Question 7 of 13: Thrust and Flow Areas of a Turbojet Engine
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
04-BS-7 Mechanics of Fluids — National Examination, 2013-Dec. Three (3) hours duration, closed book. Section A (Calculative, 9 questions, do 7) and Section B (Analytical, 4 questions, do 3); every question is answered below regardless of the exam's "do N of M" instruction, so the set is a complete study resource.
Air density is taken from the paper's own Constants table at the temperature each question states: 1.19 kg/m³ at 20°C (Q5's wind, Q7's inlet air).
Q1's touching-rod array is modelled as a repeating square unit cell of four mutually tangent rods (pitch = rod diameter, per the question's own "closely packed" wording), giving a curvilinear-square pore whose perimeter/area ratio drives the capillary rise.
Q8's Moody diagram and Q9's drag-coefficient diagram are supplied as attachments. Both are solved via the equations the charts themselves plot: the Colebrook–White equation for Q8 and the Morrison (2013) curve-fit for sphere drag vs. Reynolds number for Q9.
Question 7: Thrust and Flow Areas of a Turbojet Engine (5 marks)
Turbojet control volume: inlet air enters at the aircraft velocity, exhaust gas leaves at the stated exit velocity; fuel mass flow neglected.
Find. Engine thrust; the inlet flow area giving inlet velocity = aircraft velocity; the exhaust nozzle area giving the stated exit velocity.
Approach. Treat inlet air and exhaust gas as ideal gases at the stated pressure and temperature to get their densities, use the exhaust conditions to get the (fuel-neglected) mass flow rate, apply the momentum (thrust) equation, then use the same mass flow with the inlet density to size the inlet area.
Exhaust gas density and mass flow. $\rho_{ex}=p/(RT_{ex})=100{,}000/(287\times973.15)=0.3580\ \text{kg/m}^3$, so
$$\dot m = \rho_{ex}A_{ex}V_{ex} = 0.3580\times0.3\times900 = \boxed{96.7\ \text{kg/s}}$$
Thrust. Converting aircraft speed, $V_{ac}=900/3.6=250.0\ \text{m/s}$, and applying the momentum-thrust relation (equal inlet/exhaust pressure, fuel mass flow neglected):
$$F_{thrust} = \dot m(V_{ex}-V_{ac}) = 96.7\times(900-250) = \boxed{62{,}840\ \text{N} = 62.8\ \text{kN}}$$
Inlet air density and inlet area. $\rho_{in}=p/(RT_{in})=100{,}000/(287\times293.15)=1.189\ \text{kg/m}^3$; by mass continuity, the SAME mass flow must pass through the inlet at the aircraft's own velocity, so
$$A_{in} = \frac{\dot m}{\rho_{in}V_{ac}} = \frac{96.7}{1.189\times250.0} = \boxed{0.325\ \text{m}^2}$$
Exhaust nozzle area check. The exhaust area needed to deliver the stated 900 m/s exit velocity at this same mass flow is, by definition, the value already used in Step 1 — $A_{ex}=0.3\ \text{m}^2$ — confirming the given exhaust area is self-consistent with the required exit velocity.