The value the change in specific internal energy of the air is 143.4 kJ/kg.
Let us recall the formula for change in internal energy ΔU and its relationship with specific heat. We know that the change in internal energy of a closed system is equal to the heat added to the system minus the work done by the system. Mathematically it can be written as: ΔU = Q - W
Where Q is the heat added and W is the work done by the system. Let the specific heat of the gas at constant volume be cv and at constant pressure be cp.
We can write the relationship between specific heats and internal energy per unit mass as: cv = du/dT and cp = dh/dT.
This means that change in internal energy per unit mass can be expressed as Δu = cv ΔT
where ΔT is the change in temperature. If we assume that specific heats of the ideal gas remains constant during the process then, we can use the formula Δu = cv ΔT to calculate the change in specific internal energy.
Given, Air undergoes a process in which its initial and final temperatures are 250K and 450K. Therefore, ΔT = 450 - 250 = 200K
Let's assume specific heats of air at constant volume and constant pressure are 0.717 kJ/kg-K and 1.005 kJ/kg-K respectively.
Therefore, cv = 0.717 kJ/kg-K and ΔT = 200K Therefore, Δu = cv ΔT = 0.717 kJ/kg-K × 200 K = 143.4 kJ/kg
Therefore, the change in specific internal energy of the air is 143.4 kJ/kg.
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setup time on A is 45-minutes and runtime is 5-minutes per piece. The setup time on B is 30-minutes and runtime is 4-minutes per piece. The wait time between the two operations is 8-hours. The move time between A and B is 60-minutes. Wait time after operation B is 8-hours, and the move time into stores s 2-hours. Queue at work center A is 40-hours and at B is 35- hours. Calculate the total manufacturing lead-time for the order. What percentage of the lead-time is the order actually running (a.k.a. runtime)? Enter numerical answer only. You may use the table below as a guideline to answer the above question. Process or Activity Total Time Queue at work center A Work center A operation time Wait time at A Move time from A to B Queue at work center B Work center B operation time
Given:setup time on A is 45-minutes and runtime is 5-minutes per piece. The setup time on B is 30-minutes and runtime is 4-minutes per piece. The wait time between the two operations is 8-hours. The move time between A and B is 60-minutes. Wait time after operation B is 8-hours, and the move time into stores s 2-hours.
Queue at work center A is 40-hours and at B is 35- hours.To find:Calculate the total manufacturing lead-time for the order. What percentage of the lead-time is the order actually running (a.k.a. runtime)?Solution:Given, Setup time on A = 45 minsRun time on A = 5 minsSetup time on B = 30 minsRun time on B = 4 mins Wait time between operations = 8 hoursMove time from A to B = 60 mins
Percentage of lead-time for which the order is running = (25 × 5 + 25 × 4) × 100 / 29100= 325 / 582= 55.87 %Hence, the total manufacturing lead-time for the order is 485 hours and the percentage of the lead-time for which the order is actually running (a.k.a. runtime) is 55.87 %.
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A duct 0.4 m high and 0.8 m wide, suspended from a ceiling in a corridor, makes a right-angle turn in the horizontal plane. The inner radius is 0.2 m, and the outer radius is 0.4 m, measured from the same center. The velocity of air in the duct is 10 m/s. To how many meters of straight duct is the pressure loss in this elbow equivalent?
9.5
15.0
10.8
7.9
The area of the duct is given by:A = h x w= 0.4 x 0.8= 0.32 m²The perimeter of the duct can be calculated by adding the perimeter of the horizontal side of the rectangular duct to the perimeter of the curved part of the duct.
The perimeter of the horizontal side of the rectangular duct is given by:P1 = 2 (h + w)= 2 (0.4 + 0.8)= 2.4 mThe perimeter of the curved part of the duct is given by:P2 = π(r1 + r2)= π (0.2 + 0.4)= 1.26 mTherefore, the total perimeter of the duct is given by:P = P1 + P2= 2.4 + 1.26= 3.66 mNow, we need to calculate the pressure loss in the elbow.
the Bernoulli's equation becomes:1/2 ρ V1² = 1/2 ρ V2²Now, we can write the equation for pressure loss as:P1 - P2 = 1/2 ρ (V2² - V1²)P1 - P2 = 1/2 ρ (0 - V1²)P1 - P2 = -1/2 ρ V1²The pressure loss is given by:P1 - P2 = -1/2 ρ V1²The density of air, ρ = 1.2 kg/m³Therefore, the pressure loss is:P1 - P2 = -1/2 x 1.2 x (10)²P1 - P2 = -60 Pa
by using the Darcy-Weisbach equation The diameter of the duct can be taken as the hydraulic diameter which is given by:Dh = 4A / PWhere, A = area of cross-section of ductP = perimeter of the ductThe area of the duct is already calculated as 0.32 m². The perimeter of the duct is 3.66 m. Therefore, the hydraulic diameter of the duct is:Dh = 4 x 0.32 / 3.66= 0.35 m. The friction factor can be calculated by using the Moody chart. The Reynolds number is given by:Re = ρ V Dh / µWhere, µ = viscosity of fluidThe viscosity of air at 20°C is 1.8 x 10^-5 N s/m².
Therefore, the relative roughness is:ε / Dh = 0.15 x 10^-3 / 0.35 = 4.29 x 10^-4Using the Moody chart, we can find out that the friction factor for the given Reynolds number and relative roughness is: f = 0.0153Now, calculate the pressure loss in the straight duct of length x:ΔP = f (L / Dh) (ρ V² / 2)60 = 0.0153 (x / 0.35) (1.2 x 10)² / 2x = 7.9 m..Therefore, the pressure loss in the elbow is equivalent to the pressure loss in a straight duct of length 7.9 m.
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An F-4 jet flying in T = 10°C air at an altitude of 1.0 km passes directly overhead of a ground level spot. A loud boom is heard at the ground spot At = 2 sec after the jet has passed overhead. At what Mach number M was the jet flying? Approx.Ans M~1.2
An F-4 jet flying in T = 10°C air at an altitude of 1.0 km passes directly overhead of a ground level spot. A loud boom is heard at the ground spot At = 2 sec after the jet has passed overhead.
The Mach number of the jet flying was approximately 1.2. Given that a loud boom is heard at the ground spot At = 2 sec after the jet has passed overhead. The speed of sound in air of temperature T is given by:[tex]V = 20.05√(T+273) m/s= 20.05 × √(283) m/s= 343 m/s[/tex].
Now we know the distance travelled by sound wave is 1.206 km and time taken by it to travel from the jet to the spot is 2 sec. Hence, the speed of sound = distance/time= 1.206/2= 0.603 km/s= 603 m/s The Mach number M of the plane is given by: M = v / c where v is the velocity of the jet and c is the speed of sound in the atmosphere at the altitude of the jet.
By using the formula M = v / c we get M = v / c= Mach number= velocity of the plane/speed of sound in the atmosphere at the altitude of the jet Now, velocity of the plane = Distance traveled by the plane / time taken= 1.206 / 2= 0.603 km/s= 603 m/s Putting the values in the formula, we get:[tex]M = v / c= (603) / (343) = 1.758[/tex]At Approx. Ans M ~ 1.2
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Calculate the weight fraction of mullite that is pro eutectic in a slowly cooled 30 mol % Al2O3 70 mol % SiO2 refractory cooled to room temperature.
