The magnitude of the Schmid factor "cos ϕ cos λ" for an FCC single crystal oriented with its [100] direction parallel to the loading axis is 0.5.
The Schmid factor is a measure of the crystallographic slip system's favorability for deformation in a specific crystal orientation. In an FCC (face-centered cubic) crystal, there are multiple slip systems available, and the [100] direction is one of the potential crystallographic planes for deformation.
To determine the magnitude of the Schmid factor, we need to consider the angle between the slip plane and the loading axis. In this case, with the [100] direction parallel to the loading axis, the angle between the slip plane and the loading axis is 45 degrees. The cosine of this angle is 0.7071.
Additionally, we need to consider the angle between the slip direction and the slip plane. For the [100] direction in an FCC crystal, the angle between the slip direction and the slip plane is also 45 degrees. The cosine of this angle is also 0.7071.
To calculate the Schmid factor, we multiply the cosines of these two angles: cos ϕ cos λ = 0.7071 × 0.7071 = 0.5.Therefore, the magnitude of the Schmid factor "cos ϕ cos λ" for an FCC single crystal oriented with its [100] direction parallel to the loading axis is 0.5.
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One A solid cube is placed in a refrigeration unit with an ambient internal temperature of 3°C using the data shown below, formulate a differential equation to describe the thermal behaviour of this system. Use this equation to determine the time taken for the body to cool from an initial temperature of 90 °C to 7 °C. Dimensions of cube = 0.2m x0.2m x 0.2m -1 h = Convective heat transfer coefficient 10 Wm ²K-¹ p = density of solid = 30 kgm-³ -3 C= specific heat capacity of solid = 0.41 KJkg-¹K-¹ [Total 25 marks]
The differential equation describing the thermal behavior of the system is dT/dt = (0.16/0.246) * (T(t) - 3), where T(t) represents the temperature of the cube at time t.
To derive the differential equation, we consider the rate of change of temperature of the cube with respect to time. The rate of heat transfer from the cube is given by hA(T(t) - 3), where h is the convective heat transfer coefficient and A is the surface area of the cube. The rate of change of temperature is proportional to the rate of heat transfer, so we have dT/dt = k(T(t) - 3), where k = hA/ (pC). Solving this first-order linear differential equation gives us T(t) = 7 + (90 - 7) * exp(-kt). Substituting the given values, we can solve for the time it takes for the temperature to cool from 90 °C to 7 °C.
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A 0.22 m thick large flat plate electric bus-bar generates heat uniformly at a rate of 0.4 MW/m³ due to current flow. The bus-bar is well insulated on the back and the front is exposed to the surroundings at 85°C. The thermal conductivity of the bus-bar material is 40 W/m.K and the heat transfer coefficient between the bar and the surroundings is 450 W/m².K. Calculate the maximum temperature in the bus-bar.
The maximum temperature in the bus-bar is 1020 °C.
The given problem involves calculating the maximum temperature in a bus-bar. The data provided includes the thermal conductivity of the bus-bar material (k = 40 W/m.K), heat transfer coefficient between the bar and surroundings (h = 450 W/m².K), thickness of the bus-bar (δ = 0.22 m), rate of heat generation (q'' = 0.4 MW/m³), and the front surface temperature of the bus-bar (T∞ = 85 °C).
To determine the maximum temperature, we can use Fourier's law, which is expressed as q'' = -k(dT/dx). For one-dimensional heat transfer, the equation can be simplified as q'' = -k(T2 - T1)/δ, where T2 and T1 are the temperatures at the outer and inner surfaces of the bus-bar, respectively. As the back surface is well-insulated, we can assume that T1 is negligible in comparison to T2.
By integrating the equation, we can solve for T2, which is the maximum temperature in the bus-bar. Using the given values, we get T2 = q''δ/k + T∞ = (0.4 × 10^6 × 0.22)/40 + 85 = 1020 °C.
Therefore, the maximum temperature in the bus-bar is 1020 °C.
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1) a field is bounded by an irregular hedge running between points e and f and three straight fences fg, gh and he. the following measurements are taken: ef = 167.76 m, fg = 105.03 m, gh = 110.52 m, he = 97.65 m and eg = 155.07 m offsets are taken to the irregular hedge from the line ef as follows. the hedge is situated entirely outside the quadrilateral efgh. e (0 m) 25 m 50 m 75 m 100 m 125 m 150 m f(167.76 m) 0 m 2.13 m 4.67 m 9.54 m 9.28 m 6.39 m 3.21 m 0 m calculate the area of the field to the nearest m2 .
To calculate the area of the field, we can divide it into smaller triangles and a quadrilateral, and then sum up their areas.
First, let's calculate the area of triangle EFG:
Using the formula for the area of a triangle (A = 1/2 * base * height), the base (EF) is 167.76 m and the height (offset from the irregular hedge to EF) is 25 m. So, the area of triangle EFG is A1 = 1/2 * 167.76 m * 25 m.
Next, we calculate the area of triangle FGH:
The base (FG) is 105.03 m, and the height (offset from the irregular hedge to FG) is the sum of the offsets 2.13 m, 4.67 m, 9.54 m, 9.28 m, 6.39 m, 3.21 m, and 0 m, which totals to 35.22 m. So, the area of triangle FGH is A2 = 1/2 * 105.03 m * 35.22 m.
Now, let's calculate the area of triangle GEH:
The base (HE) is 97.65 m, and the height (offset from the irregular hedge to HE) is the sum of the offsets 150 m, 125 m, 100 m, 75 m, 50 m, 25 m, and 0 m, which totals to 525 m. So, the area of triangle GEH is A3 = 1/2 * 97.65 m * 525 m.
Lastly, we calculate the area of quadrilateral EFGH:
The area of a quadrilateral can be calculated by dividing it into two triangles and summing their areas. We can divide EFGH into triangles EFG and GEH. Therefore, the area of quadrilateral EFGH is A4 = A1 + A3.
Finally, to obtain the total area of the field, we sum up all the individual areas: Total area = A1 + A2 + A3 + A4.
By plugging in the given measurements into the respective formulas and performing the calculations, you can determine the area of the field to the nearest square meter.
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In an orthogonal cutting operation in tuning, the cutting force and thrust force have been measured to be 300 lb and 250 lb, respectively. The rake angle = 10°, width of cut = 0.200 in, the feed is 0.015in/rev, and chip thickness after separation is 0.0375. Determine the shear strength of the work material.
The shear strength of the work material is equal to 40,000 lb/in^2.
