- Practice · 6 marks
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.
If the force acts for a short time , then . 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 flows steadily. The mass flow rate is .
In time the mass enters with velocity and the same mass leaves with velocity . Momentum change of the fluid in the given direction :
Dividing by , the net external force on the fluid in the control volume (pressure forces, body force and force by the solid surface) is
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 exerted by the body on the fluid. By Newton's third law the force of the jet on the body is equal and opposite:
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 .
Special results for a jet of area and velocity :
- Flat plate normal to jet (fluid leaves along plate, so ): .
- Symmetrical curved vane turning the jet through angle (measured from the jet direction): .
These expressions are the basis for the analysis of Pelton wheel buckets and other impulse machines.
✓ Answer checked by Claude Sonnet 5.5
Related questions
- Force of jet on flat plate, stationary and moving · Fluid Machines, chapter 1
- Force of jet on symmetrical curved vane · Fluid Machines, chapter 1
- Momentum equation and its applications · Fluid Mechanics, chapter 4
- Jet on moving curved vanes, force and work · Fluid Mechanics, chapter 7
- Principle of impulse and momentum · Engineering Mechanics, chapter 4
- General energy equation for control volume · Fundamental of Thermodynamics & Heat Transfer, chapter 4