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A liquid of density rho flows along a ho...

A liquid of density `rho` flows along a horizontal pipe of uniform cross-section `A` with a velocity v through a right angled bend as shown in fig. What force has to be exerted at the bend to hold the pipe in equilibrium ? .

A

`2arhov^2`

B

`arhov^2//sqrt2`

C

`sqrt2 arhov^2`

D

`arhov^2`

Text Solution

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The correct Answer is:
To find the force that must be exerted at the bend of a horizontal pipe to hold it in equilibrium, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Situation**: - We have a liquid flowing through a horizontal pipe with a uniform cross-section and a right-angled bend. The liquid has a density \( \rho \) and flows with a velocity \( v \). 2. **Identify the Change in Momentum**: - As the liquid flows through the bend, it changes direction. The change in momentum is crucial to determine the force required to keep the pipe in equilibrium. 3. **Calculate the Mass Flow Rate**: - The mass flow rate \( \frac{dm}{dt} \) can be calculated using the formula: \[ \frac{dm}{dt} = \rho A v \] - Here, \( A \) is the cross-sectional area of the pipe, and \( v \) is the velocity of the liquid. 4. **Determine the Force**: - The force exerted by the liquid due to the change in momentum can be expressed as: \[ F = \frac{dm}{dt} \cdot v \] - Substituting the mass flow rate into this equation gives: \[ F = (\rho A v) \cdot v = \rho A v^2 \] 5. **Consider the Resultant Force at the Bend**: - At the bend, the forces acting on the pipe can be resolved into two components (one vertical and one horizontal). The resultant force \( R \) at the bend can be calculated as: \[ R = \sqrt{F^2 + F^2} = \sqrt{2F^2} = \sqrt{2}F \] - Since both components are equal, we can express this as: \[ R = \sqrt{2} \cdot (\rho A v^2) \] 6. **Final Expression for the Force**: - Therefore, the total force that must be exerted at the bend to hold the pipe in equilibrium is: \[ F = \rho A v^2 \] ### Conclusion: The force that has to be exerted at the bend to hold the pipe in equilibrium is \( F = \rho A v^2 \).
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