Step 1: Climbing upward The tension in the rope during upward motion is calculated using the formula: \[ T = m(g + a), \] where: \( m = 50 \, \text{kg} \) (mass of the monkey), \( g = 10 \, \text{m/s}^2 \) (gravitational acceleration), \( a = 5 \, \text{m/s}^2 \) (acceleration while climbing upward). Substituting the values: \[ T = 50 (10 + 5) = 750 \, \text{N}. \] Since the tension \( T \) exceeds the rope's breaking strength (\( 350 \, \text{N} \)), the rope will break during upward motion.
Step 2: Climbing downward The tension in the rope during downward motion is given by: \[ T = m(g - a), \] where \( a = 4 \, \text{m/s}^2 \) (acceleration while climbing downward). Substitute the values: \[ T = 50 (10 - 4) = 300 \, \text{N}. \] Here, the tension \( T \) is less than the breaking strength (\( 350 \, \text{N} \)), so the rope will not break during downward motion.
Final Answer: \[ \boxed{\text{Rope will break while climbing upward.}} \]
A simple pendulum is made of a metal wire of length \( L \), area of cross-section \( A \), material of Young's modulus \( Y \), and a bob of mass \( m \). This pendulum is hung in a bus moving with a uniform speed \( V \) on a horizontal circular road of radius \( R \). The elongation in the wire is: