power point presentation CHAPTER1 P2... · TANGENTIAL JET IMPINGEMENT ON A MOVING VANE . ... force...

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Hydraulic Machines power point presentation Slides has been adapted from Hydraulic Machines, K. Subramanya 1 2016-2017 Prepared by Dr. Assim Al-Daraje

Transcript of power point presentation CHAPTER1 P2... · TANGENTIAL JET IMPINGEMENT ON A MOVING VANE . ... force...

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Hydraulic Machines

power point presentation Slides has been adapted from

Hydraulic Machines, K. Subramanya

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2016-2017 Prepared by Dr. Assim Al-Daraje

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Chapter ( 1 Part 2) Prepared by Dr. Assim Al-Daraje

Jet Impingement on o Moving Plate

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Jet Impingement on o Moving Plate

In this case, the plane of the plate is inclined at an angle θ to the jet and the plate is moving with a velocity u in the direction of the jet. Figure 1(a) is a definition sketch of the flow. Notice that in this flow situation, there is a relative motion between the jet of water and the plate. Relative to the plate. the jet has a velocity of (V - u).

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Fig. (1) Jet impingement at moving plate

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Hence, to solve this problem, consider a velocity of magnitude (-u), which is equal and opposite to the velocity of the plate, being superimposed on the flow system. The resulting flow situation, which can be called the equivalent relative flow over the plate, is shown in Fig. 1(b).

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Velocity Triangles

α = Angle made by the absolute velocity vector 𝑉 with the direction of the peripheral velocity u, known as guide vane angle β = Angle made by the relative velocity vector 𝑣𝑟, with the negative direction of the peripheral velocity u; known as blade angle

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Vector relationship

The velocity triangle is a graphical relationship of this vector addition. The procedure is as follows: Referring to Fig. (4)

Fig. (4) Velocity triangle B > π/2

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refer to the inlet to the vane, then ∆ ABC is known as inlet velocity triangle. lf the velocity vectors refer to the outlet from the vane, then ∆ ABC is known as outlet velocity triangle.

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<CAB = α is known as guide vane angle. <CBA = β is known as blade angle (or vane angle).

Fig. (5) Velocity triangle B = π/2

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Fig. (5) Velocity triangle B < π/2

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The suffixes I and 2 are used to represent inlet and outlet conditions at all components and elements of the system, respectively. In general, the absolute velocity V can be resolved in to two components:

From the velocity triangles:

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TANGENTIAL JET IMPINGEMENT ON A MOVING VANE

the relative velocity vector 𝑣𝑟1 are related as:

The flow over the vane is assumed frictionless, i. e. 𝑣𝑟1= 𝑣𝑟2

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15 Fig. (6) Velocity triangles for jet impingement on a moving vane for

different outlet angle conditions

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β2 = Blade angle at the outlet. It is the angle made by the relative velocity vector �⃗� with the negative direction of the velocity of vane u at the outlet. 𝑉𝑢1= Velocity of whirl, component of the absolute velocity 𝑉1 in the direction of (u = 𝑉1 cos α1) 𝑉𝑓1 = Velocity of flow, component of the absolute velocity 𝑉1 in the direction normal to that of u - 𝑉1 sin α1

β1 = Blade angle at the inlet. It is the angle made by the relative velocity vector �⃗� with the negative direction of the velocity of vane u at the inlet.

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For the single vane moving with a velocity u, the force on the vane in the u-direction (x-direction) is given by the linear momentum equation as: 𝐹𝑥 = ϱ [relative discharge] x [change in the u-component of the velocity u at inlet = ϱ [relative discharge] x [-∆𝑉𝑢] Considering the absolute velocities:

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For all the three cases of guide vane angle α2 studied above, the power transmitted to the vane can be represented as

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EXAMPLE 1.1 A free jet issuing from a nozzle of 0.0113 m2 cross-sectional area impinges normally on a fixed vertical plate. The force on the plate due to this impingement is found to be 2.54 kN. (a) Estimate the discharge from the nozzle. (b) If the plate is allowed to move with a velocity of 3.0 m/s in the direction of the jet, what would be the (i) force on the plate and (ii) power transferred to the plate in this system? Solution: Σ Force in x-direction) = 1 (Momentum flux in x-direction)out - (Momentum flux in x direction)in

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(b) When the plate is moving, the relative velocity of the jet and also the relative discharge from the nozzle have to be considered. Attached Figure shows the relative steady flow.

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EXAMPLE: 1-2 A 6.0 cm diameter free jet of water having a velocity of 10 m/s impinges on a plane, smooth plate at angle of 30' to the normal to the plate. (a) What will be the force due to jet impingement on the plate and work done per second when the plate is (i) stationary, and (ii) moving in the direction of the jet at 5.0 m/s velocity? (b)What will be the force due to jet on the plate where u the plate is moving against the jet direction at 5.0 m/s velocity? Solution:

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(a) (i) Stationary Plate: Consider the normal and tangential directions and a control volume as in attached Figure .Let R,= Normal reaction on the control volume. Let β = Inclination of the jet axis with the normal to the plate. Since the pressure is atmospheric on all the control volume surfaces, by linear momentum equation:

where V=Velocity of the jet, and β= Inclination of the jet to the normal of the plate.

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Since there is no friction, there is no tangential component of the force on the plate.

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Since there is no friction, there is no tangential component of the force on the plate.

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EXAMPLE 1 A 6 cm diameter jet of water impinges on a moving hemispherical cup in the middle of it shallow portion and is deflected by I80".The jet has a velocity of 35m/s and the cup has a velocity of l0 m/s in the same direction as the jet. Determine (a) the rate of work done by the jet on the cup and the efficiency of the system. (b) What would be the force on the cup if the cup were moving in a direction opposite to that of the jet? Assume frictionless flow. Solution: Consider equivalent relative motion with respect to stationary cup, attached Fig. Since the flow is frictionless, Exit relative velocity 𝑣𝑟2= Inlet velocity 𝑣𝑟1=𝑣𝑟.

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Jet impingement on o moving hemispherical cup

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EX: 1.6: A I0 cm diameter jet of water strikes a curved vane with a velocity of 25 rn/s. The inlet angle of the vane is zero and the outlet angle is 150o measured with respect to the impinging jet direction. Determine the resultant force on the vane (a) when the vane is stationary, and (b) when the vane is moving in the direction of the jet at 10 m/s velocity.

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Relative flow,

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EXAMPLE 1.7 A jet of water 15 cm in diameter strikes a curved blade at 20 m/s velocity. The inlet and outlet angles of the blade are 0° and 135° respectively measured with respect to the direction of motion of the initial jet velocity. Determine the resultant force exerted on the blade when (a) the blade is stationary, and (b) the blade moves against the direction of the jet at a velocity of 5 m/s. Neglect friction along the blade. Solution: Let suffix I and2 denote the inlet and outlet conditions respectively. (a) When the jet is stationary: The definition sketch is similar to Figure of the previous problem (Example 1). Assuming no losses 𝑉1 = 𝑉2 = V = 20.0 m/s.

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(b) When the vane is moving with velocity u against the jet: The relative motion is shown in below Figure.

Relative flow,

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