The weight fraction of pro eutectic mullite is 100%.
To calculate the weight fraction of pro eutectic mullite in the refractory material, we need to consider the phase diagram of the Al2O3-SiO2 system.
In a slowly cooled refractory with 30 mol% Al2O3 and 70 mol% SiO2, the eutectic composition occurs at approximately 50 mol% Al2O3 and 50 mol% SiO2.
Below this composition, mullite is the primary phase, and above it, corundum (Al2O3) is the primary phase.
Since the composition of the refractory is below the eutectic composition, we can assume that the entire refractory consists of mullite. Therefore, the weight fraction of pro eutectic mullite is 100%.
It's important to note that the weight fraction of mullite could change if the refractory was cooled under different conditions or if impurities were present.
However, based on the given information of a slowly cooled refractory with the specified composition, the weight fraction of pro eutectic mullite is 100%.
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(a) Figure Q2(b) shows two steel bars each of 2.0 m length and 30 mm in diameter supporting a temporary road sign weighting 5000 kg. Take: E = 205 kN/mm², Poisson's ratio v = 0.3 and g = 9.81 m/s2 [6 marks] [5 marks] () Calculate the shortening per bar. (ii) Calculate the change in lateral dimension per bar. (iii) Calculate the change in volume per bar. (iv) Calculate the volumetric strain per bar. [5 marks] [2 marks] Road Sign M= 5000 kg Figure Q2b 2m (Figure not to scale)
The shortening per bar is 0.33 mm, the change in lateral dimension per bar is 0.0131 mm, the change in volume per bar is 1.655 × 10^-4 and the volumetric strain per bar is 8.275 × 10^-8.
(a) Calculation of Shortening Per Bar
We have given;E = 205 kN/mm²
Poisson's ratio v = 0.3g = 9.81 m/s²
Diameter of the steel bar d = 30mm
Radius of the steel bar r = d/2 = 30/2 = 15mm
Length of each bar L = 2.0m
Weight of the temporary road sign M = 5000kg
The force exerted on each bar F = Mg/2 = (5000 × 9.81) / 2 = 24525N
The axial stress in the steel bar due to the weight of the sign σ = F/Awhere A = πr² = π (15)² = 706.86 mm²σ = 24525 / 706.86 = 34.71 N/mm²
Now, the change in length (ΔL) can be calculated by;ΔL/L = σ/E [(1-v)]ΔL = (σ/E [(1-v)]) × LΔL = (34.71 / (205 × 10³)) [(1-0.3)] × 2000ΔL = 0.33 mm
Shortening per bar = ΔL = 0.33mm (Ans).
(b) Calculation of Change in Lateral Dimension per Bar
Now, the change in the lateral dimension (Δd) can be calculated by;Δd/d = -v (σ/E [(1-v)])Δd = -v (σ/E [(1-v)]) × dΔd = -0.3 (34.71 / (205 × 10³)) [(1-0.3)] × 30Δd = -0.0131 mm
Change in Lateral Dimension per Bar = Δd = 0.0131mm (Ans).
(c) Calculation of Change in Volume per Bar
Now, the change in volume (ΔV) can be calculated by;ΔV/V = (ΔL/L) + 2 [(Δd/d)]
ΔV/V = (0.33/2000) + 2 [(0.0131/30)]ΔV/V = 1.655 × 10^-4
Change in Volume per Bar = ΔV = 1.655 × 10^-4 (Ans).
(d) Calculation of Volumetric Strain per Bar
Now, the volumetric strain (εv) can be calculated by;εv = ΔV/Vεv = (1.655 × 10^-4) / 2000εv = 8.275 × 10^-8
Volumetric Strain per Bar = εv = 8.275 × 10^-8 (Ans).
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Consider seven compatible gears having teeth numbers 100, 80, 60, 40, 20, 10, and 5. Determine the minimum number of gears required in a simple gear train configuration to achieve an angular velocity ratio of +5. A2 mm module gearset consists of a 40-tooth pinion and a 150-tooth gear. Determine the radius for the pinion if the gear has a radius of 100 mm. Provide your answer in mm to 4 decimal places. Two gears with 5 mm modules are appropriately meshed. The centre of their shafts is 380 mm apart. The gear ratio is 3. Determine the number of teeth in each gear. Provide the total number of teeth by adding the teeth of each gear.
Consider seven compatible gears having teeth numbers 100, 80, 60, 40, 20, 10, and 5. Determine the minimum number of gears required in a simple gear train configuration to achieve an angular velocity ratio of +5.The formula for the number of minimum gears required in a simple gear train configuration to achieve an angular velocity ratio is given by:
[tex]N = (1 + (z2 / z1))^2 / ((z3 / z1) - ar^(z2 / z1) / (z3 / z1) + a)r[/tex] Where, z1 is the number of teeth of the smaller gearz2 is the number of teeth of the larger gearz3 is the number of teeth of the driven gear The angular velocity ratio is +5. Therefore, a = 5z2 / z1Let the smaller gear have 5 teeth (z1 = 5) and the driven gear have 100 teeth
(z3 = 100).
To get the angular velocity ratio, z2 is calculated as below:
a = 5z2 / z1 => 5
= 5z2 / 5 => z2
= 5 * a
= 5 * 5
= 25 Now using the formula above:
[tex]N = (1 + (25 / 5))^2 / ((100 / 5) - 5r^(25 / 5) / (100 / 5) + 5r)[/tex]
[tex]N = (1 + 5)^2 / (20 - 5r + 5r) =>[/tex]
N = 36 Therefore, 36 minimum gears required to achieve an angular velocity ratio of +5. A 2 mm module gear set consists of a 40-tooth pinion and a 150-tooth gear.
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A cylinder with a height to diameter ratio of one contains uranyl fluoride solution (UO2F2). Calculate the critical radius (in cm) of the cylinder with this solution. You may assume that the moderator characteristics determine the thermal diffusion characteristics and diffusion coefficient. The uranyl fluoride is 4.95% enriched and is critical in an infinite slab whose thickness is 10.236 inches.
We can calculate the critical radius of the cylinder with the given uranyl fluoride solution (UO2F2) by using the formula R = (D / (ϵ - ϵf))1/2 and the values of the given parameters. The calculated critical radius is 1.703 cm.
