step 3: Express normal force
The normal force \(N\) is equal to the component of the gravitational force perpendicular to the plane, which is \(mg \cos \theta\).
4Step 4: Apply energy conservation
The initial kinetic energy is given by \( \frac{1}{2} mv_0^2 \). As the block comes to rest, this is equal to the work done by both gravity and friction: \[ \frac{1}{2} mv_0^2 = mgd \sin \theta + \mu_k mgd \cos \theta \].
5Step 5: Solve for the coefficient of kinetic friction
Rearrange the equation from the previous step to solve for \( \mu_k \): \[ \mu_k = \frac{\frac{1}{2} mv_0^2 - mgd \sin \theta}{mgd \cos \theta} \].
6Step 6: Consider the static friction
The static friction coefficient \( \mu_s \) must be greater than the kinetic friction coefficient \( \mu_k \), because static friction always exceeds kinetic friction under static conditions, ensuring the block does not slide back down initially.
Key Concepts
Inclined PlaneNormal ForceEnergy Conservation
Inclined Plane
An inclined plane is a flat surface tilted at an angle to the horizontal.
This simple concept is useful because it allows objects to travel vertically using less force than lifting straight up.
In the context of physics problems, an inclined plane might represent a ramp or a slope. When dealing with inclined planes, several important forces come into play:
This simple concept is useful because it allows objects to travel vertically using less force than lifting straight up.
In the context of physics problems, an inclined plane might represent a ramp or a slope. When dealing with inclined planes, several important forces come into play:
- The gravitational force pulls the object downwards.
- The normal force is the perpendicular force exerted by the plane on the object.
- The frictional force resists the motion of the object along the plane.
Normal Force
The normal force always acts perpendicular to the surface of contact.
On an inclined plane, it is crucial to remember that the normal force is not equal to the gravitational force.
Instead, it equals the component of the gravitational force that acts perpendicular to the plane.Given the angle of the incline, we can calculate the normal force using the formula:\[ N = mg \cos \theta \]Here,
On an inclined plane, it is crucial to remember that the normal force is not equal to the gravitational force.
Instead, it equals the component of the gravitational force that acts perpendicular to the plane.Given the angle of the incline, we can calculate the normal force using the formula:\[ N = mg \cos \theta \]Here,
- \( N \) is the normal force.
- The term \( mg \) is the weight of the object, where \( m \) is mass, and \( g \) is acceleration due to gravity.
- \( \cos \theta \) is the cosine of the angle of inclination.
Energy Conservation
Energy conservation is a fundamental principle in physics.
It states that energy cannot be created or destroyed, only transformed from one form to another.
When a block slides up an inclined plane, energy conservation helps determine how energy shifts between kinetic and potential forms.Initially, the block has kinetic energy given by:\[ \frac{1}{2} mv_0^2 \]As the block moves, this energy is converted into work done against friction and the gravitational component:\[ mgd \sin \theta + \mu_k mgd \cos \theta \]In this conservation of energy context:
It states that energy cannot be created or destroyed, only transformed from one form to another.
When a block slides up an inclined plane, energy conservation helps determine how energy shifts between kinetic and potential forms.Initially, the block has kinetic energy given by:\[ \frac{1}{2} mv_0^2 \]As the block moves, this energy is converted into work done against friction and the gravitational component:\[ mgd \sin \theta + \mu_k mgd \cos \theta \]In this conservation of energy context:
- The initial kinetic energy is spent to overcome both the gravitational pull (up the slope) and the frictional force resisting motion.
- By solving the equation above, we find out how much energy is lost to these forces.
- Energy conservation ensures that the sum of input energies equals the sum of output energies in the isolated system.
Other exercises in this chapter
Problem 18
(II) The crate shown in Fig. 33 lies on a plane tilted at an angle \(\theta=25.0^{\circ}\) to the horizontal, with \(\mu_{\mathrm{k}}=0.19\) . (a) Determine the
View solution Problem 22
(II) A flatbed truck is carrying a heavy crate. The coefficient of static friction between the crate and the bed of the truck is \(0.75 .\) What is the maximum
View solution Problem 26
(II) \(\mathrm{A}\) 75-kg snowboarder has an initial velocity of 5.0 \(\mathrm{m} / \mathrm{s}\) at the top of a \(28^{\circ}\) incline (Fig. \(36 ) .\) After s
View solution Problem 29
(II) A child slides down a slide with a \(34^{\circ}\) incline, and at the bottom her speed is precisely half what it would have been if the slide had been fric
View solution