Question #87615
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Q1. Sections 1 and 2 are at the beginning and end of the bend of the 200 mm diameter pipe in which the quantity of flow is 0.28 m3/s. The angle of deflection of the water is 40. Calculate the force that the liquid exerts on the bend if the pressure in the pipe is 50 kPa. Assume no loss of pressure round the bend.

Q2. A 50 mm diameter stream of water strikes a 0.5 m by 0.5 m square plate which is at an angle of 30 degrees with the stream’s direction. The velocity of the water in the stream is 20 m/s and the jet strikes the door at its centre of gravity. If the plate is hinged at A, by neglecting the friction and self-weight of the plate, determine the normal force P applied at the upper edge of the plate to keep the plate in equilibrium. You may assume that the velocities of the jet remain unchanged after split.
1
Expert's answer
2019-04-12T09:41:35-0400

A1.


F=ma=mΔv/Δt,F=ma=m\cdot \Delta v/\Delta t,

m=ρV=ρQΔt,m=\rho V=\rho Q\Delta t,

Δv=v2v1=v1cos40v1=v1(cos401),\Delta v=v_2-v_1=v_1\text{cos}40^\circ-v_1=v_1(\text{cos}40^\circ-1),




v1=Q/A=4Q/(πd2),v_1=Q/A=4Q/(\pi d^2),


finally,


F=ρQΔt4Qπd2(cos401)1Δt=F=\rho Q\Delta t\cdot \frac{4Q}{\pi d^2}(\text{cos}40^\circ-1)\frac{1}{\Delta t}=

=4ρQ2(cos401)πd2=582 N.=\frac{4\rho Q^2(\text{cos}40^\circ-1)}{\pi d^2}=582\text{ N}.

A2. This problem can be solved likewise. First, calculate the force acting on the centre of the door. To do that, transform the expression for FF we obtained above considering that Q=v1πd2/4Q=v_1\pi d^2/4:



F=4ρ(v1πd2/4)2(cos601)πd2=F=\frac{4\rho (v_1\pi d^2/4)^2(\text{cos}60^\circ-1)}{\pi d^2}=

=ρv12πd2(cos601)4=391.9 N.=\frac{\rho v_1^2\pi d^2(\text{cos}60^\circ-1)}{4}=391.9\text{ N}.

Now simply apply equations for moment of force: our force FF calculated above acts on a centre of plate 50 cm in length:



Assume that the moments are considered in relation to the lower edge.


0=0.25F0.5Psin30,0=0.25F-0.5P\text{sin}30^\circ,

P=0.25F0.5sin30=391.9 N.P=\frac{0.25F}{0.5\text{sin}30^\circ}=391.9\text{ N}.


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