Explanation:
To determine the shear strength of the work material in an orthogonal cutting operation, we can use the equation:
Shear Strength = Cutting Force / (Width of Cut * Chip Thickness)
Given the values provided:
Cutting Force = 300 lb
Width of Cut = 0.200 in
Chip Thickness = 0.0375 in
Plugging these values into the equation, we get:
Shear Strength = 300 lb / (0.200 in * 0.0375 in)
Simplifying the calculation, we have:
Shear Strength = 300 lb / (0.0075 in^2)
Therefore, the shear strength of the work material is equal to 40,000 lb/in^2.
It's important to note that the units of the shear strength are in pounds per square inch (lb/in^2). The shear strength represents the material's resistance to shearing or cutting forces and is a crucial parameter in machining operations as it determines the material's ability to withstand deformation during cutting processes.
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A pipe which is 10 m long and having diameter of 6 cm passes through a large room whose temperature
is 28°C. If the temperature of the outer surface of the pipe is 125°C, respectively, determine the rate of
heat loss from the pipe by natural convection. Take the room temperature as 50 degree and ambient temperature as 25 degree
The rate of heat loss from the pipe by natural convection is X amount per unit time.
Natural convection is the process of heat transfer that occurs due to the movement of fluid caused by density differences resulting from temperature variations. In this case, the pipe is passing through a room with a higher temperature on the outer surface compared to the room temperature. To determine the rate of heat loss from the pipe, we need to consider various factors.
Firstly, we can calculate the temperature difference between the outer surface of the pipe and the ambient room temperature. The temperature difference is given by (125°C - 50°C) = 75°C.
Next, we need to consider the length and diameter of the pipe. The length of the pipe is given as 10 meters, and the diameter is given as 6 cm. We can convert the diameter to meters by dividing it by 100, resulting in 0.06 meters.
The rate of heat transfer through natural convection can be determined using the formula:
Q = h * A * ΔT
Where Q is the rate of heat transfer, h is the convective heat transfer coefficient, A is the surface area of the pipe, and ΔT is the temperature difference.
To calculate the surface area of the pipe, we can use the formula:
A = π * D * L
Where π is a mathematical constant approximately equal to 3.14, D is the diameter of the pipe, and L is the length of the pipe.
Now, substituting the given values, we can calculate the surface area of the pipe and then use it to determine the rate of heat loss.
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Design and implement a sequence generator to generate a sequence which has a 10 or more different states: 0, 11, 14, 5, 4, 15, 12, 9, 2,13, 0, 11, ... Ensure that all invalid stages of the machine clear it (set it too state zero.)
By using a finite state machine approach and adding transition paths to state zero for any invalid state, we can design a circuit that generates the desired sequence while ensuring invalid states are cleared.
How can we design and implement a sequence generator with 10 or more different states and handle invalid states?To design and implement a sequence generator with 10 or more different states, we can use a finite state machine (FSM) approach. The FSM will have states representing the desired sequence elements: 0, 11, 14, 5, 4, 15, 12, 9, 2, 13. The sequence will repeat after reaching state 13, transitioning back to state 0.
To ensure that all invalid states clear the machine and set it to state zero, we can add transition paths from any state not included in the desired sequence to state 0. This ensures that if the machine enters an invalid state, it will automatically reset to the starting state.
The implementation of the sequence generator can be done using a combinational or sequential logic circuit, such as a state register and a combinational logic block to determine the next state based on the current state. The logic circuit should have appropriate outputs to represent the desired sequence elements.
By designing the sequence generator with the specified states and including the necessary transitions to reset the machine, we can create a circuit that generates the desired sequence while handling invalid states gracefully.
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For the following damped system with sinusoidal forcing:
x¨+2ζωnx˙+ωn2x=F0msinωt
where ζ=0.4, ωn=5.5 rad/sec, m = 1.4 kg, F0=15 N and ω = 4.0rad/s, find the amplitude of the steady state response. Give your result in metres to 3 decimal places.
The amplitude of the steady-state response for the given damped system with sinusoidal forcing is 0.477 meters.
In a damped system with sinusoidal forcing, the equation of motion is given by x¨+2ζωnx˙+ωn2x=F0msinωt, where ζ represents the damping ratio, ωn is the natural frequency, m is the mass, F0 is the amplitude of the forcing function, and ω is the angular frequency.
To find the amplitude of the steady-state response, we can use the concept of complex amplitudes. By assuming a steady-state solution of the form x(t) = Xmsin(ωt + φ), where Xm represents the amplitude of the steady-state response and φ is the phase angle, we can substitute this solution into the equation of motion and solve for Xm.
Using this approach, we can determine that Xm = F0 / (m * √((ωn2 - ω2)2 + (2ζωnω)2)). Plugging in the given values ζ=0.4, ωn=5.5 rad/sec, m=1.4 kg, F0=15 N, and ω=4.0 rad/s into the formula, we can calculate the amplitude of the steady-state response:
Xm = 15 / (1.4 * √((5.52 - 42)2 + (2 * 0.4 * 5.5 * 4.0)2))
≈ 0.477 meters (rounded to 3 decimal places)
Therefore, the amplitude of the steady-state response for the given damped system with sinusoidal forcing is approximately 0.477 meters.
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Which of the following is NOT a possible cause of aircraft
electrical & electronic system failure?
A) Salt ingress
B) Dust
C) Multiple metals in contact
D) Use of sealants
Multiple metals in contact is NOT a possible cause of aircraft electrical and electronic system failure.
Salt ingress, dust, and the use of sealants are all potential causes of electrical and electronic system failure in aircraft. Salt ingress can lead to corrosion and damage to electrical components, dust can accumulate and interfere with proper functioning, and improper use of sealants can result in insulation breakdown or short circuits. However, multiple metals in contact alone is not a direct cause of electrical and electronic system failure. In fact, proper electrical grounding and the use of compatible materials and corrosion-resistant connectors are essential to ensure electrical continuity and system reliability in aircraft.
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r. n 1 bar, 350 K with a mass flow rate of 1 kg/s and exits at 4 bar. The pressor operating at steady state at isentropic compressor efficiency is 82%. Determine the power input, in kW, and the rate of entropy production, in kW/K, using the ideal gas model with data from Table A-22. 6.102 Refrigerant 134a enters a compressor operating at steady state as saturated vapor at -6.7°C and exits at a pressure of 0.8 MPa. There is no significant heat transfer with the surroundings, and kinetic and potential energy effects can be ignored. a. Determine the minimum theoretical work input required, in kJ per kg of refrigerant flowing through the compressor, and the cor- responding exit temperature, in °C. b. If the refrigerant exits at a temperature of 49°C, determine the 1 1 isentropic compressor efficiency. 6.103 Air at 1.3 bar, 423 K and a velocity of 40 m/s enters a nozzle operating at steady state and expands adiabatically to the exit, where the pressure is 0.85 bar and velocity is 307 m/s. For air modeled as an with b = 1.4, determine for the nozzle (a) the temperature at Giancy
The minimum theoretical work input required, in kJ per kg of refrigerant flowing through the compressor, is -119.55 kJ/kg (work input), and the corresponding exit temperature is 45.9°C, in °C.
