SHM in liquid

A thin rod of length L L and area of cross section S S is pivoted at its lowest point P inside a stationary , homogeneous , non viscous liquid as shown in the figure.

The rod is free to rotate in a vertical plane about a horizontal axis passing through p p . The density of the material of the rod D 1 D_1 is smaller than the density of liquid D 2 D_2 . The rod is displaced by a small angle θ θ from its equilibrium position and then released.

If the body performs Simple harmonic motion, calculate t's angular fequency ω \omega

Details and Assumptions

D 1 = 200 units D_1 = 200 \text {units}

D 2 = 400 units D_2 = 400 \text {units}

L = 20 cm L = 20 \text {cm}

g = 10 m s 2 g =10 \dfrac {m}{s^2}

Also try this.


The answer is 8.66.

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1 solution

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The different forces on the rod are:

Weight of the rod acting downwards = m g mg = S L D 1 g SLD_1g

Buoyant force acting upwards = S L D 2 g SLD_2g

Net thrust acting on the rod upwards; F F = S L ( D 1 D 2 ) g SL(D_1-D_2)g

Restoring torque τ τ = F L 2 s i n θ F\frac{L}{2}sinθ

If θ θ is in clockwise direction then τ τ will be in anticlockwise direction

τ τ = - F L 2 s i n θ F\frac{L}{2}sinθ

Also τ τ = I α

Where I = M L 2 3 \frac{ML^{2}}{3}

Find α α using above equation and then find angular frequency ω ω using differential equation of S . H . M S.H.M

U will get ω ω = 3 g 2 L D 2 D 1 D 1 \sqrt{\frac{3g}{2L}\frac{D_2-D_1}{D_1}}

It is interesting,, that in this case as D2= 2D1, so the SHM is just as if it was in air,, except,, upwards directing

Mvs Saketh - 6 years, 8 months ago

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Yeah that's good observation.

rajdeep brahma - 3 years, 4 months ago

Use d_1 for d 1 d_1 .

Shaan Vaidya - 7 years ago

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Thanks for your suggestion

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