Force convection is a type of convection that happens when a fluid is forced to move over a surface or in a tube. On the other hand.
Natural convection is a type of convection that occurs when a fluid is heated, causing it to expand and rise, producing a convection current that circulates the fluid. Both natural and forced convection are used for heat transfer, but there are some differences between them.In natural convection.
The convective heat transfer coefficient is lower than that in forced convection. The reason is that in natural convection, the motion of the fluid is caused by buoyancy forces, which are weaker than the forces generated by forced convection.
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A machine of mass 100 kg sits on a floor that moves vertically with amplitude of 5 cm at frequency of 400 rpm. Undamped isolator / vibration absorber are designed for this machine to fit different transmissibility requirement. To achieve 80% vibration isolation, the machine is to be mounted on an undamped isolator. Please answer (a)-(d). (a) Calculate the frequency ratio and fill the value in the following blank. (b) Determine the natural frequency (rad/s) of this system. (c) Design the undamped vibration isolator (find its spring stiffness in N/m). (d) Find out the transmitted displacement (m) of the machine with undamped isolator. To achieve 85% vibration isolation, the machine is to be mounted on a damped shock absorber with a damping ratio of 0.2. Please answer (e)-(h). (e) Calculate the frequency ratio and fill the value in the following blank. (f) Determine the natural frequency (rad/s) of this system. (g) Determine the stiffness (N/m) of the vibration absorber. (h) Determine the damping constant (N.s/m) of the vibration absorber.
Given, mass of machine, m = 100 kgAmplitude, A = 5 cm = 0.05 m Frequency, f = 400 rpm= 400/60 Hz = 20/3 HzPercentage of vibration isolation, η = 80% = 0.8
(a) Frequency ratio,ωn= 2πfnωn = (2π × 20/3) = 41.89 rad/s(b) Natural frequency,ωd=ωn(1−η2)ωd=ωn(1−η2)ωd= 41.89 (1-0.82)ωd= 21.07 rad/s(c) Spring stiffness, k = mωd2k = mωd2= 100 × (21.07)2k = 4.45 × 10^4 N/m(d) Transmitted displacement, x = Aηx = Aη= 0.05 × 0.8x = 0.04 mPercentage of vibration isolation, η = 85% = 0.85(e) Frequency ratio,ωn= 2πfnωn= (2π × 20/3) = 41.89 rad/s(f) Natural frequency,ωd=ωn(1−η2)ωd=ωn(1−η2)ωd= 41.89 (1-0.852)ωd= 33.60 rad/s(g) Stiffness of vibration absorber,k= mωd2 (1−η2)k= mωd2 (1−η2)= 100 × (33.60)2 / [1 - (0.85)2]k = 3.32 × 105 N/m(h) Damping constant, c = 2ηωdmc= 2ηωdm= 2 × 0.2 × 33.60 × 100c = 1344 N.s/mTherefore, the main answer for the given question is as follows
:(a) Frequency ratio, ωn = 41.89 rad/s(b) Natural frequency, ωd = 21.07 rad/s(c) Spring stiffness, k = 4.45 × 104 N/m(d) Transmitted displacement, x = 0.04 m(e) Frequency ratio, ωn = 41.89 rad/s(f) Natural frequency, ωd = 33.60 rad/s(g) Stiffness of vibration absorber, k = 3.32 × 105 N/m(h) Damping constant, c = 1344 N.s/m
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What advantages does worm drive have? What are the requirements for materials of worm gear in worm system? (6 scores) (8) Why should the calculation of heat balance be executed? What if the design does not achieve thermal balance? (5 scores)
The efficiency of a worm drive is higher than that of a spur gear. It also has less power loss due to friction. Because the contact between the worm and the gear teeth is always at right angles, the wear rate is low, resulting in a longer life.
In comparison to other gearboxes, the worm gearboxes are compact and can transmit higher torque with the same size, and it is possible to achieve a higher speed reduction ratio with a worm gear. The worm gear is self-locking, which means it can maintain the drive position and hold the weight on its own without the need for a brake. The material for the worm wheel is typically made of bronze or plastic, while the worm material is often constructed of steel. In worm gear systems, bronze is a common material for worm wheels because it is tough and abrasion-resistant.
Steel is also used for worm wheels in some cases because it is less expensive and more durable than bronze. In worm gear systems, steel is typically used to make the worm shaft, and it is preferred because it can be heat-treated to achieve hardness, and it is also wear-resistant.
When a device's operating temperature is too low, the heat balance calculation helps to determine the necessary amount of heat to be added to the system. If a design does not achieve thermal balance, the operating temperature of the device may not be within the safe range, and this may result in damage to the device or sub-optimal performance.
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a) Creep,
(i) What is the creep and explain stages of creep through sketch? Which stage of creep is more important for design purpose and why? [4 Marks] (ii) Why does temperature affect creep? [3 Marks]
(iii) Explain, how do we prevent jet engine turbine blades from creep (in combustion zone? [3 Marks] b) Corrosion, (i) What causes stress corrosion cracking? and how can SCC be avoided? [3 Marks]
(ii) Why is it important to study about corrosion for the structure integrity? and What are the benefits of corrosion control? [3 Marks] (iii) List two environmental parameters are known to influence the rate of crack growth and explain one parameter in detail. [4 Marks]
c) Discuss, two non-destructive testing methods and mention the application of each technique. [5 Marks]
Creep curve is a graphical representation of creep behavior that plots the strain as a function of time. The three stages of creep are: Primary creep: This is the first stage of creep. It begins with a high strain rate, which slows down over time. This stage is characterized by a rapidly decreasing rate of strain that stabilizes after a short period of time.
Secondary creep: This is the second stage of creep. It is characterized by a constant rate of strain. The rate of strain in this stage is slow and steady. The slope of the strain vs. time curve is nearly constant. Tertiary creep: This is the third stage of creep. It is characterized by an accelerating rate of strain, which eventually leads to failure. The rate of strain in this stage is exponential. The tertiary stage of creep is the most important for design purposes because this stage is when the material is most likely to fail.(ii) Why does temperature affect creep? Temperature affects creep because it influences the strength and elasticity of a material. As the temperature of a material increases, its strength decreases, while its ductility and elasticity increase.