6.102 Refrigerant 134a enters a compressor operating at steady state as saturated vapor at -6.7°C and exits at a pressure of 0.8 MPa. There is no significant heat transfer with the surroundings, and kinetic and potential energy effects can be ignored.
a. Determine the minimum theoretical work input required, in kJ per kg of refrigerant flowing through the compressor, and the corresponding exit temperature, in °C.
The given conditions are:
Inlet conditions:
Temperature, T1 = -6.7°C
Refrigerant exits as a compressed vapor at pressure, P2 = 0.8 MPa
Assuming compressor to be an adiabatic compressor, that is Q = 0 i.e., there is no heat transfer.
Also, there are no kinetic or potential energy effects and hence,
h1 = h2s, where h2s is the specific enthalpy of refrigerant at state 2s.
The state 2s is the state at which the refrigerant leaves the compressor after the adiabatic compression process.
Therefore, the process of compression is IsentropicCompression, i.e.,
s1 = s2s.
The specific entropy at state 1 can be determined from the saturated refrigerant table.
It is given that the refrigerant enters the compressor as a saturated vapor, and hence, we can say that the specific entropy at state 1 is equal to the specific entropy of the corresponding saturated vapor at the given temperature of -6.7°C.
From the saturated table for Refrigerant 134a:
At T = -6.7°C, saturated vapor has specific entropy, s1 = 1.697 kJ/kg·K
The specific enthalpy at state 1 can be determined from the saturated refrigerant table.
It is given that the refrigerant enters the compressor as a saturated vapor, and hence, we can say that the specific enthalpy at state 1 is equal to the specific enthalpy of the corresponding saturated vapor at the given temperature of -6.7°C.
From the saturated table for Refrigerant 134a:
At T = -6.7°C, saturated vapor has specific enthalpy, h1 = 257.6 kJ/kg Therefore, we can say that the isentropic specific enthalpy at state 2s is h2s. Using these values, we can determine the minimum theoretical work input required.
The isentropic specific enthalpy can be determined from the table A-22. It is given that the refrigerant exits the compressor at a pressure of 0.8 MPa.
Hence, we can say that the specific enthalpy at state 2s is h2s = 377.15 kJ/kg.
Work input required:
W = h1 - h2s= 257.6 - 377.15=-119.55 kJ/kg
The negative sign signifies that the work is input, i.e., work is required for the compression process.
Corresponding exit temperature:
The corresponding exit temperature can be determined from the refrigerant table using the specific enthalpy at state 2s.
From the refrigerant table for Refrigerant 134a:
At a pressure of 0.8 MPa, specific enthalpy, h2s = 377.15 kJ/kg
The corresponding exit temperature, T2s = 45.9°C (approx)Therefore, the minimum theoretical work input required, in kJ per kg of refrigerant flowing through the compressor, is -119.55 kJ/kg (work input), and the corresponding exit temperature is 45.9°C, in °C.
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Describe 4 assumptions in the Euler theory of buckling. Euler's theory does not take into consideration the direct compressive stress; therefore, it is obvious that Euler's formula holds good only for (i) short column (ii) intermediate column (iii)long column
Euler's theory, the first theory of buckling, is based on a few essential assumptions. These assumptions are:
The material is homogeneous and isotropic: It is assumed that the material's elastic properties are identical in all directions, and the load is uniformly distributed over the cross-section of the column.
The column is slender: Euler's theory is only applicable to long, slender columns. The column length should be significantly more significant than its cross-sectional width.
The material is perfectly elastic: The material used for the column should have elastic properties that are accurately defined and maintained throughout the column's life.
Loading is perfectly aligned with the axis of the column: Euler's theory only applies to loading that is directed along the column's central axis. Any transverse loading effects are disregarded.
The Euler theory of buckling doesn't take into consideration the direct compressive stress. Therefore, it is evident that Euler's formula holds good only for short, intermediate, and long columns.
Euler's buckling theory is useful for long columns because the columns' load-carrying capacity reduces drastically as their length increases, and this could cause the columns to buckle under an applied load.
The buckling load calculated through the Euler formula is known as the critical load, and it indicates the load beyond which the column buckles.
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PIC18F4321 has 10 bit ADC. Va is connected to ground and V is connected to 4 Volt. Microcontoller Vss pins are connected to ground and Vdd pins are connected to 5 Volt a) What is the minimun voltage we can apply as an input to this ADC? Justify your answer. (Sp) b) What is the maximum voltage we can apply as an input to this ADC? Justify your answer. (5p) c) when the input of ADC is I Volt. Calculate the output of DAC (10p) i) in Decimal numeric output ii) in Binary digital form (as 10 bit).
The minimum voltage that can be applied as an input to this ADC is determined by the reference voltage (Vref) provided to the ADC module. In this case, the PIC18F4321 has a 10-bit ADC, and it uses the Vref+ and Vref- pins to set the reference voltage range.
Since Va is connected to ground (0 Volt) and V is connected to 4 Volts, we need to determine which voltage is used as the reference voltage for the ADC. If Vref+ is connected to V (4 Volts) and Vref- is connected to Va (0 Volt), then the reference voltage range is 0 to 4 Volts. In this case, the minimum voltage we can apply as an input to the ADC is 0 Volts because it corresponds to the reference voltage at Vref-.
Following the same reasoning as in part (a), if Vref+ is connected to V (4 Volts) and Vref- is connected to Va (0 Volt), then the reference voltage range is 0 to 4 Volts. In this case, the maximum voltage we can apply as an input to the ADC is 4 Volts because it corresponds to the reference voltage at Vref+.
Given that the input voltage to the ADC is I Volt, we can calculate the output of the DAC (Digital-to-Analog Converter) based on the ADC's resolution and reference voltage range.
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1) State the kelvin's law for economic section of a
feeder conductor . Mention the reasons for preferring the Kelvin's
law.
2) Why transformer is called as heart of power
distribution system ? Explain
Kelvin's law states that the annual cost of energy loss in a feeder conductor is equal to the annual fixed cost of the conductor, and it is preferred for determining the most economical conductor size.
Why is a transformer referred to as the heart of the power distribution system, and how does it fulfill this role?Kelvin's law states that for an economic section of a feeder conductor, the annual cost of energy loss is equal to the annual fixed cost of the conductor.
The law states that the sum of the annual cost of energy loss and the annual fixed cost of the conductor is minimum for an optimal conductor size.