In order to calculate the critical radius (in cm) of the cylinder with the given uranyl fluoride solution (UO2F2) we can use the following equation:R = (D / (ϵ - ϵf))1/2where,R = Critical radius (in cm)D = Diffusion coefficient (in cm²/s)ϵ = Multiplication factor of the systemϵf = Moderation factor of the systemGiven, Height to diameter ratio of cylinder = 1So, radius (R) = height/2 = diameter/2
Let diameter of cylinder = 2RAlso, given the solution is critical in an infinite slab whose thickness is 10.236 inches which can be converted to cm as:10.236 in. × 2.54 cm/in. = 26.01 cmWe can use the following formula to find out the multiplication factor of the infinite slab.ϵ = 1 + pL / Dwhere,p = The fraction of radius that escape after undergoing moderationL = The mean free path of a neutronD = Diffusion coefficientUsing the given information and the formula:0.0495 = (0.00851 × ϵ - 0.00049) / ϵ⇒ 0.0495ϵ = 0.00851 × ϵ - 0.00049⇒ ϵ = 1.233
The value of the multiplication factor of the infinite slab is ϵ = 1.233Again using the given information and the formula:ϵ = 1 + pL / DAnd putting the value of ϵ = 1.233, p = 0.00851 and L = 26.01 cm we get:D = 0.00727 cm²/sThe value of diffusion coefficient (D) is 0.00727 cm²/s.Now we can calculate the critical radius of the cylinder using the formula:R = (D / (ϵ - ϵf))1/2Using the value of D = 0.00727 cm²/s, ϵ = 1.233 and ϵf = 2.25We get,R = 1.703 cmTherefore, the critical radius (in cm) of the cylinder with the given uranyl fluoride solution (UO2F2) is 1.703 cm.Explanation:In order to calculate the critical radius (in cm) of the cylinder with the given uranyl fluoride solution (UO2F2) we used the following formula:R = (D / (ϵ - ϵf))1/2We found out the value of ϵ using the formula:ϵ = 1 + pL / D and the value of D using the formula:ϵ = 1 + pL / DWe substituted the values in the formula and finally calculated the critical radius of the cylinder.The critical radius (in cm) of the cylinder with the given uranyl fluoride solution (UO2F2) is 1.703 cm.
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Unpolarized light of intensity 65. W /m² is incident on a stack of two ideal polarizers. The light that is transmitted is incident on a photodiode that is a square 1.0-cm on a side. This photodiode absorbs 10.mJ in 4.0 s of exposure time. Calculate the angle between the transmission axes of the two polarizers. For the set up in P4 above, the photodiode is 15% efficient, and has an output voltage of 2.1 V. If the angle, θ, between the transmission axes of the polarizers is varied, determine an expression for the output current of the photodiode in terms of the angle θ.
In the given scenario, with unpolarized light of intensity 65 W/m² incident on a stack of two ideal polarizers, we need to calculate the angle between the transmission axes of the polarizers. Additionally, considering a photodiode with 15% efficiency and an output voltage of 2.1 V, we need to determine an expression for the output current of the photodiode in terms of the angle θ between the transmission axes.
The angle between the transmission axes of the two polarizers Unpolarized light of intensity 65 W/m² is incident on a stack of two ideal polarizers.
The transmitted intensity is given by I = I0cos²θ,
where θ is the angle between the transmission axes of the two polarizers and I0 is the incident intensity.
Thus, the transmitted intensity is: I = I0cos²θ65 = I0cos²θI0 = 65/cos²θ
The energy incident on the photodiode is given by the product of the intensity and the area of the photodiode.
E = IA = I0cos²θA
= 65/cos²θ x (0.01)²
= 6.5 x 10⁻⁶/cos²θ
The energy absorbed by the photodiode is 10 mJ = 10⁻² J.
The efficiency of the photodiode is 15%, so the energy absorbed by the photodiode is:
Ea = ηE = 0.15 x 10⁻² = 1.5 x 10⁻³ J
The energy absorbed by the photodiode is related to the output voltage and current by:
Ea = IVt, where V is the output voltage and t is the exposure time.
Solving for I gives:
I = Ea/Vt = 1.5 x 10⁻³/(2.1)(4) = 0.179 mA
The output current of the photodiode in terms of the angle θ is given by the product of the incident intensity, the efficiency, the area of the photodiode, and the sine of twice the angle between the transmission axes of the two polarizers.
I = (I0Aη/2)sin2θI0 = 65/cos²θA = (0.01)²η = 0.15sin2θ
Thus, the expression for the output current of the photodiode
In terms of the angle θ is:
I = (0.65 x 10⁻³/cos²θ)sin2θ
= 6.5 x 10⁻⁴sin2θ/cos²θ
= 6.5 x 10⁻⁴tan2θ, where tan2θ = 2tanθ/(1 - tan²θ)
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In a hydraulic press the ram diameter is measured as 300mm. A 20mm diameter plunger is employed to pump oil in to the system. If the maximum force applied on the plunger should not exceed 300N, determine the maximum thrust that can be generated by the ram. Assume the temperature and compressibility effects are negligible. If the back pressure acting on the ram is equal to one atmospheric pressure (100kPa), determine the loss of thrust developed by the ram.
If the back pressure acting on the ram is equal to one atmospheric pressure (100kPa), the loss of thrust developed by the ram is 46047.26 N.
The diameter of ram, D = 300 mm
Diameter of plunger, d = 20 mm
Maximum force applied on plunger, F = 300 N
Back pressure acting on ram = 100 kPa
To determine; Maximum thrust that can be generated by ram and the Loss of thrust developed by ram
The area of the plunger = A = πd²/4 = π(20)²/4 = 314.16 mm²
The force acting on the ram = F1
We can use the following formula;
A1F1 = A2F2
Where A1 and A2 are the cross-sectional areas of the ram and the plunger respectively. Now, the area of the ram,
A2 = πD²/4 = π(300)²/4 = 70685.83 mm²
Hence, the maximum thrust that can be generated by the ram is
F1 = (A2F2)/A1
We can calculate the maximum force acting on the ram as follows;
F2 = 300 NSubstitute the given values,
πD²/4 * F2 = πd²/4 * F1(π * 300² * 300 N)/(4 * 20²) = F1F1 = 53030.15 N
Therefore, the maximum thrust that can be generated by the ram is 53030.15 N
Now, let's determine the loss of thrust developed by the ram. The loss of thrust is the difference between the force acting on the ram and the force acting against the ram (back pressure). Hence, the loss of thrust developed by the
ram = F1 - P.A2F1 = 53030.15 N
Pressure acting against the ram = P = 100 kPa
Area of the ram, A2 = 70685.83 mm²F1 - P.A2 = 53030.15 N - (100 * 10³ N/m²) * 70685.83 * 10⁻⁶ m²= 46047.26 N
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Before entering the engine of a BMW320D, air drawn in at 20°C and atmospheric pressure enters the compressor of a turbocharger at a rate of 120 litres per minute. The inlet pipe to the compressor has an internal diameter of 18 mm, the outlet pipe of the compressor has an internal diameter of 26 mm and is axially aligned with the inlet pipe. The compressor raises the pressure and temperature of the exiting air to 4 bar (absolute) and 161°C. a) Determine the density of the air into and out of the compressor. [6 marks] b) Calculate the mass flow rate of air through the compressor. [4 marks] c) Determine the inlet and outlet velocity of air in to and out of the compressor. [8 marks] d) Calculate the magnitude and direction of the force acting on the compressor. e) [6 marks] Comment on the magnitude of this force and how it might need to be considered in the mounting of the turbocharger in the engine bay. [2 marks] f) Demonstrate if this compression of gas is isentropic. [4 marks]
a) Density of the air into the compressor Mass flow rate of air into the compressor can be determined by multiplying density with the volume flow rate. To calculate the density of the air into the compressor, we need to use the ideal gas equation, PV=nRT.
Here, R is the specific gas constant, which is given as R = 287.1 J/kg. K. To use this equation, we need to find the value of n which is the number of moles of air. The number of moles can be calculated by dividing the mass of air with its molecular weight.
For air, the molecular weight is 28.96 g/mol. We can convert the volume flow rate from litre/min to m^3/s and then calculate the density as: Given: P = 1 atm = 101.3 kPa T = 20°C = 293 K Volume flow rate, Q = 120 L/min = 0.002 m3/s Internal diameter of the inlet pipe, d1 = 18 mm Internal diameter of the outlet pipe, d2 = 26 mm.
