Prove the following using dimentional analysis
v = 1 / 2l + sqrt{t/n}
v = frequency T= tension force n = mass per length.
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Fundamental resonance frequency of a transverse wave on a thin rod or rope that has a uniform mass per unit length n is given by the following formula.
T is the force of tension in the rope or string or thin rod of length L. The string is fixed firmly at both ends or open at both ends.
[tex] = \left[\begin{array}{ccc} L^{-1} \end{array}\right]\ \left[\begin{array}{ccc} (M\ L\ T^{-2})^{\frac{1}{2}} \end{array}\right]\ \left[\begin{array}{ccc} (M\ L^{-1})^{-\frac{1}{2}} \end{array}\right] \\ [/tex]
[tex] = \left[\begin{array}{ccc} (M^{\frac{1}{2}-\frac{1}{2}}\ L^{-1+\frac{1}{2}+\frac{1}{2}}\ T^{2*\frac{1}{2}} \end{array}\right] \\ \\ = \left[\begin{array}{ccc} M^0\ L^0\ T^{-1} \end{array}\right] \\ [/tex]
So the dimensions on both sides match.
Fundamental resonance frequency of a transverse wave on a thin rod or rope that has a uniform mass per unit length n is given by the following formula.
T is the force of tension in the rope or string or thin rod of length L. The string is fixed firmly at both ends or open at both ends.
[tex] = \left[\begin{array}{ccc} L^{-1} \end{array}\right]\ \left[\begin{array}{ccc} (M\ L\ T^{-2})^{\frac{1}{2}} \end{array}\right]\ \left[\begin{array}{ccc} (M\ L^{-1})^{-\frac{1}{2}} \end{array}\right] \\ [/tex]
[tex] = \left[\begin{array}{ccc} (M^{\frac{1}{2}-\frac{1}{2}}\ L^{-1+\frac{1}{2}+\frac{1}{2}}\ T^{2*\frac{1}{2}} \end{array}\right] \\ \\ = \left[\begin{array}{ccc} M^0\ L^0\ T^{-1} \end{array}\right] \\ [/tex]
So the dimensions on both sides match.
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