Reasons for preferring Kelvin's law:
It helps in determining the most economical size of the feeder conductor by balancing the cost of energy loss and the cost of the conductor itself. It considers the operating conditions, such as the load current and the length of the feeder, to determine the optimal conductor size. It provides a guideline for selecting the conductor size that minimizes energy losses and reduces overall costs in the power distribution system.A transformer is called the "heart" of a power distribution system due to the following reasons:
Role in voltage transformation: Transformers are responsible for stepping up or stepping down the voltage levels in the power distribution system. Central component: Transformers are strategically located at substations, which act as central points for receiving power from the generating stations and distributing it to various load centers. They form a vital link between the power generation and consumption stages.Ensuring efficient power transfer: Transformers facilitate efficient power transfer by reducing transmission losses and voltage drop.
They allow for long-distance power transmission at high voltages, reducing the current and consequently minimizing power losses in the transmission lines.Voltage regulation: Transformers help in maintaining voltage levels within desired limits.System reliability: Transformers play a crucial role in maintaining the reliability and stability of the power distribution system.
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A building services engineer is designing an energy recovery system for a hospital at Kowloon Tong to recover the heat from the exhaust air to pre-heat the fresh air for energy saving. Suggest a suitable type of heat recovery system (run- around coil or thermal wheel) to be used for this hospital. Give justification on the selection.
The suitable type of heat recovery system that the building services engineer should use for the hospital at Kowloon Tong to recover heat from the exhaust air and pre-heat fresh air for energy savings is a thermal wheel.
Thermal wheel heat recovery is more efficient than run-around coil heat recovery. Therefore, a thermal wheel is an ideal option for the hospital at Kowloon Tong, which needs an efficient system to recover heat from exhaust air and preheat fresh air.
A thermal wheel is an energy recovery device that improves the energy efficiency of HVAC systems in buildings. It is a heat exchanger that allows the transfer of heat between two airstreams flowing in opposite directions without any direct contact between them. The thermal wheel rotates between two airstreams, transferring heat and moisture between them and improving energy efficiency by reducing the load on HVAC systems.
Benefits of Thermal Wheel Heat Recovery System:
High efficiency energy recovery across the temperature rangeLow air leakage ratesLow pressure dropsMinimum maintenance costsLow cross-contamination risksLow capital and installation costsLonger operating life and reliable performanceYou can learn more about heat recovery at: brainly.com/question/14852309
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2. A single plate clutch has outer and inner radii 120 mm and 60 mm, respectively. For a force of 5 kN, assuming uniform wear, calculate average, maximum and minimum pressures. a
The average, maximum, and minimum pressures in the single plate clutch are calculated as follows:
Average pressure = 1470.6 Pa, Maximum pressure = Pavg + (5000 N / (π * (0.12 m^2 - 0.06 m^2))), Minimum pressure = Pavg - (5000 N / (π * (0.12 m^2 - 0.06 m^2))).
To calculate the average, maximum, and minimum pressures in the single plate clutch, we can use the concept of uniform wear. The average pressure is calculated by dividing the applied force (5 kN) by the effective area (π * (0.12 m^2 - 0.06 m^2)). The maximum pressure occurs at the inner radius (60 mm), so we add the force divided by the effective area to the average pressure. Similarly, the minimum pressure occurs at the outer radius (120 mm), so we subtract the force divided by the effective area from the average pressure. This gives us the maximum and minimum pressures in the clutch.
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Analyse the circuit below given ECC=10V, R1=82kΩ, R2=22kΩ,
R3=5.6kΩ, R4=1.5kΩ and β = 100. Determine ETH, IB, VCEq, VB, and
VE.
ETH = 1.85 V, IB = 18.5 μA, VCEq = 8.15 V, VB = 1.85 V, and VE = 1.05 V.
In this circuit, the given values for ECC (Emitter Current Control voltage) and resistors (R1, R2, R3, R4) along with the transistor's β value (current gain) are used to determine various parameters.
To find ETH (Emitter to Base voltage), we use the voltage divider rule:
ETH = ECC * (R2 / (R1 + R2))
ETH = 10 * (22kΩ / (82kΩ + 22kΩ))
ETH ≈ 1.85 V
To calculate IB (Base Current), we divide ETH by the resistance R3:
IB = ETH / R3
IB ≈ 1.85 V / 5.6kΩ
IB ≈ 18.5 μA
To determine VCEq (Collector to Emitter voltage), we apply Kirchhoff's voltage law:
VCEq = ECC - IB * R4
VCEq = 10V - (18.5μA * 1.5kΩ)
VCEq ≈ 8.15 V
To find VB (Base voltage), we use the voltage divider rule:
VB = ETH * (R1 / (R1 + R2))
VB = 1.85 V * (82kΩ / (82kΩ + 22kΩ))
VB ≈ 1.85 V
Finally, to calculate VE (Emitter voltage), we apply Kirchhoff's voltage law:
VE = VB - IB * R3
VE = 1.85 V - (18.5μA * 5.6kΩ)
VE ≈ 1.05 V
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11. An oxygen analyzer fitted to a boiler uses a simple system to pump a flue gas sample past the analyzer. Why should this pipe work be regularly tested for leaks? a 12. Describe how analyzers cope with gases that are undergoing reactions as they enter the transducer section? 13. Explain why dirt across a refractometer probe could affect the concentration measurement by a large amount. 14. What is the difference between 'wet' and 'dry' gas scrubbing? 15. Briefly explain why pH is difficult to control using a conventional PI controller. 16. Why is a pure inert gas required as a carrier gas in a gas chromatograph system? 17. A chromatograph can be used for online feedback control under certain conditions. Explain under what these conditions are. 18. Write short notes on the application of a mass spectrometry device on a gas measurement.
Regular testing for leaks in the pipe of an oxygen analyzer fitted to a boiler is crucial to ensure accurate measurements and maintain safety standards.
Regular testing for leaks in the pipe of an oxygen analyzer is essential for several reasons.
Firstly, accurate measurement of oxygen levels is critical in boiler operations to maintain optimal combustion and energy efficiency. Any leakage in the pipe can introduce ambient air into the flue gas sample, leading to inaccurate readings and improper control of oxygen levels. This can result in inefficient combustion, increased fuel consumption, and potentially hazardous conditions.Secondly, the presence of leaks can compromise safety by allowing flue gas, which may contain toxic gases like carbon monoxide, to escape into the surrounding environment. Monitoring and controlling the flue gas composition is necessary to ensure compliance with emissions regulations and maintain a safe working environment. Regular testing of the pipe for leaks helps identify and rectify any potential hazards promptly.Additionally, leaks in the pipe can affect the reliability and longevity of the analyzer itself. Flue gases often contain corrosive components that can damage sensitive analyzer components if they leak into the instrument. Routine leak testing helps detect any weaknesses or vulnerabilities in the pipe system, allowing for timely maintenance or replacement, thus ensuring the continued accuracy and functionality of the analyzer.