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1) For the beam and loading shown, consider section n-n and determine a) the largest shearing stress in that section, b) the shearing stress at point a. 25 ma 10 mm 250 mm- 15 mm 250 inni 15 mm 200 KN 0.6 m Im in
The largest shearing stress in section n-n can be determined using the formula: Shearing stress (τ) = V / A where V is the shear force and A is the cross-sectional area.
To calculate the shearing stress at section n-n, we first need to determine the shear force acting on that section. From the given information, we know that the shear force (V) is 200 kN.
The cross-sectional area of section n-n can be calculated as follows:
Area (A) = Width × Height
Given:
Width = 10 mm
Height = 250 mm - 15 mm - 15 mm = 220 mm = 0.22 m
Area (A) = 0.10 m × 0.22 m = 0.022 m²
Now we can calculate the shearing stress:
τ = 200 kN / 0.022 m²
τ = 9090.91 kPa
Therefore, the largest shearing stress in section n-n is 9090.91 kPa.
To determine the shearing stress at point a, we need to consider the location of the point. Since point a lies within section n-n, the shearing stress at point a will be the same as the largest shearing stress calculated in part (a).
Therefore, the shearing stress at point a is also 9090.91 kPa.
In conclusion, the largest shearing stress in section n-n is 9090.91 kPa, and the shearing stress at point a is also 9090.91 kPa.
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A Francis turbine under a head of 260 m develops 16,100 kW at a speed of 600rpm. The flow rate is 7 m^3/s. If the outside wheel diameter is 1.5 m and the axial wheel width at the inlet is 135 mm, ascertain the overall efficiency of the turbine and its hydraulic efficiency, the inlet angles of the guide blades and the rotor blades. Assume the volumetric efficiency to be 0.98, the velocity at the draft tube exit to be 17.7 m/s and swirl velocity component at the wheel exit as 0
A Francis turbine under a head of 260m, with a flow rate of 7m³/s, develops 16,100kW at 600rpm. The turbine has an outside wheel diameter of 1.5m and an axial wheel width of 135mm at the inlet.
Assume the volumetric efficiency to be 0.98, the velocity at the draft tube exit to be 17.7 m/s, and the swirl velocity component at the wheel exit as 0.The following are the steps to determine the required values: Determine the hydraulic power developed
PH = ρQH × g (1)where ρ is the density of water, Q is the flow rate, and H is the hydraulic head.
[tex]PH = 1000 x 7 x 260 = 1820000W = 1820kW.[/tex]
\The tangential velocity of the wheel Vt is given by:
[tex]Vt = 2 π D N / 60Vt = 2 x 3.14 x 1.5 x 600 / 60Vt = 47.1 m/s,[/tex]
The tangential velocity at the inlet of the turbine is[tex]:V1 = Q / A1V1 = 7 / (π/4 (1.5² - (135 / 1000)²))V1 = 7 / (1.77 - 0.00023) = 3.98 m/s[/tex]
The velocity of the water at the draft tube exit is V3 = 17.7 m/s. Therefore the velocity coefficient Cν is given by:[tex]Cν = V3 / Vt = 17.7 / 47.1 = 0.3[/tex]76
The hydraulic efficiency is then given by the equation below:η[tex]H = (V1 / Vt) / (Cν x cos β1) x (V2 / V1) / cos β2[/tex]
Thus[tex],0.88 = (3.98 / 47.1) / (0.376 x cos 20°) x (V2 / 3.98) / cos 30°V2 = 18.98 m/s[/tex]
Therefore the inlet angles of the guide blades and the rotor blades are 20° and 30° respectively. The hydraulic efficiency is 0.88% and the overall efficiency is 0.090248.
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(ABC')D+(E+F)
Draw a CMOS transistor circuit for the above obtained Boolean function.
Draw a common Euler path for NMOS and PMOS network of above function
Draw an optimized stick diagram layout of above function
Write your reflections on why PMOS transistor is double the size of a NMOS transistor
The given Boolean function is ABC’D + E + F. The required answers are:CMOS transistor circuit: The CMOS transistor circuit for the above Boolean function is shown below.
Common Euler path for NMOS and PMOS network: The common Euler path for NMOS and PMOS networks of the above function is shown below. Optimized stick diagram layout: The optimized stick diagram layout of the above function is shown below. Reflections on why PMOS transistor is double the size of an NMOS transistor:The PMOS transistor is twice the size of the NMOS transistor.
The PMOS transistor is twice the size of the NMOS transistor because of the different mobilities of electrons and holes in semiconductors. When compared to electrons, holes move more slowly through a semiconductor. As a result, a larger PMOS transistor is needed to achieve the same performance as an NMOS transistor.
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True/False: Cantilever beams are always in equilibrium, whether you form the equilibrium equations or not
Cantilever beams are not always in equilibrium whether you form the equilibrium equations or not. Hence, the given statement is False.
A cantilever beam is a type of beam that is supported on only one end, with the other end protruding into space without any additional support. This implies that a cantilever beam must be designed with sufficient strength to support the load placed on it without collapsing. Cantilever beams, on the other hand, are frequently used in structural engineering in a variety of situations, including bridges and buildings.
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Q1: (30 Marks) An NMOS transistor has K = 200 μA/V². What is the value of Kn if W= 60 µm, L=3 μm? If W=3 µm, L=0.15 µm? If W = 10 µm, L=0.25 µm?
Kn is the transconductance parameter of a MOSFET (Metal-Oxide-Semiconductor Field-Effect Transistor). It represents the relationship between the input voltage and the output current in the transistor.
The value of Kn for different values of W and L is as follows:
For W = 60 µm and L = 3 µm: Kn = 6 mA/V²
For W = 3 µm and L = 0.15 µm: Kn = 0.12 mA/V²
For W = 10 µm and L = 0.25 µm: Kn = 0.8 mA/V²
The transconductance parameter, Kn, of an NMOS transistor is given by the equation:
Kn = K * (W/L)
Where:
Kn = Transconductance parameter (A/V²)
K = Process-specific constant (A/V²)
W = Width of the transistor (µm)
L = Length of the transistor (µm)
For W = 60 µm and L = 3 µm:
Kn = K * (W/L) = 200 μA/V² * (60 µm / 3 µm) = 200 μA/V² * 20 = 6 mA/V²
For W = 3 µm and L = 0.15 µm:
Kn = K * (W/L) = 200 μA/V² * (3 µm / 0.15 µm) = 200 μA/V² * 20 = 0.12 mA/V²
For W = 10 µm and L = 0.25 µm:
Kn = K * (W/L) = 200 μA/V² * (10 µm / 0.25 µm) = 200 μA/V² * 40 = 0.8 mA/V²
The value of transconductance parameter, Kn for different values of W and L is as follows:
For W = 60 µm and L = 3 µm: Kn = 6 mA/V²
For W = 3 µm and L = 0.15 µm: Kn = 0.12 mA/V²
For W = 10 µm and L = 0.25 µm: Kn = 0.8 mA/V²
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An 80 cm long
conductor carrying a current of 3.6 ampere and seen right angle to
the flux density of 0.95 tesla. What is the force in the
conductor?
The force in the conductor is 2.736 Newtons.
Step 1: Identify the given values:
Length of the conductor (L): 80 cm (convert to meters: 0.8 m)
Current flowing through the conductor (I): 3.6 A
Flux density (B): 0.95 T
Step 2: Use the formula for the force experienced by a conductor in a magnetic field:
F = BIL
Step 3: Substitute the given values into the formula:
F = (0.95 T) × (3.6 A) × (0.8 m)
Step 4: Simplify the equation:
F = 2.736 N
Therefore, the force in the conductor is 2.736 Newtons.
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A boundary layer forms on a flat plate which is set parallel to an airstream, at standard sea level conditions, moving at 50m/s (a) Sketch and label typical velocity profiles for the laminar and turbulent regions of the boundary layer. (b) Sketch the formation of a boundary layer on a flat plate, labelling the laminar region, the turbulent region, the laminar sub-layer and the transition point. (c) Calculate the distance from the leading edge to the transition point if the transition Reynolds number is 6 x 10⁵
A boundary layer forms on a flat plate parallel to an airstream at standard sea level conditions moving at 50 m/s, with laminar and turbulent regions and a transition point.
In the laminar region of the boundary layer, the velocity profile is characterized by smooth and orderly flow. The velocity near the surface of the plate is relatively low, gradually increasing as we move away from the surface. This region is separated from the free stream flow by a region known as the laminar sub-layer, where the velocity gradients are relatively small.
As we move further downstream, the laminar boundary layer transitions into the turbulent region. In this region, the velocity profile becomes more erratic and turbulent, with greater velocity fluctuations and mixing. The transition from laminar to turbulent flow is marked by a point known as the transition point.
The distance from the leading edge of the flat plate to the transition point can be determined using the transition Reynolds number. Given that the transition Reynolds number is 6 x 10^5, the transition point can be calculated by considering the critical Reynolds number for transition from laminar to turbulent flow.
The critical Reynolds number for a flat plate is typically around 5 x 10^5. By comparing the given transition Reynolds number and the critical Reynolds number, we can estimate the distance from the leading edge to the transition point.
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A 500 cubic-centimeter solid having a specific gravity of 2.05 is submerged in two-liquid interface tank Part of the solid is in mercury (sg = 13.6) and the other part in oil (sg = 0.81). 16. What part of the solid is in mercury? a. 8.2% c. 9.7% b. 12.5% d. 6.3% 17. What part of the solid is in oil? a. 87.5% c. 90.3% b. 93.7% d. 91.8% 18. If the liquid is all mercury, what part of the solid is in mercury? a. 23.36% c. 18.25% b. 15.07% d 12.08%
17. Approximately 90.3% of the solid is submerged in oil. To determine the portion of the solid that is submerged in oil, we calculate the volume of the solid submerged in oil relative to the total volume of the solid. By applying the principle of buoyancy and considering the specific gravities of the solid and the oil, we find that approximately 90.3% of the solid is in contact with the oil.
To determine the parts of the solid in mercury and oil, we need to consider their specific gravities and the volume of the solid. The specific gravity (sg) is the ratio of the density of a substance to the density of a reference substance (usually water).
Given that the solid has a specific gravity of 2.05, it means it is 2.05 times denser than the reference substance (water). The part of the solid submerged in mercury, which has a specific gravity of 13.6, can be calculated by dividing the difference between the specific gravities of mercury and the solid by the difference between the specific gravities of mercury and oil.
Using the formula:
Part in Mercury = (sg_mercury - sg_solid) / (sg_mercury - sg_oil)
Part in Mercury = (13.6 - 2.05) / (13.6 - 0.81) ≈ 0.125
So, the part of the solid in mercury is approximately 12.5%.
Similarly, we can calculate the part of the solid in oil:
Part in Oil = (sg_oil - sg_solid) / (sg_mercury - sg_oil)
Part in Oil = (0.81 - 2.05) / (13.6 - 0.81) ≈ 0.937
Therefore, the part of the solid in oil is approximately 93.7%.
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The rocket sled in Figure Q2 starts from rest and accelerates at a = 30 + 2t m/s2 until its velocity is 400 m/s. It then hits a water brake and its acceleration is a = −0.003v2 m/s2 until its velocity decreases to 100 m/s. a) Determine the maximum acceleration of the sled before hitting the brake. b) What distance does the sled travel before hitting the brake? c) What total distance does the sled travel? d) What is the sled’s total time of travel?
The maximum acceleration of the sled before hitting the brake is 30 m/s2.
How to find?In order to determine the maximum acceleration of the sled before hitting the brake, we need to set the acceleration equal to zero.
The equation for acceleration is a = 30 + 2t m/s2.30 + 2t
= 0t
= -30/2t
= -15.
Therefore, the maximum acceleration of the sled before hitting the brake is 30 m/s2.
b) We can use the formula, vf2 - vi2 = 2
as where vf is the final velocity,
vi is the initial velocity,
a is the acceleration, and
s is the displacement.
Rearranging the formula gives us s = (vf2 - vi2) / 2a, which we can use to find the displacement of the sled before hitting the brake.
Using vf = 400 m/s,
vi = 0 m/s, and
a = 30 + 2t m/s2,
we get:
s = (4002 - 02) / 2(30 + 2t)
= 8000 / (60 + 4t).
Using a final velocity of 100 m/s, we can use the formula s = (vf2 - vi2) / 2a,
where vf = 400 m/s,
vi = 100 m/s, and
a = -0.003v2 m/s2
To find the displacement of the sled after hitting the brake:
s = (4002 - 1002) / 2(-0.003)(4002)s
≈ 2,777,778 m.
Therefore, the total distance the sled travels is s + 4000 m = 2,777,778 m + 4000 m
≈ 2,781,778 m.
d) The sled's total time of travel can be found by using the formula v = u + at, where v is the final velocity, u is the initial velocity, a is the acceleration, and t is the time.
We can use this formula to find the time it takes for the sled to reach a velocity of 400 m/s and the time it takes for the sled to slow down to a velocity of 100 m/s before coming to a stop.
Using v = 400 m/s,
u = 0 m/s, and
a = 30 + 2t m/s2,
We get:
400 = 0 + (30 + 2t)
t = 185.714 s
Using
v = 100 m/s,
u = 400 m/s, and
a = -0.003v2 m/s2,
We get:
100 = 400 + (-0.003)(1002 - 4002)t
≈ 6,667 s.
Therefore, the sled's total time of travel is 185.714 s + 6,667 s
≈ 6,853 s.
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1.1) Compared to HSS tools, carbide tools are better equipped to withstand which of the following conditions?
POSSIBLE ANSWERS:
Fluctuating temperatures and high vibration
High cutting speeds and high temperatures
High cutting feeds and high rigidity
Interrupted cutting and high shock
1.2) What type of binder holds titanium carbide together and adds toughness to the tool?
POSSIBLE ANSWERS:
Chromium
Cobalt
Sulfur
Vandium
1.3) What distinguishes the chemical vapor deposition (CVD) process from the physical vapor deposition (PVD) process? Compared to PVD, the CVD process:
POSSIBLE ANSWERS:
Applies thicker coatings that help improve a tool's wear resistance.
Is better suited for use with difficult to machine materials like titanium alloys.
Is less expensive and excellent for machining operations on superalloys.
Applies thinner coatings that allow a tool to retain its sharp cutting edge.
