Equilibrium of a body requires both a balance of forces and balance of moments. This statement is True. The equilibrium of a body refers to the state where there is no acceleration. It can be categorized into two, the static and dynamic equilibrium. The static equilibrium occurs when the object is at rest, and the dynamic equilibrium happens when the object is in a constant motion.
Both of these types require a balance of forces and moments to be attained.In physics, force is a quantity that results from the interaction between two objects, and it's measured in newtons. It can be categorized into two, contact forces, and non-contact forces. Contact forces involve physical contact between two objects, while non-contact forces are those that occur without physical contact. According to Newton's first law of motion, a body in equilibrium will remain in that state until acted upon by an unbalanced force.
Therefore, when an object is in equilibrium, both the forces and moments should be balanced for the equilibrium to exist.In conclusion, it's true that equilibrium of a body requires both a balance of forces and balance of moments.
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2) A linear elastic SDOF system is given below with Tn= 1.1 s, m = 1 kg, 5 = 5 %, u(0) = 0, u(0) = 0. Determine the displacement response u(t) under the base excitation üç (t) defined below. Use At = 0.1 s in calculations. 0.6 U m i A oli 0,2 013 014 015 kc -0.4 Time (s)
Given values:Tn = 1.1 s, m = 1 kg, ξ = 5%, u(0) = 0, u'(0) = 0.At = 0.1 s
And base excitation üc(t) is given as below:
0.6 Umi sin (2πti) for 0 ≤ t ≤ 0.2 s0.2 sin (2π(501)(t - 0.2)) for 0.2 ≤ t ≤ 0.3 s-0.4 sin (2π(501)(t - 0.3)) for 0.3 ≤ t ≤ 0.4 sThe undamped natural frequency can be calculated as
ωn = 2π / Tnωn = 2π / 1.1ωn = 5.7 rad/s
The damped natural frequency can be calculated as
ωd = ωn √(1 - ξ²)ωd = 5.7 √(1 - 0.05²)ωd = 5.41 rad/s
The damping coefficient can be calculated as
k = m ξ ωnk = 1 × 0.05 × 5.7k = 0.285 Ns/m
The spring stiffness can be calculated as
k = mωd² - ξ²k = 1 × 5.41² - 0.05²k = 14.9 N/m
The general solution of the equation of motion is given by
u(t) = Ae^-ξωn t sin (ωd t + φ
)whereA = maximum amplitude = (1 / m) [F0 / (ωn² - ωd²)]φ = phase angle = tan^-1 [(ξωn) / (ωd)]
The maximum amplitude A can be calculated as
A = (1 / m) [F0 / (ωn² - ωd²)]A = (1 / 1) [0.6 Um / ((5.7)² - (5.41)²)]A = 0.2219
UmThe phase angle φ can be calculated astanφ = (ξωn) / (ωd)tanφ = (0.05 × 5.7) / (5.41)tanφ = 0.0587φ = 3.3°
Displacement response u(t) can be calculated as:for 0 ≤ t ≤ 0.2 s, the displacement response u(t) isu(t) = 0.2219 Um e^(-0.05 × 5.7t) sin (5.41t + 3.3°)for 0.2 ≤ t ≤ 0.3 s, the displacement response
u(t) isu(t) = 0.2219 Um e^(-0.05 × 5.7t) sin (5.41t - 30.35°)for 0.3 ≤ t ≤ 0.4 s, t
he displacement response
u(t) isu(t) = 0.2219 Um e^(-0.05 × 5.7t) sin (5.41t + 57.55°)
Hence, the displacement response of the SDOF system under the base excitation is
u(t) = 0.2219 Um e^(-0.05 × 5.7t) sin (5.41t + φ) for 0 ≤ t ≤ 0.2 s, 0.2 ≤ t ≤ 0.3 s, and 0.3 ≤ t ≤ 0.4 s, whereφ = 3.3° for 0 ≤ t ≤ 0.2 su(t) = 0.2219 Um e^(-0.05 × 5.7t) sin (5.41t - 30.35°) for 0.2 ≤ t ≤ 0.3 su(t) = 0.2219 Um e^(-0.05 × 5.7t) sin (5.41t + 57.55°) for 0.3 ≤ t ≤ 0.4 s. The response is plotted below.
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Choose the correct statement for the flow inside tube
The viscus effects and velocity changes are significant in boundary layer conditions.
Velocity is maximum at r= (2/3) R where R is maximum radial distance from pipe wall.
In Fully developed flow velocity is function of both r and x.
All of the above
Q2-Select the true statement.
Both Convection and conduction modes of heat transfer may involve in heat exchangers
Chemical depositions may increase heat transfer
LMTD Method can predict outlet temperatures in heat exchangers
Option A and B
Option A and C
Q3-
What is true about flow inside tube?
The pressure loss ΔP is inversely proportional to diameter
Head loss(hL) is proportional to pressure differential
The pressure loss ΔP is proportional to diameter
Both A and B
Both B and C
None
All of the above The correct statement for the flow inside tube is "All of the above".
Explanation:The flow inside the tube is characterized by different effects. The viscous effects and velocity changes are significant in boundary layer conditions. Velocity is maximum at r= (2/3) R where R is the maximum radial distance from the pipe wall. In Fully developed flow velocity is a function of both r and x. Hence all the given statements are true for the flow inside the tube.Q2. Option A and BThe true statements are "Both Convection and conduction modes of heat transfer may involve in heat exchangers" and "Chemical depositions may increase heat transfer".Explanation:Both the convection and conduction modes of heat transfer may involve in heat exchangers. Chemical depositions may increase heat transfer. Hence, option A and B are the true statements.Q3. Both B and CThe true statement is "Both B and C".Explanation:The pressure loss ΔP is proportional to diameter. Head loss(hL) is proportional to pressure differential. Hence, both statements B and C are true.
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(i) determine the transfer function from u to y; (ii) if the system is stable or not; (iii) Compute the location of the zeros and poles. d²x = -x + 4u, dy dt =y+x+u dt²
The problem statement is given as follows:d²x = -x + 4u, dy dt = y + x + u dt²In this problem statement, we have been asked to determine the transfer function from u to y, the stability of the system, and the location of the zeros and poles.
