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It is claimed that an oblique shock can be analyzed like a normal shock provided that the normal component of velocity (normal to the shock surface) is used in the analysis. Do you agree with this claim?

Short Answer

Expert verified
Answer: Yes, an oblique shock can be analyzed like a normal shock, provided that the normal component of velocity is used in the analysis. This is because the normal velocity component determines the changes in fluid properties across both normal and oblique shocks.

Step by step solution

01

Understanding Normal and Oblique Shocks

Normal shocks and oblique shocks are both phenomena in fluid dynamics that involve a sudden change in the properties of a compressible fluid due to the formation of a shock wave. Normal shocks are characterized by the fact that the shock wave is perpendicular to the flow direction, while oblique shocks are characterized by a shock wave that is inclined with respect to the flow direction.
02

Identifying Similarities and Differences

Both normal and oblique shocks involve sudden changes in the fluid properties such as pressure, temperature, density, and velocity across the shock wave. However, the main difference between the two types of shock arises due to their respective shock wave orientations and the fluid flow direction. In an oblique shock, only the flow components normal to the shock wave will be affected by the shock wave, while the tangential components remain unchanged.
03

Analyzing the Role of the Normal Velocity Component

The normal component of velocity is critical when analyzing oblique shocks because it is the only component of the flow that is affected by the shock wave. The normal velocity component determines the flow properties across the oblique shock, just as it does in a normal shock. However, it is important to remember that the overall flow direction is not perpendicular to the oblique shock, unlike in a normal shock.
04

Evaluating the Claim

When analyzing an oblique shock, considering only the normal component of velocity is important because it determines how the fluid properties change across the shock wave. If one can determine the normal velocity component and analyze the oblique shock as if it were a normal shock, the correct changes in fluid properties can be obtained. Therefore, we can agree with the claim that an oblique shock can be analyzed like a normal shock, provided that the normal component of velocity is used in the analysis.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Normal Shocks
In the study of compressible fluid flow, normal shocks play a pivotal role. A normal shock is a type of shock wave that occurs when a supersonic flow encounters a sudden restriction that causes the flow to decelerate to subsonic speeds instantaneously. As a result, there are abrupt changes in various flow properties such as pressure, temperature, and density.

Imagine you're observing a high-speed airflow; once it hits this 'wall' of resistance, it's as though it has to slam on the brakes. The flow properties before and after this 'wall' can be related by the conservation of mass, momentum, and energy. These conservation equations are key in calculating the changes in the flow properties, and are expressed through relationships known as the Rankine-Hugoniot equations. You can think of normal shocks as the speed bumps in fluid dynamics that alter the vehicle (flow)'s speed and condition.
Fluid Dynamics
Fluid dynamics is the branch of physics concerned with the study of fluids (liquids and gases) in motion. It involves the analysis of the fluid flow behavior and the forces that lead to these flows. The field is crucial for understanding natural phenomena, designing various components in engineering, and solving problems involving fluid flow.

When considering fluid flow, especially in the context of shock waves, the properties of the fluid such as viscosity, compressibility, and density come into play. For instance, when dealing with shock waves, the focus often narrows down to compressible fluid dynamics, where the fluid density can change significantly alongside pressure and temperature.
Compressible Fluid
A compressible fluid is one in which the density can change significantly due to pressure and temperature variations. Unlike incompressible fluids where density is assumed to remain constant regardless of the forces applied, compressible fluids such as gases exhibit a strong coupling between their state variables, which include pressure, temperature, and density.

In scenarios like flying at high speeds or dealing with explosive gases, one cannot ignore the changes in a fluid’s density. The behavior of compressible fluids is governed by the equations of state, which relate these variables, and is essential in predicting and understanding phenomena like shock waves.
Shock Wave
A shock wave is a type of propagating disturbance in a fluid that results in a sudden and drastic change in its properties. Shock waves are typically formed when an object moves through a fluid faster than the speed of sound in that medium, or when an explosion occurs. In fluids, shock waves are characterized by an almost instantaneous rise in pressure, temperature, and density.

The study of shock waves is central to aerodynamics and astronautics, where understanding the impacts on vehicles traveling at supersonic speeds is critical. The physical representation of shock waves can be dramatic, such as the sonic boom heard when an airplane exceeds the speed of sound, which is actually the sound of the shock wave reaching an observer.
Velocity Components
In fluid dynamics, velocity components refer to the parts of the fluid's velocity vector that are parallel and perpendicular to a chosen reference direction. When analyzing fluid motion, it is sometimes convenient to decompose the velocity into components to simplify calculations or to understand the effects of fluid flow from different directions.

In the context of shock waves and particularly oblique shocks, separating the velocity into normal and tangential components against the shock allows for a targeted analysis of how the flow properties change. As we've seen with oblique shocks, the normal velocity component is the one that undergoes transformation, while the tangential component remains untouched by the shock. This distinction is crucial for accurate predictions and simulations when dealing with shock-induced flows.

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Most popular questions from this chapter

An aircraft is reported to be cruising in still air at \(-20^{\circ} \mathrm{C}\) and \(40 \mathrm{kPa}\) at a Mach number of \(0.86 .\) The velocity of the aircraft is \((a) 91 \mathrm{m} / \mathrm{s}\) \((b) 220 \mathrm{m} / \mathrm{s}\) \((c) 186 \mathrm{m} / \mathrm{s}\) \((d) 274 \mathrm{m} / \mathrm{s}\) \((e) 378 \mathrm{m} / \mathrm{s}\)

Air is approaching a converging-diverging nozzle with a low velocity at \(12^{\circ} \mathrm{C}\) and \(200 \mathrm{kPa}\), and it leaves the nozzle at a supersonic velocity. The velocity of air at the throat of the nozzle is \((a) 338 \mathrm{m} / \mathrm{s}\) \((b) 309 \mathrm{m} / \mathrm{s}\) \((c) 280 \mathrm{m} / \mathrm{s}\) \((d) 256 \mathrm{m} / \mathrm{s}\) \((e) 95 \mathrm{m} / \mathrm{s}\)

Consider a 16 -cm-diameter tubular combustion chamber. Air enters the tube at \(450 \mathrm{K}, 380 \mathrm{kPa}\), and \(55 \mathrm{m} / \mathrm{s}\) Fuel with a heating value of \(39,000 \mathrm{kJ} / \mathrm{kg}\) is burned by spraying it into the air. If the exit Mach number is \(0.8,\) determine the rate at which the fuel is burned and the exit temperature. Assume complete combustion and disregard the increase in the mass flow rate due to the fuel mass.

Consider a converging nozzle with a low velocity at the inlet and sonic velocity at the exit plane. Now the nozzle exit diameter is reduced by half while the nozzle inlet temperature and pressure are maintained the same. The nozzle exit velocity will \((a)\) remain the same \((b)\) double \((c)\) quadruple \((d)\) go down by half \((e)\) go down by one-fourth

Consider a converging nozzle with sonic speed at the exit plane. Now the nozzle exit area is reduced while the nozzle inlet conditions are maintained constant. What will happen to \((a)\) the exit velocity and \((b)\) the mass flow rate through the nozzle?

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