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IV. Numerical Problems · Q3

Q.Assuming that the frequency γ\gamma of a vibrating string may depend upon i) applied force (F) ii) length (l) iii) mass per unit length (m), prove that γ∝1lFm\gamma \propto \dfrac1l\sqrt{\dfrac Fm} using dimensional analysis. (related to JIPMER 2001)

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Step 1. Assume γ=k Falbmc\gamma=k\,F^al^bm^c, where kk is a dimensionless constant, FF is the applied force, ll is the length, and mm is mass per unit length.

Step 2. Dimensional formulas: [γ]=[T−1][\gamma]=[T^{-1}] (frequency), [F]=[MLT−2][F]=[MLT^{-2}], [l]=[L][l]=[L], [m]=[ML−1][m]=[ML^{-1}] (mass per unit length).

Step 3. Substituting: [T−1]=[MLT−2]a[L]b[ML−1]c=[Ma+cLa+b−cT−2a][T^{-1}]=[MLT^{-2}]^a[L]^b[ML^{-1}]^c=[M^{a+c}L^{a+b-c}T^{-2a}].

Step 4. Matching powers of MM, LL, TT on both sides: MM: a+c=0a+c=0; LL: a+b−c=0a+b-c=0; TT: −2a=−1⇒a=12-2a=-1\Rightarrow a=\dfrac12.

Step 5. From a+c=0a+c=0: c=−12c=-\dfrac12. From a+b−c=0a+b-c=0: 12+b+12=0⇒b=−1\dfrac12+b+\dfrac12=0\Rightarrow b=-1. …

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