The cracking occurs when the material's stress exceeds its yield strength and is assisted by the corrosive environment. SCC can be avoided by reducing the applied stress, improving the quality of the material, and avoiding exposure to corrosive media.(ii) Why is it important to study corrosion for the structure integrity? What are the benefits of corrosion control? The study of corrosion is important for structural integrity because corrosion can compromise the strength and durability of materials. Corrosion control has many benefits, including increased safety, longer service life, reduced maintenance costs, and improved performance. Corrosion control also helps to prevent accidents, downtime, and production losses.(iii) List two environmental parameters known to influence the rate of crack growth and explain one parameter in detail.
Corrosion occurs when a metal is exposed to an environment that contains moisture. The moisture reacts with the metal, causing it to corrode. The corrosion can weaken the metal and make it more susceptible to cracking. c) Discuss two non-destructive testing methods and mention the application of each technique. Two non-destructive testing methods are ultrasonic testing and magnetic particle testing.
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Steel rod made of SAE 4140 oil quenched is to be subjected to reversal axial load 180000N. Determine the required diameter of the rod using FOS= 2. Use Soderberg criteria. B=0.85, C=0.8 .
SAE 4140 oil quenched steel rod is to be subjected to reversal axial load of 180000N. We are supposed to find the required diameter of the rod using the Factor of Safety(FOS)= 2. We need to use the Soderberg criteria with B=0.85 and C=0.8.
The Soderberg equation for reversed bending stress in terms of diameter is given by:
[tex]$$\frac{[(Sa)^2+(Sm)^2]}{d^2} = \frac{1}{K^2}$$[/tex]
Where Sa = alternating stressSm = mean stressd = diameterK = Soderberg constantK = [tex](FOS)/(B(1+C)) = 2/(0.85(1+0.8))K = 1.33[/tex]
From the Soderberg equation, we get:
[tex]$$\frac{[(Sa)^2+(Sm)^2]}{d^2} = \frac{1}{1.33^2}$$$$\frac{[(Sa)^2+(Sm)^2]}{d^2} = 0.5648$$For the given loading, Sa = 180000/2 = 90000 N/mm²Sm = 0Hence,$$\frac{[(90000)^2+(0)^2]}{d^2} = 0.5648$$$$d^2 = \frac{(90000)^2}{0.5648}$$$$d = \sqrt{\frac{(90000)^2}{0.5648}}$$$$d = 188.1 mm$$[/tex]
The required diameter of the steel rod using FOS = 2 and Soderberg criteria with B=0.85 and C=0.8 is 188.1 mm.
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(DT) Consider a large parallel plate capacitor with a hemispherical bulge on the grounded plate. The bulge has radius a and bulges toward the second plate. The distance between the plates is b.b> a. The second plate is at potential V.. 1. Find the potential everywhere inside the capacitor. 2. Determine the surface charge density on the flat portion of the grounded plate. 3. Determine the surface charge density on the bulge.
In a large parallel plate capacitor with a hemispherical bulge on the grounded plate, the potential everywhere inside the capacitor can be obtained by solving the Laplace's equation.
The Laplace's equation is a second-order partial differential equation that describes the behavior of the electric potential.
It is given by the equation ∇2V = 0, where V is the electric potential and ∇2 is the Laplacian operator.
The Laplace's equation can be solved using the method of separation of variables.
We can assume that the electric potential is of the form
V(x,y,z) = X(x)Y(y)Z(z),
where x, y, and z are the coordinates of the capacitor.
Substituting this expression into the Laplace's equation, we get:
X''/X + Y''/Y + Z''/Z = 0.
Since the left-hand side of this equation depends only on x, y, and z separately, we can write it as
X''/X + Y''/Y = -Z''/Z = λ2,
where λ is a constant. Solving these equations for X(x), Y(y), and Z(z), we get:
X(x) = A cosh(μx) + B sinh(μx)
Y(y) = C cos(nπy/b) + D sin(nπy/b)
Z(z) = E cosh(λz) + F sinh(λz),
where μ = a/√(b2-a2), n = 1, 2, 3, ..., and E and F are constants that depend on the boundary conditions.
The potential everywhere inside the capacitor is therefore given by:
V(x,y,z) = ∑ Anm cosh(μmx) sin(nπy/b) sinh(λmz),
where Anm are constants that depend on the boundary conditions.
To find the surface charge density on the flat portion of the grounded plate, we can use the boundary condition that the electric field is normal to the surface of the plate.
Since the electric field is given by
E = -∇V,
where V is the electric potential, the normal component of the electric field is given by
E·n = -∂V/∂n,
where n is the unit normal vector to the surface of the plate.
The surface charge density is then given by
σ = -ε0 E·n,
where ε0 is the permittivity of free space.
To find the surface charge density on the bulge, we can use the same method and the boundary condition that the electric field is normal to the surface of the bulge.
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A streamlined train is 200 m long with a typical cross-section having a perimeter of 9 m above the wheels. If the kinematic viscosity of air at the prevailing temperature is 1.5×10-5 m²/s and density 1.24 kg/m³, determine the approximate surface drag (friction drag) of the train when running at 90 km/h. Make allowance for the fact that boundary layer changes from laminar to turbulent on the train
The approximate surface drag (friction drag) of the train when running at 90 km/h is approximately 6952.5 Newtons.
To calculate the approximate surface drag (friction drag) of the train, we can use the drag coefficient and the equation for drag force. The drag force can be expressed as:
Drag Force = 0.5 * Cd * A * ρ * V^2
Where:
Cd is the drag coefficient (depends on the flow regime - laminar or turbulent)
A is the reference area (cross-sectional area in this case)
ρ is the density of air
V is the velocity of the train
First, let's determine the reference area. The cross-sectional area is given as the perimeter of the train above the wheels, which is 9 m. Since the train is streamlined, we can assume the reference area is equal to the cross-sectional area:
A = 9 m^2
Next, we need to determine the drag coefficient (Cd). The boundary layer transition from laminar to turbulent can affect the drag coefficient. In this case, we can assume a value of Cd = 0.1 for the laminar flow regime and Cd = 0.2 for the turbulent flow regime.
Now we can calculate the drag force:
Drag Force = 0.5 * Cd * A * ρ * V^2
Let's convert the velocity from km/h to m/s:
V = 90 km/h = (90 * 1000) / 3600 m/s = 25 m/s
For the laminar flow regime:
Drag Force (laminar) = 0.5 * 0.1 * 9 * 1.24 * 25^2 = 2317.5 N
For the turbulent flow regime:
Drag Force (turbulent) = 0.5 * 0.2 * 9 * 1.24 * 25^2 = 4635 N
The approximate surface drag of the train is the sum of the drag forces for the laminar and turbulent flow regimes:
Surface Drag = Drag Force (laminar) + Drag Force (turbulent)
= 2317.5 N + 4635 N
= 6952.5 N
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Q10. Select and sketch an appropriate symbol listed in Figure Q10 for ench geometric chracteristic listed below. OV Example: Perpendicularity a) Straightness b) Flatness c) Roundness d) Parallelism e) Symmetry f) Concentricity 수 오우 ㅎㅎ V Figure Q10 10 (6 Marks)
Figure Q10 lists various symbols used in the geometric tolerance in engineering. The symbols used in engineering indicate the geometrical shape of the object. It is a symbolic representation of an object's shape that is uniform.
Geometric tolerances are essential for ensuring that manufactured components are precise and will work together smoothly. Perpendicularity is shown by a square in Figure Q10. Straightness is represented by a line in Figure Q10.Flatness is indicated by two parallel lines in Figure Q10. Roundness is shown by a circle in Figure Q10. Parallelism is represented by two parallel lines with arrows pointing out in opposite directions in Figure Q10.Symmetry is indicated by a horizontal line that runs through the centre of the shape in Figure Q10. Concentricity is shown by two circles in Figure Q10, with one inside the other. In conclusion, geometric tolerances are essential in engineering and manufacturing. They guarantee that the manufactured components are precise and will function correctly.
The symbols used in engineering represent the geometrical shape of the object and are used to describe it. These symbols make it easier for manufacturers and engineers to understand and communicate the requirements of an object's shape.
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(a) A non-liner load is connected to a 110 V, 60 Hz power supply. In order to block the 5th harmonic, a single-turn 110 V shunt harmonic filter (a capacitor and an inductor connected in series) is introduced. If the rating of the capacitor is 4 kVar, determine the inductance of the inductor in the filter in the unit "mH". (b) A non-liner load is connected to a 110 V, 60 Hz power supply. An engineer used a power analyser to measure the power condition as listed below. Determine the Total Harmonics Distortion (THD). • the current at the frequency of 60 Hz = 35 A • the current at the frequency of 180 Hz = 6 A • the current at the frequency of 420 Hz=2A
(c) Determine the power of all the harmonics supplied to the circuit if the voltage and the current of a circuit are: • v=13 sin(ot - 27º) + sin(30t +30°) + 2 sin(50t - 809) V • i= 18sin(ot - 47°) + 4sin(30t -20) + 1sin(50t - 409) A
(a) The inductance of the inductor in the filter is 883.57 μH.
(b) The Total Harmonic Distortion (THD) is 17.66%.
(c) The power of all the harmonics supplied to the circuit is 119 Watts.
(a) To determine the inductance of the inductor in the shunt harmonic filter, we can use the formula:
Xc=1/2πfc
where: Xc is the reactance of the capacitor, f is the frequency (60 Hz in this case), and C is the capacitance (4 kVar = 4000 VAr).
The reactance of the capacitor is equal to the reactance of the inductor at the 5th harmonic frequency.
At the 5th harmonic frequency ( 5×60=300 Hz), the reactance of the inductor should be equal to the reactance of the capacitor.
Therefore, we can write: XL =Xc = 1/2πfC
Solving for L (inductance):
L=1/2πfXc
Plugging in the values:
L=883.57μH (microhenries)
(b) To determine the Total Harmonic Distortion (THD), we can use the following formula:
[tex]THD=\frac{\sqrt{\sum _{n=2}^{\infty }\:I_n^2}}{I_1}\times 100[/tex]
where: THD is the Total Harmonic Distortion, In is the rms value of the current at the nth harmonic frequency,I₁ is the rms value of the fundamental frequency current.
In this case, we have: I₁ = 35A (at 60Hz), I₂ =6A (at 180 Hz)
I₃ =2 A (at 420 Hz)
Substituting the values into the THD formula:
THD=√6²+2²/I₁ × 100
THD=17.66%
(c) To determine the power of all the harmonics supplied to the circuit, we can use the formula:
[tex]P_n=\frac{V_nI_n}{2}[/tex]
Pₙ is the power of the nth harmonic, Vₙ is the rms value of the voltage at the nth harmonic frequency, Iₙ is the rms value of the current at the nth harmonic frequency.
For the 1st harmonic (fundamental frequency):
V₁ =1V , I₁ =18 A , P₁ = V₁⋅I₁ /2
For the 2nd harmonic:
V₂ =1 V , I₂ =4 A , P₁ = V₂I₂ /2
For the 3nd harmonic:
V₃ =0 V , I₃ =1A , P₁ = V₃I₃ /2 =0
Adding up all the harmonic powers:
P total = P₁+P₂+P₃
=13×18/2 + 1×4/2 + 0
=117+2
=119 watts.
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A power station supplies 60 kW to a load over 2,500 ft of 000 2-conductor copper feeder the resistance of which is 0.078 ohm per 1,000 ft. The bud-bar voltage is maintained constant at 600 volts. Determine the maximum power which can be transmitted.
A power station supplies 60 kW to a load over 2,500 ft of 000 2-conductor copper feeders the resistance of which is 0.078 ohm per 1,000 ft. The bud-bar voltage is maintained constant at 600 volts. 5.85 MW, the maximum power which can be transmitted.
[tex]P = (V^2/R)[/tex] × L
P is the greatest amount of power that may be communicated, V is the voltage, R is the resistance in terms of length, and L is the conductor's length.
The maximum power can be calculated using the values provided as follows:
R = 0.078 ohm/1,000 ft × 2,500 ft = 0.195 ohm
L = 2,500 ft
V = 600 volts
[tex]P = (V^2/R)[/tex] × L = [tex]L = (600^2[/tex]/0.195) × 2,500
= 5,853,658.54 watts
= 5.85 MW.
Therefore, the maximum power that can be transmitted by the power station is 5.85 MW.
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After building a SAP computer in Vivado, how can you manually execute instructions to the computer?
For example:
LDA $ 40H
MVA B
LDA $ 41H
ANA B (A and B)
HLT
After building a SAP computer in Vivado, the manually executing instructions to the computer can be done with the three steps mentioned as:
Step 1: Open Xilinx SDKOnce the block diagram is created and synthesized in Vivado, the SDK needs to be opened to generate the software code and to program the board.
Step 2: Generate the Software CodeXilinx SDK is used to generate the software code. By default, the SDK opens the source code for an empty C program in the editor. It is recommended that a basic program for the SAP-1 is written first. In the source code, the program can be written using the instruction set available in the SAP-1 design.
Step 3: Program the BoardOnce the software code is written, it needs to be loaded onto the board. Select "Program FPGA" from the "Xilinx" menu. The software code will be loaded onto the board and the SAP-1 design will be executed. The results will be displayed on the board's output devices.
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Five miners must be lifted from a mineshaft (vertical hole) 100m deep using an elevator. The work required to do this is found to be 341.2kJ. If the gravitational acceleration is 9.75m/s^2, determine the average mass per person in kg.
a. 65kg
b. 70kg
c. 75kg
d. 80kg
(b).Given information: Depth of mine shaft = 100 m Work done = 341.2 kJ Gravitational acceleration = 9.75 m/s²Number of persons to be lifted = 5Formula used: Work done = force × distanceIn this question, we are supposed to determine the average mass per person in kg.
The formula to calculate the average mass per person is:Average mass per person = Total mass / Number of personsLet's begin with the solution:From the given information,The work done to lift 5 persons from the mine shaft is 341.2 kJThe gravitational acceleration is 9.75 m/s²The distance covered to lift the persons is 100 mTherefore,Work done = force × distance
Using this formula, we getForce = Work done / distance= 341.2 kJ / 100 m= 3412 J / 1 m= 3412 NNow, force = mass × gravitational accelerationTherefore, mass = force / gravitational acceleration= 3412 N / 9.75 m/s²= 350.56 kgAverage mass per person = Total mass / Number of persons= 350.56 kg / 5= 70.11 kg ≈ 70 kgTherefore, the average mass per person in kg is 70 kg. Hence, the correct option is (b).
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Write a MATLAB program that will simulate and plot the response of a multiple degree of freedom system for the following problems using MODAL ANALYSIS. Problem 1: 12 - 0 (t) 10 X(t) = 0 - [ 6360 +(-2 12]-« -H 0 Initial Conditions: x(0) and x(0) = 0 Outputs Required: Problem 1: Xi(t) vs time and x2(t) vs time in one single plot. Use different colors and put a legend indicating which color plot represents which solution.
Here's a MATLAB program that simulates and plots the response of a multiple degree of freedom system using modal analysis for the given problem:
```matlab
% System parameters
M = [12 0; 0 10]; % Mass matrix
K = [6360 -12; -12 12]; % Stiffness matrix
% Modal analysis
[V, D] = eig(K, M); % Eigenvectors (mode shapes) and eigenvalues (natural frequencies)
% Initial conditions
x0 = [0; 0]; % Initial displacements
v0 = [0; 0]; % Initial velocities
% Time vector
t = 0:0.01:10; % Time range (adjust as needed)
% Response calculation
X = zeros(length(t), 2); % Matrix to store displacements
for i = 1:length(t)
% Mode superposition
X(i, :) = (V * (x0 .* cos(sqrt(D) * t(i)) + (v0 ./ sqrt(D)) .* sin(sqrt(D) * t(i)))).';
end
% Plotting
figure;
plot(t, X(:, 1), 'r', 'LineWidth', 1.5); % X1(t) in red
hold on;
plot(t, X(:, 2), 'b', 'LineWidth', 1.5); % X2(t) in blue
xlabel('Time');
ylabel('Displacement');
title('Response of Multiple Degree of Freedom System');
legend('X1(t)', 'X2(t)');
grid on;
```
In this program, the system parameters (mass matrix M and stiffness matrix K) are defined. The program performs modal analysis to obtain the eigenvectors (mode shapes) and eigenvalues (natural frequencies) of the system. The initial conditions, time vector, and response calculation are then performed using mode superposition. Finally, the program plots the responses X1(t) and X2(t) in a single plot with different colors and adds a legend for clarity.
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As an environmental consultant, you have been assigned by your client to design effective wastewater treatment for 500 dairy cows. -Calculate wastewater produce (m³/day), if 378 L/cow is generated every day.
-Calculate the suitable dimension for anaerobic pond, facultative pond and aerobic pond if safety factor 1.2 (20%). -Sketch the design of the ponds as per suggested in series or parallel and label properly.
As an environmental consultant, the effective wastewater treatment designed for 500 dairy cows is calculated as follows.
Calculation of wastewater produced (m³/day)Daily amount of wastewater produced by 1 cow = 378 L/cow1 L = 0.001 m³Amount of wastewater produced by 1 cow = 0.378 m³/day. Amount of wastewater produced by 500 cows = 0.378 m³/day x 500 cows Amount of wastewater produced by 500 cows = 189 m³/day.
Calculation of the suitable dimension for anaerobic pond, facultative pond, and aerobic pond. The total volume of the ponds is based on the organic loading rate (OLR), hydraulic retention time (HRT), and volumetric loading rate (VLR). For instance, if the OLR is 0.25-0.4 kg BOD/m³/day, HRT is 10-15 days, and VLR is 20-40 kg BOD/ha/day.
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true or false Strength of materials was concern with relation .between load and stress The slope of stress-strain called the modulus of .elasticity The unit of deformation has .the same unit as length L The Shearing strain is defined as the angular change between three perpendicular faces of a .differential elements Bearing stress is the pressure resulting from the connection of adjoining .bodies Normal force is developed when the external loads tend to push or pull on the two .segments of the body If the thickness t≤10/D,it is .called thin walled vessels The structure of the building needs to know the internal . loads at various points A balance of forces prevent the body from translating or having a accelerated motion .along straight or curved path The ratio of the shear stress to the shear strain is called .the modulus of elasticity
Strength of materials was concerned with the relation between load and stress, which is true. Strength of materials is the study of how solid objects react and deform under stress and strain, including the elasticity, plasticity, and failure of solid materials. The slope of the stress-strain curve is called the modulus of elasticity, which is also true. The modulus of elasticity is defined as the ratio of stress to strain within the elastic limit.
The unit of deformation has the same unit as length L, which is true. The unit of deformation is the same as that of length, which is typically measured in meters (m). The Shearing strain is defined as the angular change between three perpendicular faces of a differential element, which is also true. Shear strain is defined as the angular change between two parallel faces of a differential element, whereas shear stress is defined as the force per unit area that acts parallel to the face.
A balance of forces prevents the body from translating or having an accelerated motion along a straight or curved path, which is true. The principle of equilibrium states that for an object to be in a state of equilibrium, the net force acting on it must be zero. The ratio of the shear stress to the shear strain is called the modulus of rigidity or shear modulus, which is false. The correct term for the ratio of the shear stress to the shear strain is the modulus of rigidity or shear modulus.
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Consider (symmetric) beam configuration 10000mm L X 100mm W X 50mm H, with tensile strength 268MPa and complete the following tasks, supposing that the beam is made of a perfectly elasto-plastic material with a yield strength equal to 245MPa
(a) Under the conditions defined above, what is the maximum elastic moment for the section? M
(b) Identify the plastic moment P and the shape factor for the section.
(c) Produce a sketch showing the distribution of stresses across the beam section for an applied moment of =12(y+P).
(d) Produce a sketch showing the distribution of residual stress across the beam section if the moment applied in part (c) is removed.
(a) Elastic moment For a beam of dimensions, 10000mm L X 100mm W X 50mm H, under the conditions defined above and assuming that the beam is made of a perfectly elastic-plastic material with a yield strength equal to 245MPa.
The maximum elastic moment for the section is calculated by using the formula; [tex]\frac{σ_y}{f_s}[/tex] where σy is the yield strength and fs is the stress factor.
Distribution of residual stress across the beam section the distribution of residual stress across the beam section if the moment applied in part (c) is removed is shown in the figure below. The residual stress distribution is symmetric about the neutral axis and the stress value at the outermost fiber is zero.
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If the normalization values per person per year for the US in the year 2008 for each impact category is shown in the table below. Calculate the externally normalized impacts of each of the four refrigerators with this normalization data.
Normalization is the process of developing a standardized way of comparing different environmental impacts to better comprehend the actual significance of each.
This is accomplished by categorizing and establishing standards for a variety of environmental impacts so that they may be more easily compared to one another.
The normalization values per person per year for the US in the year 2008 for each impact category are provided in the table.
The following is a list of externally normalized impacts for each of the four refrigerators based on this normalization data:
We need to take the sum of the product of the normalization values and the value of each category of the impact for every refrigerator.
The results are listed below:
For refrigerator A: 4.3*100 + 2.2*150 + 2.7*200 + 5.2*80 = 430 + 330 + 540 + 416 = 1716.
For refrigerator B: 4.3*130 + 2.2*140 + 2.7*210 + 5.2*70 = 559 + 308 + 567 + 364 = 1798.
For refrigerator C: 4.3*110 + 2.2*130 + 2.7*190 + 5.2*100 = 473 + 286 + 513 + 520 = 1792.
For refrigerator D: 4.3*100 + 2.2*160 + 2.7*180 + 5.2*90 = 430 + 352 + 486 + 468 = 1736.
Thus, the externally normalized impacts of each of the four refrigerators are as follows:
Refrigerator A: 1716 Refrigerator B: 1798 Refrigerator C: 1792 Refrigerator D: 1736.
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NOTE: This is a multi-part question. Once an answer is submitted, you will be unable to return to this part. Five kilograms of air at 427°C and 600 kPa are contained in a piston-cylinder device. The air expands adiabatically until the pressure is 100 kPa and produces 690 kJ of work output. Assume air has constant specific heats evaluated at 300 K. Determine the entropy change of the air in kJ/kg.K. Use the table containing the ideal gas specific heats of various common gases. (You must provide an answer before moving on to the next part.) The entropy change of the air is kJ/kg.K.
Given that:Five kilograms of air at 427°C and 600 kPa are contained in a piston-cylinder device. The air expands adiabatically until the pressure is 100 kPa and produces 690 kJ of work output.
Assume air has constant specific heats evaluated at 300 K. We know that Adiabatic process is the process in which no heat transfer takes place. Here, ΔQ = 0.W = ΔUAdiabatic work is given by the equation.
This ΔU is change in internal energy. From the first law of thermodynamics,ΔU = Q + W= ΔU = CvΔTwhere Cv is specific heat at constant volume and ΔT is change in temperature. From the question, it is given that the specific heat is evaluated at 300 K. Therefore, we will have to calculate the change in temperature from 427°C to 300 K.
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A centrifugal flow air compressor has a total temperature rise across the stage of 180 K. There is no swirl at inlet and the impeller has radial outlet blading. The impeller outlet diameter is 45 mm. Assuming no slip, calculate the rotational speed of the compressor impeller.
In a centrifugal flow air compressor, there is a total temperature rise across the stage of 180K. Therefore, it is necessary to calculate the rotational speed of the compressor impeller, assuming no slip. Impeller outlet velocity: where, $N$ is the speed of rotation in rpm.
Where, $b$ is blade angle at outlet in radian. Delta T_{total} = T_{02} - T_{01}$$ where, $T_{02}$ is stagnation temperature at the outlet, and $T_{01}$ is stagnation temperature at the inlet. The stagnation temperature at the inlet and outlet of a compressor stage can be assumed to be constant.
Thus, for a stage of a compressor: is the specific heat at constant pressure. Solving the above equation for $u_2$, we get:$$u_2 = \sqrt{2C_p\Delta T_{total}}$$ By substituting the value of $u_2$ in the equation derived earlier, we can write:$$\sqrt{2C_p\Delta T_{total}} = \frac{\pi \times 0.045 \times N}{60} - \frac{\pi \times 0.045 \times bN}{60}$$ By simplifying the above equation,
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true false
If the thickness t≤10/D,it is called thin walled vessels.
The statement that "If the thickness t ≤ 10/D, it is called thin-walled vessels" is True. When designing a pressure vessel, engineers have to specify the wall thickness to ensure that the stresses in the wall do not exceed the allowable stress of the material used.
Thin-walled vessels are generally used to store gases or liquids under high pressure. The most commonly used thin-walled vessels are pipes and tubes, boilers, pressure vessels, and storage tanks. These types of vessels are used in various industries, such as the chemical, pharmaceutical, and petrochemical industries.
