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1. A horizontal water jet strikes a plate with mass flow rate $\boldsymbol{m}_{l...
May 1, 2024
1. A horizontal water jet strikes a plate with mass flow rate ml\boldsymbol{m}_{l} and velocity VlV_{l} as shown in Figure 1. Upon striking the plate, the jet is split into two streams, mass flow rate m2m_{2} flowing upwards and m3m_{3} flowing downwards, with velocity V2V_{2} and V3V_{3} respectively. The exit diameter of the jet nozzle is 30 mm30 \mathrm{~mm} and its corresponding velocity is 8 m/s8 \mathrm{~m} / \mathrm{s} (a) When θ\theta is 9090^{\circ}, what is the force required to hold the plate stationary? (5 marks) (b) When θ\theta is 9090^{\circ} and the plate is moving horizontally towards the jet at 3 m/s3 \mathrm{~m} / \mathrm{s}, what is the power required? (7 marks) (c) Derive an expression for m2m_{2} and m3m_{3} in terms of mlm_{l} and angle θ\theta. (10 marks) (d) Determine mass flow rate m2m_{2} and m3m_{3} when θ\theta is 6060^{\circ}. (3 marks) Figure 1
Solution
a
Apply conservation of linear momentum for the horizontal direction: pinitial=pfinal\sum p_{\text{initial}} = \sum p_{\text{final}}
b
Calculate the initial momentum: pinitial=mlVlp_{\text{initial}} = m_{l}V_{l}
c
Calculate the final momentum: pfinal=m2V2cos(θ)m3V3cos(θ)p_{\text{final}} = m_{2}V_{2} \cos(\theta) - m_{3}V_{3} \cos(\theta)
d
Since the plate is stationary, the net horizontal force required is the rate of change of momentum: F=ΔpΔt=mlVl(m2V2cos(θ)m3V3cos(θ))F = \frac{\Delta p}{\Delta t} = m_{l}V_{l} - (m_{2}V_{2} \cos(\theta) - m_{3}V_{3} \cos(\theta))
e
For θ=90\theta = 90^{\circ}, the cosines become zero, so the force is: F=mlVlF = m_{l}V_{l}
Answer
F=mlVlF = m_{l}V_{l}
Key Concept
Conservation of Linear Momentum: The total linear momentum of a closed system remains constant if no external forces are acting on it.
Explanation
The force required to hold the plate stationary is equal to the rate of change of momentum of the water jet, which is the initial momentum since the final horizontal momentum is zero when θ=90\theta = 90^{\circ}.
Solution
a
Calculate the relative velocity of the water jet to the moving plate: Vrel=Vl+3 m/sV_{\text{rel}} = V_{l} + 3 \text{ m/s}
b
The power required is the force times the velocity of the plate: P=FVplateP = F \cdot V_{\text{plate}}
c
Use the force from part (a) and the velocity of the plate: P=mlVl3 m/sP = m_{l}V_{l} \cdot 3 \text{ m/s}
Answer
P=mlVl3 m/sP = m_{l}V_{l} \cdot 3 \text{ m/s}
Key Concept
Power: Power is the rate at which work is done or energy is transferred. It is equal to the force times the velocity of the object in the direction of the force.
Explanation
The power required to move the plate horizontally towards the jet is the product of the force required to hold the plate stationary and the velocity of the plate.
Solution
a
Apply conservation of mass: ml=m2+m3m_{l} = m_{2} + m_{3}
b
Apply conservation of linear momentum in the vertical direction: 0=m2V2sin(θ)m3V3sin(θ)0 = m_{2}V_{2} \sin(\theta) - m_{3}V_{3} \sin(\theta)
c
Solve the system of equations to express m2m_{2} and m3m_{3} in terms of mlm_{l} and θ\theta: m2=mlV3sin(θ)V2sin(θ)+V3sin(θ)m_{2} = \frac{m_{l}V_{3} \sin(\theta)}{V_{2} \sin(\theta) + V_{3} \sin(\theta)} and m3=mlV2sin(θ)V2sin(θ)+V3sin(θ)m_{3} = \frac{m_{l}V_{2} \sin(\theta)}{V_{2} \sin(\theta) + V_{3} \sin(\theta)}
Answer
m2=mlV3sin(θ)V2sin(θ)+V3sin(θ)m_{2} = \frac{m_{l}V_{3} \sin(\theta)}{V_{2} \sin(\theta) + V_{3} \sin(\theta)} and m3=mlV2sin(θ)V2sin(θ)+V3sin(θ)m_{3} = \frac{m_{l}V_{2} \sin(\theta)}{V_{2} \sin(\theta) + V_{3} \sin(\theta)}
Key Concept
Conservation of Mass and Momentum: In a fluid system, the mass flow rate must be conserved, and the momentum must be conserved in each direction.
Explanation
By applying the conservation of mass and momentum, we can derive expressions for m2m_{2} and m3m_{3} in terms of mlm_{l} and θ\theta.
