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BITSAT 2012
Exam
BITSAT
Year
2012
Subject
Physics
Chapter
Mechanical Properties of Solids

BITSAT 2012 · Physics · Mechanical Properties of Solids

One end of a long metallic wire of length L tied to the ceiling....

One end of a long metallic wire of length L\mathrm{L} tied to the ceiling. The other end is tied with a massless spring of spring constant K\mathrm{K}. Amass hangs freely from the free end of the spring. The area of cross section and the young's modulus of the wire are A and Y respectively. If the mass slightly pulled down and released, it will oscillate with a time period T equal to:One end of a long metallic wire of length L tied to the ceiling. The other end is tied with a massless spring of spring

Options

  1. A2π(m/K)2 \pi \sqrt{(\mathrm{m} / \mathrm{K})}
  2. B2πm(YA+KL)/(YAK)2 \pi \sqrt{\mathrm{m}(\mathrm{YA}+\mathrm{KL}) /(\mathrm{YAK})}
  3. C2π(mYA/KL)2 \pi \sqrt{(\mathrm{m} \mathrm{YA} / \mathrm{KL})}
  4. D2π(mL/YA)2 \pi \sqrt{(\mathrm{mL} / \mathrm{YA})}

Correct answer

B. 2πm(YA+KL)/(YAK)2 \pi \sqrt{\mathrm{m}(\mathrm{YA}+\mathrm{KL}) /(\mathrm{YAK})}

Step-by-step solution

Calculation of spring constant of wire Young's modulus of wire, (\mathrm{Y}=\frac{\Delta \mathrm{F} / \mathrm{A}}{\Delta \mathrm{L} / \mathrm{L}}=\frac{\Delta \mathrm{F}}{\Delta \mathrm{L}} \times \frac{\mathrm{L}}{\mathrm{A}}) Due to elasticity of the wire, it behaves as equivalent spring (\left(\mathrm{K}_{\text{spring }}=\mathrm{F}/ \Delta \mathrm{x}\right)). Hence, Spring constant for Wire, (\mathrm{K}_{\mathrm{w}}=\frac{\Delta \mathrm{F}}{\Delta \mathrm{L}}=\mathrm{Y} \frac{\mathrm{A}}{\mathrm{L}})CalculationofEquivalentspringconstantLetaforce(F) Calculation of Equivalent spring constant Let a force (\mathrm{F}) be applied to the end of the spring. The wire will extend. Total extension (\Delta S=x\mathrm{S}=\mathrm{x}_{\mathrm{wire}}+\mathrm{x}_{\text{spring }}=\frac{\mathrm{F}_{\mathrm{w}}}{\mathrm{K}_{\mathrm{w}}}+\frac{\mathrm{F}_{\mathrm{S}}}{\mathrm{K}})But(FS=Fw) But (\mathrm{F}_{\mathrm{S}}=\mathrm{F}_{\mathrm{w}} \quad) (By Newton's, third Law, Both will apply equal and opposite forces at their joint A ) (\therefore Δ\Delta\mathrm{S}=\mathrm{F}w(1Kw+1K)_{\mathrm{w}} \left(\frac{1}{\mathrm{ K}_{\mathrm{w}}}+\frac{1}{\mathrm{ K}}\right)) So, Equivalent spring constant \((Keq )( \left(\mathrm{K}_{\text{eq }}\right)) is given by: (\mathrm{K}_{\mathrm{eq}}=\frac{\mathrm{F}_{\mathrm{eq}}}{\mathrm{x}_{\mathrm{eq}}}=\frac{\mathrm{F}_{\mathrm{w}}}{\Delta \mathrm{S}}=\frac{1}{\frac{1}{\mathrm{ K}_{\mathrm{w}}}+\frac{1}{\mathrm{ K}}}) \(Keq=(K)(Kw)Kw+K=KYALYAL+K=KYAYA+KL(\mathrm{K}_{\mathrm{eq}}=\frac{(\mathrm{K})\left(\mathrm{K}_{\mathrm{w}}\right)}{\mathrm{K}_{\mathrm{w}}+\mathrm{K}}=\frac{\mathrm{KY} \frac{\mathrm{A}}{\mathrm{L}}}{\mathrm{Y} \frac{\mathrm{A}}{\mathrm{L}}+\mathrm{K}}=\frac{\mathrm{KYA}}{\mathrm{YA}+\mathrm{KL}}) Calculation of Time period Angular frequency (\omega) for spring block system is given by: \($omega=Keq m=KYAm(YA+KL)(\$omega=\sqrt{\frac{\mathrm{K}_{\text{eq }}}{\mathrm{m}}}=\sqrt{\frac{\mathrm{KYA}}{\mathrm{m}(\mathrm{YA}+\mathrm{KL})}}) (\therefore) Time period, (\mathrm{T}=\frac{2 \pi}{\omega}=2π2 \pi\sqrt{\frac{(\mathrm{YA}+\mathrm{KL}) \mathrm{m}}{\mathrm{KYA}}}$) Hence, Option B is correct One end of a long metallic wire of length L tied to the ceiling. The other end is tied with a massless spring of spring
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