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Linear momentum and impulse-momentum equation

Short answer

Newton's second law: force equals rate of change of momentum. For steady flow, net force on fluid equals mass flow rate times change in velocity. For a jet on a stationary body, force equals ρQ(V1x - V2x). For a flat plate normal to jet, F = ρaV²; for a curved vane turning through angle θ, F = ρaV²(1 - cosθ).

State Newton's second law in terms of linear momentum. Derive the impulse-momentum equation and the force exerted by a fluid jet on a stationary body using the control volume approach.

Momentum principle

Newton's second law: the rate of change of linear momentum of a body is equal to the resultant force acting on it, and takes place in the direction of that force.

F⃗=d(mV⃗)dt\vec F = \frac{d(m\vec V)}{dt}

If the force FF acts for a short time dtdt, then F dt=d(mV)F\,dt = d(mV). The left side is the impulse and the right side is the change of momentum. This is the impulse-momentum equation.

Control volume form (steady flow)

Consider a fixed control volume with one inlet (section 1) and one outlet (section 2), through which fluid of density ρ\rho flows steadily. The mass flow rate is m=ρQ=ρA1V1=ρA2V2m = \rho Q = \rho A_1 V_1 = \rho A_2 V_2.

In time dtdt the mass dm=ρQ dtdm = \rho Q\,dt enters with velocity V1V_1 and the same mass leaves with velocity V2V_2. Momentum change of the fluid in the given direction xx:

dm (V2x−V1x)=ρQ dt (V2x−V1x)dm\,(V_{2x} - V_{1x}) = \rho Q\,dt\,(V_{2x}-V_{1x})

Dividing by dtdt, the net external force on the fluid in the control volume (pressure forces, body force and force by the solid surface) is

∑Fx=ρQ (V2x−V1x),∑Fy=ρQ (V2y−V1y)\sum F_x = \rho Q\,(V_{2x} - V_{1x}), \qquad \sum F_y = \rho Q\,(V_{2y} - V_{1y})

Force of jet on a stationary body

For a free jet, the pressure is atmospheric everywhere on the control surface, so pressure forces cancel and the body force is negligible. The only force on the fluid is the force RR exerted by the body on the fluid. By Newton's third law the force of the jet on the body is equal and opposite:

Fx=ρQ (V1x−V2x)F_x = \rho Q\,(V_{1x} - V_{2x})

Hence the force on a body equals the rate at which the fluid loses momentum in that direction. Direction of the force is found by the sign of (V1x−V2x)(V_{1x}-V_{2x}).

Special results for a jet of area aa and velocity VV:

  • Flat plate normal to jet (fluid leaves along plate, so V2x=0V_{2x}=0): F=ρaV2F = \rho a V^2.
  • Symmetrical curved vane turning the jet through angle θ\theta (measured from the jet direction): F=ρaV2(1−cos⁡θ)F = \rho a V^2(1-\cos\theta).

These expressions are the basis for the analysis of Pelton wheel buckets and other impulse machines.

✓ Answer checked by Claude Sonnet 5.5

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