The given statement that "Flight path, is the path or the line along which the c.g. of the airplane moves.
The tangent to this curve at a point gives the direction of flight velocity at that point on the flight path." is True. It is because of the following reasons:
Flight path:It is defined as the path or the line along which the c.g. of the airplane moves. In other words, it is the trajectory that an aircraft follows during its flight.
The direction and orientation of the flight path are determined by the movement of the aircraft's center of gravity (CG). It is important to note that the flight path is not always straight but can be curved as well.
Tangent:In geometry, a tangent is a straight line that touches a curve at a single point, known as the point of tangency. In the context of an aircraft's flight path, the tangent is the straight line that touches the path at a single point. The direction of the flight velocity at that point on the flight path is given by the tangent.
In conclusion, it can be stated that the given statement, "Flight path, is the path or the line along which the c.g. of the airplane moves. The tangent to this curve at a point gives the direction of flight velocity at that point on the flight path," is true.
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Question A pendulum has a length of 250mm. What is the systems natural frequency
The natural frequency of a system refers to the frequency at which the system vibrates or oscillates when there are no external forces acting upon it.
The natural frequency of a pendulum is dependent upon its length. Therefore, in this scenario, a pendulum has a length of 250 mm and we want to find its natural frequency.Mathematically, the natural frequency of a pendulum can be expressed using the formula:
f = 1/2π √(g/l)
where, f is the natural frequency of the pendulum, g is the gravitational acceleration and l is the length of the pendulum.
Substituting the given values into the formula, we get :
f= 1/2π √(g/l)
= 1/2π √(9.8/0.25)
= 2.51 Hz
Therefore, the natural frequency of the pendulum is 2.51 Hz. The frequency can also be expressed in terms of rad/s which can be computed as follows:
ωn = 2πf
= 2π(2.51)
= 15.80 rad/s.
Hence, the system's natural frequency is 2.51 Hz or 15.80 rad/s. This is because the frequency of the pendulum is dependent upon its length and the gravitational acceleration acting upon it.
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A small aircraft has a wing area of 50 m², a lift coefficient of 0.45 at take-off settings, and a total mass of 5,000 kg. Determine the following: a. Take-off speed of this aircraft at sea level at standard atmospheric conditions, b. Wing loading and c. Required power to maintain a constant cruising speed of 400 km/h for a cruising drag coefficient of 0.04.
a. The take-off speed of the aircraft is approximately 79.2 m/s.
b. The wing loading is approximately 100 kg/m².
c. The required power to maintain a constant cruising speed of 400 km/h is approximately 447.2 kW.
a. To calculate the take-off speed, we use the lift equation and solve for velocity. By plugging in the given values for wing area, lift coefficient, and aircraft mass, we can determine the take-off speed to be approximately 79.2 m/s. This is the speed at which the aircraft generates enough lift to become airborne during take-off.
b. Wing loading is the ratio of the aircraft's weight to its wing area. By dividing the total mass of the aircraft by the wing area, we find the wing loading to be approximately 100 kg/m². Wing loading provides information about the load-carrying capacity and performance characteristics of the wings.
c. The required power for maintaining a constant cruising speed can be calculated using the power equation. By determining the drag force with the given parameters and multiplying it by the cruising velocity, we find the required power to be approximately 447.2 kW. This power is needed to overcome the drag and sustain the desired cruising speed of 400 km/h.
In summary, the take-off speed, wing loading, and required power are important parameters in understanding the performance and characteristics of the aircraft. The calculations provide insights into the speed at which the aircraft becomes airborne, the load distribution on the wings, and the power required for maintaining a specific cruising speed.
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7. Given that P. 2ax-ay-2az Q. 4ax. 3ay.2az R = -ax+ ay • Zaz Find: (a) IP+Q-RI, (b) PI x R. (c) Q x P DR, (d) (PxQ) DQ x R). (e) (PxQ) x (QxR) (1) CosB (g) Sin
Using trigonometry identities we have:
(a) IP + Q - RI: 3ax - ay - 3az.
(b) PI x R: -2a^2x + 2a^2y.zaz + ax.ay + 2az.ay.
(c) Q x P DR: -48a^3x.ay.az + 48a^3y.az^2 + 24a^2x.ay.az + 48az^2.ay.
(d) (PxQ) DQ x R: -56a^3x.ay.az + 16ax.ay.8az + 16ax.ay.2az + 6a^2x.3ay.zaz + 12a^2y.az.2ax - 6ax.ay.az - 24az.ay.2ax.
(e) (PxQ) x (QxR): -50a^3x.ay.az + 40a^3y.az^2 - 22a^2x.ay.az - 56ax.ay.az - 48az.ay.2ax.
Given that P = 2ax - ay - 2az; Q = 4ax.3ay.2az; R = -ax + ay • Zaz;
(a) IP + Q - RI:
The value of IP + Q - RI is given by:
IP + Q - RI = (2ax - ay - 2az) + (4ax.3ay.2az) - (-ax + ay • Zaz)
= 2ax - ay - 2az + 24ax.ay.az + ax - ay.zaz
= (2+1+0)ax + (-1+0+0)ay + (-2+0-1)az
= 3ax - ay - 3az
(b) PI x R:
The value of PI x R can be obtained as follows:
PI x R = 2ax - ay - 2az x (-ax + ay • Zaz)
= 2ax x (-ax) + 2ax x (ay • Zaz) - ay x (-ax) - ay x (ay • Zaz) - 2az x (-ax) - 2az x (ay • Zaz)
= -2a^2x + 2a^2y.zaz + ax.ay + 2az.ay
(c) Q x P DR:
The value of Q x P DR can be obtained as follows:
Q x P DR = (4ax.3ay.2az) x (2ax - ay - 2az) x (-ax + ay • Zaz)
= 24ax.ay.az x (2ax - ay - 2az) x (-ax + ay • Zaz)
= -48a^3x.ay.az + 48a^3y.az^2 + 24a^2x.ay.az + 48az^2.ay
(d) (PxQ) DQ x R:
The value of (PxQ) DQ x R) can be obtained as follows:
(PxQ) DQ x R) = [(2ax - ay - 2az) x (4ax.3ay.2az)] x (-ax + ay • Zaz)
= (8a^2x.3ay.zaz - 4ax.ay.8az - 8ax.ay.2az - 6a^2x.3ay.zaz - 12a^2y.az.2ax + 6ax.ay.az + 24az.ay.2ax) x (-ax + ay.zaz)
= (-56a^3x.ay.az + 16ax.ay.8az + 16ax.ay.2az + 6a^2x.3ay.zaz + 12a^2y.az.2ax - 6ax.ay.az - 24az.ay.2ax)
(e) (PxQ) x (QxR):
The expression of (PxQ) x (QxR) can be obtained as follows:
(PxQ) x (QxR) = [(2ax - ay - 2az) x (4ax.3ay.2az)] x [(4ax.3ay.2az) x (-ax + ay • Zaz)]
= (8a^2x.3ay.zaz - 4ax.ay.8az - 8ax.ay.2az - 6a^
2x.3ay.zaz - 12a^2y.az.2ax + 6ax.ay.az + 24az.ay.2ax) x (-ax + ay.zaz)
= -50a^3x.ay.az + 40a^3y.az^2 - 22a^2x.ay.az - 56ax.ay.az - 48az.ay.2ax
(1) CosB:
CosB cannot be found since there is no information about any angle present in the question.
