Thermofluids - Bernoulli Applications

Problem Solving

  • Problem-solving requires factual and procedural knowledge.
    • Factual knowledge: knowledge of "things."
    • Procedural knowledge: knowledge of "how to do things."
  • Schema: A specific type of problem.
  • Improving problem-solving:
    1. Increase domain knowledge.
    2. Learn schema for various problem types.
    3. Become more conscious of the problem-solving process.
  • Focus on the solution process rather than just obtaining the answer.

Problem Solving Strategy

  1. Understand the problem.
  2. Devise a plan.
  3. Carry out the plan.
  4. Look back and check the solution.

Bernoulli's Equation

  • Relates pressure PP, speed vv, and height hh of two points in a steady streamline of fluid with density ρρ.
  • Equation:
    P<em>1+12ρv</em>12+ρgh<em>1=P</em>2+12ρv<em>22+ρgh</em>2P<em>1 + {1 \over 2} ρv</em>1^2 + ρgh<em>1 = P</em>2 + {1 \over 2} ρv<em>2^2 + ρgh</em>2
  • Alternative expressions:
    • Specific energy (J/kg): P<em>1ρ+V</em>122+gz<em>1=P</em>2ρ+V<em>222+gz</em>2\frac{P<em>1}{ρ} + \frac{V</em>1^2}{2} + gz<em>1 = \frac{P</em>2}{ρ} + \frac{V<em>2^2}{2} + gz</em>2
    • Pressure (Pa): P<em>1+ρV</em>122+ρgz<em>1=P</em>2+ρV<em>222+ρgz</em>2P<em>1 + ρ \frac{V</em>1^2}{2} + ρgz<em>1 = P</em>2 + ρ \frac{V<em>2^2}{2} + ρgz</em>2
    • Head (m): P<em>1ρg+V</em>122g+z<em>1=P</em>2ρg+V<em>222g+z</em>2\frac{P<em>1}{ρg} + \frac{V</em>1^2}{2g} + z<em>1 = \frac{P</em>2}{ρg} + \frac{V<em>2^2}{2g} + z</em>2
  • At any point on a streamline:
    Pρ+V22+gz=constant\frac{P}{ρ} + \frac{V^2}{2} + gz = constant

Bernoulli's Equation - Application

  • Most fluid problems use both mass conservation and Bernoulli's equations.
  • Mass conservation:
    m˙=ρAvˉ=ρAV [kg/s]\dot{m} = ρA\bar{v} = ρAV \ [kg/s]
    ρ<em>1A</em>1V<em>1=ρ</em>2A<em>2V</em>2ρ<em>1A</em>1V<em>1 = ρ</em>2A<em>2V</em>2
    A<em>1V</em>1=A<em>2V</em>2A<em>1V</em>1 = A<em>2V</em>2
    V<em>2=A</em>1A<em>2V</em>1V<em>2 = \frac{A</em>1}{A<em>2} V</em>1
  • Bernoulli's equation (horizontal flow, zz constant):
    Pρ+V22=constant\frac{P}{ρ} + \frac{V^2}{2} = constant
  • Example: Tank with a hole at the bottom:
    • Velocity at the hole: V2=2gHV_2 = \sqrt{2gH}
    • Mass flow rate: m˙=ρA22gH\dot{m} = ρA_2 \sqrt{2gH}

General Information

  • Practical induction: Tuesday the 11th of March at 14:00 in room 234.
  • Email emlyn.wright@canterbury.ac.nz to arrange participation.