Thin-walled vessels have many advantages over thick-walled vessels. For instance, they require less material, which makes them less expensive. Additionally, thin-walled vessels have lower thermal inertia, which means that they can heat up or cool down quickly. However, there are also disadvantages to using thin-walled vessels. They can be more prone to buckling, and they are less resistant to corrosion than thick-walled vessels.
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a single cylinder IC engine generates an output power of 10KW when operating at 2000rpm. the engine consumes 2cc/s of petrol and had a compression ratio of 10. the engine is capable of converting 40% of combustion heat energy into power stroke. the volume of charge inside the cylinder at the end of compression stroke is 0.2 litre. if the engine is designed such that the power is developed for every two revolution of crankshaft in a given cycle of operation,
(i) what will be brake torque,
(ii) what is mean effective pressure,
(iii) what is brake specific fuel consumption in kg/kWh? assume calorific value of fuel ad 22000 kj/kg and specific gravity of fuel as 0.7 and density of water as 1000kg/m cube
Answer:
Explanation:
To calculate the brake torque, mean effective pressure, and brake specific fuel consumption, we need to use the given information and apply relevant formulas. Let's calculate each parameter step by step:
Given:
Output power (P) = 10 kW
Engine speed (N) = 2000 rpm
Fuel consumption rate (Vdot) = 2 cc/s
Compression ratio (r) = 10
Combustion heat energy to power conversion efficiency (η) = 40%
Volume of charge at the end of compression stroke (Vc) = 0.2 liters
Calorific value of fuel (CV) = 22000 kJ/kg
Specific gravity of fuel (SG) = 0.7
Density of water (ρw) = 1000 kg/m³
(i) Brake Torque (Tb):
Brake power (Pb) = P
Pb = Tb * 2π * N / 60 (60 is used to convert rpm to seconds)
Tb = Pb * 60 / (2π * N)
Substituting the given values:
Tb = (10 kW * 60) / (2π * 2000) = 0.954 kNm
(ii) Mean Effective Pressure (MEP):
MEP = (P * 2 * π * N) / (4 * Vc * r * η)
Note: The factor 2 is used because the power is developed for every two revolutions of the crankshaft in a given cycle.
Substituting the given values:
MEP = (10 kW * 2 * π * 2000) / (4 * 0.2 liters * 10 * 0.4)
MEP = 49.348 kPa
(iii) Brake Specific Fuel Consumption (BSFC):
BSFC = (Vdot / Pb) * 3600
Note: The factor 3600 is used to convert seconds to hours.
First, we need to convert the fuel consumption rate from cc/s to liters/hour:
Vdot_liters_hour = Vdot * 3600 / 1000
Substituting the given values:
BSFC = (2 liters/hour / 10 kW) * 3600
BSFC = 0.72 kg/kWh
Therefore, the brake torque is approximately 0.954 kNm, the mean effective pressure is approximately 49.348 kPa, and the brake specific fuel consumption is approximately 0.72 kg/kWh.
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Answer:
The brake torque is approximately 0.954 kNm, the mean effective pressure is approximately 49.348 kPa, and the brake specific fuel consumption is approximately 0.72 kg/kWh.
Explanation:
To calculate the brake torque, mean effective pressure, and brake specific fuel consumption, we need to use the given information and apply relevant formulas. Let's calculate each parameter step by step:
Given:
Output power (P) = 10 kW
Engine speed (N) = 2000 rpm
Fuel consumption rate (Vdot) = 2 cc/s
Compression ratio (r) = 10
Combustion heat energy to power conversion efficiency (η) = 40%
Volume of charge at the end of compression stroke (Vc) = 0.2 liters
Calorific value of fuel (CV) = 22000 kJ/kg
Specific gravity of fuel (SG) = 0.7
Density of water (ρw) = 1000 kg/m³
(i) Brake Torque (Tb):
Brake power (Pb) = P
Pb = Tb * 2π * N / 60 (60 is used to convert rpm to seconds)
Tb = Pb * 60 / (2π * N)
Substituting the given values:
Tb = (10 kW * 60) / (2π * 2000) = 0.954 kNm
(ii) Mean Effective Pressure (MEP):
MEP = (P * 2 * π * N) / (4 * Vc * r * η)
Note: The factor 2 is used because the power is developed for every two revolutions of the crankshaft in a given cycle.
Substituting the given values:
MEP = (10 kW * 2 * π * 2000) / (4 * 0.2 liters * 10 * 0.4)
MEP = 49.348 kPa
(iii) Brake Specific Fuel Consumption (BSFC):
BSFC = (Vdot / Pb) * 3600
Note: The factor 3600 is used to convert seconds to hours.
First, we need to convert the fuel consumption rate from cc/s to liters/hour:
Vdot_liters_hour = Vdot * 3600 / 1000
Substituting the given values:
BSFC = (2 liters/hour / 10 kW) * 3600
BSFC = 0.72 kg/kWh
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Fifth percentile U.K. male has forward reach of 777 mm. His
shoulder is 375 mm above a horizontal work surface. Calculate the
radius of the "zone of convenient reach" (ZCR) on the desktop.
The radius of the "zone of convenient reach" (ZCR) on the desktop is approximately 863.29 mm.
To calculate the radius of the "zone of convenient reach" (ZCR) on the desktop, we can use the Pythagorean theorem. The ZCR is the maximum distance that the Fifth percentile U.K. male can comfortably reach from the shoulder height to the forward reach.
Given:
Forward reach of the Fifth percentile U.K. male = 777 mm
Shoulder height above the work surface = 375 mm
Let's consider a right-angled triangle with the ZCR as the hypotenuse, the forward reach as one side, and the vertical distance from the work surface to the shoulder height as the other side.
Using the Pythagorean theorem:
ZCR² = forward reach² + shoulder height²
Substituting the given values:
ZCR² = (777 mm)² + (375 mm)²
Calculating the sum:
ZCR² = 604,929 mm² + 140,625 mm²
ZCR² = 745,554 mm²
Taking the square root of both sides to find ZCR:
ZCR = √745,554 mm
ZCR ≈ 863.29 mm
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Which of the following devices is used for atomizing and vaporizing the fuel before mixing it with air in varying proportions? O Spark plug O Carburetor O Flywheel o Governor
The carburetor is a device that is used for atomizing and vaporizing the fuel before mixing it with air in varying proportions. The carburetor is a device used to combine fuel and air in the proper ratio for an internal combustion engine.
