The energy of a photon is given as 3600 eV. The electron volt (eV) is a unit of energy commonly used in the field of particle physics and quantum mechanics. It represents the amount of energy gained or lost by an electron when it is accelerated through an electric potential difference of one volt.
To convert this energy to joules (J), we need to use the conversion factor between electron volts and joules. The conversion factor is 1 eV = 1.6 x[tex]10^(-19)[/tex] J. Multiplying the given energy of the photon (3600 eV) by the conversion factor, we can find the energy in joules:
Energy in J = 3600 eV * (1.6 x [tex]10^(-19)[/tex] J/eV)
Calculating this expression, we get:
Energy in J = 5.76 x [tex]10^(-16)[/tex] J
Therefore, the energy of the photon is 5.76 x[tex]10^(-16)[/tex]) J.
The electron volt (eV) is a unit of energy commonly used in the field of particle physics and quantum mechanics. It represents the amount of energy gained or lost by an electron when it is accelerated through an electric potential difference of one volt. On the other hand, the joule (J) is the standard unit of energy in the International System of Units (SI).
The conversion factor between eV and J is based on the charge of an electron and is derived from fundamental constants. Multiplying the energy in eV by the conversion factor allows us to convert it to joules. In this case, the energy of the photon is found to be 5.76 x [tex]10^(-16)[/tex] J.
The resulting value, written as ×[tex]10^(-15[/tex]) J, indicates that the energy is in the order of [tex]10^(-15[/tex]) J. This represents a very small amount of energy on the scale of everyday experiences, but it is significant in the realm of quantum phenomena, where particles and photons exhibit discrete energy levels.
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Mary is an avid game show fan and one of the contestants on a popular game show. She spins the wheel and after 1.5 revolutions, the wheel comes to rest on a space that has a $1,500.00 prize. If the Initial angular speed of the wheel is 3.20 rad/s, find the angle through which the wheel has turned when the angular speed is 1.60rad/s. _________________
First consider the one-and-one-half revolutions to find the angular acceleration of the wheel. rev
Answer: the wheel has turned through an angle of 6.74 radians when the angular speed is 1.60 rad/s.
Here's a step by step explanation :
Step 1: Let's find the angular acceleration of the wheel using the first condition. I
ω1 = 3.20 rad/s.
Number of revolutions = 1.5 revolutions.
Time taken to complete 1.5 revolutions, t = 1.5 x 1/f = 1.5 x 1/T
where f = frequency = 1/T (T = time period).
Now, the wheel rotates 1 revolution in T seconds and rotates 1.5 revolutions in 1.5T seconds. Taking time for 1 revolution, T = 1/f
Initial angular displacement, θ1 = (1.5 revolutions) x (2π radians/revolution) = 3π radians.
Final angular displacement, θ2 = 0 rad. The angular acceleration of the wheel: ω2 = ω1 + αtθ2 = θ1 + ω1t + 0.5 α t².
At the end, angular speed of the wheel,
ω2 = 0 rad/sθ2
= θ1 + ω1t + 0.5 α t²0
= θ1 + ω1 (1.5T) + 0.5 α (1.5T)²0
= 3π + 3.20 (1.5T) + 0.5 α (1.5T)²
α = -2.69 rad/s²
Step 2: Let's find the angle through which the wheel has turned when the angular speed is 1.60 rad/s.
ω1 = 3.20 rad/s
ω2 = 1.60 rad/s.
The angle through which the wheel has turned is given by
θ = θ1 + 0.5 (ω1 + ω2)
tθ = θ1 + 0.5 (ω1 + ω2)
tθ = 3π + 0.5 (3.20 + 1.60)
tθ = 3π + 2.40 t.
we know that α = -2.69 rad/s²
From the kinematic equation, ω2 = ω1 + αt. By rearranging, we get t = (ω2 - ω1)/α. Substitute the given values to find the value of t.
t = (1.60 - 3.20)/-2.69t
= 1.119 seconds.
Substitute the value of t in the equation for θ.
θ = 3π + 2.40 t
θ = 3π + 2.40 (1.119)
θ = 6.74 radians.
Therefore, the wheel has turned through an angle of 6.74 radians when the angular speed is 1.60 rad/s.
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A 10 gram mass is hung vertically from a spring. At rest, it stretches the spring 20 cm. A damper imparts a damping force of 560 dynes when the mass is moving at a peed of 4 cm/sec. Assume that the spring force is proportional to the displacement, that the damping force is proportional to velocity, and that there are no other forces. At t=0 the mass is displaced 3 cm below its rest position and is released with an upward 1dyne=lgramcm/sec 2
(a) Write an initial-value problem for the displacement u(t) for any time any time t>0. DO NOT SOLVE THE EQUATION. (b) Is the system undamped, under damped, critically damped, or over damped. Justify your answer giving reasons.
