Fundamentals of Engineering

11 (B): Fluid Statics

Practice Problems

1)   The atmospheric pressure on an Earth-like planet (far far away) is \(80 \, kPa\). If humans were to build a habitat on this planet what should the gage pressure on the inside be

  1. \(17 \, kPa\)
  2. \(21 \, kPa\)
  3. \(26 \, kPa\)
  4. \(31 \, kPa\)

The correct answer is (B)    

Solution: Based on the local atmospheric pressure of \(80 \, kPa \) and assuming that the desired habitat pressure is \(101 \, kPa\) abs. the gage pressure inside the hab should be $$ \text{gage pressure} = \text{abs pressure in hab} - \text{local atm pressure} $$ $$ \begin{align} \text{gage pressure} &= 101 kPa - 80 kPa \\ &= 21 kPa \end{align} $$ The correct answer is (B)  

2)   The absolute pressure inside a container is \(25 \, kPa\). What is the vacuum pressure. Assume the local atmospheric pressure to be \(101 \, kPa\)

  1. \(55 \, kPa\)
  2. \(68 \, kPa\)
  3. \(76 \, kPa\)
  4. \(91 \, kPa\)

The correct answer is (C)    

Solution: Vacuum pressure is the difference between atmospheric pressure and abs pressure inside the container $$ \text{vacuum pressure} = 101 \, kPa - 25 \, kPa = 76 \, kPa $$ The correct answer is (C)  

3)   What pressure is equivalent to \(600 \, mm\) of mercury (SG \(13.6\)).

  1. \(43 \, kPa\)
  2. \(58 \, kPa\)
  3. \(72 \, kPa\)
  4. \(80 \, kPa\)

The correct answer is (D)    

Solution: Given the height of mercury in the column $$ \begin{align} P_{gage} &= \rho g h \\ &= 13{,}600 \, kg/m^3 \times 9.81 \, m/s^2 \times 0.6 \, m \\ &= 80{,}050 \, Pa \\ &= 80 \, kPa \end{align} $$ The correct answer is (D)  

4)   A closed cylindrical tank, shown in the figure has a pressure \( 60 \, kPa\) inside the dome. Determine the pressure in pipe B.

Fig 4
  1. \(89 \, kPa\)
  2. \(103 \, kPa\)
  3. \(124 \, kPa\)
  4. \(135 \, kPa\)

The correct answer is (B)    

Solution: Note that \( P_1 = P_2 = P_3\), so $$ \begin{align} P_B &= P_A + (\rho g h)_{oil} + (\rho g h)_{water} \\\\ P_B &= 60{,}000 Pa \\ &+ 800 \, kg/m^3 \times 9.81 \, m/s^2 \times 3 m \\ &+ 1000 \, kg/m^3 \times 9.81 \, m/s^2 \times 2 m\\\\ P_B &= 103 \, kPa \end{align} $$ The correct answer is (B)  

5)   Pipe \(A\) and \(B\) both contain water. The gage fluid in the manometer shown has a specific gravity of \(3.46\). Calculate the differential pressure

Fig 5
  1. \(15.5 \, kPa\)
  2. \(17.9 \, kPa\)
  3. \(21.5 \, kPa\)
  4. \(30.1 \, kPa\)

The correct answer is (A)    

Solution: Note that the pressure at points marked 2 and 3 are going to be the same. $$ P_A + \gamma_w \cdot (0.6 m + 0.4 m) + \gamma_{gf} \cdot 0.4 m = P_B + \gamma_w \cdot (0.4 m + 0.4 m) $$ Rearrange and cancel terms to get $$ \begin{align} P_A - P_B &= \gamma_w \cdot 0.2 \, m + \gamma_{gf} \cdot 0.4 \, m \\ &= 9810 \, N/m^3 \times 0.2 \, m + 3.46 \times 9810 \, N/m^3 \times 0.4 \, m \\ &= 15{,}539 \, Pa \\ &= 15.5 \, kPa \end{align}$$ The correct answer is (A)  

6)   A tank containing water has a gate hinged at the bottom as shown in the figure below. The gate is \(5 \, m\) wide. Calculate the force on the gate due to water pressure.