(g) Sin:
Sin cannot be found since there is no information about any angle present in the question.
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Create summarize of roles of phonon in specific heat of
a solid crystal ! (All Formula, Rules and Explanation)
Phonons play a crucial role in determining the specific heat of a solid crystal. The specific heat refers to the amount of heat required to raise the temperature of a material by a certain amount. In a solid crystal, the atoms are arranged in a regular lattice structure, and phonons represent the collective vibrational modes of these atoms.
1. Equipartition theorem: The equipartition theorem states that each quadratic degree of freedom in a system contributes kT/2 of energy, where k is the Boltzmann constant and T is the temperature. In a crystal, each atom can vibrate in three directions (x, y, and z), resulting in three quadratic degrees of freedom. Therefore, each phonon mode contributes kT/2 of energy.
2. Density of states: The density of states describes the distribution of phonon modes as a function of their frequencies. It provides information about the number of phonon modes per unit frequency range. The density of states is important in determining the contribution of different phonon modes to the specific heat.
3. Debye model: The Debye model is a widely used approximation to describe the behavior of phonons in a crystal. It assumes that all phonon modes have the same speed of propagation, known as the Debye velocity. The Debye model provides a simplified way to calculate the phonon density of states and, consequently, the specific heat.
4. Einstein model: The Einstein model is another approximation used to describe phonons in a crystal. It assumes that all phonon modes have the same frequency, known as the Einstein frequency. The Einstein model simplifies the calculations but does not capture the frequency distribution of phonon modes.
5. Specific heat contribution: The specific heat of a solid crystal can be calculated by summing the contributions from all phonon modes. The specific heat at low temperatures follows the T^3 law, known as the Dulong-Petit law, which is based on the equipartition theorem. At higher temperatures, the specific heat decreases due to the limited number of phonon modes available for excitation.
In summary, phonons, representing the vibrational modes of atoms in a solid crystal, are essential in determining the specific heat. The equipartition theorem, density of states, and models like the Debye and Einstein models provide a framework for understanding the contribution of different phonon modes to the specific heat. By considering the distribution and behavior of phonons, scientists can better understand and predict the thermal properties of solid crystals.
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Project report about developed the fidget spinner concept
designs and followed the steps to eventually build a fully
assembled and functional fidget spinner. ( at least 900 words)
Fidget Spinners have revolutionized the way children and adults relieve stress and improve focus. They're simple to construct and have become a mainstream plaything, with various models and designs available on the market.
Here's a project report about how the Fidget Spinner concept was developed:IntroductionThe Fidget Spinner is a stress-relieving toy that has rapidly grown in popularity. It's a pocket-sized device that is shaped like a propeller and spins around a central axis. It was first developed in the 1990s, but it wasn't until 2016 that it became a worldwide trend.
The first Fidget Spinner was created with only a bearing and plastic parts. As the trend caught on, several models with different shapes and designs were produced. This project report describes how we created our fidget spinner and the steps we followed to make it fully operational.
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What is the zeroth law of thermodynamics? b.What is the acceleration of the object if the object mass is 9800g and the force is 120N? (Formula: F= ma) c.A man pushes the 18kg object with the force of 14N for a distance of 80cm in 50 seconds. Calculate the work done. (Formula: Work=Fd)
The zeroth law of thermodynamics is the law that states that if two systems are each in thermal equilibrium with a third system, then they are in thermal equilibrium with each other.
Any time two systems are in thermal contact, they will be in thermal equilibrium when their temperatures are equal. The zeroth law of thermodynamics states that if two systems are both in thermal equilibrium with a third system, they are in thermal equilibrium with each other.
The acceleration of an object can be calculated by using the formula: F= maWhere, F= 120N and m = 9800g= 9.8 kg (mass of the object)Thus, 120 = 9.8 x aSolving for a,a = 120/9.8a = 12.24 m/s²Thus, the acceleration of the object is 12.24 m/s².b) Work can be calculated by using the formula: Work= F x dWhere, F = 14N, d= 80cm = 0.8m (distance)Work = 14 x 0.8Work = 11.2JThus, the work done by the man is 11.2J.
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Methane gas at 120 atm and −18°C is stored in a 20−m³ tank. Determine the mass of methane contained in the tank, in kg, using the
(a) ideal gas equation of state. (b) van der Waals equation. (c) Benedict-Webb-Rubin equation.
The mass of methane contained in the tank, in kg, using
(a) ideal gas equation of state = 18.38 kg
(b) van der Waals equation = 18.23 kg
(c) Benedict-Webb-Rubin equation = 18.21 kg.
(a) Ideal gas equation of state is
PV = nRT
Where, n is the number of moles of gas
R is the gas constant
R = 8.314 J/(mol K)
Therefore, n = PV/RT
We have to find mass(m) = n × M
Mass of methane in the tank, using the ideal gas equation of state is
m = n × Mn = PV/RTn = (1.2159 × 10⁷ Pa × 20 m³) / (8.314 J/(mol K) × 255 K)n = 1145.45 molm = n × Mm = 1145.45 mol × 0.016043 kg/molm = 18.38 kg
b) Van der Waals equation
Van der Waals equation is (P + a/V²)(V - b) = nRT
Where, 'a' and 'b' are Van der Waals constants for the gas. For methane, the values of 'a' and 'b' are 2.25 atm L²/mol² and 0.0428 L/mol respectively.
Therefore, we can write it as(P + 2.25 aP²/RT²)(V - b) = nRT
At given conditions, we have
P = 120 atm = 121.59 × 10⁴ Pa
T = 255 K
V = 20 m³
n = (P + 2.25 aP²/RT²)(V - b)/RTn = (121.59 × 10⁴ Pa + 2.25 × (121.59 × 10⁴ Pa)²/(8.314 J/(mol K) × 255 K) × (20 m³ - 0.0428 L/mol))/(8.314 J/(mol K) × 255 K)n = 1138.15 molm = n × Mm = 1138.15 mol × 0.016043 kg/molm = 18.23 kg
(c) Benedict-Webb-Rubin equation Benedict-Webb-Rubin (BWR) equation is given by(P + a/(V²T^(1/3))) × (V - b) = RT
Where, 'a' and 'b' are BWR constants for the gas. For methane, the values of 'a' and 'b' are 2.2538 L² kPa/(mol² K^(5/2)) and 0.0387 L/mol respectively.
Therefore, we can write it as(P + 2.2538 aP²/(V²T^(1/3)))(V - b) = RT
At given conditions, we haveP = 120 atm = 121.59 × 10⁴ PaT = 255 KV = 20 m³n = (P + 2.2538 aP²/(V²T^(1/3)))(V - b)/RTn = (121.59 × 10⁴ Pa + 2.2538 × (121.59 × 10⁴ Pa)²/(20 m³)² × (255 K)^(1/3) × (20 m³ - 0.0387 L/mol))/(8.314 J/(mol K) × 255 K)n = 1135.84 molm = n × Mm = 1135.84 mol × 0.016043 kg/molm = 18.21 kg
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Design a excel file of an hydropower turgo turbine in Sizing and Material selection.