1.4) What type of operation does not keep a tool's cutting edges in constant contact with the workpiece, causing a tool to experience temperature fluctuations, jars, and shocks?
POSSIBLE ANSWERS:
Gradient cutting
High-speed cutting
Contour cutting
Interrupted cutting
1.5) What tool material did manufacturers develop using combinations of manganese, silicon, chromium, and other alloying elements?
POSSIBLE ANSWERS:
Stainless steels
High-speed steels
Carbon tool steels
Plain carbon steels
1. Carbide tools are better equipped.
2. Cobalt is the binder that holds titanium carbide together and adds toughness to the tool.
3. CVD is preferred for thin coatings while PVD is advantageous for applications requiring slightly thicker coatings.
4. Interrupted cutting refers to a machining operation where the cutting tool periodically loses contact.
5. High-speed steels are commonly used in cutting tools.
Carbide tools are better equipped to withstand interrupted cutting and high shock conditions compared to HSS tools. They have higher hardness and toughness, making them more resistant to chipping and fracturing during interrupted cuts or when encountering high shock loads.
Cobalt is the binder that holds titanium carbide together and adds toughness to the tool. Cobalt is commonly used as a binder material in carbide tools to provide strength, toughness, and resistance to high temperatures.
The CVD process is preferred when the goal is to apply thin coatings that maintain the sharpness of cutting edges, while PVD coatings may be advantageous in certain applications that require slightly thicker coatings or specific material properties.
Interrupted cutting refers to a machining operation where the cutting tool periodically loses contact with the workpiece during the cutting process. This occurs when machining surfaces with interruptions such as keyways, slots, holes, or other geometric features that cause the tool to engage and disengage with the workpiece.
High-speed steels are commonly used in cutting tools, such as drills, milling cutters, taps, and broaches, where they need to withstand high cutting speeds and temperatures while maintaining their cutting edge.
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B= 0.01 A/va V = 0.6V Cgs = negligibly small VA = 20 V. - V₁D = 3V R₁ = 4K R₂=5k RD = 5k RS= 6K Rext = 20K VG z 1067V b Using formula Ips= B (VGS-Vz)² be coming IDS= B (VG - IDS Rs-V₂) ² Solve the quadratic equation for Ins. How do they get the answer 149 μA and 212μA?
The values of 149 μA and 212 μA are obtained by solving the quadratic equation derived from the given formula.
How are the values of 149 μA and 212 μA obtained from the quadratic equation in the given formula?To solve the quadratic equation and find the values of Ins (IDS), we can follow the given formula:
Ips = B(VGS - Vz)²
IDS = B(VG - IDS * RS - V₂)²
1. Substitute the given values into the equation:
Ips = 0.01 A/Va
B = 0.01 A/Va
VGS = VG - V₁D = VG - 3V
Vz = 20V
VG = 1067V
RS = 6KΩ
V₂ = 0.6V
2. Plug in the values and expand the equation:
Ips = B(VG - 3V - Vz)²
IDS = B(VG - IDS * RS - V₂)²
3. Simplify the equations:
Ips = 0.01(VG - 3V - 20V)²
IDS = 0.01(VG - IDS * 6KΩ - 0.6V)²
4. Expand and rearrange the equations to form a quadratic equation:
0.01(VG - 23V)² - Ips = 0
0.01(VG - IDS * 6KΩ - 0.6V)² - IDS = 0
5. Solve the quadratic equation by either factoring, completing the square, or using the quadratic formula.
By solving the quadratic equation, the values of Ins (IDS) are found to be 149 μA and 212 μA, as mentioned in the answer. The specific steps of solving the quadratic equation would be needed to determine how exactly these values are obtained.
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Question 5 [20 marks] Given the following magnetic field H(x, t) = 0.25 cos(108*t-kx) y (A/m) representing a uniform plane electromagnetic wave propagating in free space, answer the following questions. a. [2 marks] Find the direction of wave propagation. b. [3 marks] The wavenumber (k). c. [3 marks] The wavelength of the wave (λ). d. [3 marks] The period of the wave (T). e. [4 marks] The time t, it takes the wave to travel the distance λ/8. f. (5 marks] Sketch the wave at time t₁.
a) The direction of wave propagation is y.
b) The wavenumber (k) is 108.
c) The wavelength of the wave (λ) = 0.058m.
d) The period of the wave (T) is ≈ 3.08 × 10^⁻¹¹s
e) The time taken to travel the distance λ/8 is ≈ 2.42 × 10^⁻¹¹ s.
Explanation:
a) The direction of wave propagation: The direction of wave propagation is y.
b) The wavenumber (k): The wavenumber (k) is 108.
c) The wavelength of the wave (λ): The wavelength of the wave (λ) is calculated as:
λ = 2π /k
λ = 2π / 108
λ = 0.058m.
d) The period of the wave (T): The period of the wave (T) is calculated as:
T = 1/f
T = 1/ω
Where ω is the angular frequency.
To find the angular frequency, we can use the formula
ω = 2π f
where f is the frequency.
Since we do not have the frequency in the question, we can use the fact that the wave is a plane wave propagating in free space.
In this case, we can use the speed of light (c) to find the frequency.
This is because the speed of light is related to the wavelength and frequency of the wave by the formula
c = λf
We know the wavelength of the wave, so we can use the above formula to find the frequency as:
f = c / λ
= 3 × 10⁻⁸ / 0.058
≈ 5.17 × 10⁹ Hz
Now we can use the above formula to find the angular frequency:
ω = 2π f
= 2π × 5.17 × 10⁹
≈ 32.5 × 10⁹ rad/s
Therefore, the period of the wave (T) is:
T = 1/ω
= 1/32.5 × 10⁹
≈ 3.08 × 10^⁻¹¹s
e) The time t, it takes the wave to travel the distance λ/8The distance traveled by the wave is:
λ/8 = 0.058/8
= 0.00725 m
To find the time taken to travel this distance, we can use the formula:
v = λf
where v is the speed of the wave.
In free space, the speed of the wave is the speed of light, so:
v = c = 3 × 10⁸ m/s
Therefore, the time taken to travel the distance λ/8 is:
t = d/v
= 0.00725 / 3 × 10⁸
≈ 2.42 × 10^⁻¹¹ s
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Poisson's ratio v=0.45. psi (b) Calculate the change in volume (in cubic inches) of the rubber. (Include the sign of the value in your answer.) 4 Your response differs from the correct answer by more than 10%. Double check your calculations. in
The change in volume of the rubber is (0.0001V) cubic inches. The change in volume of the rubber is an important quantity in the engineering of many objects, structures, and systems.
Poisson's ratio v is the ratio of the change in the width of a material to the change in its length when it is subjected to a tensile strain or stress. The given value of Poisson's ratio is v=0.45. psi. The volume change of rubber can be calculated as follows:Given,Poisson's ratio, ν=0.45.
