The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved. Concept Introduction : The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition. The Navier-Stokes equation in vector form is, ρ D V → D t = ρ g → − ∇ P + μ ∇ 2 V →

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Answer 1

Question

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

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The power out of an adiabatic steam turbine is 5 MW and the steam enters turbine at 2 MPa and velocity of 50 m/s, specific enthalpy (h) of 3248 kJ/kg. The elevation of the inlet is 10 m higher than at the datum. The vapor mixture exits at 15 kPa and a velocity of 180 m/s, specific enthalpy (h) of 2361.01 kJ/kg. The elevation of the exit is 6 m higher than at the datum. Let g = 9.81 m/s². Assuming the ideal gas model and R = 0.462 KJ/(kg.K). The steam specific heat ratio is 1.283. Calculate:

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Answer 2

Question

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Expert Solution & Answer

Want to see the full answer?

Check out a sample textbook solution

See solution

Answer 3

Question

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Expert Solution & Answer

Want to see the full answer?

Check out a sample textbook solution

See solution

Answer 4

Question

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Expert Solution & Answer

Want to see the full answer?

Check out a sample textbook solution

See solution

Answer 5

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Answer 6

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

Answer 7

Chapter 9, Problem 9.13P

(a)

Interpretation Introduction

Interpretation:

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved.

Concept Introduction :

The fluid acceleration, pressure force, and viscous force all lie in the same plane are to be proved by using the Navier-Stokes equation in the vector form and the law of the vector addition.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

Answer 8

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

Answer 9

(b)

Interpretation Introduction

Interpretation:

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is to be proved.

Concept Introduction :

The fluid accelerates in the direction of the decreasing pressure in the absence of the viscous forces is proved by suing the Navier-Stokes equation in vector form.

The Navier-Stokes equation in vector form is,

ρDV→Dt = ρg→−∇P+μ∇2V→

Answer 10

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Answer 11

(c)

Interpretation Introduction

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Answer 12

Expert Solution & Answer

Answer 13

Expert Solution & Answer

Answer 14

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Answer 15

Ch. 9 - Prob. 9.1P Ch. 9 - Prob. 9.2P Ch. 9 - Prob. 9.3P Ch. 9 - Prob. 9.4P Ch. 9 - Prob. 9.5P Ch. 9 - Prob. 9.6P Ch. 9 - Prob. 9.7P Ch. 9 - Prob. 9.8P Ch. 9 - Prob. 9.9P Ch. 9 - Prob. 9.10P

Solution Summary: The author explains how the fluid acceleration, pressure force, and viscous force all lie in the same plane. The Navier-Stokes equation in vector form is written as follows:

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Want to see the full answer?

Chapter 9 Solutions

Solution Summary: The author explains how the fluid acceleration, pressure force, and viscous force all lie in the same plane. The Navier-Stokes equation in vector form is written as follows:

Interpretation: A static fluid will always start to move in the direction of the decreasing pressure is to be proved. Concept Introduction : The Bernoulli’sprinciple is used to prove the flow condition of a static fluid. The Bernoulli’sequation is, P1ρ+V122+gZ1 = P2ρ+V222+gZ2

Want to see the full answer?

Chapter 9 Solutions

Interpretation:

A static fluid will always start to move in the direction of the decreasing pressure is to be proved.

Concept Introduction :

The Bernoulli’sprinciple is used to prove the flow condition of a static fluid.

The Bernoulli’sequation is,

P1ρ+V122+gZ1 = P2ρ+V222+gZ2