(a) The initial-value problem for the displacement u(t) for any time t > 0 is u''(t) + bu'(t) + ku(t) = 0, where u''(t) represents the second derivative of u(t) with respect to time, b represents the damping coefficient, and k represents the spring constant. 0.01u''(t) + 0.14u'(t) + 0.1*u(t) = 0 (b) The system is underdamped because the damping force is less than the critical damping value, causing the system to oscillate before reaching its equilibrium position. In this case, b = 0.14 N sec/m, while the critical damping value is approximately 2 * sqrt(0.01 kg * 0.1 N/m) = 0.632 N sec/m.
(a) To write the initial-value problem for the displacement u(t), we can use Newton's second law for a damped harmonic oscillator. The equation is given by mu''(t) + bu'(t) + k*u(t) = 0, where m is the mass, u''(t) is the second derivative of u(t) with respect to time, b is the damping coefficient, and k is the spring constant.
Considering the given values, we have:
m = 10 g = 0.01 kg (mass)
k = F/x = (1 dyne)/(1 g cm/sec^2) = 1 g cm = 0.01 N/cm = 0.1 N/m (spring constant)
b = F/v = 560 dyne / 4 cm/sec = 140 dyne sec/cm = 0.14 N sec/m (damping coefficient)
Substituting these values into the initial-value problem, we obtain:
0.01u''(t) + 0.14u'(t) + 0.1*u(t) = 0
(b) To determine whether the system is undamped, underdamped, critically damped, or overdamped, we compare the damping coefficient (b) to the critical damping value. The critical damping occurs when the damping coefficient is equal to 2 times the square root of the mass times the spring constant, i.e., b = 2sqrt(mk).
In this case, b = 0.14 N sec/m, while the critical damping value is approximately 2 * sqrt(0.01 kg * 0.1 N/m) = 0.632 N sec/m.
Since b < 0.632 N sec/m, the system is underdamped. This means that the damping force is not strong enough to prevent oscillations, and the mass will undergo damped oscillations before eventually reaching its equilibrium position.
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What is the magnification for a simple magnifier of focal length 5 cm, assuming the user has a normal near point of 25 cm ? 5 25 12.5 125
the magnification for a simple magnifier of focal length 5 cm, assuming the user has a normal near point of 25 cm is 6.Please note that the answer is 75 words.
The magnification for a simple magnifier of focal length 5 cm, assuming the user has a normal near point of 25 cm is 5. This can be computed using the formula:
Magnification of simple microscope = (D/f) + 1, where D is the least distance of clear vision or near point, and f is the focal length of the lens or magnifying glass.
Given that focal length of simple magnifier, f = 5 cmLeast distance of clear vision, D = 25 cmMagnification = (25/5) + 1= 5 + 1= 6
Therefore, the magnification for a simple magnifier of focal length 5 cm, assuming the user has a normal near point of 25 cm is 6.Please note that the answer is 75 words.
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A 189-turn circular coil of radius 3.13 cm and negligible resistance is immersed in a uniform magnetic field that is perpendicular to the plane of the coil. The coil is connected to a 17.7Ω resistor to create a closed circuit. During a time interval of 0.193 s, the magnetic field strength decreases uniformly from 0.643 T to zero. Find the energy E in millijoules that is dissipated in the resistor during this time interval. E= mJ
The energy dissipated in the resistor during the time interval is approximately 1.118 millijoules (mJ).
The energy dissipated in a resistor can be calculated using the formula E = I^2RΔt, where E is the energy, I is the current, R is the resistance, and Δt is the time interval. First, we need to calculate the current in the circuit. The current can be found using Ohm's Law: I = V/R, where V is the voltage. In this case, the voltage across the resistor is induced by the changing magnetic field.
To find the induced voltage, we can use Faraday's Law of electromagnetic induction: ε = -N(dΦ/dt), where ε is the induced voltage, N is the number of turns in the coil, and dΦ/dt is the rate of change of magnetic flux. Since the magnetic field strength decreases uniformly from 0.643 T to zero over a time interval of 0.193 s, we can calculate the rate of change of magnetic flux.
The magnetic flux through the coil is given by Φ = BA, where B is the magnetic field strength and A is the area of the coil. Substituting the given values, we get Φ = 0.643 T * π * (0.0313 m)^2. Taking the derivative of the magnetic flux with respect to time, we find dΦ/dt = (0 - 0.643 T) / 0.193 s.
Now we can calculate the induced voltage: ε = -189 * (0.643 T / 0.193 s). Finally, we can calculate the current: I = ε / R = (-189 * (0.643 T / 0.193 s)) / 17.7 Ω. Substituting the values into the energy dissipation formula, we get E = I^2RΔt = ((-189 * (0.643 T / 0.193 s)) / 17.7 Ω)^2 * 17.7 Ω * 0.193 s, which is approximately 1.118 mJ.
