Aerospace Engineering GATE 2015 Questions with Answer

Ques 1 Aerodynamics


Consider the density and altitude at the base of an isothermal layer in the standard atmosphere to be ρ1 and h1, respectively. The density variation with altitude (ρ versus h) in that layer is governed by
(R: specific gas constant, T: temperature, go: acceleration due to gravity at sea level)

A

ρ/ρ1=e-[ρ0/RT](h-h1)

B

ρ/ρ1=e-[ρ0/RT](h1-h)

C

ρ/ρ1=e-[RT/ρo](h-h1)

D

ρ/ρ1=e-[RT/ρo](h1-h)


Ques 2 Aerodynamics


For constant free stream velocity and density, a change in lift for a large aspect ratio straight wing, with thin cambered airfoil section at small angles of attack, leads to

A

a shift of the aerodynamic center and no shift of the center of pressure

B

a shift of the center of pressure and no shift of the aerodynamic center

C

shift of both the aerodynamic center and the center of pressure

D

no shift either of the aerodynamic center or of the center of pressure


Ques 3 Aerodynamics


As a candidate for a vertical tail, which one of the following airfoil sections is appropriate?

A

NACA 0012

B

NACA 2312

C

NACA 23012

D

Clarke Y profile


Ques 4 Aerodynamics


The primary purpose of a trailing edge flap is to

A

avoid flow separation

B

increase Cl,max

C

reduce wave drag

D

reduce induced drag


Ques 5 Aerodynamics


Consider a monoplane wing and a biplane wing with identical airfoil sections, wingspans and incidence angles in identical conditions in a wind tunnel. As compared to the monoplane, the biplane experiences

A

a higher lift and a higher drag

B

a higher lift and a lower drag

C

a lower lift and a lower drag

D

a lower lift and a higher drag


Ques 6 Aerodynamics


Consider a wing of elliptic planform, with its aspect ratio AR→∞ Its lift-curve slope, dCI/dα=_______


Ques 7 Aerodynamics


The Reynolds number, Re is defined as UαL/ν where L is the length scale for a flow, Uα is its reference velocity and ν is the coefficient of kinematic viscosity. In the laminar boundary layer approximation, comparison of the dimensions of the convection term and the viscous term u ∂u/∂x ν∂2u/∂x2 leads to the following relation between the boundary layer thickness δ and Re:

A

δ∝√Re

B

δ=1/√Re

C

δ∝Re

D

δ∝1/Re


Ques 8 Aerodynamics


For a thin flat plate at 2 degrees angle of attack, the pitching moment coefficient about the trailing edge is


Ques 9 Aerodynamics


For a thin flat plate at 2 degrees angle of attack, the pitching moment coefficient about the trailing edge is


Ques 10 Aerodynamics


The velocity profile of an incompressible laminar boundary layer over a flat plate developing under constant pressure is given by u(y)/Uα=3y/(2δ)-1/2(y/δ)3. The freestream velocity U=10 m/s and the dynamic viscosity of the fluid μ=1.8×10-skg/(ms) At a streamwise station where the boundary layer thickness δ=5 mm, the wall shear stress is _______ ×10-3Pa


Ques 11 Aerodynamics


Consider a NACA 0012 aerofoil of chord c in a freestream with velocity V at a non-zero positive angle of attack α. The average time-of-flight for a particle to move from the leading edge to the trailing edge on the suction and pressure sides are t1 and t2, respectively. Thin aerofoil theory yields the velocity perturbation to the freestream as -Vx(1+cos θ)α/sin θ on the suction side and as Vx(1+cos θ)α/sin θ on the pressure side, where θ corresponds to the chordwise position, x=c/2(1-cos θ). Then t2-t1 is

A

-8παc/(Vx(4-π2α2))

B

0

C

4παc/(Vx(4-π2α2))

D

8παc/(Vx(4-π2α2))


Ques 12 Aerodynamics


Consider a 2-D blunt body in an incompressible fluid stream. The flow is irrotational and can be modeled as a linear combination of a uniform flow and a line source (Rankine half body) as shown below. Let s be the distance of the line source from the front stagnation point. Let d be the upstream distance from the stagnation point to the streamwise location (labeled below as P) where the oncoming stream reaches 90% of its undisturbed velocity. Then d/s=_______


Ques 13 Aerodynamics


For a normal shock, the relation between the upstream Mach number (M1) and the downstream Mach number (M2) is given by M22=((γ-1)M12+2)/(2γM12+1-γ) For an ideal gas with γ=1.4 the asymptotic value of the downstream Mach number is


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