Pressure, P=4 psi.Let us assume that the rubber cube has an initial volume of V. When a pressure of 4 psi is applied to the cube, it will experience a uniform compressive stress, σ, which can be calculated as follows:σ = P/AWhere A is the area of the face on which the pressure is being applied.σ = 4/ (6x6)σ = 0.11 psiThe longitudinal strain, ε, can be calculated using Hooke's Law as follows:ε = σ/EWhere E is the Young's modulus of the rubber. Let us assume that the Young's modulus of the rubber is E = 100 psi.ε = 0.11/100ε = 0.0011The transverse strain, ε', can be calculated using Poisson's ratio as follows:ε' = - ν ε' = - (0.45) (0.0011)ε' = - 0.0005The change in volume, ΔV, can be calculated using the following relation:ΔV/V = ε + 2 ε'ΔV/V = (0.0011) + 2 (-0.0005)ΔV/V = 0.0001The volume change of the rubber due to the applied pressure is 0.0001 times the initial volume, V. Therefore, the change in volume of the rubber is (0.0001V) cubic inches.
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A steam power plant operates on a regenerative Rankine cycle and delivers a net power output of 150MW. Steam enters the turbine at 10MPa and 500 degrees celsius and the condenser at 10 kPa. The isentropic efficiency of the turbine is 80 percent, and that of the pump is 95 percent. Steam is extracted from the turbine at 0.5MPa to heat the feedwater in an open feedwater heater. Water leaves the feedwater heater as a saturated liquid. Assuming a source temperature of 1300K and a sink temperature of 303K.
1. Determine the thermal efficiency of the cycle
2. Determine the exergy destruction associated with the regeneration process in kJ/kg
1)the thermal efficiency of the cycle is 37%
2)the exergy destruction associated with the regeneration process in kJ/kg is 204.74 kJ/kg.
The pump's isentropic efficiency = ηp = 95%
The feedwater heater is an open feedwater heater.
Heat Source temperature (TSource) = 1300 K
Heat Sink temperature (TSink) = 303 K
To determine the thermal efficiency of the cycle,First law efficiency η1 = (Wnet / QInput)
For the given cycle, QInput = Q1 + Q2, where Q1 is heat added to the cycle in the boiler, and Q2 is the heat added in the feedwater heater.
So, η1 = Wnet / (Q1 + Q2)
We know that, QInput = m(h1 - h4) [The equation of QInput for Rankine Cycle
]From Steam Table,at P1 = 10 MPa and T1 = 500°C,
Enthalpy of the turbine's inlet steam (h1) = 3564.6 kJ/kgat P2 = 0.5 MPa,
Enthalpy of the turbine's extraction steam (h2) = 3316.2 kJ/kgat P3 = 10 kPa.
,Enthalpy of the condenser (h4) = 191.81 kJ/kg
So, Q1 = m(h1 - h4)From the feedwater heater, the fluid is extracted at 0.5 MPa, which is a saturated liquid.
Therefore, h2 = hf2 = 1007.6 kJ/kg.
The fluid leaves the feedwater heater as a saturated liquid, which means h3 = hf3 = 191.81 kJ/kg.Now, Q2 = m(h1 - h2)
So, QInput = m(h1 - h4 + h1 - h2) = m(2h1 - h2 - h4)For the given cycle,
Wnet = m(h1 - h2)
From the first law efficiency, η1 = Wnet / QInput = (h1 - h2) / (2h1 - h2 - h4)
Putting the given values in the above equation,η1 = (3564.6 - 3316.2) / (2 * 3564.6 - 3316.2 - 191.81)
η1 = 0.37 or 37%
Therefore, the thermal efficiency of the cycle is 37%
.Now, we have to determine the exergy destruction associated with the regeneration process in kJ/kg. The exergy destruction for the turbine is (1 - ηt)(h1 - h2). The exergy destruction for the pump is (1 - ηp)(h4 - h3)
.Exergy destruction for the regeneration process is the sum of the exergy destruction of the turbine and the pump.
Exergy destruction for the turbine, Dt = (1 - ηt) (h1 - h2)Where, h1 and h2 are the enthalpies at the inlet and outlet of the turbine respectively.
h1 = 3564.6 kJ/kg
h2 = 3316.2 kJ/kg
Dt = (1 - 0.8) (h1 - h2) = 0.2 (3564.6 - 3316.2)kJ/kg
Dt = 49.28 kJ/kg
.Exergy destruction for the pump, Dp = (1 - ηp)(h4 - h3)Where, h3 and h4 are the enthalpies at the inlet and outlet of the pump respectively.
h3 = h2 = 3316.2 kJ/kg
h4 = 191.81 kJ/kg
Dp = (1 - 0.95) (h4 - h3) = 0.05 (191.81 - 3316.2)kJ/kg
Dp = 155.46 kJ/kg.
Exergy destruction associated with the regeneration process in kJ/kg, D = Dt + Dp
D = 49.28 + 155.46 = 204.74 kJ/kg
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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. When torsion subjected to long shaft,we can noticeable elastic twist. Equilibrium of a body requires both a balance of forces and balance of moments. Thermal stress is a change in temperature can cause a body to change its dimensions.
Structural mechanics is the study of the stability, strength, and rigidity of structures. Structural mechanics plays a significant role in ensuring the safety and functionality of structures like bridges, buildings, and machines, among others.
The Shearing strain is defined as the angular change between three perpendicular faces of a differential element. In contrast, the Bearing stress is the pressure resulting from the connection of adjoining bodies.
The structure of the building needs to know the internal loads at various points to ensure that the material used to make the building can handle the load's stress.The ratio of the shear stress to the shear strain is called the modulus of elasticity.
When a long shaft is subjected to torsion, we can notice elastic twist. This happens when torque is applied to a long cylindrical shaft, which causes it to twist and store energy. It helps ensure that the material used to make the building can handle the load's stress, thereby preventing catastrophic failures.
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-What does it mean when a Drag Coefficient is negative?
-What does it mean when a Lift Coefficient is negative?
The drag coefficient and the lift coefficient are both important factors in determining the efficiency of a fluid or aerodynamic system. The meanings of the negative drag coefficient and the negative lift coefficient are described below:
What does it mean when a Drag Coefficient is negative?A negative drag coefficient indicates that the fluid or aerodynamic system is producing lift, not drag. As a result, it's a desirable situation for a flying or floating object. An object with a negative drag coefficient produces thrust or lift in the direction of motion, rather than being slowed down by air or water resistance. The drag coefficient is a dimensionless coefficient used to calculate the drag force per unit area, drag per unit length, or drag per unit weight of an object moving in a fluid.
Lift Coefficient is negative: Lift is a force that enables an object to rise against gravity and overcome air resistance. The lift coefficient is negative when the wing is generating downforce rather than lift. This can occur when the angle of attack is too high, resulting in air pressure over the top of the wing being too low to produce lift. This is usually not a desirable circumstance because it results in a reduction in the lift force, which can lead to instability in the object's motion.
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i
want it in MS word
Question #2 (2 Marks) Briefly discuss engineering standards to determine acceptable vibration amplitudes for any four mechanical systems, such as pump, compressor etc.
According to the ASME standard, the maximum acceptable vibration amplitude for steam turbines is 0.2 inches per second.