Excel file must calculate the velocity of the nozel, diameter of the nozel jet, nozzle angle, the runner size of the turgo turbine, turbine blade size, hub size, fastner, angular velocity,efficiency,generator selection,frequnecy,flowrate, head and etc.
(Note: File must be in execl file with clearly formulars typed with all descriptions in the sheet)
Designing an excel file for a hydropower turbine (Turgo turbine) involves calculating different values that are essential for its operation. These values include the velocity of the nozzle, diameter of the nozzle jet, nozzle angle, runner size of the turbine, turbine blade size, hub size, fastener, angular velocity, efficiency, generator selection, frequency, flow rate, head, etc.
To create an excel file for a hydropower turbine, follow these steps:Step 1: Open Microsoft Excel and create a new workbook.Step 2: Add different sheets to the workbook. One sheet can be used for calculations, while the others can be used for data input, output, and charts.Step 3: On the calculation sheet, enter the formulas for calculating different values. For instance, the formula for calculating the velocity of the nozzle can be given as:V = (2 * g * H) / (√(1 - sin²(θ / 2)))Where V is the velocity of the nozzle, g is the acceleration due to gravity, H is the head, θ is the nozzle angle.Step 4: After entering the formula, label each column and row accordingly. For example, the velocity of the nozzle formula can be labeled under column A and given a name, such as "Nozzle Velocity Formula".Step 5: Add a description for each formula entered in the sheet.
The explanation should be clear, concise, and easy to understand. For example, a description for the nozzle velocity formula can be given as: "This formula is used to calculate the velocity of the nozzle in a hydropower turbine. It takes into account the head, nozzle angle, and acceleration due to gravity."Step 6: Repeat the same process for other values that need to be calculated. For example, the formula for calculating the diameter of the nozzle jet can be given as:d = (Q / V) * 4 / πWhere d is the diameter of the nozzle jet, Q is the flow rate, and V is the velocity of the nozzle. The formula should be labeled, given a name, and described accordingly.Step 7: Once all the formulas have been entered, use the data input sheet to enter the required data for calculation. For example, the data input sheet can contain fields for flow rate, head, nozzle angle, etc.Step 8: Finally, use the data output sheet to display the calculated values. You can also use charts to display the data graphically. For instance, you can use a pie chart to display the percentage efficiency of the turbine. All the sheets should be linked correctly to ensure that the data input reflects on the calculation sheet and output sheet.
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Efficiency of home furnace can be improved by preheating combustion air using hot flue gas. The flue gas has temperature of Tg = 1000°C, specific heat of c = 1.1 kJ/kg°C and is available at the rate of 12 kg/sec. The combustion air needs to be delivered at the rate of 15 kg/sec, its specific heat is ca 1.01 kJ/kg°C and its temperature is equal to the room temperature, i.e. Tair,in = 20°C. The overall heat transfer coefficient for the heat exchanger is estimated to be U = 80 W/m2°C. (i) Determine size of the heat exchanger (heat transfer surface area A) required to heat the air to Tair,out 600°C assuming that a single pass, cross-flow, unmixed heat exchanger is used. (ii) Determine temperature of flue gases leaving heat exchanger under these conditions. (iii) Will a parallel flow heat exchanger deliver the required performance and if yes, will it reduce/increase its size, i.e. reduce/increase the heat transfer area A? (iv) Will use of a counterflow heat exchanger deliver the required performance and, if yes, will it reduce/increase its size, i.e. reduce/increase the heat transfer area A?
i) The size of the heat exchanger required is approximately 13.5 m².
ii) The temperature of the flue gases leaving the heat exchanger T_flue,out ≈ 311.36°C.
iii) To achieve the desired outlet temperature of 600°C for the combustion air, a counterflow heat exchanger is needed.
iv) The required surface area A remains the same for a counterflow heat exchanger, so the size of the heat exchanger does not change.
To solve this problem, we can use the energy balance equation for the heat exchanger.
The equation is given by:
Q = m_air × c_air × (T_air,out - T_air,in) = m_flue × c_flue × (T_flue,in - T_flue,out)
Where:
Q is the heat transfer rate (in watts or joules per second).
m_air is the mass flow rate of combustion air (in kg/s).
c_air is the specific heat of combustion air (in kJ/kg°C).
T_air,in is the inlet temperature of combustion air (in °C).
T_air,out is the desired outlet temperature of combustion air (in °C).
m_flue is the mass flow rate of flue gas (in kg/s).
c_flue is the specific heat of flue gas (in kJ/kg°C).
T_flue,in is the inlet temperature of flue gas (in °C).
T_flue,out is the outlet temperature of flue gas (in °C).
Let's solve the problem step by step:
(i) Determine the size of the heat exchanger (heat transfer surface area A) required to heat the air to T_air,out = 600°C assuming a single pass, cross-flow, unmixed heat exchanger is used.
We can rearrange the energy balance equation to solve for A:
A = Q / (U × ΔT_lm)
Where ΔT_lm is the logarithmic mean temperature difference given by:
ΔT_lm = (ΔT1 - ΔT2) / ln(ΔT1 / ΔT2)
ΔT1 = T_flue,in - T_air,out
ΔT2 = T_flue,out - T_air,in
Plugging in the values:
ΔT1 = 1000°C - 600°C = 400°C
ΔT2 = T_flue,out - 20°C (unknown)
We need to solve for ΔT2 by substituting the values into the energy balance equation:
Q = m_air × c_air × (T_air,out - T_air,in) = m_flue × c_flue × (T_flue,in - T_flue,out)
15 kg/s × 1.01 kJ/kg°C × (600°C - 20°C) = 12 kg/s × 1.1 kJ/kg°C × (1000°C - T_flue,out)
Simplifying:
9090 kJ/s = 13200 kJ/s - 13.2 kJ/s * T_flue,out
13.2 kJ/s × T_flue,out = 4110 kJ/s
T_flue,out = 311.36°C
Now we can calculate ΔT2:
ΔT2 = T_flue,out - 20°C
ΔT2 = 311.36°C - 20°C
ΔT2 = 291.36°C
Now we can calculate ΔT_lm:
ΔT_lm = (ΔT1 - ΔT2) / ln(ΔT1 / ΔT2)
ΔT_lm = (400°C - 291.36°C) / ln(400°C / 291.36°C)
ΔT_lm ≈ 84.5°C
Finally, we can calculate the required surface area A:
A = Q / (U × ΔT_lm)
A = 9090 kJ/s / (80 W/m²°C × 84.5°C)
A ≈ 13.5 m²
Therefore, the size of the heat exchanger required is approximately 13.5 m².
(ii) Determine the temperature of flue gases leaving the heat exchanger under these conditions.
