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NEET PHYSICSMedium

A body of mass mm is kept on a rough horizontal surface (coefficient of friction = μ\mu). A horizontal force is applied to the body, but it does not move. The resultant of normal reaction and the frictional force acting on the object is given by F\vec{F}, where:

A

F=mg+μmg|\vec{F}| = mg + \mu mg

B

F=μmg|\vec{F}| = \mu mg

C

Fmg1+μ2|\vec{F}| \le mg\sqrt{1+\mu^2}

D

F=mg|\vec{F}| = mg

Step-by-Step Solution

  1. Identify Forces: The forces exerted by the surface on the body are the Normal Reaction (NN) and the Static Friction (fsf_s).
  • Since the body is on a horizontal surface and there is no vertical acceleration, N=mgN = mg [NCERT Class 11, Physics Part I, Chapter 5, Section 5.9].
  • The static friction fsf_s balances the applied horizontal force to keep the body at rest. Its magnitude adjusts such that 0fsfs,max0 \le f_s \le f_{s,max}, where the limiting friction fs,max=μN=μmgf_{s,max} = \mu N = \mu mg [NCERT Class 11, Physics Part I, Eq. 4.14].
  1. Resultant Force (Contact Force): The resultant force F\vec{F} (often called the total contact force) is the vector sum of N\vec{N} and fs\vec{f_s}. Since N\vec{N} is vertical and fs\vec{f_s} is horizontal, they are perpendicular. F=N2+fs2|\vec{F}| = \sqrt{N^2 + f_s^2}
  2. Apply Limits: Substituting N=mgN = mg and the inequality for friction:
  • Minimum F|\vec{F}| occurs when fs=0f_s = 0 (no applied force): Fmin=(mg)2+0=mg|\vec{F}|_{min} = \sqrt{(mg)^2 + 0} = mg.
  • Maximum F|\vec{F}| occurs when friction is limiting (fs=μmgf_s = \mu mg): Fmax=(mg)2+(μmg)2=mg1+μ2|\vec{F}|_{max} = \sqrt{(mg)^2 + (\mu mg)^2} = mg\sqrt{1+\mu^2}.
  1. Conclusion: The magnitude of the resultant force satisfies the condition: Fmg1+μ2|\vec{F}| \le mg\sqrt{1+\mu^2}
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