Hydraulics Lab - ECIV 3122 Experiment (5): Flow through small orifices Exp. (5): Flow through small orifices Purpose: To study the flow through small orifice discharging to atmosphere and determine the discharge coefficient, velocity coefficient and the actual jet profile. Apparatus: Small Orifices Apparatus (Fig. 1). Figure (1): Small orifices apparatus Theory: Figure(2) : Vena Contracta The stream line of the orifice contract reducing the area of flow (Vena Contraction). π΄πππ‘π’ππ = πΆπ . π΄ Where: Cc is the coefficient of contraction. 1 Hydraulics Lab - ECIV 3122 Experiment (5): Flow through small orifices Figure (3) : Apply Bernoulli eqn For water at a level of H above the orifice, apply Bernoulli’s equation from the top surface to the orifice: ππ»π΄ = ππ»π΅ + π»πΏ π΄→π΅ Then the velocity of water discharge through the orifice can be written as: ππ΅(πβ.) = √2ππ» Where: - Head losses assumed to be zero. - g is acceleration due to gravity (m/s2) - H is the water height (m) Figure (4) : Trajectory Motion The jet velocity trajectory consists of two components. At the exit of the orifice the vertical component is zero, thus the velocity leaves the orifice horizontally. Neglecting air resistance, the horizontal velocity can be considered as a constant and equal to V. Apply the law of constant velocity motion in x-direction and third law of constant acceleration motion (g) in y-direction: π₯ π‘= π£ 1 π¦ = π£°π¦ π‘ + ππ‘ 2 2 2 Hydraulics Lab - ECIV 3122 Experiment (5): Flow through small orifices Then the velocity of water discharge through the orifice can be written as: π π£πππ‘. = π₯ . √ 2π¦ πΆπ = π£πππ‘ π₯ = … … … … … … … … … . . πππ (1) π£π‘β 2√π» √π¦ So, there are two reasons for the difference between theoretical and actual discharge: πΆπ = ππππ‘. π ⁄π‘ = ππβ. π΄√2ππ» … … … … … … … . … πππ (2) The range of Cd values (0.60-0.65) πΆπ = πΆπ£ × πΆπ … … … … … … … … … … … … . πππ (3) Procedure: 1. Fix 8 mm diameter orifice in the side of the tank. 2. Switch the pump on; allow water to rise until reaching a height of 25 cm. 3. Measure the flow rate (volume collected in certain time) . 4. Measure the trajectory of jet using Hook Gauge. 5. Record the value of x and the corresponding y value. 6. Control the flow valve to increase water height to 50 cm, then repeat the previous steps. 3 Hydraulics Lab - ECIV 3122 Experiment (5): Flow through small orifices Data & Results: 1. Draw a relationship between Qact. in y-axis & √π» in x-axis. Determine the slope of the graph, then calculate Cd ( eqn.2). πΆπ = π ππππ π΄√2π 2. Draw the trajectory of jet for H=50cm (x & -y values). 3. Plot graphs of π₯ against √π¦ (x in y-axis & √π¦ in x-axis) for H=50cm. Determine the slope of the graph, then calculate Cv (eqn.1). πΆπ£ = 4. π ππππ 2√π» Calculate the coefficient of contraction (eqn.3). H (cm) 50 25 Qth (m3/s) V (L) t (sec) Qact (m3/s) √π» (m) H=50cm x (cm) 0 10 15 20 25 y (mm) x (m) y (m) √π¦(π) 4 30 35 40 45 50