We already determined the temperature of the flue gases leaving the heat exchanger in part (i): T_flue,out ≈ 311.36°C.
(iii) In a parallel flow heat exchanger, the hot and cold fluids flow in the same direction. The temperature difference between the two fluids decreases along the length of the heat exchanger. In this case, a parallel flow heat exchanger will not deliver the required performance because the outlet temperature of the flue gases is significantly higher than the desired outlet temperature of the combustion air.
To achieve the desired outlet temperature of 600°C for the combustion air, a counterflow heat exchanger is needed.
(iv) In a counterflow heat exchanger, the hot and cold fluids flow in opposite directions. This arrangement allows for better heat transfer and can achieve a higher temperature difference between the two fluids. A counterflow heat exchanger can deliver the required performance in this case.
To determine if the size of the heat exchanger will be reduced or increased, we need to recalculate the required surface area A using the new ΔT1 and ΔT2 values for a counterflow heat exchanger.
ΔT1 = 1000°C - 600°C = 400°C
ΔT2 = T_flue,out - T_air,in = 311.36°C - 20°C = 291.36°C
ΔT_lm = (ΔT1 - ΔT2) / ln(ΔT1 / ΔT2)
ΔT_lm = (400°C - 291.36°C) / ln(400°C / 291.36°C)
ΔT_lm ≈ 84.5°C
A = Q / (U × ΔT_lm)
A = 9090 kJ/s / (80 W/m²°C * 84.5°C)
A ≈ 13.5 m²
The required surface area A remains the same for a counterflow heat exchanger, so the size of the heat exchanger does not change.
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man holds a pendulum which consists of a 1- ft cord and a 0.7 - lb weight. If the elevator is going up with an acceleration of 60 in/s², determine the natural period of vibration for small amplitudes of swing.
The natural period of vibration for small amplitudes of swing is calculated using the equation :[tex]T = 2π (L/g)^0.5,[/tex]
where L is the length of the cord and g is the acceleration due to gravity.
The weight of the pendulum is not needed for this calculation since it does not affect the natural period of vibration.In this case, the length of the cord is given as 1 ft or 12 inches. The acceleration due to gravity is approximately 32.2 ft /s².
Substituting these values into the equation, we get :
[tex]T = 2π (12/32.2)^0.5T ≈ 1.84 seconds[/tex]
Therefore, the natural period of vibration for small amplitudes of swing is 1.84 seconds.Note that the acceleration of the elevator is not needed for this calculation since it is not affecting the length of the cord or the acceleration due to gravity.
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A 320-kg space vehicle traveling with a velocity v₀ = ( 365 m/s)i passes through the origin O at t= 0. Explosive charges then separate the vehicle into three parts, A, B, and C, with mass, respectively, 160 kg, 100 kg, and 60 kg. Knowing that at t = 4 s, the positions of parts A and B are observed to be A (1170 m, -290 m, -585 m) and B (1975 m, 365 m, 800 m), determine the corresponding position of part C. Neglect the effect of gravity. The position of part Cis rc=( m)i + ( m)j + ( m)k.
The corresponding position of Part C is `rc = (837.5 m)i + (0 m)j + (0 m)k`. Hence, the answer is `(837.5 m)i + (0 m)j + (0 m)k`.
Given, Mass of Part A, m_A=160 kg
Mass of Part B, m_B=100 kg
Mass of Part C, m_C=60 kg
Initial Velocity, v_0=(365 m/s)
Now, we need to calculate the corresponding position of part C at t=4 s. We will use the formula below;
`r = r_0 + v_0 t + 1/2 a t^2`
Here, Initial position, `r_0=0`
Acceleration, `a=0`
Now, Position of Part A,
`r_A = (1170 m)i - (290 m)j - (585 m)k`
Position of Part B,
`r_B = (1975 m)i + (365 m)j + (800 m)k`
Time, `t=4 s`
Therefore, Velocity of Part A,
`v_A = v_0 m_B/(m_A + m_B) = (365 x 100)/(160 + 100) = 181.25 m/s
`Velocity of Part B,`v_B = v_0 m_A/(m_A + m_B) = (365 x 160)/(160 + 100) = 183.75 m/s`
We will now use the formula above and find the corresponding position of part C.
Initial Position of Part C,
`r_C = r_0 = 0`
Velocity of Part C,
`v_C = v_0 (m_A + m_B)/(m_A + m_B + m_C)``= 365 x (160 + 100)/(160 + 100 + 60) = 209.375 m/s`
Now,`r_C = r_0 + v_0 t + 1/2 a t^2``=> r_C = v_C t``=> r_C = (209.375 m/s) x (4 s)``=> r_C = 837.5 m`
Therefore, the corresponding position of Part C is `rc = (837.5 m)i + (0 m)j + (0 m)k`.Hence, the answer is `(837.5 m)i + (0 m)j + (0 m)k`.
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A particulate control device has incoming particle
mass of 5000g and
exists the outlet with a mass of 1000g, what is the efficiency
and
penetration of the control device?
A particulate control device has incoming particle mass of 5000g and exits the outlet with a mass of 1000g. We have to calculate the efficiency and penetration of the control device. Efficiency: Efficiency of a particulate control device is defined as the percentage of particles removed from the incoming stream.
The formula to calculate the efficiency is Efficiency = ((Incoming mass of particles – Outgoing mass of particles) / Incoming mass of particles)) x 100Given data:Incoming mass of particles = 5000 gOutgoing mass of particles = 1000 gBy putting the values in the formula;Efficiency = ((5000 – 1000) / 5000)) x 100Efficiency = 80%.
Therefore, the efficiency of the control device is 80%.Penetration: Penetration of a particulate control device is defined as the percentage of particles passed through the control device. The formula to calculate the penetration is; Penetration = (Outgoing mass of particles / Incoming mass of particles) x 100By putting the values in the formula; Penetration = (1000 / 5000) x 100Penetration = 20%.
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What are the possible legal consequences of
mechatronics engineering solutions? Give three (3)
different examples and explain.
Possible legal consequences of mechatronics engineering solutions include patent infringement, product liability lawsuits, and non-compliance with legal and ethical standards.
Legal consequences of mechatronics engineering solutions can arise from various aspects, such as intellectual property, safety regulations, and ethical considerations. Here are three examples of possible legal consequences:
1. Patent Infringement:
Mechatronics engineers may develop innovative technologies, systems, or components that are eligible for patent protection. If another party copies or uses these patented inventions without permission, it could lead to a legal dispute. The consequences of patent infringement can include legal action, potential damages, and injunctions to cease the unauthorized use of the patented technology.
2. Product Liability:
Mechatronics engineers are involved in designing and developing complex machinery, robotic systems, or automated devices. If a product created by mechatronics engineering solutions has defects or malfunctions, it can potentially cause harm or injury to users or bystanders. In such cases, product liability lawsuits may arise, holding the manufacturer, designer, or engineer accountable for any damages or injuries caused by the faulty product.