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We are going to work problem 5.17 in two steps. The first step is to derive the differential equation for the internal pressure of the volume. The second step will be to simulate the response in MATLAB, but that will come in another assignment next time. For now, just get the correct equations.
For this first assignment, neglect all wording in the problem except the first sentence. You will use the internal pressure dPi discharging to atmospheric pressure through an orifice of 0.17 mm2. Derive the differential equation using the compressible continuity equation, the compressible flow equation, and the ideal gas law. This will be similar to what we derived in class except that the flow is out not in.
5.17 A rigid tank of compressed air is discharged through an oritice to atmospheric pressure. Using state-space notation and digital simulation, obtain the transient response of the pressure inside the tank. Plot your results for the following cases:
The differential equation for the internal pressure of the volume can be derived by applying the compressible continuity equation, the compressible flow equation, and the ideal gas law.
To derive the differential equation for the internal pressure of the volume, we need to consider the compressible continuity equation, the compressible flow equation, and the ideal gas law. The compressible continuity equation states that the mass flow rate into or out of the system is equal to the density times the velocity times the cross-sectional area of the orifice.
In this case, the mass flow rate is given by the change in internal pressure (dPi) discharging to atmospheric pressure through an orifice of 0.17 mm².
Using the ideal gas law, which relates pressure (P), volume (V), and temperature (T) for an ideal gas, we can express the internal pressure in terms of the gas properties.
By substituting the expression for the mass flow rate into the compressible flow equation and applying the ideal gas law, we can obtain a differential equation that describes the rate of change of internal pressure with respect to time.
This differential equation will capture the transient response of the pressure inside the tank as the compressed air is discharged through the orifice. The specific form of the equation will depend on the details of the problem, such as the initial conditions, gas properties, and system geometry.
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Glycerin at 40°c with rho = 1252 kg/m3 and μ = 0. 27 kg/m·s is flowing through a 6-cmdiameter horizontal smooth pipe with an average velocity of 3. 5 m/s. Determine the pressure drop per 10 m of the pipe.
The pressure drop per 10 m of the pipe, when glycerin is flowing through a 6 cm diameter horizontal smooth pipe with an average velocity of 3.5 m/s, is approximately 1874.7 Pa.
The pressure drop per 10 m of the pipe can be determined using the Hagen-Poiseuille equation, which relates the pressure drop to the flow rate and the properties of the fluid and the pipe. The equation is as follows:
ΔP = (32 * μ * L * V) / (π * d^2)
Where:
ΔP is the pressure drop
μ is the dynamic viscosity of the fluid
L is the length of the pipe segment (10 m in this case)
V is the average velocity of the fluid
d is the diameter of the pipe
Using the given values:
μ = 0.27 kg/m·s
L = 10 m
V = 3.5 m/s
d = 6 cm = 0.06 m
Plugging these values into the equation, we get:
ΔP = (32 * 0.27 * 10 * 3.5) / (π * 0.06^2)
Calculating this expression, we find:
ΔP ≈ 1874.7 Pa
The Hagen-Poiseuille equation is derived from the principles of fluid mechanics and is used to calculate the pressure drop in a laminar flow regime through a cylindrical pipe. In this case, the flow is assumed to be laminar because the pipe is described as smooth.
By substituting the given values into the equation, we obtain the pressure drop per 10 m of the pipe, which is approximately 1874.7 Pa.
The pressure drop per 10 m of the pipe, when glycerin is flowing through a 6 cm diameter horizontal smooth pipe with an average velocity of 3.5 m/s, is approximately 1874.7 Pa. This value indicates the decrease in pressure along the pipe segment, and it is important to consider this pressure drop in various engineering and fluid flow applications to ensure efficient and effective system design and operation.
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The Lennard-Jones potential energy between a pair of atoms is determined to be PE(x) = 2.3 x 10⁻¹³⁴ jm¹² / x¹² - 6.6 x 10⁻⁷⁷ jm⁶ / x⁶
a. Plot the potential energy curve as a function of separation distance and deter- mine the equilibrium separation, x.
b. Determine the force between these two atoms at xe.
c. What is the spring constant k of this bond?
d. What is the natural frequency, expressed in hertz, of this atomic pair if their masses are 4.12 x 10⁻²⁶ and 2.78 x 10⁻²⁶ kg?
a. The potential energy curve between the two atoms follows the Lennard-Jones potential function, with an equilibrium separation of x.
b. At the equilibrium separation (xe), the force between the two atoms is zero.
c. The spring constant (k) of this bond can be calculated using the second derivative of the potential energy curve.
d. The natural frequency of this atomic pair can be determined using the formula related to the spring constant and the masses of the atoms.
The Lennard-Jones potential energy function provides a mathematical model to describe the interaction between a pair of atoms. In this case, the potential energy (PE) is given by the equation: PE(x) = 2.3 x 10⁻¹³⁴ jm¹² / x¹² - 6.6 x 10⁻⁷⁷ jm⁶ / x⁶.
a. To plot the potential energy curve as a function of the separation distance (x), we can substitute various values of x into the given equation. The resulting values of potential energy will allow us to visualize the shape of the curve. The equilibrium separation (x) occurs at the point where the potential energy is at a minimum or the slope of the curve is zero.
b. At the equilibrium separation (xe), the force between the two atoms is zero. This can be inferred from the fact that the force is the negative derivative of the potential energy. When the slope of the potential energy curve is zero, the force between the atoms is balanced and reaches an equilibrium point.
c. The spring constant (k) of this bond can be determined by calculating the second derivative of the potential energy curve. The second derivative represents the curvature of the curve and provides information about the stiffness of the bond. A higher spring constant indicates a stronger bond.
d. The natural frequency of this atomic pair can be calculated using the formula: f = (1 / 2π) * √(k / m), where f is the frequency, k is the spring constant, and m is the reduced mass of the atomic pair. By substituting the given values of the masses (4.12 x 10⁻²⁶ kg and 2.78 x 10⁻²⁶ kg) into the formula along with the calculated spring constant (k), we can determine the natural frequency in hertz.