A carburetor is a component of the internal combustion engine that mixes fuel with air in a combustible gas form that can be burned in the engine cylinders. The carburetor combines fuel from the fuel tank with air that is taken in through the air filter before delivering it to the engine cylinders.
The process of atomization and vaporization of the fuel happens when the fuel is sprayed into the airstream by a nozzle and broken into tiny droplets or mist. Then, the fuel droplets are suspended in the air, creating a fuel-air mixture. The carburetor regulates the fuel-air ratio in the mixture.
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Two pipes with 400 and 600 mm diameters, and 1000 and 1500 m lengths, respectively, are connected in series through one 600 * 400 mm reducer, consist of the following fittings and valves: Two 400-mm 90o elbows, One 400-mm gate valve, Four 600-mm 90o elbows, Two 600-mm gate valve. Use
the Hazen Williams Equation with a C factor of 130 to calculate the total pressure drop due to friction in the series water piping system at a flow rate of 250 L/s?
The total pressure drop due to friction in the series water piping system at a flow rate of 250 L/s is 23.12 meters.
To calculate the total pressure drop, we need to determine the friction losses in each section of the piping system and then add them together. The Hazen Williams Equation is commonly used for this purpose.
In the first step, we calculate the friction loss in the 400-mm diameter pipe. Using the Hazen Williams Equation, the friction factor can be calculated as follows:
f = (C / (D^4.87)) * (L / Q^1.85)
where f is the friction factor, C is the Hazen Williams coefficient (130 in this case), D is the pipe diameter (400 mm), L is the pipe length (1000 m), and Q is the flow rate (250 L/s).
Substituting the values, we get:
f = (130 / (400^4.87)) * (1000 / 250^1.85) = 0.000002224
Next, we calculate the friction loss using the Darcy-Weisbach equation:
ΔP = f * (L / D) * (V^2 / 2g)
where ΔP is the pressure drop, f is the friction factor, L is the pipe length, D is the pipe diameter, V is the flow velocity, and g is the acceleration due to gravity.
For the 400-mm pipe:
ΔP1 = (0.000002224) * (1000 / 400) * (250 / 0.4)^2 / (2 * 9.81) = 7.17 meters
Similarly, we calculate the friction loss for the 600-mm pipe:
f = (130 / (600^4.87)) * (1500 / 250^1.85) = 0.00000134
ΔP2 = (0.00000134) * (1500 / 600) * (250 / 0.6)^2 / (2 * 9.81) = 15.95 meters
Finally, we add the friction losses in each section to obtain the total pressure drop:
Total pressure drop = ΔP1 + ΔP2 = 7.17 + 15.95 = 23.12 meters
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(a) How line drawing method can be applied for suggesting solution for unclear cases of ethical misconduct. (b) How middle way solution can be suggested for tackling moral situations efficiently.
a)When faced with a moral dilemma, the nurse's first step should be to carefully assess the situation. This includes gathering all relevant information and facts, as well as understanding the values and beliefs of all parties involved.
b)The nurse should also consider the potential consequences of each possible course of action.
Once the situation has been thoroughly assessed, the nurse should then consult with other healthcare professionals, such as the patient's physician, a bioethicist, or the hospital's ethics committee. This can provide the nurse with additional perspectives and guidance on how to proceed.
It is also important for the nurse to consider their own values and beliefs, and how they may impact their decision-making in the situation. The nurse should strive to maintain their professionalism and objectivity, while also respecting the autonomy and dignity of the patient.
Ultimately, the nurse should strive to make a decision that is consistent with their ethical obligations and that upholds the highest standards of patient care. This may require difficult choices and uncomfortable conversations, but it is essential for ensuring the best possible outcome for the patient.
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What is the ductile brittle transition temperature in steels. Explain in detail the factors affecting this property in steels. How can the ductile-brittle transition temperature property of steels be improved without reducing the weldability, ductility, hardness and strength values? Explain in detail (draw the relevant figures and graphics you deem necessary).
Ductile-brittle transition temperature is the temperature at which ductile to brittle transition takes place. Heat treatment is another method that can be used to improve the ductile-brittle transition temperature of steels. Heat treatment can change the microstructure of steels, which affects their ductility and toughness.
It is the temperature at which a material's toughness and ductility drops suddenly from high to low values. This transition temperature varies from one material to another, and it is usually tested with the Charpy impact test.Ductile-brittle transition temperature in steelsDuctile-brittle transition temperature is important in engineering as it influences the mechanical behavior of materials at low temperatures. Ductile materials have the ability to deform plastically when subjected to an applied force
Composition: The composition of steels affects their mechanical properties. The addition of alloying elements can change the microstructure of steels, which in turn affects their ductility and toughness.
Grain size: Grain size also plays an important role in determining steel's mechanical properties. A fine-grained microstructure tends to enhance ductility, while a coarse-grained microstructure tends to reduce ductility.
Heat treatment: Heat treatment can change the microstructure of steels, which affects their ductility and toughness.
Rate of loading: The rate of loading can affect the ductile-brittle transition temperature. A slow loading rate can result in ductile behavior, while a fast loading rate can result in brittle behavior.
Alloying elements such as nickel and manganese have been shown to improve the ductile-brittle transition temperature of steels. Another method is by refining the grain size. A fine-grained microstructure tends to enhance ductility, while a coarse-grained microstructure tends to reduce ductility.
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A particle is moving along a straight line through a fluid medium such that its speed is measured as v = (80 m/s, where t is in seconds. If it is released from rest at determine its positions and acceleration when 2 s.
To determine the position and acceleration of the particle at t = 2 s, we need to integrate the velocity function with respect to time.
Given:
Velocity function: v = 80 m/s
Initial condition: v₀ = 0 (particle released from rest)
To find the position function, we integrate the velocity function:
x(t) = ∫v(t) dt
= ∫(80) dt
= 80t + C
To find the value of the constant C, we use the initial condition x₀ = 0 (particle released from rest):
x₀ = 80(0) + C
C = 0
So, the position function becomes:
x(t) = 80t
To find the acceleration, we differentiate the velocity function with respect to time:
a(t) = d(v(t))/dt
= d(80)/dt
= 0
Therefore, the position of the particle at t = 2 s is x(2) = 80(2) = 160 m, and the acceleration at t = 2 s is a(2) = 0 m/s².
