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Luden [163]
3 years ago
9

A vertical scale on a spring balance reads from 0 to 200 N . The scale has a length of 11.0 cm from the 0 to 200 N reading. A fi

sh hanging from the bottom of the spring oscillates vertically at a frequency of 2.55 Hz .Ignoring the mass of the spring, what is the mass m of the fish?
Physics
1 answer:
Andreyy893 years ago
4 0

Answer:

7.08 kg

Explanation:

Given:

Length of scale (x) = 11.0 cm = 0.110 m [1 cm = 0.01 m]

Range of scale is from 0 to 200 N.

Frequency of oscillation of fish (f) = 2.55 Hz

Mass of the fish (m) = ?

Now, range of scale is from 0 to 200 N. So, maximum force, the spring can hold is 200 N. For this maximum force, the extension in the spring is equal to the length of the scale. So, x = 0.11\ m

Now, we know that, spring force is given as:

F=kx\\\\k=\frac{F}{x}

Where, 'k' is spring constant.

Now, plug in the given values and solve for 'k'. This gives,

k=\frac{200\ N}{0.11\ m}=1818.18\ N/m

Now, the oscillation of the fish represents simple harmonic motion as it is attached to the spring.

So, the frequency of oscillation is given as:

f=\frac{1}{2\pi}\sqrt{\frac{k}{m}}

Squaring both sides and expressing it in terms of 'm', we get:

\frac{k}{m}=4\pi^2f^2\\\\m=\dfrac{k}{4\pi^2f^2}

Now, plug in the given values and solve for 'm'. This gives,

m=\frac{1818.18\ N/m}{4\pi^2\times (2.55\ Hz)^2}\\\\m=\frac{1818.18\ N/m}{256.708\ Hz^2}\\\\m=7.08\ kg

Therefore, the mass of the fish is 7.08 kg.

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Suppose, an arrangement with a horizontal pipe carrying fluid of density p . The fluid rises to heights h1 and h2 in the two open-ended tubes (see figure). The cross-sectional area of the pipe is A1 at the position of tube 1, and A2 at the position of tube 2.

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P_{1}=\rho g h_{1}

(b). We need to calculate the speed of the fluid in the left end of the main pipe

Using bernoulli equation

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Pressure for second pipe,

P_{2}=\rho gh_{2}.....(II)

From equation (I) and (II)

P_{2}-P_{1}=\dfrac{1}{2}\rho(v_{1}^2-v_{2}^2)

Put the value of P₁ and P₂

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The continuity equation

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Put the value of v₂ in equation (III)

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Here, \dfrac{A_{1}}{A_{2}}=\gamma

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(b).  The speed of the fluid in the left end of the main pipe \sqrt{\dfrac{2g(h_{2}-h_{1})}{(1-(\gamma)^2)}}

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