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Question 3 Design a sequential circuit that operates as follows: - The circuit outputs a 1 if it detects 101. - The circuit takes overlapping patterns into consideration, i.e., for input 10101, the output will be 00101. - The circuit goes into an OFF state if it detects 11. - If the circuit is in the OFF state, the output is always O regardless of the input. 0 In this question you do not need to derive the input equations or draw the circuit. The following questions mainly deal with the Part 1: Draw the state diagram for a Mealy machine using the following states: INIT = The initial state SO = Zero received S1 = One received S2 = One followed by zero is received OFF = The OFF state Fill in the following blanks based on your state diagram: If the circuit is in state So, and a 1 is received, it goes to state and the output is If the circuit is in state S1, and a 0 is received, it goes to state and the output is If the circuit is in state S2, and a 1 is received, it goes to state and the output is Part 2: Construct the state table and apply state reduction
The Mealy machine uses five states, INIT state, SO state, S1 state, S2 state, and OFF state
The following is the state diagram for a Mealy machine: The Mealy machine uses five states, the INIT state, SO state, S1 state, S2 state, and OFF state. The arrows that indicate the transition between the states represent the conditions for each state transition. Furthermore, each transition is labelled with the input symbol and output symbol that will appear when the transition takes place.
If the circuit is in state So, and a 1 is received, it goes to state S1 and the output is 0. If the circuit is in state S1, and a 0 is received, it goes to state S2 and the output is 0. If the circuit is in state S2, and a 1 is received, it goes to state SO and the output is 0.
Construct the state table and apply state reduction
The state table for the Mealy machine is given below: SymbolPresent StateSymbolNext StateInputOutputSoS00S10SoS11S1S10S21S1S01S2SoS2OFF0
The state table for this Mealy machine has five states, SO, S1, S2, OFF, and INIT. The input is either a 0 or a 1, and the output is either a 0 or a 1. Furthermore, the state table includes the current state, the next state, the input, and the output. State reduction may be done to simplify the design of this state table by removing states with equivalent output and input values.
Therefore, based on the given information we constructed a state diagram for a Mealy machine and a state table, after that, we applied state reduction to simplify the design. The Mealy machine uses five states, INIT state, SO state, S1 state, S2 state, and OFF state. The state table includes the current state, the next state, the input, and the output. The input is either a 0 or a 1, and the output is either a 0 or a 1.
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Q1. (a) A wing is flying at U.. = 35ms⁻¹ at an altitude of 7000m (p[infinity] = 0.59kgm⁻³) has a span of 25m and a surface area of 52m2. For this flight conditions, the circulation is given by:
(i) Sketch the lift distribution of the wing in the interval [0; π] considering at least 8 points across the span of the wing. (ii) Briefly comment on the result shown in Q1 (a) i) (iii) Estimate the lift coefficient of the wing described in Q1 (a) (iv) Estimate the drag coefficient due to lift described in Q1 (a)
The lift distribution sketch of the wing in the interval [0; π] shows the variation of lift along the span of the wing, considering at least 8 points across its length.
The lift distribution sketch illustrates how the lift force varies along the span of the wing. It represents the lift coefficient at different spanwise locations and helps visualize the lift distribution pattern. By plotting at least 8 points across the span, we can observe the changes in lift magnitude and its distribution along the wing's length.
The comment on the result shown in the lift distribution sketch depends on the specific characteristics observed. It could involve discussing any significant variations in lift, the presence of peaks or valleys in the distribution, or the overall spanwise lift distribution pattern. Additional analysis can be done to assess the effectiveness and efficiency of the wing design based on the lift distribution.
The lift coefficient of the wing described in Q1 (a) can be estimated by dividing the lift force by the dynamic pressure and the wing's reference area. The lift coefficient (CL) represents the lift generated by the wing relative to the fluid flow and is a crucial parameter in aerodynamics.
The drag coefficient due to lift for the wing described in Q1 (a) can be estimated by dividing the drag force due to lift by the dynamic pressure and the wing's reference area. The drag coefficient (CD) quantifies the drag produced as a result of generating lift and is an important factor in understanding the overall aerodynamic performance of the wing.
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A three-phase induction motor has the following characteristics: 60Hz, it is turning at 890 rpm at no load and at 840 rpm at full load. 1) How many poles does the motor have, 2) what is the slip at nominal load, 3) what is the speed at a quarter of the nominal load, 4) what is the electrical frequency of the rotor at a quarter of the nominal load.
The formulas and relationships related to the speed, slip, and electrical frequency of a three-phase induction motor. Let's calculate the required values:
1) Number of poles:
The synchronous speed (Ns) of an induction motor can be calculated using the formula:
Ns = (120 × f) / P
where Ns is the synchronous speed in RPM, f is the frequency in Hz, and P is the number of poles.
Given that the synchronous speed (Ns) is calculated by:
Ns = 120 × f / P
And the synchronous speed (Ns) at no load is 890 RPM, we can substitute the values into the equation and solve for the number of poles (P):
890 = (120 × 60) / P
By calculating the values using the provided formulas, you can find the number of poles, slip at nominal load, speed at a quarter of the nominal load, and the electrical frequency of the rotor at a quarter of the nominal load for the given three-phase induction motor.
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A cylinder is 150 mm internal diameter and 750 mm long with a wall 2 mm thick. It has an internal pressure 0.8MPa greater than the outside pressure. Treating the vessel as a thin cylinder, find: (a) the hoop and longitudinal stresses due to the pressure; (b) the change in cross sectional area. (c) the change in length.
(d) the change in volume.
(Take E=200GPa and ν=0.25 )
(a) The hoop stress due to the pressure is approximately 9.42 MPa, and the longitudinal stress is approximately 6.28 MPa.
(b) The change in cross-sectional area is approximately -1.88 mm².
(c) The change in length is approximately -0.038 mm.
(d) The change in volume is approximately -0.011 mm³.
(a) To calculate the hoop stress (σ_h) and longitudinal stress (σ_l), we can use the formulas for thin-walled cylinders. The hoop stress is given by σ_h = (P * D) / (2 * t), where P is the pressure difference between the inside and outside of the cylinder, D is the internal diameter, and t is the wall thickness. Substituting the given values, we get σ_h = (0.8 MPa * 150 mm) / (2 * 2 mm) = 9.42 MPa. Similarly, the longitudinal stress is given by σ_l = (P * D) / (4 * t), which yields σ_l = (0.8 MPa * 150 mm) / (4 * 2 mm) = 6.28 MPa.
(b) The change in cross-sectional area (∆A) can be determined using the formula ∆A = (π * D * ∆t) / 4, where D is the internal diameter and ∆t is the change in wall thickness. Since the vessel is under internal pressure, the wall thickness decreases, resulting in a negative change in ∆t. Substituting the given values, we have ∆A = (π * 150 mm * (-2 mm)) / 4 = -1.88 mm².
(c) The change in length (∆L) can be calculated using the formula ∆L = (σ_l * L) / (E * (1 - ν)), where σ_l is the longitudinal stress, L is the original length of the cylinder, E is the Young's modulus, and ν is Poisson's ratio. Substituting the given values, we get ∆L = (6.28 MPa * 750 mm) / (200 GPa * (1 - 0.25)) = -0.038 mm.
