Give step-by-step solution with explanation and final answer:The man continues pushing the same (46kg) box onto a ramp that is set at 100
above the horizontal. With the man pushing with a constant force of 300N purely
horizontally (not parallel to the ramp, but parallel to the ground), the box stops
accelerating and continues at a constant velocity on the ramp. Find the coefficient
of kinetic friction between the box and the ramp while the box is at this constant
velocity.
Question:
Give step-by-step solution with explanation and final answer:The man continues pushing the same (46kg) box onto a ramp that is set at 100
above the horizontal. With the man pushing with a constant force of 300N purely
horizontally (not parallel to the ramp, but parallel to the ground), the box stops
accelerating and continues at a constant velocity on the ramp. Find the coefficient
of kinetic friction between the box and the ramp while the box is at this constant
velocity.
This is AI generated Response.
Asked by: gvr
Created at: 2025-06-12 04:58:44
Final Answer:
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Let's break down the problem step by step:
**Given:**
- Mass of box, \( m = 46 \) kg
- Ramp angle, \( \theta = 10^\circ \)
- Applied force, \( F_{\text{push}} = 300 \) N (horizontal)
- Box moves at constant velocity (i.e., net force along the ramp is zero)
- We need to find the coefficient of kinetic friction, \( \mu_k \).
---
## **Step 1: Draw a Free-Body Diagram**
Let's identify the forces acting on the box:
- Weight, \( mg \), vertically downward
- Normal force, \( N \), perpendicular to the ramp
- Friction force, \( f_k = \mu_k N \), opposite to motion, parallel to the ramp
- Applied force, \( F_{\text{push}} \), horizontal (not parallel to the ramp)
---
## **Step 2: Resolve Forces**
Let's align the axes with the ramp:
- **x-axis**: along the ramp (up the ramp)
- **y-axis**: perpendicular to the ramp (into the ramp)
### **Breakdown of Forces:**
**Weight (\(mg\)):**
- Along ramp (down): \( mg \sin \theta \)
- Perpendicular to ramp: \( mg \cos \theta \)
**Applied Force (\(F_{\text{push}}\)):**
- Along ramp: \( F_{\text{push}} \cos \theta \)
- Perpendicular to ramp: \( F_{\text{push}} \sin \theta \)
---
## **Step 3: Write Equations**
### **Along the Ramp (x-axis):**
Since the box moves at constant velocity, net force is zero:
\[
F_{\text{push}} \cos \theta - mg \sin \theta - f_k = 0
\]
\[
F_{\text{push}} \cos \theta - mg \sin \theta = f_k
\]
\[
F_{\text{push}} \cos \theta - mg \sin \theta = \mu_k N
\]
### **Perpendicular to the Ramp (y-axis):**
Net force perpendicular to the ramp is zero:
\[
N + F_{\text{push}} \sin \theta = mg \cos \theta
\]
\[
N = mg \cos \theta - F_{\text{push}} \sin \theta
\]
---
## **Step 4: Plug in Values**
Given:
- \( m = 46 \) kg
- \( g = 9.8 \) m/s²
- \( \theta = 10^\circ \)
- \( F_{\text{push}} = 300 \) N
Calculate the trigonometric values:
- \( \sin 10^\circ \approx 0.1736 \)
- \( \cos 10^\circ \approx 0.9848 \)
### **Calculate the Normal Force:**
\[
N = mg \cos \theta - F_{\text{push}} \sin \theta
\]
\[
N = (46)(9.8)(0.9848) - 300(0.1736)
\]
\[
N = 446.3376 - 52.08 = 394.2576 \text{ N}
\]
### **Calculate Forces Along the Ramp:**
\[
F_{\text{push}} \cos \theta = 300 \times 0.9848 = 295.44 \text{ N}
\]
\[
mg \sin \theta = 46 \times 9.8 \times 0.1736 = 78.217 \text{ N}
\]
\[
F_{\text{push}} \cos \theta - mg \sin \theta = 295.44 - 78.217 = 217.223 \text{ N}
\]
---
## **Step 5: Solve for \( \mu_k \)**
Recall:
\[
F_{\text{push}} \cos \theta - mg \sin \theta = \mu_k N
\]
\[
\mu_k = \frac{F_{\text{push}} \cos \theta - mg \sin \theta}{N}
\]
\[
\mu_k = \frac{217.223}{394.2576} \approx 0.551
\]
---
## **Final Answer:**
\[
\boxed{\mu_k \approx 0.55}
\]
**The coefficient of kinetic friction between the box and the ramp is approximately 0.55.**
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