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III. Long Answer Questions · Q6

Q.Explain in detail the idea of weightlessness using a lift as an example.

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Step 1. Setup. A person of mass mm stands on a scale inside a lift. Two forces act: gravity F⃗G=−mgj^\vec F_G=-mg\hat j (downward) and the scale's normal reaction N⃗=Nj^\vec N=N\hat j (upward). The scale reading equals NN, the apparent weight.

Step 2. Case (i): lift at rest / constant velocity. Net acceleration is zero, so applying Newton's second law: N−mg=0⇒N=mgN-mg=0\Rightarrow N=mg. Apparent weight equals true weight.

Step 3. Case (ii): lift accelerating upward with acceleration aa. Applying F⃗G+N⃗=ma⃗\vec F_G+\vec N=m\vec a along the vertical: −mg+N=ma⇒N=m(g+a)-mg+N=ma\Rightarrow N=m(g+a). Apparent weight is greater than mgmg -- the "heavy" feeling as an elevator starts moving up.

Step 4. Case (iii): lift accelerating downward with acceleration aa. Similarly, −mg+N=−ma⇒N=m(g−a)-mg+N=-ma\Rightarrow N=m(g-a). Apparent weight is less than mgmg -- the "light" feeling as a lift starts moving down.

Step 5. Case (iv): free fall (e.g. cable cut), a=ga=g downward. Substituting a=ga=g into Case (iii)'s result: N=m(g−g)=0N=m(g-g)=0. The scale reads exactly zero -- weightlessness. The person and the lift accelerate downward at exactly the same rate, so the person never presses on the floor, and the floor never pushes back. …

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