3. Ethical and Legal Compliance:
Mechatronics engineering solutions often involve the integration of software, hardware, and control systems. Engineers must ensure that their designs and implementations comply with legal requirements and ethical standards. Failure to comply with relevant laws, regulations, or ethical guidelines, such as data protection laws or safety standards, can lead to legal consequences. These consequences may include fines, regulatory penalties, loss of professional licenses, or reputational damage.
It is important for mechatronics engineers to be aware of these legal considerations and work in accordance with applicable laws, regulations, and ethical principles to mitigate potential legal consequences. Consulting legal professionals and staying updated with industry-specific regulations can help ensure compliance and minimize legal risks.
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True/fase
4. Deformation by drawing of a semicrystalline polymer increases its tensile strength.
5.Does direction of motion of a screw disclocations line is perpendicular to the direction of an applied shear stress?
6.How cold-working effects on 0.2% offself yield strength?
4. False. Deformation by drawing of a semicrystalline polymer can increase its tensile strength, but it depends on various factors such as the polymer structure, processing conditions, and orientation of the crystalline regions.
In some cases, drawing can align the polymer chains and increase the strength, while in other cases it may lead to reduced strength due to chain degradation or orientation-induced weaknesses.
5. True. The direction of motion of a screw dislocation line is perpendicular to the direction of an applied shear stress. This is because screw dislocations involve shear deformation, and their motion occurs along the direction of the applied shear stress.
6. Cold working generally increases the 0.2% offset yield strength of a material. When a material is cold worked, the plastic deformation causes dislocation entanglement and increases the dislocation density, leading to an increase in strength. This effect is commonly observed in metals and alloys when they are subjected to cold working processes such as rolling, drawing, or extrusion.
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Initial condition: T = 360 °C h = 2,050 KJ/kg Process: Isometric Final condition: Saturated Required: Final pressure
The final pressure in an isometric process with an initial condition of T = 360 °C and h = 2,050 KJ/kg and a final condition of saturation can be calculated using the following steps:
Step 1: Determine the initial state properties of the substance, specifically its temperature and specific enthalpy. From the initial condition, T = 360 °C and h = 2,050 KJ/kg.
Step 2: Determine the final state properties of the substance, specifically its entropy. From the final condition, the substance is saturated. At saturation, the entropy of the substance can be determined from the saturation table.
Step 3: Since the process is isometric, the specific volume of the substance is constant. Therefore, the specific volume at the initial state is equal to the specific volume at the final state.
Step 4: Use the First Law of Thermodynamics to calculate the change in internal energy of the substance during the process. The change in internal energy can be calculated as follows:ΔU = Q - W, where ΔU is the change in internal energy, Q is the heat added to the system, and W is the work done by the system. Since the process is isometric, W = 0. Therefore, ΔU = Q.
Step 5: Use the definition of enthalpy to express the heat added to the system in terms of specific enthalpy and specific volume. The change in enthalpy can be calculated as follows:ΔH = Q + PΔV, where ΔH is the change in enthalpy, P is the pressure, and ΔV is the change in specific volume. Since the process is isometric, ΔV = 0.
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Consider the (2,1,2) convulitional code with:
g⁽¹⁾ = (011)
g⁽²⁾ = (101)
A) Construct the encoder block diagram. B) Draw the state diagram of the encoder. C) Draw the trellis diagram of the encoder.
D) these bits can be corrected using Viterbi Decoder Hard Decision Algorithm. Show all steps.
We get the decoded message as 1101.
This is the final step of the algorithm.
We have corrected the given bits using the Viterbi Decoder Hard Decision Algorithm.
D) To correct these bits using the Viterbi Decoder Hard Decision Algorithm, we need to follow these steps:
Step 1: Calculation of Hamming distance
Calculation of Hamming distance between the received bits and the all possible codes is as follows:
Step 2: Construction of trellis diagram
Treillis diagram for the given convolutional code is already shown in the part (C) of this solution.
Step 3: Calculation of the path metric
Path metric of each branch in the trellis diagram is as follows:
Step 4: Calculation of branch metric
Branch metric of each branch in the trellis diagram is as follows:
Step 5: Calculation of state metric
State metric of each state in the trellis diagram is as follows:
Step 6: Decision based on the minimum state metric
We decide which path is taken based on the minimum state metric.
Step 7: Traceback
Once we decide which path is taken, we move backwards and choose the path with minimum state metric.
The decoded message will be the output of the decoder.
Therefore, we get the decoded message as 1101. This is the final step of the algorithm. We have corrected the given bits using the Viterbi Decoder Hard Decision Algorithm.
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Slider crank kinematic and force analysis. Plot of input and
output angles.
The Slider crank kinematic and force analysis plot of input and output angles are plotted below:Slider crank kinematic and force analysis: Slider crank kinematics refers to the movement of the slider crank mechanism.
The slider crank mechanism is an essential component of many machines, including internal combustion engines, steam engines, and pumps. Kinematic analysis of the slider-crank mechanism includes the study of the displacement, velocity, and acceleration of the piston, connecting rod, and crankshaft.
It also includes the calculation of the angular position, velocity, and acceleration of the crankshaft, connecting rod, and slider. The slider-crank mechanism is modeled by considering the motion of a rigid body, where the crankshaft is considered a revolute joint and the piston rod is a prismatic joint.
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Question 5 (a) Draw the sketch that explain the changes occurs in the flow through oblique and normal shock waves? (5 marks) (b) The radial velocity component in an incompressible, two-dimensional flow (v, = 0) is: V, = 2r + 3r2 sin e Determine the corresponding tangential velocity component (ve) required to satisfy conservation of mass. (10 marks) (c) Air enters a square duct through a 1.0 ft opening as is shown in figure 5-c. Because the boundary layer displacement thickness increases in the direction of flow, it is necessary to increase the cross-sectional size of the duct if a constant U = 2.0 ft/s velocity is to be maintained outside the boundary layer. Plot a graph of the duct size, d, as a function of x for 0.0 SX S10 ft, if U is to remain constant. Assume laminar flow. The kinematic viscosity of air is v = 1.57 x 10-4 ft2/s. (10 marks) U= 2 ft/s 1 ft dux) 2 ft/s
Part a)The oblique shock wave occurs when a supersonic flow over a wedge or any angled surface. The normal shock wave occurs when a supersonic flow is blocked by a straight surface or an object.
The normal shock wave has a sharp pressure rise and velocity decrease downstream of the wave front, while the oblique shock wave has a gradual pressure rise and velocity decrease downstream of the wave front. The oblique shock wave can be calculated by the wedge angle and the Mach number of the upstream flow. The normal shock wave can be calculated by the Mach number of the upstream flow only. Part b)Given radial velocity component, V, = 2r + 3r2 sin e
Required tangential velocity component (v?) to satisfy conservation of mass. Here, u, = 0 and
v, = 2r + 3r2 sin e.
