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Lesechka [4]
3 years ago
12

In the well-insulated trans-Alaska pipeline, the high viscosity of the oil and long distances cause significant pressure drops,

and it is reasonable to question whether flow work would be significant. Consider an 150 km length of pipe of diameter 1.2 m, with oil flow rate 500 kg/s. The oil properties are 900 kg/m3, 2000 J/kg·K, 0.765 N·s/m2. Calculate the pressure drop, the flow work, and the temperature rise caused by the flow work. Recall from chapter 1, for steady flow, one inlet, one outlet, no heat transfer, no work, and negligible kinetic and protential energy changes, the enthalpy of the fluid remains constant. Enthalpy is the sum of internal energy and flow work.
Engineering
1 answer:
s2008m [1.1K]3 years ago
5 0

Our values are defined by,

L=150*10^3m

\Phi = 1.2m

\dot{m}=700kg/s

\rho_o=900km/m^3

Sp=2000J/KgK

\mu_k = 0.765Ns/m^2

With this data we can easily calculate first the mean velocity of the flow,

The velocity is given by,

\nu=\frac{\dot{m}}{\rho_o A_c}

\nu = \frac{\dot{m}}{\rho_o \pi/4\Phi^2}

\nu = \frac{4*700}{900\pi(1.2)^4}

\nu=0.688m/s

With the mean velocity is now possible determine if the flow is Laminar or turbulent, for that we need Number Reynolds.

Remember that a Laminar Flow is given when Reynolds number is minor to 2300, then

Re_x = \frac{4\dot{m}}{\pi D\mu_k}

Re_x = \frac{4*700}{\pi*1.2*0.765}

Re_x = 970.8798

Re_x < 2300, then the flow is laminar.

For this section we will consider the Pressure drop to calculate the flow Work and the Total Energy conservation of this flow.

To calculate the Pressure drop we need the Friction factor, which is given by,

f= \frac{64}{Re}=\frac{64}{970.8789}

f= 0.06591

Then the Pressure drop is given by,

\Delta P = \frac{f\rho_o \nu^2 L}{2D}

\Delta P = \frac{0.06591*900*(0.688)^2*183*10^3}{2*1.2}

\Delta P = 2.141*10^6Pa

We can now calculate the Flow Work given by,

W_f = \frac{\Delta P\dot{m}}{\rho_o}

W_f = \frac{2.141*10^6*700}{900}

W_f = 1.6651*10^6J

From energy conservation we have

W_f=q

W_f = \dot{m}c_p\Delta T

Re-arrange for \Delta T

\Delta T = \frac{W_f}{\dot{m}c_p}

\Delta T = \frac{1.56*10^6}{700*2000}

\Delta T = 1.1894\°c

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Answer:

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Explanation:

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Now, in turbines in thermodynamics, the work done is produced by the flow required to turn the turbine and shaft. Recall that from the law of conservation of energy, the work in the turbine per mass airflow would be equal to the change in specific enthalpy of the flow from the entrance to the exit point of the turbine.

Thus, the property required to determine the work is Enthalpy.

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3 years ago
Knowing that v = –8 m/s when t = 0 and v = 8 m/s when t = 2 s, determine the constant k. (Round the final answer to the nearest
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Answer:

a)We know that acceleration a=dv/dt

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dv=kt^2dt

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v(t)=kt^3/3+C

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-8=C

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3 years ago
Briefly explain what are the following AIDC technologies for industry automation:
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If an elevator repairer observes that cables begin to fray after 15 years, what process might he or she use to create a maintena
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inductive reasoning

Explanation:

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3 years ago
The wheel and the attached reel have a combined weight of 50lb and a radius of gyration about their center of 6 A k in = . If pu
marishachu [46]

The complete question is;

The wheel and the attached reel have a combined weight of 50 lb and a radius of gyration about their center of ka = 6 in. If pulley B that is attached to the motor is subjected to a torque of M = 50 lb.ft, determine the velocity of the 200lb crate after the pulley has turned 5 revolutions. Neglect the mass of the pulley.

The image of this system is attached.

Answer:

Velocity = 11.8 ft/s

Explanation:

Since the wheel at A rotates about a fixed axis, then;

v_c = ω•r_c

r_c is 4.5 in. Let's convert it to ft.

So, r_c = 4.5/12 ft = 0.375 ft

Thus;

v_c = 0.375ω

Now the mass moment of inertia about of wheel A about it's mass centre is given as;

I_a = m•(k_a)²

The mass in in lb, so let's convert to slug. So, m = 50/32.2 slug = 1.5528 slug

Also, let's convert ka from inches to ft.

So, ka = 6/12 = 0.5

So,I_a = 1.5528 × 0.5²

I_a = 0.388 slug.ft²

The kinetic energy of the system would be;

T = Ta + Tc

Where; Ta = ½•I_a•ω²

And Tc = ½•m_c•(v_c)²

So, T = ½•I_a•ω² + ½•m_c•(v_c)²

Now, m_c is given as 200 lb.

Converting to slug, we have;

m_c = (200/32.2) slugs

Plugging in the relevant values, we have;

T = (½•0.388•ω²) + (½•(200/32.2)•(0.375ω)²)

This now gives;

T = 0.6307 ω²

The system is initially at rest at T1 = 0.

Resolving forces at A, we have; Ax, Ay and Wa. These 3 forces do no work.

Whereas at B, M does positive work and at C, W_c does negative work.

When pulley B rotates, it has an angle of; θ_b = 5 revs × 2π rad/revs = 10π

While the wheel rotates through an angle of;θ_a = (rb/ra) • θ_b

Where, rb = 3 in = 3/12 ft = 0.25 ft

ra = 7.5 in = 7.5/12 ft = 0.625 ft

So, θ_a = (0.25/0.625) × 10π

θ_a = 4π

Thus, we can say that the crate will have am upward displacement through a distance;

s_c = r_c × θ_a = 0.375 × 4π

s_c = 1.5π ft

So, the work done by M is;

U_m = M × θ_b

U_m = 50lb × 10π

U_m = 500π

Also,the work done by W_c is;

U_Wc = -W_c × s_c = -200lb × 1.5π

U_Wc = -300π

From principle of work and energy;

T1 + (U_m + U_Wc) = T

Since T1 is zero as stated earlier,

Thus ;

0 + 500π - 300π = 0.6307 ω²

0.6307ω² = 200π

ω² = 200π/0.6307

ω² = 996.224

ω = √996.224

ω = 31.56 rad/s

We earlier derived that;v_c = 0.375ω

Thus; v_c = 0.375 × 31.56

v_c = 11.8 ft/s

3 0
4 years ago
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