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Question: The speed of airflow on the upper and lower surfaces of a wing of an aeroplane are \({v_1}\) and \({...

The speed of airflow on the upper and lower surfaces of a wing of an aeroplane are v1{v_1} and v2{v_2} respectively. If A is the cross section area of the wing and ρ\rho is the density of air, then the upward lift is :
A) 12ρA(v1v2)\dfrac{1}{2}\rho A\left( {{v_1} - {v_2}} \right)
B) 12ρA(v1+v2)\dfrac{1}{2}\rho A\left( {{v_1} + {v_2}} \right)
C) 12ρA(v12v22)\dfrac{1}{2}\rho A\left( {v_1^2 - v_2^2} \right)
D) 12ρA(v12+v22)\dfrac{1}{2}\rho A\left( {v_1^2 + v_2^2} \right)

Explanation

Solution

According to Bernoulli's principle for any streamline motion total energy associated to the system i.e. the sum of fluid pressure, gravitational potential energy and kinetic energy always remain constant. For the motion of aeroplane, this principle simply explains the reason behind the extra pressure exerted by air on its wing due to the velocity difference at both sides.

Formula Used:
Bernoulli's principle applied at two points of streamline fluid motion:
ρv122+ρgh1+P1=ρv222+ρgh2+P2\dfrac{{\rho v_1^2}}{2} + \rho g{h_1} + {P_1} = \dfrac{{\rho v_2^2}}{2} + \rho g{h_2} + {P_2} (1)
Where,
ρ\rho is the density of the fluid,
v1{v_1} and v2{v_2} are the velocity of the fluid at first and second point respectively,
h1{h_1} and h2{h_2} are elevation of the first and second point respectively,
g is acceleration due to gravity,
P1{P_1} and P2{P_2} are pressure exerted by the fluid at the first and second point respectively.

Force and pressure relationship:
F=P.AF = P.A (2)
Where,
F is total force experienced,
P is pressure exerted,
A is the total surface area.

Complete step by step answer:
Given:
1. Speed of airflow on the upper surface of the wing is v1{v_1}.
2. Speed of airflow on the lower surface of the wing is v2{v_2}.
3. Density of air is ρ\rho .
4. Cross-section area of the wing is A.
5. Aeroplane wing is very thin compared to the plane’s elevation. So, effectively h1=h2=h{h_1} = {h_2} = h.

To find: Upward lift on the plane’s wing.

Step 1
Substitute all the variables of eq.(1) with the given value to find the pressure difference ΔP=P2P1\Delta P = {P_2} - {P_1} as:
ρv122+ρgh+P1=ρv222+ρgh+P2 ΔP=P2P1=12ρ(v12v22)  \dfrac{{\rho v_1^2}}{2} + \rho gh + {P_1} = \dfrac{{\rho v_2^2}}{2} + \rho gh + {P_2} \\\ \therefore \Delta P = {P_2} - {P_1} = \dfrac{1}{2}\rho \left( {v_1^2 - v_2^2} \right) \\\ (3)

Step 2
Now, use the value of pressure difference from eq.(3) in eq.(2) to get the upward lift force value as:
F=ΔP.A F=12ρA(v12v22)  F = \Delta P.A \\\ \therefore F = \dfrac{1}{2}\rho A\left( {v_1^2 - v_2^2} \right) \\\

Correct answer:
The upward lift is (c) 12ρA(v12v22)\dfrac{1}{2}\rho A\left( {v_1^2 - v_2^2} \right).

Note: This problem can be solved without doing any calculation just by using logic. For the total energy to remain constant the difference of pressure between two surfaces must arise from their kinetic energy difference since the gravitational potential is effectively the same for both surfaces. Now, the kinetic energy is proportional to square of velocity. Hence, the only possible option is option (c).