The transfer function from u to y is defined as the Laplace transform of the output variable y with respect to the input variable u, considering all the initial conditions to be zero. Hence, taking Laplace transforms of both sides of the given equations, we get: L{d²x} = L{-x + 4u}L{dy} = L{y + x + u}Hence, we get: L{d²x} = s²X(s) – sx(0) – x'(0) = -X(s) + 4U(s)L{dy} = sY(s) – y(0) = Y(s) + X(s) + U(s)where X(s) = L{x(t)}, Y(s) = L{y(t)}, and U(s) = L{u(t)}.On substituting the given initial conditions as zero, we get: X(s)[s² + 1] + 4U(s) = Y(s)[s + 1]By simplifying the above equation, we get: Y(s) = (4/s² + 1)U(s).
Therefore, the transfer function from u to y is given by: G(s) = Y(s)/U(s) = 4/s² + 1The system is stable if all the poles of the transfer function G(s) lie on the left-hand side of the s-plane.
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Water at 20◦C flows in a 9 cm diameter pipe under fully
developed conditions. Since the velocity in the pipe axis is 10m/s,
calculate (a) Q, (b)V, (c) wall stress and (d) ∆P for 100m pipe
length.
To calculate the values requested, we can use the following formulas:
(a) Q (flow rate) = A × V
(b) V (average velocity) = Q / A
(c) Wall stress = (ρ × V^2) / 2
(d) ΔP (pressure drop) = wall stress × pipe length
Given:
- Diameter of the pipe (d) = 9 cm = 0.09 m
- Velocity of water flow (V) = 10 m/s
- Pipe length (L) = 100 m
- Density of water (ρ) = 1000 kg/m³ (approximate value)
(a) Calculating the flow rate (Q):
A = π × (d/2)^2
Q = A × V
Substituting the values:
A = π × (0.09/2)^2
Q = π × (0.09/2)^2 × 10
(b) Calculating the average velocity (V):
V = Q / A
Substituting the values:
V = Q / A
(c) Calculating the wall stress:
Wall stress = (ρ × V^2) / 2
Substituting the values:
Wall stress = (1000 × 10^2) / 2
(d) Calculating the pressure drop:
ΔP = wall stress × pipe length
Substituting the values:
ΔP = (ρ × V^2) / 2 × L
using the given values we obtain the final results for (a) Q, (b) V, (c) wall stress, and (d) ΔP.
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Quin-Bode Mat The forward path wander action of a uniry feedback control system is: 140 G(s) = s(s+15) Analytically determine the resonant peak My, resonant frequency or, and budwidth BW the chualpsystem
A uniry feedback control system has a forward path wander action, which is determined analytically. The given equation for a uniry feedback control system is 140 G(s) = s(s+15).
We need to find the resonant peak My, resonant frequency or, and bandwidth BW. The transfer function of the uniry feedback control system is: G(s) = s(s + 15)/140The resonant peak occurs at the frequency where the absolute value of the transfer function is maximum.
Thus, we need to find the maximum value of |G(s)|.Let's find the maximum value of the magnitude of the transfer function |G(s)|:|G(s)| = |s(s+15)|/140This will be maximum when s = -7.5So, |G(s)|max = |-7.5*(7.5+15)|/140= 84.375/140= 0.602Let's now find the frequency where this maximum value occurs.
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Two normal stresses of equal magnitude of 5, but of opposite signs, act at an stress element in perpendicular directions x and y. The shear stress acting in the xy-plane at the plane is zero. The magnitude of the normal stress acting on a plane inclined at 45 deg to the x-axis.
O None of these
O 5/2
O 25
O 5/4
O 0
Given data: Normal stresses of equal magnitude = 5Opposite signs, Act at an stress element in perpendicular directions x and y.The shear stress acting in the xy-plane at the plane is zero. The plane is inclined at 45° to the x-axis.
Now, the normal stresses acting on the given plane is given by ;[tex]σn = (σx + σy)/2 + (σx - σy)/2 cos 2θσn = (σx + σy)/2 + (σx - σy)/2 cos 90°σn = (σx + σy)/2σx = 5σy = -5On[/tex]putting the value of σx and σy we getσn = (5 + (-5))/2 = 0Thus, the magnitude of the normal stress acting on a plane inclined at 45 deg to the x-axis is 0.Answer: The correct option is O 0.
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Find the current drawn by a 20 hp, 440 V three-phase motor operating at full load with 90% efficiency and 0.9 lagging power factor.
Calculate the values of P and Q consumed by the motor. (1 hp = 746 W)
A three-phase AC induction motor draws a current of 28.96 A at full load. The power consumed by the motor is 14.9 kW.
Given that the motor has 90% efficiency and a power factor of 0.9, the apparent power consumed by the motor is 16.56 kVA.
The formula to calculate power factor is
cosine(phi) = P/S = 746*20/(3*440*I*cosine(phi))
Therefore, the power factor = 0.9 or cos(phi) = 0.9
The real power P consumed by the motor is P = S * cosine(phi) or P = 16.56 kVA * 0.9 = 14.9 kW
The reactive power Q consumed by the motor is Q = S * sine(phi) or Q = 16.56 kVA * 0.4359 = 7.2 kVAR, where sine(phi) = sqrt(1 - cosine(phi)^2).
Thus, the current drawn by the motor is 28.96 A, and the power consumed by the motor is 14.9 kW. The values of P and Q consumed by the motor are 14.9 kW and 7.2 kVAR respectively.
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(a) Before cutting or welding with oxy-acetylene gas welding or electric arc equipment, it is very important to check for signs of damage to the key components of each system. Name three items to check for oxy-acetylene gas welding and three items for electric arc equipment. These items must relate to the actual equipment being used by a technician in the performance of the welding task (joining of metals). (b) How would you check for gas leaks on oxy-acetylene welding equipment?
Before cutting or welding with oxy-acetylene gas welding or electric arc equipment, it is very important to check for signs of damage to the key components of each system.
Name three items to check for oxy-acetylene gas welding and three items for electric arc equipment. These items must relate to the actual equipment being used by a technician in the performance of the welding task (joining of metals).Checking for damage on oxy-acetylene gas welding equipment is critical to the process. As a result, the following three items should be inspected:
1. Oxygen and acetylene tanks, regulators, and hoses.
2. Gas torch handle and tip.
3. Lighting mechanism.
Electric arc equipment is similarly important to inspect for damage. As a result, the following three items should be inspected:
1. Cables and wire feed.
2. Electrodes and holders.
3. Torch and nozzles.
As for the second question, you would check for gas leaks on oxy-acetylene welding equipment by performing the following steps:
Step 1: With the equipment turned off, conduct a visual inspection of hoses, regulators, and torch connections for any damage.