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A battery applies 1 V to a circuit, while an ammeter reads 10 mA. Later the current drops to 7.5 mA. If the resistance is unchanged, the voltage must have:
O increased to 1.5 V O decreased to 0.5 V O remained constant O decreased by 25% from its old value
A battery applies 1 V to a circuit, while an ammeter reads 10 mA. Later, the current drops to 7.5 mA. If the resistance is unchanged, the voltage must have remained constant (C).
This can be easily explained by using Ohm's Law which is given as V= IR
Where V is voltage, I is current, and R is resistance.
The above expression shows that voltage is directly proportional to current. So, when the current through the circuit drops, the voltage through it also decreases accordingly. The battery applies a voltage of 1V, and the ammeter reads 10mA of current. Hence, applying Ohm's law: R = V/I = 1 V/0.01 A = 100 ΩAfter some time, the current drops to 7.5 mA and the resistance of the circuit is unchanged. Therefore, applying Ohm's Law again, the voltage can be calculated as follows: V = IR = 0.0075 A × 100 Ω = 0.75 VSo, the voltage drops to 0.75V when the current drops to 7.5 mA, and the resistance is unchanged. Therefore, the voltage must have remained constant (C) when the current dropped by 25%.
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How is acceleration of particles achieved in an electromagnetic
propulsion system?
An electromagnetic propulsion system is the technology that uses the interaction between electric and magnetic fields to propel a projectile. The system consists of a power source that converts electrical energy into a magnetic field.
The magnetic field then interacts with the metallic object on the projectile, generating a force that propels the projectile forward.The acceleration of particles in an electromagnetic propulsion system is achieved through the Lorentz force. This force acts upon charged particles in a magnetic field.
The Lorentz force can be expressed as:
F = q(E + v × B), where
F is the force on the particle,
q is the charge of the particle,
E is the electric field,
v is the velocity of the particle, and
B is the magnetic field.
The Lorentz force can be manipulated to achieve the desired acceleration of particles in an electromagnetic propulsion system. By adjusting the strength and direction of the magnetic field, the force acting on the charged particles can be increased or decreased. The electric field can also be adjusted to achieve the desired acceleration.
The electromagnetic propulsion system has several advantages over conventional propulsion systems. It is highly efficient and has a lower environmental impact. The system also has a higher thrust-to-weight ratio, making it ideal for space travel.
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An air-cooled condenser has an h value of 30 W/m² −K based on the air-side area. The air-side heat transfer area is 190 m² with air entering at 27°C and leaving at 40°C. If the condensing temperature is constant at 49°C, what is the air mass flow rate in kg/s ? Let Cₚ₍ₐᵢᵣ₎ = 1.006 kJ/kg−K.(20pts) Draw and label the temperature-flow diagram. Round off your answer to three (3) decimal places.
The air-side heat transfer area is 190 m² with air entering at 27°C and leaving at 40°C. The condensing temperature is constant at 49°C. We need to find the air mass flow rate in kg/s. Also,[tex]Cₚ₍ₐᵢᵣ₎ = 1.006 kJ/kg−K.[/tex]The heat flow from the condenser is given by[tex]Q = m . Cp .[/tex]
Heat flow from the condenser is given by [tex]Q = m . Cp . ∆T[/tex]
Now, heat is transferred from the refrigerant to air.The formula for heat transfer is given by,
[tex]Q = U . A . ∆T[/tex]Where,Q = heat flow in kJ/sU = overall heat transfer coefficient in W/m²-KA = heat transfer area in [tex]m²∆T[/tex] = difference between the temperatures of refrigerant and air in K
Now, the overall heat transfer coefficient is given by,U = h / δWhere,h = heat transfer coefficient of air in W/m²-Kδ = thickness of the boundary layer in metersWe know the value of h as 30 W/m²-K, but the value of δ is not given. Therefore, we need to assume a value of δ as 0.0005 m.Then, the overall heat transfer coefficient is given by
[tex]U = 30 / 0.0005 = 60000 W/m²-K[/tex]
Now, heat flow from the refrigerant is given by
[tex]Q = U . A . ∆TQ = 60000 x 190 x 9Q = 102600000 W = 102600 kWAlso,Q = m . Cp . ∆T102600 = m . 1.006 . 9m = 11402.65 kg/s[/tex]
Therefore, the air mass flow rate in the air-cooled condenser is 11402.65 kg/s.
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Air with a uniform current at a speed of 100 ft per sec is flowing around a ROTATING cylinder with a radius of 15 in. The cylinder is rotating about 100 times per minute. The freestream is said to be at Standard Sea Level Condition. At an angle of 20 deg with the direction of the flow, what is the pressure at that point?
Given parameters:Speed of the current = 100 ft per secRadius of cylinder = 15 in Revolution = 100 per minuteAngle = 20 degreesFind: Pressure at that pointThe answer to the question is:P = (dynamic pressure) + (static pressure)Where dynamic pressure is the pressure exerted by the fluid due to its motion and static pressure is the pressure exerted by the fluid when it is at rest.
To find the dynamic pressure we can use the formula below.Q = (density of fluid) x (velocity)^2/2Where Q is dynamic pressureDensity of air at sea level condition = 1.23 kg/m^3Let's convert the given parameters into SI units:Speed of the current = 100 ft per sec = 30.48 m/sRadius of cylinder = 15 in = 0.381 mRevolution = 100 per minute = 100/60 rev per sec = 1.67 rev per secAngle = 20 degrees = 0.349 radians
Now, substitute the values into the formula of dynamic pressure.Q = 1.23 x (30.48)^2/2Q = 5587.79 N/m^2Let's find the static pressure of the fluid.P = (density of fluid) x (gravity) x (height)Where gravity = 9.81 m/s^2, and height is the distance between the surface of the fluid and the point where we want to find the pressure. Here the height is the radius of the cylinder, which is 0.381 m.P = 1.23 x 9.81 x 0.381P = 4.64 N/m^2
Now, find the pressure at the point using the formula:P = Q + PP = 5587.79 + 4.64P = 5592.43 N/m^2Therefore, the pressure at that point is 5592.43 N/m^2 when the air with a uniform current at a speed of 100 ft per sec is flowing around a ROTATING cylinder with a radius of 15 in at an angle of 20 degrees with the direction of the flow.
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