Correct Answer : Both Time and Direction
Explanation : Moving shock wave is an example of unsteady flow which means that all its flow properties such as density, velocity, temperature are a function of both the direction (x) and time (t). Although stationary shock wave are steady flow, thus the flow properties are only a function of direction (x).
Correct Answer : False
Explanation : Shock tube makes use of unsteady wave motion. It is a closed tube at both ends having a diaphragm which separates high pressure region known as the driver section and low pressure region known as the driven section.
Correct Answer : Constant
Explaination : For a stationary shock wave, the total enthalpy remains constant across the shock wave which means that h02 = h01. Although, in case of moving shock wave, this is not the case. The enthalpy does not remain constant across the shock.
Correct Answer : Appears stationary
Explanation : Usually shock waves propagate with subsonic or supersonic speed but when the shockwave propagates in a flow that moves as well, and it is in the opposite direction with the same velocity as the flow, then it appears to be stationary known as ‘standing shock wave’.
Correct Answer : Induces gas behind it
Explanation : When the normal shock wave is not opposed to the flow velocity, it propagates with some velocity W into the laboratory facility. This leads to the induction of gas behind it to move in the wave direction.
Correct Answer : 2.37
Explanation :
Correct Answer : Pressure ratio
Explanation : In a stationary wave, changes across the shock wave is governed by the Mach number. But, in a moving shock wave it is dependent majorly on the pressure ratio as seen in the formula below which shows the equation for density and pressure ratio across a moving shock wave.
Correct Answer : ρ1W = ρ2(W – up)
Explaination : Continuity equation across a shock wave is given by the formulaρ1u1 = ρ2u2Where, subscripts 1 and 2 are the sections behind and ahead of the shock wave. The above formula is valid only for stationary wave. For a moving wave, there is a induced gas formation behind the shock wave resulting in (W – up) being the velocity behind the shock wave which is relative to the wave, and W is the velocity of the gas ahead of the shock wave. Thus, the continuity equation becomes:ρ1W = ρ2(W – up)up is the velocity of induced mass motion due to the gasW is the velocity of the normal shock wave.
Correct Answer : 1.2331
Explaination :
Correct Answer : ρ2(WR + up) = ρ5WR
Explaination : Continuity equation across a shock wave is given by the formulaρ1u1 = ρ2u2Where, subscripts 1 and 2 are the sections behind and ahead of the shock wave. This above formula is valid only for stationary wave. For a reflected unsteady shock wave, the velocity ahead of the shock relative to wave is WR + up and the velocity behind the shock relative to the wave is WR. Thus, the continuity equation becomes:ρ2(WR + up) = ρ5WR
Correct Answer : Zero
Explanation : The intensity of this reflected shock (WR) is such that with velocity up, the originally induced mass motion is stopped dead at the wall. The mass motion behind the shock wave that is reflected must be zero. Therefore, the reflected shock wave maintains the zero – velocity boundary state.
Correct Answer : Plot of wave motion between t and x
Explanation : When unsteady wave motion i.e. moving shock wave is studied, wave diagram is often constructed. It is a sketch of the wave diagram plot on a graph with x – axis representing distance and y – axis representing the time. The diagram shows where the incident, reflected shock occurs after applying the boundary conditions.
Correct Answer : Waves with large perturbations
Explanation : The traveling waves have small perturbations in ambient conditions having small changes in pressure, density etc. Such waves are weak waves but finite waves have large perturbations at ambient conditions.
Correct Answer : True
Explanation : Finite waves which propagate in some direction x have properties such as temperature, pressure, density, velocity a function of distance x for time t at an instant. The flow is supposed to be isentropic.
Correct Answer : Linear equations are used to govern the flow variables
Explanation : Finite waves unlike the sound waves have high perturbation of density, velocity, temperature etc. They are known to propagate at speed which is an addition of local speed of mass velocity and speed of sound. The shape of the finite wave does not remain constant like the sound waves and the flow variables are governed by the nonlinear equations.
Correct Answer : Compression region
Explanation : The density of the finite wave varies along the distance of its propagation. The region where the density increases is known as the finite compression region, and the portion where the density decreases is known as the finite expansion region.
Correct Answer : u – a
Explaination : At a point (x,y) in an x – y plane there exists paths through this point known as C+ and C– characteristic lines. They represent the path of sound waves which are left and right running. The slope for a C– characteristic line is given by u – a and for C+ characteristic is u + a.