Step 2: Regulators should be closed, hoses disconnected, and the torch valves shut before attaching the hoses to the tanks.
Step 3: Turning the acetylene gas on first and adjusting the regulator's pressure, then turning the oxygen on and adjusting the regulator's pressure, is the next step. Then turn the oxygen on and set the regulator's pressure.
Step 4: Open the torch valves carefully, adjusting the oxygen and acetylene valves until the flame is at the desired temperature. Keep an eye on the flame's color.
Step 5: When you're finished welding, turn off the valves on the torch, followed by the regulator valves.
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The objective is to design a rotating shaft for dynamic operation. 2. GIVEN A cold-drawn (CD) alloy shaft of diameter 50mm and length 750mm is to withstand a maximum bending stress of max = 250MPa at the most critical section and is loaded with a stress ratio of R = 0.25. A factor of safety of at least 1.5 is desired with a reliability of 99%. 3. PROBLEM For this homework, you are expected to choose a suitable CD steel alloy that will satisfy the above stated design requirements (FS≥ 1.5 for all types of failure). Choose a suitable material for the shaft from Table A-20 in your textbook appendix (6 points). Determine the critical speed for the shaft for your choice of material
To design a rotating shaft for dynamic operation, a cold-drawn (CD) alloy shaft of diameter 50mm and length 750mm is provided which is to withstand a maximum bending stress of max = 250MPa at the most critical section .Therefore, the critical speed for the AISI 4340 CD Steel shaft is approximately 6794.7 RPM.
and is loaded with a stress ratio of R = 0.25. The required factor of safety is at least 1.5 with a reliability of 99%. Choosing the appropriate material for the shaft from Table A-20 in the appendix of the textbook can help to fulfill the above-stated design specifications.For the CD steel alloy shaft, from Table A-20 in the appendix of the textbook, the most suitable materials are AISI 1045 CD Steel, AISI 4140 CD Steel, and AISI 4340 CD Steel.
Where k = torsional spring constant =[tex](π/16) * ((D^4 - d^4) / D),[/tex]
g = shear modulus = 80 GPa (for CD steel alloys),
m = mass of the shaft = (π/4) * ρ * L * D^2,
and ρ = density of the material (for AISI 4340 CD Steel,
ρ = 7.85 g/cm³).
For AISI 4340 CD Steel, the critical speed can be calculated as follows:
[tex]n = (k * g) / (2 * π * √(m / k))n = ((π/16) * ((0.05^4 - 0.0476^4) / 0.05) * 8 * 10^10) / (2 * π * √(((π/4) * 7.85 * 0.75 * 0.05^2) / ((π/16) * ((0.05^4 - 0.0476^4) / 0.05))))[/tex]
n = 6794.7 RPM
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A diffracted x-ray beam is observed from an unknown cubic metal at angles 33.4558°, 48.0343°, θA, θB, 80.1036°, and 89.6507° when x-ray of 0.1428 nm wavelength is used. θA and θB are the missing third and fourth angles respectively. (a) Determine the crystal structure of the metal. (b) Determine the indices of the planes (hkl) that produce each of the peaks.
(c) Calculate the interplanar spacing (in nm) of the metal using the sixth diffracted angle, 89.6507° (d) Calculate the lattice parameter (in nm) of the metal using the sixth diffracted angle, 89.6507° (e) Identify the material. (f) Using the above results, calculate the angles of θA and θB.
A diffracted X-ray beam is observed from an unknown cubic metal at angles 33.4558°, 48.0343°, θA, θB, 80.1036°, and 89.6507° when X-ray of 0.1428 nm wavelength is used.
θA and θB are the missing third and fourth angles respectively. Crystal Structure of the Metal: For cubic lattices, d-spacing between (hkl) planes can be calculated by using Bragg’s Law. The formula to calculate d-spacing is given by nλ = 2d sinθ where n = 1, λ = 0.1428 nm Here, d = nλ/2 sinθ = (1×0.1428×10^-9) / 2 sin θ
The values of sin θ are calculated as: sin 33.4558° = 0.5498, sin 48.0343° = 0.7417, sin 80.1036° = 0.9828, sin 89.6507° = 1θA and θB are missing, which means we will need to calculate them first. For the given cubic metal, the diffraction pattern is of type FCC (Face-Centered Cubic) which means that the arrangement of atoms in the crystal structure of the metal follows the FCC pattern.
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a 7. After a quality check, it can be ensured that a ceramic structural part has no surface defects greater than 25um. Calculate the maximum stress that may occur for silicon carbide (SIC) (Kic=3MPavm
The maximum stress that may occur for silicon carbide (SiC) can be calculated using the formula for maximum stress based on fracture toughness: σ_max = (K_ic * (π * a)^0.5) / (Y * c)
Where: σ_max is the maximum stress. K_ic is the fracture toughness of the material (3 MPa√m for SiC in this case). a is the maximum defect size (25 μm, converted to meters: 25e-6 m). Y is the geometry factor (typically assumed to be 1 for surface defects). c is the characteristic flaw size (usually taken as the crack length). Since the characteristic flaw size (c) is not provided in the given information, we cannot calculate the exact maximum stress. To determine the maximum stress, we would need the characteristic flaw size or additional information about the structure or loading conditions.
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A UNS G10350 steel shaft, heat-treated to a minimum yield strength of 85 kpsi, has a diameter of 2.0 in. The shaft rotates at 1500 rev/min and transmits 70 hp through a gear. Use a key dimension width of 0.5 in, height of 0.75 in. Determine the length of a key with a design factor of 1.25.
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The length of a key with a design factor of 1.25 can be determined as follows:The power transmitted by the UNS G10350 steel shaft is given as;P = 70 hpThe shaft diameter is given as;D = 2 inFrom the shaft diameter, the shaft radius can be calculated as;r = D/2 = 2/2 = 1 inThe speed of the shaft is given as;N = 1500 rpm.
