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- Let's create and solve a rigid body statics problem.
- **Problem:**
- A uniform beam AB, weighing 200 N and 4 meters long, is supported by a pin at A and a cable BC. The cable BC is attached to the beam at point B and makes an angle of 30 degrees with the horizontal. A 100 N weight is suspended from the beam at point D, which is 1 meter from A. Determine the tension in the cable BC and the horizontal and vertical components of the reaction force at pin A.
- **Diagram:**
- (Unfortunately, I can't draw a diagram here, but I'll describe it. Imagine a horizontal beam AB, with A on the left. The 100N weight hangs down from D, closer to A. The cable BC goes from B (the right end of the beam) up and to the right, angled at 30 degrees. The pin at A allows rotation but resists horizontal and vertical movement.)
- **Solution:**
- 1. **Free Body Diagram:** We consider the beam AB as the free body. The forces acting on it are:
- * The weight of the beam (200 N) acting downwards at the center of the beam (2 meters from A).
- * The 100 N weight acting downwards at point D (1 meter from A).
- * The tension in the cable BC (T), acting at an angle of 30 degrees.
- * The horizontal reaction force at A (Ax), acting to the right.
- * The vertical reaction force at A (Ay), acting upwards.
- 2. **Equilibrium Equations:** For the beam to be in static equilibrium, the sum of the forces and the sum of the moments about any point must be zero. We have three unknowns (T, Ax, and Ay), so we need three equations.
- * **Sum of forces in the x-direction = 0:**
- Ax + Tcos(30°) = 0
- * **Sum of forces in the y-direction = 0:**
- Ay + Tsin(30°) - 200 N - 100 N = 0
- * **Sum of moments about point A = 0:** (Choosing point A eliminates Ax and Ay from the moment equation, simplifying it). We'll consider counterclockwise moments as positive.
- -(200 N)(2 m) - (100 N)(1 m) + Tsin(30°)(4 m) = 0
- 3. **Solving the Equations:**
- * **From the moment equation:**
- -400 Nm - 100 Nm + 2T = 0
- 2T = 500 Nm
- T = 250 N
- * **From the y-direction force equation:**
- Ay + (250 N)sin(30°) - 300 N = 0
- Ay + 125 N - 300 N = 0
- Ay = 175 N
- * **From the x-direction force equation:**
- Ax + (250 N)cos(30°) = 0
- Ax + 216.5 N = 0
- Ax = -216.5 N (The negative sign indicates that Ax acts to the left, opposite to our initial assumption).
- **Results:**
- * Tension in cable BC (T) = 250 N
- * Horizontal reaction force at A (Ax) = -216.5 N (acting to the left)
- * Vertical reaction force at A (Ay) = 175 N (acting upwards)
- Therefore, the tension in the cable is 250 N, and the reaction force at A has a horizontal component of 216.5 N to the left and a vertical component of 175 N upwards.
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