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A block A of mass m1m_1 rests on a horizontal table. A light string connected to it passes over a frictionless pulley at the edge of table and from its other end another block B of mass m2m_2 is suspended. The coefficient of kinetic friction between the block and the table is μk\mu_k. When the block A is sliding on the table, the tension in the string is:

A

(m2+μkm1)gm1+m2\frac{(m_2 + \mu_k m_1)g}{m_1 + m_2}

B

(m2μkm1)gm1+m2\frac{(m_2 - \mu_k m_1)g}{m_1 + m_2}

C

m1m2(1+μk)gm1+m2\frac{m_1 m_2 (1 + \mu_k)g}{m_1 + m_2}

D

m1m2(1μk)gm1+m2\frac{m_1 m_2 (1 - \mu_k)g}{m_1 + m_2}

Step-by-Step Solution

  1. Free Body Diagram of Block B (m2m_2):
  • Forces acting are gravity (m2gm_2g) downwards and tension (TT) upwards.
  • Equation of motion: m2gT=m2am_2g - T = m_2a ... (i) (assuming acceleration aa downwards).
  1. Free Body Diagram of Block A (m1m_1):
  • Forces acting horizontally are tension (TT) towards the pulley and kinetic friction (fkf_k) opposing motion.
  • Vertical forces balance: N=m1gN = m_1g, so fk=μkN=μkm1gf_k = \mu_k N = \mu_k m_1g.
  • Equation of motion: Tfk=m1a    Tμkm1g=m1aT - f_k = m_1a \implies T - \mu_k m_1g = m_1a ... (ii).
  1. Solve for Acceleration (aa):
  • Adding (i) and (ii): m2gμkm1g=(m1+m2)am_2g - \mu_k m_1g = (m_1 + m_2)a.
  • a=g(m2μkm1)m1+m2a = \frac{g(m_2 - \mu_k m_1)}{m_1 + m_2}.
  1. Solve for Tension (TT):
  • Substitute aa into equation (ii): T=m1(a+μkg)T = m_1(a + \mu_k g).
  • T=m1[g(m2μkm1)m1+m2+μkg]T = m_1 \left[ \frac{g(m_2 - \mu_k m_1)}{m_1 + m_2} + \mu_k g \right].
  • T=m1gm1+m2[m2μkm1+μk(m1+m2)]T = \frac{m_1 g}{m_1 + m_2} [ m_2 - \mu_k m_1 + \mu_k(m_1 + m_2) ].
  • T=m1gm1+m2[m2μkm1+μkm1+μkm2]T = \frac{m_1 g}{m_1 + m_2} [ m_2 - \mu_k m_1 + \mu_k m_1 + \mu_k m_2 ].
  • T=m1gm1+m2[m2+μkm2]=m1m2g(1+μk)m1+m2T = \frac{m_1 g}{m_1 + m_2} [ m_2 + \mu_k m_2 ] = \frac{m_1 m_2 g (1 + \mu_k)}{m_1 + m_2}. (Reference: NCERT Class 11, Physics Part I, Chapter 5: Laws of Motion, Section 5.9 Friction).
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