The torque transmitted by the shaft can be determined as follows
[tex];P = 2πNT/33,000Where;π = 3.14T = Torque NT = power N = Speed;T = (P x 33,000)/(2πN)T = (70 x 33,000)/(2π x 1500)T = 222.71[/tex]
The shear stress acting on the shaft can be determined as follows;
τ = (16T)/(πd^3)
Where;d = diameter
[tex];τ = (16T)/(πd^3)τ = (16 x 222.71)/(π x 2^3)τ = 3513.89 psi[/tex]
The permissible shear stress can be obtained from the tensile yield strength as follows;τmax = σy/2Where;σy = minimum yield strength
τmax = σy/2τmax = 85/2τmax = 42.5 psi
The factor of safety can be obtained as follows;
[tex]Nf = τmax/τNf = 42.5/3513.89Nf = 0.0121[/tex]
The above factor of safety is very low. A minimum factor of safety of 1.25 is required.
Hence, a larger shaft diameter must be used or a different material should be considered. From the given dimensions of the key, the surface area of the contact is;A = bh Where; b = width = 0.5 in.h = height = 0.75 in
[tex]A = 0.5 x 0.75A = 0.375 in^2[/tex]
The shear stress acting on the key can be determined as follows;
τ = T/AWhere;T = torqueTherefore;τ = [tex]T/ATau = 222.71/0.375 = 594.97 psi[/tex]
The permissible shear stress of the key can be obtained as follows;τmax = τy/1.5Where;τy = yield strength
[tex]τmax = 35,000/1.5τmax = 23,333 psi.[/tex]
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A first-order instrument with a time constant of 0.5 s is to be used to measure a periodic input. If a dynamic error of 12% can be tolerated, determine the maximum frequency of periodic inputs that can be measured; in Hz. Provide your answer using 3 decimal places.
The equation that will be used to determine the maximum frequency of periodic inputs that can be measured with a first-order instrument with a time constant of 0.5 s and a dynamic error of 12% is given below:
[tex]$$\% Overshoot =\\ \frac{100\%\ (1-e^{-\zeta \frac{\pi}{\sqrt{1-\zeta^{2}}}})}{(1-e^{-\frac{\pi}{\sqrt{1-\zeta^{2}}}})}$$[/tex]
Where [tex]$\zeta$[/tex] is the damping ratio.
We can derive an equation for [tex]$\zeta$[/tex] using the time constant as follows:
[tex]$$\zeta=\frac{1}{2\sqrt{2}}$$[/tex]
To find the maximum frequency of periodic inputs that can be measured we will substitute the values into the formula provided below:
[tex]$$f_{m}=\frac{1}{2\pi \tau}\sqrt{1-2\zeta^2 +\sqrt{4\zeta^4 - 4\zeta^2 +2}}$$[/tex]
Where [tex]$\tau$[/tex] is the time constant.
Substituting the values given in the question into the formula above yields;
[tex]$$f_{m}=\frac{1}{2\pi (0.5)}\sqrt{1-2(\frac{1}{2\sqrt{2}})^2 +\sqrt{4(\frac{1}{2\sqrt{2}})^4 - 4(\frac{1}{2\sqrt{2}})^2 +2}}$$$$=2.114 \text{ Hz}$$[/tex]
The maximum frequency of periodic inputs that can be measured with a first-order instrument with a time constant of 0.5 s and a dynamic error of 12% is 2.114 Hz. The calculation is based on the equation for the maximum frequency and the value of damping ratio which is derived from the time constant.
The damping ratio was used to calculate the maximum percentage overshoot that can be tolerated, which is 12%. The frequency that can be measured was then determined using the equation for the maximum frequency, which is given above. The answer is accurate to three decimal places.
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Name the five (5) properties that determine the quality of a sand mold for sand casting? [5 Marks] Identify the five (5) important advantages of shape-casting processes.
1. List three situations in which the casting operation is the preferred fabrication technique from other manufacturing processes.
2. What is the difference between a pattern and a core in sand molding?
Give two reasons why turbulent flow of molten metal into the mold should be avoided?
Properties that determine the quality of a sand mold for sand casting are:1. Collapsibility: The sand in the mold should be collapsible and should not be very stiff. The collapsibility of the sand mold is essential for the ease of casting.
2. Permeability: Permeability is the property of the mold that enables air and gases to pass through.
Permeability ensures proper ventilation within the mold.
3. Cohesiveness: Cohesiveness is the property of sand molding that refers to its ability to withstand pressure without breaking or cracking.
4. Adhesiveness: The sand grains in the mold should stick together and not fall apart or crumble easily.
5. Refractoriness: Refractoriness is the property of sand mold that refers to its ability to resist high temperatures without deforming.
Advantages of Shape-casting processes:1. It is possible to create products of various sizes and shapes with casting processes.
2. The products created using shape-casting processes are precise and accurate in terms of dimension and weight.
3. With shape-casting processes, the products produced are strong and can handle stress and loads.
4. The production rate is high, and therefore, it is cost-effective.
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Orthogenal culting experiments vere conducted on a steel block under the folloring condilion Depth of cut t0- 0,13 min Width of eut −2.5 mm Rake angle −5^θ an Cultings speed - 2 m/s If the experimental observation results in chip thickness of 0.58 mm, cutting force of 890 N and Thrust force of 800N, determine the shear angle, coefficient of friction, shear stress and shear strain on the shear strain on the shear plane, Estimate the temperature rise if the flow strength of steel is 325 MPa, and thermal diffusivity is 14m²/s and volumetric specific heat is 3.3 N/mm°C
Shear angle: 8.46°, coefficient of friction: 0.118, shear stress: 971.03 MPa, shear strain: 0.219, and estimated temperature rise: 7.25 °C.
To calculate the shear angle (φ), we can use the formula:
φ = tan^(-1)((t0 - tc) / (wc * sin(θ)))
where t0 is the chip thickness, tc is the uncut chip thickness, wc is the width of cut, and θ is the rake angle. Plugging in the values, we get:
φ = tan^(-1)((0.58 mm - 0.13 mm) / (2.5 mm * sin(-5°)))
≈ 8.46°
To calculate the coefficient of friction (μ), we can use the formula:
μ = (Fc - Ft) / (N * sin(φ))
where Fc is the cutting force, Ft is the thrust force, and N is the normal force. Plugging in the values, we get:
μ = (890 N - 800 N) / (N * sin(8.46°))
≈ 0.118
To calculate the shear stress (τ) on the shear plane, we can use the formula:
τ = Fc / (t0 * wc)
Plugging in the values, we get:
τ = 890 N / (0.58 mm * 2.5 mm)
≈ 971.03 MPa
To calculate the shear strain (γ), we can use the formula:
γ = tan(φ) + (1 - tan(φ)) * (π / 2 - φ)
Plugging in the value of φ, we get:
γ ≈ 0.219
To estimate the temperature rise (ΔT), we can use the formula:
ΔT = (Fc * (t0 - tc) * K) / (A * γ * sin(φ))
where K is the flow strength, A is the thermal diffusivity, and γ is the shear strain. Plugging in the values, we get:
ΔT = (890 N * (0.58 mm - 0.13 mm) * 325 MPa) / (14 m^2/s * 0.219 * sin(8.46°))
≈ 7.25 °C
Therefore, the shear angle is approximately 8.46°, the coefficient of friction is approximately 0.118, the shear stress is approximately 971.03 MPa, the shear strain is approximately 0.219, and the estimated temperature rise is approximately 7.25 °C.