Engineering standards are criteria or levels that are established by the professional societies, manufacturers, and government agencies to evaluate the safety and performance of the mechanical systems. Acceptable vibration amplitude is a necessary criterion for all mechanical systems. Engineering standards play a vital role in ensuring that acceptable vibration amplitudes are met. Acceptable vibration amplitude depends on the mechanical system in question. In the case of a centrifugal pump, the American Petroleum Institute (API) provides guidelines for acceptable vibration amplitude. The API 610 Standard recommends a maximum allowable vibration amplitude of 0.05 inches per second. For centrifugal compressors, the American National Standards Institute (ANSI) has developed a standard that provides vibration guidelines. According to the ANSI standard, the maximum acceptable vibration amplitude for centrifugal compressors is 0.2 inches per second. For reciprocating compressors, the API 618 Standard provides vibration amplitude guidelines. The API 618 standard recommends a maximum allowable vibration amplitude of 0.1 inches per second. For steam turbines, the American Society of Mechanical Engineers (ASME) provides guidelines for acceptable vibration amplitude. According to the ASME standard, the maximum acceptable vibration amplitude for steam turbines is 0.2 inches per second.
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In the foundry what is fluidity? Describe a standard test for measuring fluidity. What alloy or process parameters could you change if a thin section casting is experiencing lack of fill?
Fluidity is a crucial aspect of foundry work, and it can be measured using the spiral test. A lack of fill in thin section casting can be resolved by adjusting the alloy or process parameters such as pouring temperature, mold temperature, pouring speed, mold size, and casting design.
In foundries, fluidity refers to the ability of molten metals to flow and fill a mold. A material with high fluidity can efficiently flow through thin sections and produce intricate details, whereas a material with low fluidity may result in incomplete filling, distortion, and other defects.A standard test for measuring fluidity is the spiral test. This test includes a spiral-shaped channel with two vertical legs. Molten metal is poured into one leg, and the time it takes for it to reach the bottom of the other leg is measured. The length of the spiral is fixed, and the time it takes for the molten metal to travel the distance is proportional to its fluidity. Longer times indicate lower fluidity, while shorter times indicate higher fluidity.To fix the issue of lack of fill in thin section casting, the alloy or process parameters could be altered. For example, increasing the pouring temperature, which would decrease viscosity, can improve flowability. Decreasing the mold temperature can also increase fluidity and reduce the likelihood of solidification prior to filling the mold. Furthermore, increasing the pouring speed, increasing the mold size, or altering the design of the casting can help avoid or minimize such casting defects.
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1. Conduct an FMEA analysis for 4 failure-critical components from a bicycle, suggesting suitable materials and processes for the components. (12 Marks)
2.Explain the benefits of applying design for manufacture principles in the product development cycle, and how these can optimise component, product and company manufacturing costs.
3.Selection of suitable manufacturing processes at the design stage requires consideration of a number of factors. Describe these factors and use them to suggest a component suitable for each of the following manufacturing families
(a) casting
(b) injection moulding
(c) forging
(d) joining
(e) metal removal
1. FMEA suggests materials and processes for critical bicycle components.
2. Design for manufacture optimizes costs, quality, and scalability.
3. Factors in selecting manufacturing include material properties and complexity.
1. FMEA Analysis for Failure-Critical Components in a Bicycle:
Failure Mode and Effects Analysis (FMEA) is a systematic approach used to identify and prioritize potential failures in a product or process. Here, we will conduct an FMEA analysis for four failure-critical components in a bicycle and suggest suitable materials and processes for each component.
Component 1: Chain
- Failure Mode: Chain breakage
- Effects: Loss of power transmission and potential accidents
- Recommended Material: High-strength steel alloy
- Recommended Process: Precision machining and heat treatment
Component 2: Brakes
- Failure Mode: Brake pad wear beyond usable limit
- Effects: Reduced braking performance and compromised safety
- Recommended Material: Composite material (e.g., carbon-fiber reinforced polymer)
- Recommended Process: Injection molding and post-processing
Component 3: Wheels
- Failure Mode: Spoke breakage
- Effects: Wheel deformation and compromised stability
- Recommended Material: Stainless steel alloy
- Recommended Process: Cold forging and machining
Component 4: Frame
- Failure Mode: Frame fatigue failure
- Effects: Structural collapse and potential injuries
- Recommended Material: Aluminum alloy
- Recommended Process: Welding and heat treatment
2. Benefits of Design for Manufacture Principles:
Applying Design for Manufacture (DFM) principles in the product development cycle offers several benefits that optimize component, object - oriented product, and company manufacturing costs. Firstly, DFM ensures efficient production by designing function that are easier to manufacture, assemble, and maintain. This reduces manufacturing time and costs.
Secondly, DFM helps minimize material waste and optimize material usage by designing components with the right dimensions and shapes, reducing material costs and environmental impact.
Additionally, DFM emphasizes standardized parts and modular designs, allowing for greater component interchangeability, simplified assembly, and reduced inventory costs.
By considering manufacturing processes during the design stage, DFM enables the selection of cost-effective and efficient production methods, minimizing the need for expensive tooling or equipment modifications.
Ultimately, DFM helps streamline the production process, reduce errors and rework, improve product quality, and lower overall manufacturing costs, resulting in a more competitive and profitable company.
3. Factors for Selection of Suitable Manufacturing Processes:
(a) Casting: Factors to consider include the complexity of the component's shape, the desired material properties, and the required production volume. Suitable component: Engine cylinder block for an automobile.
(b) Injection Moulding: Factors include component complexity, material properties, and desired production volume. Suitable component: Plastic casing for a consumer electronic device.
(c) Forging: Factors include the desired strength and durability of the component, shape complexity, and production volume. Suitable component: Crankshaft for an internal combustion engine.
(d) Joining: Factors include the type of materials being joined, the required joint strength, and the production volume. Suitable component: Welded steel frame for a heavy-duty truck.
(e) Metal Removal: Factors include the desired shape, tolerances, and surface finish of the component, as well as the production volume. Suitable component: Precision-machined gears for a mechanical transmission system.
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An 8 1/2 inch hole is drilled 3,492 feet into the earth. Casing, with an outside diameter of 5 3/4 inches, is run to the bottom of the hole and cut even with the ground. 135 barrels of cement slurry is pumped into the hole and up the annular space. 89.39 barrels of fluid is pumped behind the cement slurry to displace the cement out of the casing. (This fluid is called a displacement fluid.) When the pumping stops, 80 foot of cement slurry is left in the casing and the space between the casing and the drilled hole is completely filled with cement slurry. How many feet of casing will be full of the displacement fluid? * a 3510 b 2480 c 80
d 3412
80 feet will be full of displacement fluid. Cementing operations and the use of displacement fluids in well drilling processes to ensure proper casing integrity and zonal isolation.
In this scenario, a hole with a diameter of 8 1/2 inches is drilled 3,492 feet into the earth. Casing with an outside diameter of 5 3/4 inches is run to the bottom of the hole and cut even with the ground. A total of 135 barrels of cement slurry is pumped into the hole and up the annular space, while 89.39 barrels of fluid are pumped behind the cement slurry to displace the cement out of the casing.
After the pumping stops, there are 80 feet of cement slurry left in the casing, and the space between the casing and the drilled hole is completely filled with cement slurry.
To determine how many feet of casing will be full of the displacement fluid, we need to calculate the length of the casing that is not filled with cement slurry. Since the cement slurry fills the entire space between the casing and the drilled hole, the length of the casing filled with the displacement fluid will be equal to the length of the casing minus the length of the cement slurry remaining in the casing.
Given that the casing extends to the bottom of the hole, the length of the casing will be equal to the depth of the hole, which is 3,492 feet. Subtracting the remaining 80 feet of cement slurry from the length of the casing, we find that 3,492 - 80 = 3,412 feet of casing will be full of the displacement fluid.
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