
(a)
To compute: the pressure just downstream of this shock.

Answer to Problem 9.55P
Explanation of Solution
Given information:
Stagnation pressure is equal to
Throat area is
Shock is at
The pressure ratio is defined as,
Where,
Calculation:
Calculate the area ratio,
According to the table B.1 which represents the isentropic flow of perfect gas
By interpolation,
Calculate the pressure at point 1,
According to the table B.2 which represents the normal shock relations for a perfect gas,
By interpolation,
Therefore, the pressure
Conclusion:
The pressure just downstream of shock is equal to
(b)
To estimate:

Answer to Problem 9.55P
Explanation of Solution
Given information:
Stagnation pressure is equal to
Throat area is
Shock is at
The pressure ratio is defined as,
Where,
Calculation:
According to sub-part a,
We have found,
According to the table B.2 which represents the normal shock relations for a perfect gas,
By interpolation,
Therefore,
At
Therefore, calculate the relevant Mach number
According to table B.1
According to the table B.2 which represents the normal shock relations for a perfect gas,
By interpolation,
Therefore,
Calculate the pressure at point 3,
Conclusion:
The pressure at point 3 is equal to
(c)
To estimate: throat area.

Answer to Problem 9.55P
Explanation of Solution
Given information:
Stagnation pressure is equal to
Throat area is
Shock is at
According to sub-part a,
We have found,
Therefore, by using table B.2, we can find the relevant area ratio.
Calculation:
According to the table B.2 which represents the normal shock relations for a perfect gas,
By interpolation,
Therefore,
Conclusion:
The throat area is equal to
(d)
To estimate:

Answer to Problem 9.55P
Explanation of Solution
Given information:
Stagnation pressure is equal to
Throat area is
Shock is at
According to sub-part a,
We have found,
Therefore, by using table B.2 and B.1 we can able to estimate the Mach number at point 3
Calculation:
According to the table B.2 which represents the normal shock relations for a perfect gas,
By interpolation,
Therefore,
At
Therefore, calculate the relevant Mach number
According to table B.1
Conclusion:
The Mach number at point 3 is equal to
Want to see more full solutions like this?
Chapter 9 Solutions
Fluid Mechanics
- Problem 1 (65 pts, suggested time 50 mins). An elastic string of constant line tension1T is pinned at x = 0 and x = L. A constant distributed vertical force per unit length p(with units N/m) is applied to the string. Under this force, the string deflects by an amountv(x) from its undeformed (horizontal) state, as shown in the figure below.The PDE describing mechanical equilibrium for the string isddx Tdvdx− p = 0 . (1)(a) [5pts] Identify the BCs for the string and identify their type (essential/natural). Writedown the strong-form BVP for the string, including PDE and BCs.(b) [10pts] Find the analytical solution of the BVP in (a). Compute the exact deflectionof the midpoint v(L/2).(c) [15pts] Derive the weak-form BVP.(d) [5pts] What is the minimum number of linear elements necessary to compute the deflection of the midpoint?(e) [15pts] Write down the element stiffness matrix and the element force vector for eachelement.arrow_forwardProblem 1 (35 pts). An elastic string of constant line tension1 T is pinned at x = 0 andx = L. A constant distributed vertical force per unit length p (with units N/m) is appliedto the string. Under this force, the string deflects by an amount v(x) from its undeformed(horizontal) state, as shown in the figure below.Force equilibrium in the string requires thatdfdx − p = 0 , (1)where f(x) is the internal vertical force in the string, which is given byf = Tdvdx . (2)(a) [10pts] Write down the BVP (strong form) that the string deflection v(x) must satisfy.(b) [2pts] What order is the governing PDE in the BVP of (a)?(c) [3pts] Identify the type (essential/natural) of each boundary condition in (a).(d) [20pts] Find the analytical solution of the BVP in (a).arrow_forwardProblem 2 (25 pts, (suggested time 15 mins). An elastic string of line tension T andmass per unit length µ is pinned at x = 0 and x = L. The string is free to vibrate, and itsfirst vibration mode is shown below.In order to find the frequency of the first mode (or fundamental frequency), the string isdiscretized into a certain number of linear elements. The stiffness and mass matrices of thei-th element are, respectivelyESMi =TLi1 −1−1 1 EMMi =Liµ62 11 2 . (2)(a) [5pts] What is the minimum number of linear elements necessary to compute the fundamental frequency of the vibrating string?(b) [20pts] Assemble the global eigenvalue problem and find the fundamental frequency ofvibration of the stringarrow_forward
- I need part all parts please in detail (including f)arrow_forwardProblem 3 (10 pts, suggested time 5 mins). In class we considered the mutiphysics problem of thermal stresses in a rod. When using linear shape functions, we found that the stress in the rod is affected by unphysical oscillations like in the following plot E*(ux-a*T) 35000 30000 25000 20000 15000 10000 5000 -5000 -10000 0 Line Graph: E*(ux-a*T) MULT 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Arc length (a) [10pts] What is the origin of this issue and how can we fix it?arrow_forwardanswer the questions and explain all of it in words. Ignore where it says screencast and in class explanationarrow_forward
- Elements Of ElectromagneticsMechanical EngineeringISBN:9780190698614Author:Sadiku, Matthew N. O.Publisher:Oxford University PressMechanics of Materials (10th Edition)Mechanical EngineeringISBN:9780134319650Author:Russell C. HibbelerPublisher:PEARSONThermodynamics: An Engineering ApproachMechanical EngineeringISBN:9781259822674Author:Yunus A. Cengel Dr., Michael A. BolesPublisher:McGraw-Hill Education
- Control Systems EngineeringMechanical EngineeringISBN:9781118170519Author:Norman S. NisePublisher:WILEYMechanics of Materials (MindTap Course List)Mechanical EngineeringISBN:9781337093347Author:Barry J. Goodno, James M. GerePublisher:Cengage LearningEngineering Mechanics: StaticsMechanical EngineeringISBN:9781118807330Author:James L. Meriam, L. G. Kraige, J. N. BoltonPublisher:WILEY