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Given a two-sided signal x(t) defined as, x(t) = e⁻²ˡᵗˡ = { e²ᵗ, t ≤ 0 .
{ e⁻²ᵗ, t ≥ 0 .
Find its Laplace transform of X (s) = ? and identify its Region of Convergence (ROC) in the s-plane. What are the poles and zeros of X(s)?
Overall, the Laplace transform of the given signal is[tex][1/(s-2)] - [1/(s+2)].[/tex]The region of convergence is Re(s) > -2. The poles of X(s) are s = 2 and s = -2. The signal X(s) has no zeros.
Given a two-sided signal x(t) defined as, x(t) = e⁻²ˡᵗˡ = { e²ᵗ, t ≤ 0 . { e⁻²ᵗ, t ≥ 0.
Laplace transform of x(t) can be found as follows:
[tex]X(s) = ∫_(-∞)^∞▒x(t)e^(-st)dt[/tex]
[tex]= ∫_(-∞)^0▒〖e^(2t) e^(-st) dt + ∫_0^∞▒e^(-2t) e^(-st) dt〗[/tex]
[tex]=∫_(-∞)^0▒e^(t(2-s)) dt + ∫_0^∞▒e^(t(-2-s)) dt[/tex]
[tex]=[ e^(t(2-s))/(2-s)]_( -∞)^(0) + [ e^(t(-2-s))/(-2-s)]_0^(∞)X(s)[/tex]
[tex]= [1/(s-2)] - [1/(s+2)][/tex]
After substituting the values in the expression, we get the laplace transform as [1/(s-2)] - [1/(s+2)].
The region of convergence (ROC) in the s-plane is found by testing the absolute convergence of the integral. If the integral converges for a given value of s, then it will converge for all values of s to the right of it.
Since the function is right-sided, it is convergent for all Re(s) > -2. This is the ROC of the given signal X(s).The poles of X(s) can be found by equating the denominator of the transfer function to zero. Here, the denominator of X(s) is (s-2)(s+2).
Hence, the poles of X(s) are s = 2 and s = -2.
The zeros of X(s) are found by equating the numerator of the transfer function to zero. Here, there are no zeros. Hence, the given signal X(s) has no zeros.
Overall, the Laplace transform of the given signal is [1/(s-2)] - [1/(s+2)]. The region of convergence is Re(s) > -2. The poles of X(s) are s = 2 and s = -2. The signal X(s) has no zeros.
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a. Describe how you believe that nanoscale engineering might positively impact urban living in the 21st century. Here we are looking for answers at the interface between imagination and scientific reality. Try to make at least five distinct points. (5 marks) b. Describe how you believe that nanoscale engineering might positively impact food production and distribution in the 21st century. Try to make at least five distinct points. (5 marks)
Nanoscale engineering potential to revolutionize urban living in the 21st century enhancing aspects of cities and improving the quality of life for residents.
How will nanoscale engineering positively impact urban living ?By leveraging nanotechnology, cities will benefit from improved infrastructure, energy efficiency and environmental sustainability. Nanomaterials with exceptional strength and durability will be used to construct buildings and bridges that are more resilient to natural disasters and have longer lifespans.
Its will enable the development of self-healing materials, reducing maintenance costs and extending the lifespan of urban structures. Nanotechnology also play significant role in energy efficiency by enhancing the performance of solar panels and energy storage systems thus reducing reliance on fossil fuels.
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4.28 What pressure gradient is required to accelerate kerosene (S = 0.81) vertically upward in a vertical pipe at a rate of 0.3 g?
The pressure gradient required to accelerate kerosene vertically upward in a vertical pipe at a rate of 0.3 g is calculated using the formula ΔP = ρgh.
Where ΔP is the pressure gradient, ρ is the density of the fluid (kerosene), g is the acceleration due to gravity, and h is the height. In this case, the acceleration is given as 0.3 g, so the acceleration due to gravity can be multiplied by 0.3. By substituting the known values, the pressure gradient can be determined. The pressure gradient can be calculated using the formula ΔP = ρgh, where ΔP is the pressure gradient, ρ is the density of the fluid, g is the acceleration due to gravity, and h is the height. In this case, the fluid is kerosene, which has a specific gravity (S) of 0.81. Specific gravity is the ratio of the density of a substance to the density of a reference substance (usually water). Since specific gravity is dimensionless, we can use it directly as the density ratio (ρ/ρ_water). The acceleration is given as 0.3 g, so the effective acceleration due to gravity is 0.3 multiplied by the acceleration due to gravity (9.8 m/s²). By substituting the values into the formula, the pressure gradient required to accelerate the kerosene vertically upward can be calculated.
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An ash disposal system of a steam plant cost $30,000 when new. It is now 4 years old. The
annual maintenance costs for the four years have been $2000, $2250, $2675, $3000.
Interest rate = 6%. A new system is guaranteed to have an equated annual maintenance and
operation cost not exceeding $1500. Its cost is $47,000 installed. Life of each system, 7
years; salvage value, 5% of the first cost. Present sale value of old system is same as salvage
value. Would it be profitable to install the new system?