Fig 6
  1. \(1104 \, kN\)
  2. \(1380 \, kN\)
  3. \(1655 \, kN\)
  4. \(2152 \, kN\)

The correct answer is (A)    

Solution: The total force on the gate will be equal to the average pressure times the area. $$ \begin{align} F &= P_{avg} \times A \\ &= (\gamma_w \cdot h_{avg}) \times A \\ &= 9810 \, N/m^3 \times 4.5 \, m \times 25 \, m^2 \\ &= 1{,}103{,}625 \, N \\ &= 1104 \, kN \\ \end{align}$$ The correct answer is (A)  

7)   A \(4 \, m\) wide curved gate is located in the bottom of a reservoir containing water. Determine the magnitude of the resultant force of water on the gate.

Fig 7
  1. \( 281 \, kN \)
  2. \( 352 \, kN \)
  3. \( 470 \, kN \)
  4. \( 587 \, kN \)

The correct answer is (D)    

Solution: For curved surfaces calculate the horizontal and vertical forces and then combine them to find the resultant. $$ \begin{align} F_{hor} &= P_{avg} \times A_{projected} \\ &= \gamma_w \cdot {h_1 + h_2 \over 2} \times A_{projected} \\ &= 9810 \, N/m^3 \cdot {4+6 \over 2} \, m \times (2m \cdot 4m) \\ &= 392{,}400 \, N \\\\ F_{ver} &= \gamma_w \times (V_1 + V_2) \\ &= 9810 \, N/m^3 \times \left( (4m \cdot 2m \cdot 4m) + { \pi \cdot (2m)^2 \cdot 4m \over 4} \right) \\ &= 437{,}196 \, N \\\\ F &= \sqrt{392{,}400^2 + 437{,}196^2} \\ &= 587{,}468 \, N \\ &= 587 \, kN \end{align} $$ The correct answer is (D)  

8)   A log floats with one fourth of its volume protruding above the water surface. Determine the specific weight of the log.

  1. \(2345.2 \, N/m^3\)
  2. \(4690.4 \, N/m^3\)
  3. \(6253.9 \, N/m^3\)
  4. \(7357.5 \, N/m^3\)

The correct answer is (D)    

Solution: Since the log is in equilibrium we can equate the weight of the log to the bouyant force. $$ \gamma_{log} \times V_{log} = \gamma_{water} \times V_{disp} $$ $$ \begin{aligned} \gamma_{log} &= \gamma_{water} \times { V_{disp} \over V_{log} } \\ &= 9810 \, N/m^3 \times \frac 34 \\ &= 7357.5 \, N/m^3 \end{aligned} $$ The correct answer is (D)  

9)   A cylindrical block of concrete is suspended by a cable and completely immersed in seawater (density \(1025 \, kg/m^3\)). The diameter is \(0.75 \, m\), height \(1 \, m\) and density of concrete is \(2300 \, kg/m^3\). Calculate the tension in the cable

  1. \(4245 \, N \)
  2. \(5526 \, N \)
  3. \(6631 \, N \)
  4. \(9670 \, N \)

The correct answer is (B)    

Solution: The tension in the cable can be found using \( T = W - F_B \) Where, $$\begin{aligned} W &= m \cdot g = \rho_C \cdot V \cdot g \text{, and} \\ F_B &= \rho_W \cdot V \cdot g \end{aligned}$$ (HINT: Use a FBD and sum forces in the vertical direction.) $$ \begin{aligned} T &= (\rho_C - \rho_W) \cdot V \cdot g \\ &= (2300-1025) \, kg/m^3 \cdot (pi/4*0.75^2*1.0) \, m^3 \cdot 9.81 \,m/s^2 \\ &= 5526 \, N \end{aligned}$$ The correct answer is (B)  

Fundamentals of Engineering