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.

  • 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 Theorem Applications

  • P1+12ρv12+ρgh1=P2+12ρv22+ρgh2P1 + \frac{1}{2} \rho v1^2 + \rho g h1 = P2 + \frac{1}{2} \rho v2^2 + \rho g h2

  • Specific energy (J/kg): P1ρ+V122+gz1=P2ρ+V222+gz2\frac{P1}{\rho} + \frac{V1^2}{2} + gz1 = \frac{P2}{\rho} + \frac{V2^2}{2} + gz2

  • Pressure (Pa): P1+ρV122+ρgz1=P2+ρV222+ρgz2P1 + \rho \frac{V1^2}{2} + \rho gz1 = P2 + \rho \frac{V2^2}{2} + \rho gz2

  • Head (m): P1ρg+V122g+z1=P2ρg+V222g+z2\frac{P1}{\rho g} + \frac{V1^2}{2g} + z1 = \frac{P2}{\rho g} + \frac{V2^2}{2g} + z2

  • At any point on a streamline: Pρ+V22+gz=constant\frac{P}{\rho} + \frac{V^2}{2} + gz = constant

Bernoulli's Equation - Application

  • Most fluid problems require using both mass conservation and Bernoulli equations.

  • Mass conservation:

    • m˙=ρAv=ρAV[kg/s]\dot{m} = \rho A \overline{v} = \rho A V [kg/s]

    • ρ<em>1A</em>1V<em>1=ρ</em>2A<em>2V</em>2\rho<em>1 A</em>1 V<em>1 = \rho</em>2 A<em>2 V</em>2

    • A<em>1V</em>1=A<em>2V</em>2A<em>1 V</em>1 = A<em>2 V</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 equation:

    • Pρ+V22+gz=constant\frac{P}{\rho} + \frac{V^2}{2} + gz = constant

    • Pρ+V22=constant\frac{P}{\rho} + \frac{V^2}{2} = constant

  • Example: Tank with a hole at the bottom

    • Bernoulli Equation: P<em>1ρ+v</em>122+gz<em>1=P</em>2ρ+v<em>222+gz</em>2\frac{P<em>1}{\rho} + \frac{\overline{v}</em>1^2}{2} + gz<em>1 = \frac{P</em>2}{\rho} + \frac{\overline{v}<em>2^2}{2} + gz</em>2

    • P<em>1=P</em>2=P<em>atmP<em>1 = P</em>2 = P<em>{atm}, v</em>1=0\overline{v}</em>1 = 0

    • v<em>2=2g(z</em>1z2)=2gH\overline{v}<em>2 = \sqrt{2g(z</em>1 - z_2)} = \sqrt{2gH}

    • m˙=ρA<em>2v</em>2=ρA22gH\dot{m} = \rho A<em>2 \overline{v}</em>2 = \rho A_2 \sqrt{2gH}

General Points

  • Water clock progress should tested before to ensure delivery to timeframe.