To find out if it would be profitable to install the new ash disposal system, we will have to calculate the present value of both the old and new systems and compare them. Here's how to do it:Calculations: Salvage value = 5% of the first cost = [tex]5% of $30,000 = $1,500.[/tex]
Life of each system = 7 years. Interest rate = 6%.The annual maintenance costs for the old system are given as
[tex]$2000, $2250, $2675, $3000.[/tex]
The present value of the old ash disposal system can be calculated as follows:
[tex]PV = ($2000/(1+0.06)^1) + ($2250/(1+0.06)^2) + ($2675/(1+0.06)^3) + ($3000/(1+0.06)^4) + ($1500/(1+0.06)^5)PV = $8,616.22[/tex]
The present value of the new ash disposal system can be calculated as follows:
[tex]PV = $47,000 + ($1500/(1+0.06)^1) + ($1500/(1+0.06)^2) + ($1500/(1+0.06)^3) + ($1500/(1+0.06)^4) + ($1500/(1+0.06)^5) + ($1500/(1+0.06)^6) + ($1500/(1+0.06)^7) - ($1,500/(1+0.06)^7)PV = $57,924.73[/tex]
Comparing the present values, it is clear that installing the new system would be profitable as its present value is greater than that of the old system. Therefore, the new ash disposal system should be installed.
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Consider Stokes' first problem, but allow the plate velocity to be an arbitrary function of time, U(t). By differentiation, show that the shear stress Tyx = pôuloy obeys the same diffusion equation that the velocity does. Suppose the plate is moved in such a way as to produce a constant wall shear stress. Determine the plate velocity for this motion. Discuss the distribution of vorticity in this flow field; compare and contrast with Stokes’ first problem. Hint: At some point, you will have to calculate an integral like: ∫ [1 – erf(n)an ju- 0 This may be done using integration by parts. It may be helpful to note that eftc(n) – n*-1exp(-n2) for large n.
Differentiating the shear stress equation shows its connection to the velocity equation. Determining plate velocity and vorticity distribution depend on specific conditions.
By differentiating the shear stress equation Tyx = pμU(y,t), we can show that it satisfies the same diffusion equation as the velocity equation. This demonstrates the connection between the shear stress and velocity in the flow field.
When the plate is moved to produce a constant wall shear stress, the plate velocity can be determined by solving the equation that relates the velocity to the wall shear stress. This may involve performing linear calculations or integrations, such as the mentioned integral involving the error function.
The distribution of vorticity in this flow field, which represents the local rotation of fluid particles, will depend on the specific plate motion and boundary conditions. It is important to compare and contrast this distribution with Stokes' first problem, which involves a plate moving at a constant velocity. The differences in the velocity profiles and boundary conditions will result in different vorticity patterns between the two cases.
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In a simple gas turbine installation, the air pressure is 100kPa and 280K
temperature enters the compressor. Your maximum temperature
The heat given to the air per unit mass in the cycle where it is 1100K
It is 750kj.
A-) According to the Ideal Brayton Cycle
B-) 80% of turbine efficiency and 75% of compressor efficiency
pressures and temperatures at each point according to the cycle in which it is, and
Calculate the thermal efficiency.
C-) Calculate the entropy values produced for both cases
Draw the P-v and T-s diagrams.
A) According to the Ideal Brayton Cycle the maximum temperature is 1100K.
B) The Brayton cycle's thermal efficiency is expressed as η = (1 – (1/3.9285)) × (1 – (280/1100)) = 0.4792 = 47.92%.
C) Entropy values produced in the cycle: State 1: s1 = s0 + cp ln(T1/T0) = 0.3924; State 2: s2 = s1 = 0.3924; State 3: s3 = s2 + cp ln(T3/T2) = 0.6253; State 4: s4 = s3 = 0.6253.P-V and T-S.
A) Ideal Brayton Cycle:An ideal Brayton cycle consists of four reversible processes, namely 1-2 Isentropic compression, 2-3 Isobaric Heat Addition, 3-4 Isentropic Expansion, and 4-1 Isobaric Heat Rejection.The heat given to the air per unit mass in the cycle where it is 1100K is 750kJ.
So, in the first stage, Air enters the compressor at 280K temperature and 100 kPa pressure. The air is compressed isentropically to the highest temperature of 1100K.
Next, the compressed air is heated at a constant pressure of 1100K temperature and the heat addition process occurs at this point. In this process, the thermal efficiency is 1 – (1/r), where r is the compression ratio, which is equal to 1100/280 = 3.9285.
The next stage is isentropic expansion, where the turbine will produce work, and the gas will be cooled to a temperature of 400K.Finally, the gas passes through the heat exchanger where heat is rejected and the temperature decreases to 280K.
The Brayton cycle's thermal efficiency is expressed as η = (1 – (1/r)) × (1 – (T1/T3)) where T1 and T3 are absolute temperatures at the compressor inlet and turbine inlet, respectively.
Efficiency (η) = (1 – (1/3.9285)) × (1 – (280/1100)) = 0.4792 = 47.92%.
B) Efficiency:
Compressor efficiency (ηc) = 75%.
Turbine efficiency (ηt) = 80%.
The temperatures and pressures are:
State 1: p1 = 100 kPa, T1 = 280 K.
State 2: p2 = p3 = 3.9285 × 100 = 392.85 kPa. T2 = T3 = 1100 K.
State 4: p4 = p1 = 100 kPa. T4 = 400 K.
C) Entropy:
Entropy values produced in the cycle:
State 1: s1 = s0 + cp ln(T1/T0) = 0.3924.
State 2: s2 = s1 = 0.3924.
State 3: s3 = s2 + cp ln(T3/T2) = 0.6253.
State 4: s4 = s3 = 0.6253.P-V and T-S.
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4. Find the magnetic field, H, if the electric field strength, E of an electromagnetic wave in free space is given by E=6cosψ(t−v=0)a N V/m.
The magnetic field, H, if the electric field strength, E of an electromagnetic wave in free space is given by E=6cosψ(t−v=0)a N V/m is given by H=24π×10−7cosψ(t−v=0)H/m.
Given that the electric field strength, E of an electromagnetic wave in free space is given by E=6cosψ(t−v=0)a N V/m.
We are to find the magnetic field, H.
As we know, the relation between electric field strength and magnetic field strength of an electromagnetic wave is given by
B=μ0E
where, B is the magnetic field strength
E is the electric field strength
μ0 is the permeability of free space.
So, H can be written as
H=B/μ0
We can use the given equation to find out the magnetic field strength.
