Give step-by-step solution with explanation and final answer:A
A homogeneous rod AB with length = 1 m and mass A
m = 1 Kg is supported by pin C. At the instant shown, Juss
the rod is at rest and a 2 = 1 kN force is applied at B. a 5
Determine
a. angular acceleration of the rod, tpg.
b. components of the reaction at C. 2L/3
¢. acceleration of the centre of gravity of the rod.
ag and point A, aa. P
B
6 marks
SOLUTIONS
Question:
Give step-by-step solution with explanation and final answer:A
A homogeneous rod AB with length = 1 m and mass A
m = 1 Kg is supported by pin C. At the instant shown, Juss
the rod is at rest and a 2 = 1 kN force is applied at B. a 5
Determine
a. angular acceleration of the rod, tpg.
b. components of the reaction at C. 2L/3
¢. acceleration of the centre of gravity of the rod.
ag and point A, aa. P
B
6 marks
SOLUTIONS
This is AI generated Response.
Asked by: Rahul
Created at: 2026-01-10 15:40:50
Final Answer:
RenderedRaw Text
Did you like this answer?
Let's solve the problem step by step.
---
## **Given Data**
- Length of rod, \( L = 1 \) m
- Mass of rod, \( m = 1 \) kg
- Force applied at \( B \), \( P = 1 \) kN \( = 100 \) N
- Rod is supported by pin at \( C \), located \( \frac{L}{3} \) from \( A \)
- Rod is at rest at the instant shown.
---
## **Step 1: Free Body Diagram & Moments**
Let's define:
- \( A \): Top of rod
- \( B \): Bottom of rod (where force is applied)
- \( C \): Pin support (\( \frac{L}{3} \) from \( A \), \( \frac{2L}{3} \) from \( B \))
**Forces acting:**
- Weight \( mg \) acting at the center (midpoint, \( \frac{L}{2} \) from \( A \))
- Applied force \( P \) at \( B \) (horizontal)
- Reactions at \( C \): \( C_x \), \( C_y \)
---
## **(a) Angular Acceleration of the Rod (\( \alpha_{AB} \))**
### **Moment of Inertia about C**
For a rod of length \( L \) and mass \( m \), the moment of inertia about a point \( d \) from the center is:
\[
I = I_{\text{center}} + m d^2 = \frac{1}{12} mL^2 + m d^2
\]
Here, \( d = | \text{distance from center to C} | = \left| \frac{L}{2} - \frac{L}{3} \right| = \frac{L}{6} \)
So,
\[
I_C = \frac{1}{12} mL^2 + m \left( \frac{L}{6} \right)^2 = \frac{1}{12} mL^2 + \frac{1}{36} mL^2 = \frac{1}{9} mL^2
\]
### **Moment Equation about C**
Sum of moments about \( C \):
\[
\sum M_C = I_C \alpha
\]
Moments due to:
- \( P \) at \( B \): Perpendicular distance from \( C \) to \( B \) is \( \frac{2L}{3} \)
- Weight passes through the center, which is at a distance \( \frac{L}{6} \) from \( C \)
\[
P \cdot \frac{2L}{3} - mg \cdot \frac{L}{6} = I_C \alpha
\]
Plug in values:
- \( P = 100 \) N
- \( m = 1 \) kg
- \( g = 9.81 \) m/s²
- \( L = 1 \) m
- \( I_C = \frac{1}{9} \) kg·m²
\[
100 \cdot \frac{2 \times 1}{3} - 1 \cdot 9.81 \cdot \frac{1}{6} = \frac{1}{9} \alpha
\]
\[
= 100 \cdot \frac{2}{3} - 9.81 \cdot \frac{1}{6} = \frac{1}{9} \alpha
\]
\[
= 666.67 - 1.635 = \frac{1}{9} \alpha
\]
\[
= 665.035 = \frac{1}{9} \alpha
\]
\[
\alpha = 9 \times 665.035 = 5985.32 \ \text{rad/s}^2
\]
**Final Answer:**
\[
\boxed{\alpha_{AB} = 5985 \ \text{rad/s}^2}
\]
---
## **(b) Components of the Reaction at \( C \) (\( C_x \), \( C_y \))**
### **Equations of Motion**
1. **Sum of Forces in \( x \):**
\[
C_x - P = m a_{Gx}
\]
2. **Sum of Forces in \( y \):**
\[
C_y - mg = m a_{Gy}
\]
3. **Acceleration of Center of Mass \( G \):**
- \( a_{Gx} = \alpha \cdot r_{G/C} \) (horizontal because rotation is about \( C \))
- \( r_{G/C} = \frac{L}{2} - \frac{L}{3} = \frac{L}{6} \)
- Acceleration is perpendicular to rod, so horizontal at this instant.
\[
a_{Gx} = \alpha \cdot \frac{L}{6}
\]
\[
a_{Gx} = 5985 \cdot \frac{1}{6} = 997.5 \ \text{m/s}^2
\]
So,
\[
C_x - 100 = 1 \times 997.5
\]
\[
C_x = 1997.5 \ \text{N}
\]
- \( a_{Gy} = \) (since angular acceleration is horizontal at instant shown)
\[
C_y - 9.81 = 1 \times
\]
\[
C_y = 9.81 \ \text{N}
\]
**Final Answers:**
\[
\boxed{C_x = 1997.5 \ \text{N}} \\
\boxed{C_y = 9.81 \ \text{N}}
\]
---
## **(c) Acceleration of Centre of Gravity (\( a_G \)) and Point \( A \) (\( a_A \))**
### **Centre of Gravity (\( a_G \))**
- \( a_{Gx} = \alpha \cdot r_{G/C} = 5985 \cdot \frac{1}{6} = 997.5 \) m/s² (right)
- \( a_{Gy} = \)
\[
\boxed{a_G = 997.5 \ \text{m/s}^2 \text{ (right)}}
\]
---
### **Point \( A \) (\( a_A \))**
- Distance from \( C \) to \( A \) is \( -\frac{L}{3} \) (upwards from \( C \))
- Acceleration of \( A \) relative to \( C \) is \( a_{A/C} = \alpha \cdot r_{A/C} \) (perpendicular to rod, i.e., horizontal at this instant)
So,
\[
a_{A, x} = \alpha \cdot \left( -\frac{L}{3} \right) = 5985 \cdot \left( -\frac{1}{3} \right) = -1995 \ \text{m/s}^2
\]
- (Negative means to the left)
\[
\boxed{a_A = 1995 \ \text{m/s}^2 \text{ (left)}}
\]
---
## **Summary Table**
| Quantity | Value | Direction |
|------------------------|-------------|--------------|
| Angular acceleration (\( \alpha_{AB} \)) | 5985 rad/s² | - |
| Reaction at C, \( C_x \) | 1997.5 N | Right |
| Reaction at C, \( C_y \) | 9.81 N | Up |
| Acceleration of G, \( a_G \) | 997.5 m/s² | Right |
| Acceleration of A, \( a_A \) | 1995 m/s² | Left |
---
### **Let me know if you need further clarification or a diagram!**
VIPSolutions focuses on clear, step‑by‑step explanations so you can learn quickly. Whether you need an AI‑generated walkthrough or a short hint to get unstuck, each solution is organized for fast reading and easy review later.
Search similar questions, compare approaches, and bookmark the best answers for revision. Our goal is simple: quick, reliable study help that feels natural—not noisy.