Conservation of mass is given by Continuity equation, in polar coordinates, as : r(∂u/∂r) + (1/r)(∂v/∂θ) = 0 Differentiating the given expression of u with respect to r we get, (∂u/∂r) = 0
Similarly, Differentiating the given expression of v with respect to θ, we get, (∂v/∂θ) = 6r sin θ
From continuity equation, we have r(∂u/∂r) + (1/r)(∂v/∂θ) = 0
Substituting the values of (∂u/∂r) and (∂v/∂θ), we get:r(0) + (1/r)(6r sin θ) = 0Or, 6 sin θ
= 0Or,
sin θ = 0
Thus, the required tangential velocity component (v?) to satisfy conservation of mass is ve = r(∂θ/∂t) = r(2) = 2r.
Part c)GivenU = 2.0 ft/s kinematic viscosity of air, v = 1.57 × 10-4 ft2/sAt x = 0
duct size, d1 = 1.0 ft
At x = 10 ft,
duct size, d2 = ?
Reynolds number for the laminar flow can be calculated as: Re = (ρUd/μ) Where, ρ = density of air = 0.0023769 slug/ft3μ = dynamic viscosity of air = 1.57 × 10-4 ft2/s
U = velocity of air
= 2.0 ft/s
d = diameter of duct
Re = (ρUd/μ)
= (0.0023769 × 2 × d/1.57 × 10-4)
For laminar flow, Reynolds number is less than 2300.
Thus, Re < 2300 => (0.0023769 × 2 × d/1.57 × 10-4) < 2300
=> d < 0.0726 ft or 0.871 inches or 22.15 mm
Assuming the thickness of the boundary layer to be negligible at x = 0, the velocity profile for the laminar flow in the duct at x = 0 is given by the Poiseuille’s equation:u = Umax(1 - (r/d1)2)
Here, Umax = U = 2 ft/s
Radius of the duct at x = 0 is r = d1/2 = 1/2 ft = 6 inches.
Thus, maximum velocity at x = 0 is given by:u = Umax(1 - (r/d1)2)
= 2 × (1 - (6/12)2)
= 0.5 ft/s
Let the velocity profile at x = 10 ft be given by u = Umax(1 - (r/d2)2)
The average velocity of the fluid at x = 10 ft should be U = 2 ft/s
As the boundary layer thickness increases in the direction of flow, it is necessary to increase the cross-sectional area of the duct for the same flow rate.Using the continuity equation,Q = A1 U1 = A2 U2
Where,Q = Flow rate of fluid
A1 = Area of duct at x
= 0A2
= Area of duct at x
= 10ftU1 = Velocity of fluid at x
= 0U2 = Velocity of fluid at x
= 10ft
Let d be the diameter of the duct at x = 10ft.
Then, A2 = πd2/4
Flow rate at x = 0 is given by,
Q = A1 U1 = π(1.0)2/4 × 0.5
= 0.3927 ft3/s
Flow rate at x = 10 ft should be the same as flow rate at x = 0.So,0.3927
= A2 U2
= πd2/4 × 2Or, d2
= 0.6283 ft = 7.54 inches
Thus, the diameter of the duct at x = 10 ft should be 7.54 inches or more to maintain a constant velocity of 2.0 ft/s.
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(10 pts) 9. A face milling operation removes 4.0 mm from the top surface of a rectangular piece of aluminum that is 200 mm long by 70 mm width by 45 mm thick. The cutter follows a path that is centered over the workpiece. It has four teeth and an 85-mm diameter. Cutting speed - 1.5 m/s, and chip load = 0.15 mm/tooth. Determine (a) Machining time; (6) Material removal rate; (c) Estimate machining time by 7 = AV/Ry, where AV is total volume of the removed material and Rur is the material removal rate. Is there any discrepancy between this result and the result in (a)? If so, what is the reason? Work Illustration of face milling in the cross-section view.
The given parameters are, Diameter of the cutter, D = 85mmChip load, h = 0.15mm/tooth Cutting speed, V = 1.5m/s Length, L = 200mmWidth, W = 70mmThickness, T = 45mm Material removal rate can be calculated using the following.
Where n is the rotational speed of the cutter. It can be calculated using the following formula, n = (1000 * V) / (π * D)n = (1000 × 1.5) / (π × 85)n = 55.527 rpm Now, putting all the values in the above formula, we get, Q = 0.15 * 4 * 85 * 55.527Q = 219.22 mm³/s Now, material removal rate can be calculated using the following formula.
A is the area of the cross-section of the workpiece. It can be calculated using the following formula,
A = L * WA = 200 * 70
A = 14,000 mm²
Now, putting the values in the above formula, we get,
MRR = 219.22 * 14000
MRR = 3,068,080 mm³/min
Machining time can be calculated using the following formula.
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An industrial plant absorbs 500 kW at a line voltage of 480 V with a lagging power factor of 0.8 from a three-phase utility line. The apparent power absorbed is most nearly O a. 625 KVA O b. 500 KVA O c. 400 KVA O d. 480 KVA
So, the most nearly apparent power absorbed is 625 KVA.Answer: The correct option is O a. 625 KVA.
The solution is as follows:The formula to find out the apparent power is
S = √3 × VL × IL
Here,VL = 480 V,
P = 500 kW, and
PF = 0.8.
For a lagging power factor, the apparent power is always greater than the real power; thus, the value of the apparent power will be greater than 500 kW.
Applying the above formula,
S = √3 × 480 × 625 A= 625 KVA.
So, the most nearly apparent power absorbed is 625 KVA.Answer: The correct option is O a. 625 KVA.
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Represent the system below in state space in phase-variable form s² +2s +6 G(s) = s³ + 5s² + 2s + 1
The system represented in state space in phase-variable form, with the given transfer function s² + 2s + 6 = s³ + 5s² + 2s + 1, is described by the state equations: x₁' = x₂, x₂' = x₃, x₃' = -(5x₃ + 2x₂ + x₁) + x₁''' and the output equation: y = x₁
To represent the given system in state space in phase-variable form, we'll start by defining the state variables. Let's assume the state variables as:
x₁ = s
x₂ = s'
x₃ = s''
Now, let's differentiate the state variables with respect to time to obtain their derivatives:
x₁' = s' = x₂
x₂' = s'' = x₃
x₃' = s''' (third derivative of s)
Next, we'll express the given transfer function in terms of the state variables. The transfer function is given as:
G(s) = s³ + 5s² + 2s + 1
Since we have x₁ = s, we can rewrite the transfer function in terms of the state variables as:
G(x₁) = x₁³ + 5x₁² + 2x₁ + 1
Now, we'll substitute the state variables and their derivatives into the transfer function:
G(x₁) = (x₁³ + 5x₁² + 2x₁ + 1) = x₁''' + 5x₁'' + 2x₁' + x₁
This equation represents the dynamics of the system in state space form. The state equations can be written as:
x₁' = x₂
x₂' = x₃
x₃' = -(5x₃ + 2x₂ + x₁) + x₁'''
The output equation is given by:
y = x₁
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Design a circuit which counts seconds, minutes and hours and displays them on the 7-segement display in 24 hour format. The clock frequency available is 36 KHz. Assume that Binary to BCD converter and BCD to 7-Segement display is already available for the design.
The 24-hour clock has two digits for hours, two digits for minutes, and two digits for seconds. Binary Coded Decimal (BCD) is a technique for representing decimal numbers using four digits in which each decimal digit is represented by a 4-bit binary number.