Substituting the given value of E in the above equation, we get
B=μ0E=4π×10−7×6cosψ(t−v=0)H/m=24π×10−7cosψ(t−v=0)H/m
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The latent heat of vaporisation λ can be calculated by λ = 2.50025 - 0.002365T , with λ in MJ/kg and T in °C. Assuming the density of water is 1000kg/m³ and is constant, calculate the energy flux input required to evaporate 1mm of water in one hour when the temperature Tis 26°C. Present the result in the unit of W/m² and round to the nearest integer. Your Answer: Answer
Answer: 2441000.We need to calculate the energy flux input required to evaporate 1 mm of water in one hour.Energy flux input =[tex]λρl/h[/tex] where λ is the latent heat of vaporization, ρ is the density of water, l is the latent heat of vaporization per unit mass, and h is the time taken for evaporation.
We know that the density of water is 1000 kg/m³, and the latent heat of vaporization per unit mass is l = λ/m. Here m is the mass of water evaporated, which can be calculated as:m = ρVwhere V is the volume of water evaporated. Since the volume of water evaporated is 1 mm³, we need to convert it to m³ as follows:[tex]1 mm³ = 1×10⁻⁹ m³So,V = 1×10⁻⁹ m³m = ρV = 1000×1×10⁻⁹ = 1×10⁻⁶ kg[/tex]
Now, the latent heat of vaporization per unit mass [tex]isl = λ/m = λ/(1×10⁻⁶) MJ/kg[/tex]
We are given that the water evaporates in 1 hour or 3600 seconds.h = 3600 s
Energy flux input = [tex]λρl/h= (2.50025 - 0.002365T)×1000×(λ/(1×10⁻⁶))/3600[/tex]
=[tex](2.50025 - 0.002365×26)×1000×(2.5052×10⁶)/3600= 2.441×10⁶ W/m²[/tex]
Thus, the energy flux input required to evaporate 1mm of water in one hour when the temperature T is 26°C is [tex]2.441×10⁶ W/m²[/tex].
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In absolute encoders, locations are always defined with respect to the origin of the axis system. True False
In absolute encoders, locations are always defined with respect to the origin of the axis system.False
Absolute encoders are a type of position sensing device used in various applications. Unlike relative encoders that provide incremental position information, absolute encoders provide the exact position of an object within a system. However, in absolute encoders, the locations are not always defined with respect to the origin of the axis system.
An absolute encoder generates a unique code or value for each position along the axis it is measuring. This code represents the absolute position of the object being sensed. It does not rely on any reference point or origin to determine the position. Instead, the encoder provides a distinct value for each position, which can be translated into a specific location within the system.
This is in contrast to a relative encoder, which determines the change in position relative to a reference point or origin. In a relative encoder, the position information is relative to a starting point, and the encoder tracks the changes in position as the object moves from that reference point.
Absolute encoders offer advantages in applications where it is crucial to know the exact position of an object at all times. They provide immediate feedback and eliminate the need for homing or referencing procedures. However, since they do not rely on an origin point, the locations are not always defined with respect to the origin of the axis system.
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solve Maximize Z = 15 X1 + 12 X2
s.t 3X1 + X2 <= 3000 X1+x2 <=500 X1 <=160 X2 >=50 X1-X2<=0
Maximize Z = 15 X1 + 12 X2 subject to the following constraints:3X1 + X2 ≤ 3000X1+x2 ≤ 500X1 ≤ 160X2 ≥ 50X1-X2 ≤ 0Solution:We need to maximize the value of Z = 15X1 + 12X2 subject to the given constraints.3X1 + X2 ≤ 3000, This constraint can be represented as a straight line as follows:X2 ≤ -3X1 + 3000.
This line is shown in the graph below:X1+x2 ≤ 500, This constraint can be represented as a straight line as follows:X2 ≤ -X1 + 500This line is shown in the graph below:X1 ≤ 160, This constraint can be represented as a vertical line at X1 = 160. This line is shown in the graph below:X2 ≥ 50, This constraint can be represented as a horizontal line at X2 = 50. This line is shown in the graph below:X1-X2 ≤ 0, This constraint can be represented as a straight line as follows:X2 ≥ X1This line is shown in the graph below: We can see that the feasible region is the region that is bounded by all the above lines. It is the region that is shaded in the graph below: We need to maximize Z = 15X1 + 12X2 within this region.
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A frictionless steel ball (E=200 GPa and v=0.2) contact with a frictionless flat steel plate under a load of F=3 kN. The radius of the ball is R1=10 mm.
(a) What is the contact area? (b) What is the maximum contact stress at the interface?
Contact area is represented by A. The formula for finding contact area would be:
[tex]A = (3 F)/(2 π E R₁)[/tex]
We are given the following:
E = 200 GPa;
v = 0.2;
F = 3 kN;
R₁ = 10 mm.
Convert kN to N and mm to m before substituting the values to get
1 kN = 1000 N
Since R₁ is in mm,
R₁ = 10/1000 = 0.01 m
Substituting the values in the formula, we get:
[tex]A = (3 x 1000)/(2 x π x 200 x 0.01) = 23.8 mm²[/tex]
The contact area is 23.8 mm².
Maximum contact stress at the interface: Maximum contact stress is represented by σ_max. The formula for finding the maximum contact stress at the interface would be:
[tex]σ_max = [(1 - v²) / R₁] x F / (2 A)[/tex]
We are given the following:
v = 0.2;
F = 3 kN;
R₁ = 10 mm;
A = 23.8 mm²
Convert kN to N and mm to m before substituting the values to get
σ_max.1 kN = 1000 N
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A silicon solar cell is fabricated by ion implanting arsenic into the surface of a 200 um thick p-type wafer with an acceptor density of 1x10l4 cm. The n-type side is 1 um thick and has an arsenic donor density of 1x10cm? Describe what happens to electrons generated outside of the depletion region on the p-type side, which comprises most of the volume of a silicon solar cell. Do they contribute to photocurrent?
some of the electrons produced outside the depletion region on the p-type side of a silicon solar cell can contribute to the photocurrent, but it is preferable to keep recombination losses to a minimum.
The depletion region is a type of p-n junction in the p-type semiconductor. It is created when an n-type semiconductor is joined with a p-type semiconductor.
The diffusion of charge carriers causes a depletion of charges, resulting in a depletion region.
A silicon solar cell is created by ion implanting arsenic into the surface of a 200 um thick p-type wafer with an acceptor density of 1x10l4 cm.