Solution
a
Use the expressions derived in part (c) for m2m_{2} and m3m_{3}
b
Substitute θ=60\theta = 60^{\circ} into the expressions: m2=mlV3sin(60)V2sin(60)+V3sin(60)m_{2} = \frac{m_{l}V_{3} \sin(60^{\circ})}{V_{2} \sin(60^{\circ}) + V_{3} \sin(60^{\circ})} and m3=mlV2sin(60)V2sin(60)+V3sin(60)m_{3} = \frac{m_{l}V_{2} \sin(60^{\circ})}{V_{2} \sin(60^{\circ}) + V_{3} \sin(60^{\circ})}
c
Calculate m2m_{2} and m3m_{3} using the given values for V2V_{2} and V3V_{3}
Answer
The mass flow rates m2m_{2} and m3m_{3} when θ=60\theta = 60^{\circ} are calculated using the expressions from part (c) with the given velocities.
Key Concept
Conservation of Mass and Momentum: In a fluid system, the mass flow rate must be conserved, and the momentum must be conserved in each direction.
Explanation
By substituting θ=60\theta = 60^{\circ} into the expressions derived in part (c), we can determine the mass flow rates m2m_{2} and m3m_{3}.
1 (a) A steady stream of water jet discharges from the nozzle with a uniform velocity of 10 m/s\mathrm{m} / \mathrm{s} at angle 6060^{\circ} as shown in Figure 1. The jet strikes a horizontal plate 2 m2 \mathrm{~m} above the nozzle exit. Upon impact, part of the flow is guided towards the left while the remainder towards the right, and the plate is suspended in the air. The weight of the plate is 25 N25 \mathrm{~N}. Assume frictionless flow along the plate and weight of water to be neglected. (i) Write down the momentum equation for x\mathrm{x} and y\mathrm{y} direction. (ii) Determine the diameter of the nozzle (at the exit). (iii) Determine the mass flow rate A\mathrm{A} and B\mathrm{B}. (12 marks) Figure 1
Solution
a
Write down the momentum equation for the x direction: Fx=m˙ΔVx\sum F_x = \dot{m} \Delta V_x where m˙\dot{m} is the mass flow rate and ΔVx\Delta V_x is the change in velocity in the x direction
b
Write down the momentum equation for the y direction: Fy=m˙ΔVyW\sum F_y = \dot{m} \Delta V_y - W where WW is the weight of the plate
c
To find the diameter of the nozzle, use the continuity equation A1V1=A2V2A_1 V_1 = A_2 V_2 and the fact that the velocity and area are related through the mass flow rate m˙=ρAV\dot{m} = \rho A V where ρ\rho is the density of water
d
Determine the mass flow rate A and B by using the momentum equations in the x and y directions and solving for m˙A\dot{m}_A and m˙B\dot{m}_B
Answer
The diameter of the nozzle and the mass flow rates A and B cannot be determined without additional information such as the density of water and the velocity of the jet at the exit.
Key Concept
Dynamics deals with the study of forces and torques and their effect on motion, particularly Newton's Laws of Motion and the conservation of momentum. In fluid mechanics, the continuity equation and the momentum equation are essential for analyzing fluid flow.
Explanation
The momentum equations in the x and y directions are used to analyze the forces due to the change in momentum of the fluid as it strikes the plate. The continuity equation relates the area and velocity of the jet at different points. Without the density of water or the velocity at the exit, the diameter and mass flow rates cannot be calculated.
1 (a) A steady stream of water jet discharges from the nozzle with a uniform velocity of 10 m/s\mathrm{m} / \mathrm{s} at angle 6060^{\circ} as shown in Figure 1. The jet strikes a horizontal plate 2 m2 \mathrm{~m} above the nozzle exit. Upon impact, part of the flow is guided towards the left while the remainder towards the right, and the plate is suspended in the air. The weight of the plate is 25 N25 \mathrm{~N}. Assume frictionless flow along the plate and weight of water to be neglected. (i) Write down the momentum equation for x\mathrm{x} and y\mathrm{y} direction. (ii) Determine the diameter of the nozzle (at the exit). (iii) Determine the mass flow rate A\mathrm{A} and B\mathrm{B}. (12 marks) Figure 1
Solution
a
Write down the momentum equation for the x and y direction:
b
For the x-direction, apply conservation of momentum: ρQvincos(θ)=ρAvAcos(α)ρBvBcos(β) \rho Q v_{\text{in}} \cos(\theta) = \rho A v_A \cos(\alpha) - \rho B v_B \cos(\beta)
c
For the y-direction, the momentum equation is: ρQvinsin(θ)=Fplate+ρAvAsin(α)+ρBvBsin(β) \rho Q v_{\text{in}} \sin(\theta) = F_{\text{plate}} + \rho A v_A \sin(\alpha) + \rho B v_B \sin(\beta)
d
Determine the diameter of the nozzle: Use the continuity equation Q=Anozzlevin Q = A_{\text{nozzle}} v_{\text{in}} and solve for the area to find the diameter
e
Determine the mass flow rate A and B: Use the momentum equations from steps b and c to solve for A and B
Answer
The momentum equations for the x and y directions are needed to solve for the mass flow rates A and B. The diameter of the nozzle can be found using the continuity equation.
Key Concept
Conservation of Momentum: In the absence of external forces, the momentum of a system remains constant. The momentum equation in fluid dynamics is given by ρQv=ρAvAρBvB \rho Q v = \rho A v_A - \rho B v_B where ρ \rho is the density, Q Q is the volume flow rate, and v v , vA v_A , and vB v_B are the velocities of the jet, flow A, and flow B, respectively.
Explanation
The momentum equation is used to relate the incoming flow to the outgoing flows A and B, taking into account the angle of deflection and the forces acting on the plate.
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