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Two men A and B are carrying a uniform b...

Two men `A` and `B` are carrying a uniform bar of length `L` on their shoulders. The bar is held horizontally such that A gets one-fourth load. If `A` is at one end of the bar, the distance of `B` from that end is

A

`L/3`

B

`L/4`

C

`(2L)/3`

D

`(3L)/4`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to determine the distance of man B from the end of the bar where man A is located. Here’s a step-by-step solution: ### Step 1: Understand the Load Distribution Given that man A carries one-fourth of the total load, we can denote the total force exerted by the bar as \( F \). Therefore, the force on man A (denoted as \( F_A \)) is: \[ F_A = \frac{1}{4} F \] And the force on man B (denoted as \( F_B \)) is: \[ F_B = F - F_A = F - \frac{1}{4} F = \frac{3}{4} F \] ### Step 2: Set Up the Torque Equation Since the bar is uniform and horizontal, we can analyze the torques about the center of mass of the bar. The center of mass of a uniform bar of length \( L \) is located at \( \frac{L}{2} \). The torque exerted by A about the center of mass is given by: \[ \tau_A = F_A \cdot d_A \] where \( d_A \) is the distance from A to the center of mass, which is \( \frac{L}{2} \). The torque exerted by B about the center of mass is given by: \[ \tau_B = F_B \cdot d_B \] where \( d_B \) is the distance from B to the center of mass. ### Step 3: Equate the Torques Since the bar is in equilibrium, the torques must be equal: \[ \tau_A = \tau_B \] Substituting the expressions for torque: \[ F_A \cdot \frac{L}{2} = F_B \cdot d_B \] Substituting \( F_A \) and \( F_B \): \[ \left(\frac{1}{4} F\right) \cdot \frac{L}{2} = \left(\frac{3}{4} F\right) \cdot d_B \] ### Step 4: Simplify the Equation We can cancel \( F \) from both sides (assuming \( F \neq 0 \)): \[ \frac{1}{4} \cdot \frac{L}{2} = \frac{3}{4} \cdot d_B \] This simplifies to: \[ \frac{L}{8} = \frac{3}{4} \cdot d_B \] ### Step 5: Solve for \( d_B \) To find \( d_B \), multiply both sides by \( \frac{4}{3} \): \[ d_B = \frac{L}{8} \cdot \frac{4}{3} = \frac{L}{6} \] ### Step 6: Calculate the Distance of B from the End The distance of B from the end of the bar (where A is located) is the distance from A to the center of mass plus the distance from the center of mass to B: \[ \text{Distance from A to B} = \frac{L}{2} + d_B = \frac{L}{2} + \frac{L}{6} \] To add these fractions, find a common denominator (which is 6): \[ \frac{L}{2} = \frac{3L}{6} \] Thus, \[ \text{Distance from A to B} = \frac{3L}{6} + \frac{L}{6} = \frac{4L}{6} = \frac{2L}{3} \] ### Final Answer The distance of B from the end where A is located is: \[ \boxed{\frac{2L}{3}} \]
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