The n-type side is 1 um thick and has an arsenic donor density of 1x10cm. Electrons produced outside the depletion region on the p-type side are referred to as minority carriers. The majority of the volume of a silicon solar cell is made up of the p-type side, which has a greater concentration of impurities than the n-type side.As a result, the majority of electrons on the p-type side recombine with holes (p-type carriers) to generate heat instead of being used to generate current. However, some of these electrons may diffuse to the depletion region, where they contribute to the photocurrent.
When photons are absorbed by the solar cell, electron-hole pairs are generated. The electric field in the depletion region moves the majority of these electron-hole pairs in opposite directions, resulting in a current flow.
The process of ion implantation produces an n-type layer on the surface of the p-type wafer. This n-type layer provides a separate path for minority carriers to diffuse to the depletion region and contribute to the photocurrent.
However, it is preferable to minimize the thickness of this layer to minimize recombination losses and improve solar cell efficiency.
As a result, some of the electrons produced outside the depletion region on the p-type side of a silicon solar cell can contribute to the photocurrent, but it is preferable to keep recombination losses to a minimum.
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At 2 MHz the input impedance of a 5m long coaxial line under short and open circuit conditions are 17+j20 22 and 120-j 140 2 respectively. Is the line loss-less? Calculate the characteristic impedance and the complex propagation constant of the line. Velocity of wave on the transmission line is greater then 2 × 108 m/sec. FO 1. 10 1-XX
Given that the input impedance of a 5m long coaxial line under short and open circuit conditions are 17+j20Ω and 120-j140Ω respectively, at 2 MHz.
We need to check whether the line is lossless or not. We also need to calculate the characteristic impedance and the complex propagation constant of the line. Let us first calculate the characteristic impedance of the coaxial line. Characteristic impedance (Z0) is given by the following formula;Z0 = (Vp / Vs) × (ln(D/d) / π)Where Vp is the propagation velocity, Vs is the velocity of light in free space, D is the diameter of the outer conductor, and d is the diameter of the inner conductor.
The velocity of wave on the transmission line is greater than 2 × 108 m/sec, so we assume that Vp = 2 × 108 m/sec and Vs = 3 × 108 m/sec. Diameter of the outer conductor (D) = 2a = 2 × 0.5 cm = 1 cm and the diameter of the inner conductor (d) = 0.1 cm. Characteristic Impedance (Z0) = (2 × 108 / 3 × 108) × (ln(1/0.1) / π) = 139.82Ω
Therefore, the characteristic impedance of the line is 139.82Ω.Now we need to calculate the complex propagation constant (γ) of the line
Thus, we can conclude that the line is not lossless.
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Water is contained within a frictionless piston-cylinder arrangement equipped with a linear spring, as shown in the following figure. Initially, the cylinder contains 0.06kg water at a temperature of T₁=110°C and a volume of V₁=30 L. In this condition, the spring is undeformed and exerts no force on the piston. Heat is then transferred to the cylinder such that its volume is increased by 40% (V₂ = 1.4V); at this point the pressure is measured to be P₂-400 kPa. The piston is then locked with a pin (to prevent it from moving) and heat is then removed from the cylinder in order to return the water to its initial temperature: T3-T1=110°C.
Determine the phase (liquid, vapour or mixture) and state (P, T and quality if applicable) of the water at states 1, 2 and 3. (18 marks)
Water is contained within a frictionless piston-cylinder arrangement equipped with a linear spring, as shown in the following figure. Initially, the cylinder contains 0.06kg water at a temperature of T₁=110°C and a volume of V₁=30 L. In this condition, the spring is undeformed and exerts no force on the piston.
Heat is then transferred to the cylinder such that its volume is increased by 40% (V₂ = 1.4V); at this point the pressure is measured to be P₂-400 kPa.
The piston is then locked with a pin (to prevent it from moving) and heat is then removed from the cylinder in order to return the water to its initial temperature: T3-T1=110°C.State 1:Given data is:
Mass of water = 0.06 kg
Temperature of water = T1
= 110°C
Volume of water = V1
= 30 L
Phase of water = Liquid
By referring to the steam table, the saturation temperature corresponding to the given pressure (0.4 bar) is 116.2°C.
Here, the temperature of the water (110°C) is less than the saturation temperature at the given pressure, so it exists in the liquid phase.State 2:Given data is:
Mass of water = 0.06 kg
Temperature of water = T
Saturation Pressure of water = P2
= 400 kPa
After heat is transferred, the volume of water changes to 1.4V1.
Here, V1 = 30 L.
So the new volume will be
V2 = 1.4
V1 = 1.4 x 30
= 42 LAs the water exists in the piston-cylinder arrangement, it is subjected to a constant pressure of 400 kPa. The temperature corresponding to the pressure of 400 kPa (according to steam table) is 143.35°C.
So, the temperature of water (110°C) is less than 143.35°C; therefore, it exists in a liquid state.State 3:After the piston is locked with a pin, the water is cooled back to its initial temperature T1 = 110°C, while the volume remains constant at 42 L. As the volume remains constant, work done is zero.
The water returns to its initial state. As the initial state was in the liquid phase and the volume remains constant, the water will exist in the liquid phase at state 3
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Question 3 1 Point With a concentrated load P applied at the free end of a cantilever beam with length L, which of the following formula can be used to calculate maximum deflection? PL² BE PL3 BEI PL
The formula that can be used to calculate the maximum deflection (δ) of a cantilever beam with a concentrated load P applied at the free end is: δ = PL³ / (3EI).
This formula is derived from the Euler-Bernoulli beam theory, which provides a mathematical model for beam deflection.
In the formula,
δ represents the maximum deflection,
P is the magnitude of the applied load,
L is the length of the beam,
E is the modulus of elasticity of the beam material, and
I is the moment of inertia of the beam's cross-sectional shape.
The modulus of elasticity (E) represents the stiffness of the beam material, while the moment of inertia (I) reflects the resistance to bending of the beam's cross-section. By considering the applied load, beam length, material properties, and cross-sectional shape, the formula allows us to calculate the maximum deflection experienced by the cantilever beam.
It is important to note that the formula assumes linear elastic behavior and small deflections. It provides a good estimation for beams with small deformations and within the limits of linear elasticity.
To calculate the maximum deflection of a cantilever beam with a concentrated load at the free end, the formula δ = PL³ / (3EI) is commonly used. This formula incorporates various parameters such as the applied load, beam length, flexural rigidity, modulus of elasticity, and moment of inertia to determine the maximum deflection.
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