Math Problem Statement

A venturimeter has its axis vertical, the inlet

and throat diameters being 150 mm and 75 mm

respectively. The throat is 225 mm above inlet

and venturimeter constant = 0.96. Petrol of sp.

gravity 0.78 Àows up through the meter at a

rate of 0.029 m3

/s. Find the pressure difference

between inlet and throat.

Solution

To find the pressure difference between the inlet and throat in the venturimeter, we can use Bernoulli’s equation and continuity equation.

Given dataTo find the pressure difference between the inlet and throat in the venturimeter, we can use Bernoulli’s equation and continuity equation.

Given

  • Inlet diameter (D₁) = 150 mm = 0.15 m
  • Throat diameter (D₂) = 75 mm = 0.075 m
  • Height difference (hh) = 225 mm = 0.225 m
  • Venturimeter constant (Cₓ) = 0.96
  • Specific gravity of petrol = 0.78 → Density of petrol ρ\rho = 0.78 ×\times 1000 = 780 kg/m³
  • Flow rate (QQ) = 0.029 m³/s

We need to find the pressure difference (ΔP) between the inlet and the throat.

Step 1: Calculate the velocities at the inlet and throat using the continuity equation.

The continuity equation states: Q=A1V1=A2V2Q = A_1 V_1 = A_2 V_2 where A1A_1 and A2A_2 are the cross-sectional areas at the inlet and throat, respectively, and V1V_1 and V2V_2 are the velocities at the inlet and throat.

The area of a circular section is given by: A=πD24A = \frac{\pi D^2}{4}

  1. Calculate A1A_1 and A2A_2:

    A1=π×(0.15)24=0.01767m2A_1 = \frac{\pi \times (0.15)^2}{4} = 0.01767 \, \text{m}^2 A2=π×(0.075)24=0.00442m2A_2 = \frac{\pi \times (0.075)^2}{4} = 0.00442 \, \text{m}^2

  2. Calculate V1V_1 and V2V_2:

    V1=QA1=0.0290.01767=1.641m/sV_1 = \frac{Q}{A_1} = \frac{0.029}{0.01767} = 1.641 \, \text{m/s} V2=QA2=0.0290.00442=6.56m/sV_2 = \frac{Q}{A_2} = \frac{0.029}{0.00442} = 6.56 \, \text{m/s}

Step 2: Apply Bernoulli's equation between the inlet and throat

Using Bernoulli's equation, including the height difference, we have: P1+12ρV12+ρgz1=P2+12ρV22+ρgz2P_1 + \frac{1}{2} \rho V_1^2 + \rho g z_1 = P_2 + \frac{1}{2} \rho V_2^2 + \rho g z_2 where:

  • P1P_1 and P2P_2 are the pressures at the inlet and throat,
  • V1V_1 and V2V_2 are the velocities at the inlet and throat,
  • z1z_1 and z2z_2 are the heights of the inlet and throat, with z2z1=hz_2 - z_1 = h,
  • gg is the gravitational acceleration (9.81 m/s²).

Rearrange to find ΔP=P1P2\Delta P = P_1 - P_2: ΔP=12ρ(V22V12)+ρgh\Delta P = \frac{1}{2} \rho (V_2^2 - V_1^2) + \rho g h

Substituting the values:

  1. Calculate the dynamic pressure term: 12ρ(V22V12)=12×780×(6.5621.6412)=14809.4Pa\frac{1}{2} \rho (V_2^2 - V_1^2) = \frac{1}{2} \times 780 \times (6.56^2 - 1.641^2) = 14809.4 \, \text{Pa}

  2. Calculate the hydrostatic pressure term: ρgh=780×9.81×0.225=1715.4Pa\rho g h = 780 \times 9.81 \times 0.225 = 1715.4 \, \text{Pa}

  3. Total pressure difference ΔP\Delta P (considering the Venturimeter constant Cx=0.96C_x = 0.96): ΔP=Cx(14809.4+1715.4)=0.96×16524.8=15844.6Pa\Delta P = C_x \left(14809.4 + 1715.4\right) = 0.96 \times 16524.8 = 15844.6 \, \text{Pa}

Answer:

The pressure difference between the inlet and throat is approximately 15,844.6 Pa.


Would you like further explanation, or have any questions?

Related Questions

  1. How does the height difference affect the pressure drop in a Venturimeter?
  2. What are the limitations of using the Venturimeter constant (Cₓ) in real-life applications?
  3. How would the pressure difference change if a denser fluid were used?
  4. Can a Venturimeter be used horizontally, and how would this affect the calculations?
  5. Why is the throat diameter smaller than the inlet in a Venturimeter?

Tip

Remember, specific gravity relates the density of a fluid to water, which is useful in converting it directly into density (kg/m³) by multiplying by 1000.

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Math Problem Analysis

Mathematical Concepts

Fluid Mechanics
Continuity Equation
Bernoulli’s Equation
Pressure Difference

Formulas

Continuity equation: Q = A1 * V1 = A2 * V2
Cross-sectional area of a circle: A = π * D² / 4
Bernoulli's equation with height difference: ΔP = 1/2 * ρ * (V2² - V1²) + ρ * g * h
Density from specific gravity: ρ = specific gravity * 1000

Theorems

Bernoulli’s Theorem

Suitable Grade Level

Undergraduate Engineering