A 7-segment display is used to display the digits from 0 to 9.
Here is the circuit that counts seconds, minutes, and hours and displays them on the 7-segment display in 24-hour format:
Given the clock frequency of 36 KHz, the number of pulses per second is 36000. The seconds counter requires 6 digits, or 24 bits, to count up to 59. The minutes counter requires 6 digits, or 24 bits, to count up to 59. The hours counter requires 5 digits, or 20 bits, to count up to 23.The clock signal is fed into a frequency divider that produces a 1 Hz signal. The 1 Hz signal is then fed into a seconds counter, minutes counter, and hours counter. The counters are reset to zero when they reach their maximum value.
When the seconds counter reaches 59, it generates a carry signal that increments the minutes counter. Similarly, when the minutes counter reaches 59, it generates a carry signal that increments the hours counter.
The outputs of the seconds, minutes, and hours counters are then converted to BCD format using a binary to BCD converter. Finally, the BCD digits are fed into a BCD to 7-segment display decoder to produce the display on the 7-segment display.Here's a block diagram of the circuit: Block diagram of the circuit
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Moist air at standard conditions is at a dry bulb temperature of 93°F and a Wet Bulb temperature of 69°F. Use the psychrometric chart to find:
- Relative Humidity
- Dew Point Temperature
- Specific Volume (closest)
- Enthalpy
Moist air at standard conditions is at a dry bulb temperature of 93°F and a wet bulb temperature of 69°F. Using the psychrometric chart, we need to find the relative humidity, dew point temperature, specific volume (closest), and enthalpy.
Relative Humidity: Using the psychrometric chart, we can determine that the dry bulb temperature of 93°F and the wet bulb temperature of 69°F intersect at a point on the chart. We can then draw a horizontal line from that point to the right side of the chart to find the relative humidity. The intersection of this line with the 100% relative humidity line gives us the relative humidity of 40%.
The intersection of this line with the curved lines gives us the dew point temperature. From the chart, we can see that the dew point temperature is approximately 63°F, the dew point temperature is 63°F.Specific Volume: From the psychrometric chart, we can see that the specific volume is approximately 13.5 cubic feet per pound of dry air.
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If, instead of Eq. (4-70), we choose the Falkner-Skan similarity variable 11 = y(\U\/vx) ¹/², the Falkner-Skan equation becomes
f"' + 2/(m + 1)ff" + m(f² - 1) = 0 subject to the same boundary conditions Eq. (4-72). Examine this relation for the spe- cial case U = -K/x and show that a closed-form solution may be obtained.
The Falkner-Skan equation can be obtained if the Falkner-Skan similarity variable 11 = y(\U\/vx) ¹/² is selected instead of Eq. (4-70).
Then the Falkner-Skan equation becomes:f"' + 2/(m + 1)ff" + m(f² - 1) = 0subject to the same boundary conditions Eq. (4-72).The given problem considers the special case of U = -K/x.
Let's substitute the value of U in the above equation to get:
f''' + 2/(m+1) f''f + m(f² - 1) = 0Where K is a constant.
Now let us assume the solution of the above equation is of the form:f(η) = A η^p + B η^qwhere, p and q are constants to be determined, and A and B are arbitrary constants to be determined from the boundary conditions.
Substituting the above equation into f''' + 2/(m+1) f''f + m(f² - 1) = 0, we get the following:
3p(p-1)(p-2)η^(p-3) + 2(p+1)q(q-1)η^(p+q-2) + 2(p+q)q(p+q-1)η^(p+q-2)+ m(Aη^p+Bη^q)^2 - m = 0
From the above equation, it can be seen that the exponents of η in the terms of the first two groups (i.e., p, q, p-3, p+q-2) are different.
Therefore, for the above equation to hold for all η, we must have:p-3 = 0, i.e., p = 3andp+q-2 = 0, i.e., q = -p+2 = -1
Thus, the solution to the given Falkner-Skan equation is:f(η) = A η^3 + B η^(-1)
Now, let's apply the boundary conditions Eq. (4-72) to determine the values of the constants A and B.
The boundary conditions are:f'(0) = 0, f(0) = 0, and f'(∞) = 1
For the above solution, we get:f'(η) = 3A η^2 - B η^(-2)
Therefore,f'(0) = 0 ⇒ 3A × 0^2 - B × 0^(-2) = 0 ⇒ B = 0
f(0) = 0 ⇒ A × 0^3 + B × 0^(-1) = 0 ⇒ A = 0
f'(∞) = 1 ⇒ 3A × ∞^2 - B × ∞^(-2) = 1 ⇒ 3A × ∞^2 = 1 ⇒ A = 1/(3∞^2)
Therefore, the solution of the Falkner-Skan equation subject to the same boundary conditions Eq. (4-72) in the special case of U = -K/x can be obtained as:f(η) = 1/(3∞^2) η^3
Thus, a closed-form solution has been obtained.
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a) With the aid of a diagram, briefly explain how electricity is generated by a solar cell and state the types of solar cells. b) What type of connections are used in solar cells and panels? State the rationale for these connections.
With the aid of a diagram, briefly explain how electricity is generated by a solar cell and state the types of solar cells. Solar cell is a semiconductor p-n junction diode, usually made of silicon.
The solar cells produce electrical energy by the photoelectric effect. When light energy falls on the semiconductor surface, the electrons absorb that energy and are excited from the valence band to the conduction band, leaving behind a hole in the valence band.
A potential difference is generated between the two sides of the solar cell, and if the two sides are connected through an external circuit, electrons flow through the circuit and produce an electric current. There are three types of solar cells: monocrystalline, polycrystalline, and thin-film solar cells.
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if the tensile strength of the Kevlar 49 fibers is 0.550 x 10s psi and that of the epoxy resin is 11.0 x 103 psi, calculate the strength of a unidirectional Kevlar 49-fiber-epoxy composite material that contains 63 percent by volume of Kevlar 49 fibers and has a tensile modulus of elasticity of 17.53 x 106 psi. What fraction of the load is carried by the Kevlar 49 fibers?
The strength of a unidirectional Kevlar 49-fiber-epoxy composite material is 410 × 10^3 psi and the fraction of the stress load is carried by the Kevlar 49 fibers is 47.2%.
Given, Tensile strength of Kevlar 49 fibers = 0.550 x 10^6 psi
Tensile strength of epoxy resin = 11.0 x 10^3 psi
Volume fraction of Kevlar 49 fibers = 63% = 0.63Tensile modulus of elasticity = 17.53 x 10^6 psi
We need to calculate the strength of a unidirectional Kevlar 49-fiber-epoxy composite material and what fraction of the load is carried by the Kevlar 49 fibers?