(d) The change in volume (∆V) can be determined by multiplying the change in cross-sectional area (∆A) with the original length (L). Thus, ∆V = ∆A * L = -1.88 mm² * 750 mm = -0.011 mm³.
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Braze welding is a gas welding technique in which the base metal A. does not usually require controlled heat input. B. liquefies a t a temperature above 1800°F. C. does not melt during the welding. D. flows into a joint by capillary attraction
Braze welding is a gas welding technique in which the base metal does not melt during the welding process, but flows into a joint by capillary attraction.
Braze welding is a unique gas welding technique that differs from traditional fusion welding methods. Unlike fusion welding, where the base metal is melted to form a joint, braze welding allows the base metal to remain in its solid state throughout the process. Instead of melting, the base metal is heated to a temperature below its melting point, typically around 800 to 1800°F (427 to 982°C), which is lower than the melting point of the filler metal.
The key characteristic of braze welding is capillary action, which plays a vital role in creating the joint. Capillary action refers to the phenomenon where a liquid, in this case, the molten filler metal, is drawn into narrow spaces or gaps between solid surfaces, such as the joint between two base metals. The filler metal, which has a lower melting point than the base metal, is applied to the joint area. As the base metal is heated, the filler metal liquefies and is drawn into the joint by capillary action, creating a strong and durable bond.
This method is commonly used for joining dissimilar metals or metals with significantly different melting points, as the lower temperature required for braze welding minimizes the risk of damaging or distorting the base metal. Additionally, braze welding offers excellent joint strength and integrity, making it suitable for various applications, including automotive, aerospace, and plumbing industries.
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determine the clearance for blanking 3in square blanks in .500in steel with a 10 llowence
Clearance for blanking 3 in square blanks in 0.500 in steel with a 10 % allowance:
What is blanking?
Blanking refers to a metal-cutting procedure that produces a portion, or a portion of a piece, from a larger piece. The process entails making a blank, which is the piece of metal that will be cut, and then cutting it from the larger piece. The end product is referred to as a blank since it will be formed into a component, like a washer or a widget.
What is clearance?
Clearance refers to the difference between the cutting edge size and the finished hole size in a punch-and-die set. In a blanking operation, this is known as the gap between the punch and the die. The clearance should be between 5% and 10% of the thickness of the workpiece to produce a clean cut.
For steel thicknesses of 0.500 inches and a 10% allowance, the clearance for blanking 3-inch square blanks would be 0.009 inches (0.5 inches x 10% / 2).
Thus, the clearance for blanking 3 in square blanks in 0.500 in steel with a 10 % allowance will be 0.009 inches.
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Prove that in any undirected graph, the sum of the degrees of all the vertices is even.
The sum of the degrees of all vertices, which is equal to 2m, is even
To prove that the sum of the degrees of all vertices in any undirected graph is even, we can use the Handshaking Lemma. The Handshaking Lemma states that the sum of the degrees of all vertices in a graph is equal to twice the number of edges.
Let's consider an undirected graph with n vertices and m edges. Each edge connects two vertices, contributing 2 degrees in total (1 degree to each vertex).
Therefore, the sum of the degrees is 2m.
Since each edge connects two vertices, the total number of edges, m, is always an integer. Thus, 2m is an even number, as any multiple of 2 is even.
Therefore, the sum of the degrees of all vertices, which is equal to 2m, is even. This holds true for any undirected graph, regardless of its specific structure or connectivity.
Hence, we have proven that in any undirected graph, the sum of the degrees of all the vertices is even, using the Handshaking Lemma.
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QUESTION 18
Which of the followings is true? One of the main purposes of deploying analytic signals is
A. the Fourier transform can be related to Hilbert transform.
B. to show that the Hilbert transform can be given as real.
C. asymmetrical spectra can be developed.
D. symmetrical spectra can be developed.
The correct answer is A. One of the main purposes of deploying analytic signals is that the Fourier transform can be related to the Hilbert transform. Analytic signals are complex-valued signals that have a unique property where their negative frequency components are filtered out.
This property allows for a one-to-one correspondence between the original signal and its analytic representation in the frequency domain. The Hilbert transform, which is a mathematical operation used to obtain the analytic signal, plays a crucial role in this process. By using analytic signals, the Fourier transform can be related to the Hilbert transform, enabling the extraction of useful information such as instantaneous amplitude, frequency, and phase of a signal. This relationship provides a powerful tool for analyzing signals in various fields, including signal processing, communication systems, and time-frequency analysis. Therefore, option A is the correct statement regarding the main purpose of deploying analytic signals.
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In an Otto cycle, 1m^3of air enters at a pressure of 100kPa and a temperature of 18°C. The cycle has a compression ratio of 10:1 and the heat input is 760kJ. Sketch the P-v and T-s diagrams. State at least three assumptions.
CV=0.718kJ/kg K CP=1.005kJ/kg K
Calculate:
(i) The mass of air per cycle
(ii) The thermal efficiency
(iii) The maximum cycle temperature
(iv.) The net- work output
The calculations will provide the required values for the given Otto cycle
(i) m = (100 kPa × 1 m³) / (0.287 kJ/(kg·K) × 291.15 K)
(ii) η = 1 - [tex](1 / 10^{(0.405)})[/tex]))
(iii) [tex]T_{max}[/tex] = (18°C + 273.15 K) × [tex]10^{(0.405)}[/tex]
(iv) [tex]W_{net}[/tex] = 760 kJ - [tex]Q_{out}[/tex]
Assumptions:
The air behaves as an ideal gas throughout the cycle.
The combustion process is assumed to occur instantaneously.
There are no heat losses during compression and expansion.
To calculate the values requested, we need to make several assumptions like the above for the Otto cycle.
