0 above Consider an object sliding down a frictionless ramp that is inclined an angle the horizontal. What should the acceleration down the ramp ar be when the angle becomes zero? 0 mg
0 above Consider an object sliding down a frictionless ramp that is inclined an angle the horizontal. What should the acceleration down the ramp ar be when the angle becomes zero? 0 mg
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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![**Physics Problem: Frictionless Ramp Motion**
**Problem Statement:**
Consider an object sliding down a frictionless ramp that is inclined at an angle θ above the horizontal. What should the acceleration down the ramp \( a_x \) be when the angle θ becomes zero?
**Diagram Explanation:**
The provided diagram shows a setup with an inclined ramp and an object placed on it. The important elements include:
- A solid block (representing the object) resting on the inclined plane.
- The angle of inclination, represented by θ.
- The force of gravity acting on the object, denoted by 'mg' directed downwards.
- A coordinate system with the x-axis parallel to the ramp and the y-axis perpendicular to the ramp.
### Analyzing the Forces
When analyzing the forces acting on the object on the inclined plane:
1. The gravitational force \( F_g = mg \) acts vertically downwards.
2. This force can be decomposed into two components:
- Parallel to the inclined plane: \( F_{\parallel} = mg \sin(θ) \)
- Perpendicular to the inclined plane: \( F_{\perp} = mg \cos(θ) \)
### Acceleration Calculation
Since there is no friction, the only force causing the block to accelerate down the plane is \( F_{\parallel} \).
Using Newton's Second Law along the inclined plane:
\[ F_{\parallel} = ma_x \]
\[ mg \sin(θ) = ma_x \]
\[ a_x = g \sin(θ) \]
### Special Case: θ = 0
When the angle θ becomes zero, the plane becomes horizontal. Substituting \( θ = 0 \) in the formula for acceleration:
\[ a_x = g \sin((0)) \]
\[ a_x = g \cdot 0 \]
\[ a_x = 0 \]
Therefore, the acceleration down the ramp \( a_x \) becomes zero when the angle θ is zero.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fae25ab45-ae90-481a-a08d-38576354b5ac%2F000c59f0-4fbf-499c-a6b9-06f1dbba38d7%2Fe9xmt8_processed.jpeg&w=3840&q=75)
Transcribed Image Text:**Physics Problem: Frictionless Ramp Motion**
**Problem Statement:**
Consider an object sliding down a frictionless ramp that is inclined at an angle θ above the horizontal. What should the acceleration down the ramp \( a_x \) be when the angle θ becomes zero?
**Diagram Explanation:**
The provided diagram shows a setup with an inclined ramp and an object placed on it. The important elements include:
- A solid block (representing the object) resting on the inclined plane.
- The angle of inclination, represented by θ.
- The force of gravity acting on the object, denoted by 'mg' directed downwards.
- A coordinate system with the x-axis parallel to the ramp and the y-axis perpendicular to the ramp.
### Analyzing the Forces
When analyzing the forces acting on the object on the inclined plane:
1. The gravitational force \( F_g = mg \) acts vertically downwards.
2. This force can be decomposed into two components:
- Parallel to the inclined plane: \( F_{\parallel} = mg \sin(θ) \)
- Perpendicular to the inclined plane: \( F_{\perp} = mg \cos(θ) \)
### Acceleration Calculation
Since there is no friction, the only force causing the block to accelerate down the plane is \( F_{\parallel} \).
Using Newton's Second Law along the inclined plane:
\[ F_{\parallel} = ma_x \]
\[ mg \sin(θ) = ma_x \]
\[ a_x = g \sin(θ) \]
### Special Case: θ = 0
When the angle θ becomes zero, the plane becomes horizontal. Substituting \( θ = 0 \) in the formula for acceleration:
\[ a_x = g \sin((0)) \]
\[ a_x = g \cdot 0 \]
\[ a_x = 0 \]
Therefore, the acceleration down the ramp \( a_x \) becomes zero when the angle θ is zero.
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