Fluid Kinematics: Worked Examples

These examples progress from one-dimensional continuity to velocity-field differentiation and two-dimensional flow representations. Each solution states the kinematic assumptions used.

Problem 1: Continuity Through a Converging Pipe

Water flows steadily through a full pipe that contracts from D1=200 mmD_1=200\text{ mm} to D2=100 mmD_2=100\text{ mm}. The upstream mean velocity is V1=2.00 m/sV_1=2.00\text{ m/s}. Determine the discharge and downstream mean velocity.

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Problem 2: Flow Division at a Junction

A main pipe delivers 0.100 m3/s0.100\text{ m}^3/\text{s} to a junction. Branch 1 has D1=150 mmD_1=150\text{ mm} and V1=2.00 m/sV_1=2.00\text{ m/s}. Branch 2 has D2=200 mmD_2=200\text{ mm}. Determine the Branch 2 discharge and mean velocity.

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Problem 3: Compressible Mass Continuity

Air enters a duct with ρ1=1.20 kg/m3\rho_1=1.20\text{ kg/m}^3, A1=0.500 m2A_1=0.500\text{ m}^2, and V1=10.0 m/sV_1=10.0\text{ m/s}. It exits where ρ2=0.900 kg/m3\rho_2=0.900\text{ kg/m}^3 and A2=0.300 m2A_2=0.300\text{ m}^2. For steady flow with no leakage, determine mass flow rate and exit velocity.

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Problem 4: Acceleration from a Two-Dimensional Velocity Field

A steady velocity field is u=2xyu=2xy and v=x2−y2v=x^2-y^2, with coordinates in meters and velocities in m/s\text{m/s}. Determine the acceleration vector at (x,y)=(1.00,2.00)(x,y)=(1.00,2.00).

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Problem 5: Local and Convective Acceleration

A one-dimensional unsteady velocity field is u=x(1+2t)u=x(1+2t), with xx in meters and tt in seconds. Determine local, convective, and total acceleration at x=2.00 mx=2.00\text{ m} and t=1.00 st=1.00\text{ s}.

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Problem 6: Velocity and Discharge from a Stream Function

A two-dimensional incompressible flow has ψ=3xy\psi=3xy in m2/s\text{m}^2/\text{s}. Using u=∂ψ/∂yu=\partial\psi/\partial y and v=−∂ψ/∂xv=-\partial\psi/\partial x, determine the velocity at (2.00,1.00)(2.00,1.00) and discharge per unit depth between ψ=3\psi=3 and ψ=12 m2/s\psi=12\text{ m}^2/\text{s}.

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Problem 7: Incompressibility and Irrotationality Check

For the two-dimensional field u=4xu=4x and v=−4yv=-4y, determine whether the flow is compatible with constant-density incompressibility and whether it is irrotational.

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Problem 8: Unsteady Storage in a Tank

A vertical tank has constant plan area At=10.0 m2A_t=10.0\text{ m}^2. Water enters at 0.0800 m3/s0.0800\text{ m}^3/\text{s} and leaves at 0.0300 m3/s0.0300\text{ m}^3/\text{s}. Determine the water-level rise rate and the rise after 5.00 min5.00\text{ min} if both flows remain constant.

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Problem 9: Equation of a Streamline

A steady two-dimensional field is u=2xu=2x and v=−yv=-y. Determine the streamline passing through (x,y)=(1.00,2.00)(x,y)=(1.00,2.00) and find yy where that streamline reaches x=4.00x=4.00.

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Problem 10: Velocity Potential and Laplace Check

A proposed velocity potential is ϕ=2x2−2y2\phi=2x^2-2y^2 in m2/s\text{m}^2/\text{s}. Determine the velocity at (1.00,2.00)(1.00,2.00) and verify incompressibility.

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Problem 11: Seepage Discharge from a Flow Net

A two-dimensional isotropic seepage flow net has hydraulic conductivity k=2.00×10−5 m/sk=2.00\times10^{-5}\text{ m/s}, total head loss H=6.00 mH=6.00\text{ m}, Nf=4N_f=4 flow channels, and Nd=12N_d=12 equipotential drops. Determine seepage discharge per unit thickness.

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