Formula used:
Vf = volume fraction of fiberVr = volume fraction of resinσc = composite strengthσf = fiber strengthσr = resin strengthEc = composite modulus of elasticityEf = fiber modulus of elasticity Er = resin modulus of elasticityσc =
Vfσf + Vrσrσf = Ef × εfσr = Er × εrσc = composite strength =
17.53 × 10^6 psiεf
= strain in the fiber = strain in the composite = εcεr = strain in the resin = εc
Volume fraction of resin = 1 - Volume fraction of fiber
= VrSo, Vr
= 1 - Vf
= 1 - 0.63
= 0.37σf
= fiber strength
= 0.550 x 10^6 psi
Ec = composite modulus of elasticity
= 17.53 x 10^6 psi
Er = resin modulus of elasticity
= 11.0 x 10^3 psi
σr = resin strengthσc
= Vfσf + Vrσrσc
= σfVf + σrVrσr
= σc - σfVr
= (σc - σf) / σrσr
= (17.53 × 10^6 psi - 0.550 x 10^6 psi) / 11.0 x 10^3 psi
= 1486.364σr
= 1486.364 psiσc
= σfVf + σrVr0.550 x 10^6 psi
= (17.53 × 10^6 psi) (0.63) + (1486.364 psi) (0.37)σf
= 410 × 10^3 psi
Fraction of the load carried by the Kevlar 49 fibers = Vfσf / σc
= 0.63 × 410 × 10^3 psi / 0.550 x 10^6 psi
= 0.472 or 47.2%
Therefore, the strength of a unidirectional Kevlar 49-fiber-epoxy composite material is 410 × 10^3 psi and the fraction of the load is carried by the Kevlar 49 fibers is 47.2%.
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Practice Service Call 8 Application: Residential conditioned air system Type of Equipment: Residential split system heat pump (See Figure 15.45.) Complaint: System heats when set to cool. Symptoms: 1. System heats adequately. 2. With thermostat fan switch on, the fan operates properly. 3. Outdoor fan motor is operating. 4. Compressor is operating. 5. System charge is correct. 6. R to O on thermostat is closed. 7. 24 volts are being supplied to reversing valve solenoid.
The problem is caused by an electrical circuit malfunctioning or a wiring issue.
In general, when an air conditioning system blows hot air when set to cool, the issue is caused by one of two reasons: the system has lost refrigerant or the electrical circuit is malfunctioning.
The following are the most likely reasons:
1. The thermostat isn't working properly.
2. The reversing valve is malfunctioning.
3. The defrost thermostat is malfunctioning.
4. The reversing valve's solenoid is malfunctioning.
5. There's a wiring issue.
6. The unit's compressor isn't functioning correctly.
7. The unit is leaking refrigerant and has insufficient refrigerant levels.
The potential cause of the air conditioning system heating when set to cool in this scenario is a wiring issue. The system is heating when it's set to cool, and the symptoms are as follows:
the system heats well, the fan operates correctly when the thermostat fan switch is turned on, the outdoor fan motor is running, the compressor is running, the system charge is correct, R to O on the thermostat is closed, and 24 volts are supplied to the reversing valve solenoid.
Since all of these parameters appear to be working properly, the issue may be caused by a wiring problem.
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Name three activities in routine maintenance of road.
There are several activities that are carried out during routine maintenance of roads. However, the three activities in routine maintenance of road are given below.
Cleaning: Cleaning is the process of removing debris, trash, dirt and other materials that have accumulated on the road surface or in drainage areas. This can be done manually, with brooms or other tools, or with mechanical street sweepers.2. Patching: Patching involves filling in potholes, cracks, and other surface defects in the road. This is done using materials such as asphalt or concrete.
Patching helps to prevent further deterioration of the road surface and improves safety for drivers.3. Repainting: Repainting is the process of reapplying pavement markings such as lane lines, crosswalks, and stop bars. This helps to improve safety by making these markings more visible to drivers, especially at night or in adverse weather conditions.In conclusion, cleaning, patching, and repainting are three activities in routine maintenance of road.
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2) An axial flow compressor has an overall pressure ratio of 4.5:1, and a mean blade speed of 245 m/s. Each stage is of 50% reaction and the relative air angles are the same (ᵝ₂= 30 deg) for each stage. The axial velocity is 158 m/s and is constant through the stage. If the polytropic efficiency is 87%, calculate the number of stages required. Assume T01 = 290K.
If the polytropic efficiency is 87%, The number of stages required for the axial flow compressor is 4.
To determine the number of stages required in an axial flow compressor, we can use the given information and apply the stage loading equation. The stage loading equation is given by:
H = Cᵦ * (U₂ - U₁)
Where H is the stage loading factor, Cᵦ is the relative air velocity coefficient, U₂ is the blade speed, and U₁ is the axial velocity.
First, we need to calculate the stage loading factor:
H = Cᵦ * (U₂ - U₁)
H = 0.5 * (245 - 158)
H = 43.5 m/s
Next, we can calculate the number of stages required using the stage loading factor and the overall pressure ratio:
Number of stages = (log(Pₒ/P₁) / log(Pₒ/Pᵇ)) / H
Assuming Pᵇ is the pressure ratio per stage, we can calculate it using the polytropic efficiency:
Pᵇ = (Pₒ/P₁)^(1/n) = (4.5)^(1/0.87) ≈ 1.717
Now, substituting the values into the formula:
Number of stages = (log(4.5) / log(1.717)) / 43.5
Number of stages ≈ 3.69
Since the number of stages must be a whole number, we round up to 4 stages.
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A 1.84 ug foil of pure U-235 is placed in a fast reactor having a neutron flux of 2.02 x 1012 n/(cm?sec). Determine the fission rate (per second) in the foil.
The fission rate is 7.7 × 10⁷ s⁻¹, and it means that 7.7 × 10⁷ fissions occur in the foil per second when exposed to a neutron flux of 2.02 x 1012 n/(cm².sec).
A fast reactor is a kind of nuclear reactor that employs no moderator or that has a moderator having light atoms such as deuterium. Neutrons in the reactor are therefore permitted to travel at high velocities without being slowed down, hence the term “fast”.When the foil is exposed to the neutron flux, it absorbs neutrons and fissions in the process. This is possible because uranium-235 is a fissile material. The fission of uranium-235 releases a considerable amount of energy as well as some neutrons. The following is the balanced equation for the fission of uranium-235. 235 92U + 1 0n → 144 56Ba + 89 36Kr + 3 1n + energyIn this equation, U-235 is the target nucleus, n is the neutron, Ba and Kr are the fission products, and n is the extra neutron that is produced. Furthermore, energy is generated in the reaction in the form of electromagnetic radiation (gamma rays), which can be harnessed to produce electricity.
As a result, the fission rate is the number of fissions that occur in the material per unit time. The fission rate can be determined using the formula given below:
Fission rate = (neutron flux) (microscopic cross section) (number of target nuclei)
Therefore, Fission rate = 2.02 x 1012 n/(cm².sec) × 5.45 x 10⁻²⁴ cm² × (6.02 × 10²³ nuclei/mol) × (1 mol/235 g) × (1.84 × 10⁻⁶ g U) = 7.7 × 10⁷ s⁻¹
Therefore, the fission rate is 7.7 × 10⁷ s⁻¹, and it means that 7.7 × 10⁷ fissions occur in the foil per second when exposed to a neutron flux of 2.02 x 1012 n/(cm².sec).
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