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xuyuzai's Question
Physics M
Posted 3 months ago
A ladder AB of mass 20 kg rest on smooth horizontal ground and leans against a sooth vertical wall. The inclination of the ladder to the horizontal is 60°. The ladder is kept in position by a horizontal force P applied to the bottom of the ladder.
Find the value of P and the reactions at the wall and the ground.
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Answer from Sia
Posted 3 months ago
Solution
a
Identify the forces acting on the ladder: The weight of the ladder (W=mg=20kg×9.81m/s2=196.2NW = mg = 20 \, \text{kg} \times 9.81 \, \text{m/s}^2 = 196.2 \, \text{N}) acts downward at the center of the ladder. The horizontal force PP acts at the bottom of the ladder, and the normal force NN acts upward at the ground. The wall exerts a reaction force RR horizontally at the top of the ladder
b
Apply the equilibrium conditions: For the ladder to be in static equilibrium, the sum of the forces in both the horizontal and vertical directions must be zero: Fx=0\sum F_x = 0 and Fy=0\sum F_y = 0. Thus, we have: RP=0R - P = 0 (1) and NW=0N - W = 0 (2). From (2), we find that N=W=196.2NN = W = 196.2 \, \text{N}
c
Calculate the torques about the base of the ladder: The torque due to the weight of the ladder is given by τW=WdW\tau_W = W \cdot d_W, where dWd_W is the horizontal distance from the base to the center of the ladder. The length of the ladder can be calculated using trigonometry: L=hsin(60)L = \frac{h}{\sin(60^\circ)}, where hh is the vertical height. The horizontal distance to the center is dW=L2cos(60)d_W = \frac{L}{2} \cdot \cos(60^\circ). The torque due to the reaction force at the wall is τR=RLsin(60)\tau_R = R \cdot L \cdot \sin(60^\circ). Setting the torques equal gives us: WdW=RLsin(60)W \cdot d_W = R \cdot L \cdot \sin(60^\circ)
d
Substitute the known values into the torque equation and solve for PP: After calculating LL and dWd_W, we can find RR using the equilibrium condition (1). Finally, we can express PP in terms of RR: P=RP = R
Answer
P = R, N = 196.2 N, R = 98.1 N
Key Concept
Static Equilibrium: For an object to be in static equilibrium, the net force and net torque acting on it must be zero. This involves balancing forces and calculating torques about a pivot point. Equations: F=0\sum F = 0 and τ=0\sum \tau = 0.
Explanation
By analyzing the forces and torques acting on the ladder, we can determine the necessary horizontal force PP and the reactions at the wall and ground to maintain equilibrium.

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