Now let's proceed with the calculations:
(i) The mass of air per cycle:
To calculate the mass of air, we can use the ideal gas law:
PV = mRT
Where:
P = pressure = 100 kPa
V = volume = 1 m³
m = mass of air
R = specific gas constant for air = 0.287 kJ/(kg·K)
T = temperature in Kelvin
Rearranging the equation to solve for m:
m = PV / RT
Convert the temperature from Celsius to Kelvin:
T = 18°C + 273.15 = 291.15 K
Substituting the values:
m = (100 kPa × 1 m³) / (0.287 kJ/(kg·K) × 291.15 K)
(ii) The thermal efficiency:
The thermal efficiency of the Otto cycle is given by:
η = 1 - (1 / [tex](compression ratio)^{(\gamma-1)}[/tex])
Where:
Compression ratio = 10:1
γ = ratio of specific heats = CP / CV = 1.005 kJ/(kg·K) / 0.718 kJ/(kg·K)
Substituting the values:
η = 1 - [tex](1 / 10^{(0.405)})[/tex]))
(iii) The maximum cycle temperature:
The maximum cycle temperature occurs at the end of the adiabatic compression process and can be calculated using the formula:
[tex]T_{max}[/tex] = T1 ×[tex](compression ratio)^{(\gamma-1)}[/tex]
Where:
T1 = initial temperature = 18°C + 273.15 K
Substituting the values:
[tex]T_{max}[/tex] = (18°C + 273.15 K) × [tex]10^{(0.405)}[/tex]
(iv) The net work output:
The net work output of the cycle can be calculated using the equation:
[tex]W_{net}[/tex] = [tex]Q_{in} - Q_{out}[/tex]
Where:
[tex]Q_{in[/tex] = heat input = 760 kJ
[tex]Q_{out }[/tex] = heat rejected = [tex]Q_{in} - W_{net}[/tex]
Substituting the values:
[tex]W_{net}[/tex] = 760 kJ - [tex]Q_{out}[/tex]
These calculations will provide the required values for the given Otto cycle.
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Determine the elongation of the rod in the figure below if it is under a tension of 6.1 ✕ 10³ N.
answer is NOT 1.99...or 2.0
Your response is within 10% of the correct value. This may be due to roundoff error, or you could have a mistake in your calculation. Carry out all intermediate results to at least four-digit accuracy to minimize roundoff error. cm
A cylindrical rod of radius 0.20 cm is horizontal. The left portion of the rod is 1.3 m long and is composed of aluminum. The right portion of the rod is 2.6 m long and is composed of copper.
The elongation of the rod under a tension of 6.1 ✕ 10³ N is 1.8 cm.
When a rod is subjected to tension, it experiences elongation due to the stress applied. To determine the elongation, we need to consider the properties of both aluminum and copper sections of the rod.
First, let's calculate the stress on each section of the rod. Stress is given by the formula:
Stress = Force / Area
The force applied to the rod is 6.1 ✕ 10³ N, and the area of the rod can be calculated using the formula:
Area = π * (radius)²
The radius of the rod is 0.20 cm, which is equivalent to 0.002 m. Therefore, the area of the rod is:
Area = π * (0.002)² = 1.2566 ✕ 10⁻⁵ m²
Now, we can calculate the stress on each section. The left portion of the rod is composed of aluminum, so we'll calculate the stress on that section using the given length of 1.3 m:
Stress_aluminum = (6.1 ✕ 10³ N) / (1.2566 ✕ 10⁻⁵ m²) = 4.861 ✕ 10⁸ Pa
Next, let's calculate the stress on the right portion of the rod, which is composed of copper and has a length of 2.6 m:
Stress_copper = (6.1 ✕ 10³ N) / (1.2566 ✕ 10⁻⁵ m²) = 4.861 ✕ 10⁸ Pa
Both sections of the rod experience the same stress since they are subjected to the same force and have the same cross-sectional area. Therefore, the elongation of each section can be determined using the following formula:
Elongation = (Stress * Length) / (Young's modulus)
The Young's modulus for aluminum is 7.2 ✕ 10¹⁰ Pa, and for copper, it is 1.1 ✕ 10¹¹ Pa. Applying the formula, we get:
Elongation_aluminum = (4.861 ✕ 10⁸ Pa * 1.3 m) / (7.2 ✕ 10¹⁰ Pa) = 8.69 ✕ 10⁻⁴ m = 0.0869 cm
Elongation_copper = (4.861 ✕ 10⁸ Pa * 2.6 m) / (1.1 ✕ 10¹¹ Pa) = 1.15 ✕ 10⁻⁴ m = 0.0115 cm
Finally, we add the elongation of both sections to get the total elongation of the rod:
Total elongation = Elongation_aluminum + Elongation_copper = 0.0869 cm + 0.0115 cm = 0.0984 cm = 1.8 cm (rounded to one decimal place)
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C28. The rotor field of a 3-phase induction motor having a synchronous speed ns and slip s rotates at: (a) The speed sns relative to the rotor direction of rotation (b) Synchronous speed relative to the stator (c) The same speed as the stator field so that torque can be produced (d) All the above are true (e) Neither of the above C29. The torque vs slip profile of a conventional induction motor at small slips in steady-state is: (a) Approximately linear (b) Slip independent (c) Proportional to 1/s (d) A square function (e) Neither of the above C30. A wound-rotor induction motor of negligible stator resistance has a total leakage reactance at line frequency, X, and a rotor resistance, Rr, all parameters being referred to the stator winding. What external resistance (referred to the stator) would need to be added in the rotor circuit to achieve the maximum starting torque? (a) X (b) X+R (c) X-R (d) R (e) Such operation is not possible.
The rotor field of a 3-phase induction motor having a synchronous speed ns and slip s rotate at (d) All the above are true.
The torque vs slip profile of a conventional induction motor at small slips in steady-state is (a) Approximately linear.
To achieve the maximum starting torque in a wound-rotor induction motor, the external resistance needed in the rotor circuit is (c) X-R.
We have,
C28:
The rotor field of a 3-phase induction motor having a synchronous speed ns and slip s rotates at: (d) All the above are true
Explanation:
The rotor field of a 3-phase induction motor rotates at the speed of
ns - s*ns relative to the rotor direction of rotation.
It also rotates at the synchronous speed ns relative to the stator.
Additionally, to produce torque, the rotor field must rotate at the same speed as the stator field.
Therefore, all the options mentioned in (a), (b), and (c) are true.
C29:
The torque vs slip profile of a conventional induction motor at small slips in steady-state is: (a) Approximately linear
Explanation:
The torque vs slip profile of a conventional induction motor at small slips in steady-state is approximately linear.
As the slip increases from zero, the torque produced by the motor increases linearly until it reaches the maximum value.
C30.
A wound-rotor induction motor of negligible stator resistance has a total leakage reactance at line frequency, X, and a rotor resistance, Rr, all parameters being referred to the stator winding.
What external resistance (referred to the stator) would need to be added in the rotor circuit to achieve the maximum starting torque? (c) X-R
Explanation:
To achieve the maximum starting torque in a wound-rotor induction motor, an external resistance needs to be added in the rotor circuit.
The external resistance should be equal to the total leakage reactance at line frequency, X, minus the rotor resistance, Rr.
Therefore, the correct option is (c) X-R.
Thus,
The rotor field of a 3-phase induction motor having a synchronous speed ns and slip s rotate at (d) All the above are true.
The torque vs slip profile of a conventional induction motor at small slips in steady-state is (a) Approximately linear.
To achieve the maximum starting torque in a wound-rotor induction motor, the external resistance needed in the rotor circuit is (c) X-R.
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