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A solid 56-kg sphere of U-235 is just large enough to constitute a critical mass. If the sphere were flattened into a pancake shape, would it still be critical? Briefly explain.
The critical mass of a fissile material, such as U-235, is the minimum amount required to sustain a self-sustaining chain reaction. It depends on various factors, including the shape, density, and enrichment of the material.
In the case of a solid sphere of U-235 with a mass of 56 kg, it is critical because the shape and density of the sphere are carefully designed to ensure a self-sustaining chain reaction. Any change in the shape or density of the material can potentially affect its criticality.
If the sphere were flattened into a pancake shape, the distribution of the material would change. The pancake shape would increase the surface area of the U-235, which could lead to increased neutron leakage and reduced neutron multiplication. This change in geometry can disrupt the criticality of the system.
Moreover, the pancake shape may also alter the density of the U-235 material. The critical mass depends on the density of the material because a higher density allows for a more efficient neutron capture and fission process. Flattening the sphere could potentially decrease the density, further affecting the criticality.
In summary, changing the shape of the U-235 sphere from a solid sphere to a pancake shape can disrupt the criticality of the system. The specific critical mass and shape requirements for a self-sustaining chain reaction depend on the detailed design and calculations for a particular nuclear reactor or weapon.
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A subject is given a sugar pill and is told it may treat anxiety. This person may experience:
A woman is sitting on a roof with a pitch of 19.02°, relaxing in the quiet by reading a book. If she has a mass of 65.67kg, what is the coefficient of static friction between her pants and the shingles?
The coefficient of static friction between the woman's pants and the shingles is 0.35.
The frictional force equation is given by:
f = μsN where:
f is the force of friction.
μs is the coefficient of static friction.
N is the normal force.
In this scenario, a woman is sitting on a roof with a pitch of 19.02°. The frictional force acting upon her is that of static friction. If the woman has a mass of 65.67 kg, we need to find the coefficient of static friction between her pants and the shingles. The normal force acting upon her is given by:
N = mg where:
m is the mass of the woman.
g is the acceleration due to gravity.
Substituting the given values, we get:
N = 65.67 kg × 9.8 m/s² = 644.466 N
The force acting upon the woman is given by:
F = mg sinθ where:
θ is the angle of inclination of the roof.
Substituting the given values, we get:
F = 65.67 kg × 9.8 m/s² × sin(19.02°) = 226.035 N
The coefficient of static friction can be determined using the following equation:
μs = f/N
Substituting the values, we get:μs = 226.035 N / 644.466 N = 0.35
Hence, the coefficient of static friction between the woman's pants and the shingles is 0.35.
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My Account Class Management Help Exam3 PRACTICE Begin Date: 5/16 2022 12:00:00 AM - Due Date: 5/20/2022 11:59.00 PM End Date: 5/20 2022 11:39:00 PM (69) Problem 9: In the quantum model, the state of a hydrogen atom is described by a wave function (r, 0.6), which is a solution of the Schrödinge equation. Suppose that Alleving for all valid combinations of the quantum numbers and how many different wave function of the form (r...) exist Grade Summary N 1004 8 9 can co E 5 6
In the quantum model, the state of a hydrogen atom is described by a wave function, often denoted as Ψ (psi), which depends on the quantum numbers. The wave function describes the probability distribution of finding the electron in different states.
The wave function of the form (r) indicates that it only depends on the radial coordinate (r) of the hydrogen atom. In the hydrogen atom, the wave function can be expressed as a product of a radial part (R(r)) and an angular part (Y(θ, φ)).
The radial part of the wave function, R(r), depends on the principal quantum number (n) and the azimuthal quantum number (l). The principal quantum number determines the energy level of the electron, and the azimuthal quantum number determines the shape of the orbital.
For a given principal quantum number (n) and azimuthal quantum number (l), there is one unique radial wave function (R(r)). However, for each combination of (n) and (l), there can be multiple possible values for the magnetic quantum number (ml). The magnetic quantum number determines the orientation of the orbital in space.
Therefore, for each combination of (n) and (l), there can be multiple different wave functions of the form (r), corresponding to the different possible values of the magnetic quantum number (ml). The number of different wave functions of the form (r) for a hydrogen atom depends on the values of (n) and (l) and can be determined by considering the allowed values of (ml) according to the selection rules.
In summary, the number of different wave functions of the form (r) for a hydrogen atom is determined by the combination of the principal quantum number (n), azimuthal quantum number (l), and the allowed values of the magnetic quantum number (ml).
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A metal cylindrical wire of radius of 1.2 mm and length 4.2 m has a resistance of 42 Ω. What is the resistance of a wire made of the same metal that has a square crosssectional area of sides 3.1 mm and length 4.2 m ? (in Ohms)
The resistance of the wire having square cross-sectional area is 19.78 Ω.
The resistance of the wire having square cross-sectional area can be determined using the given formula; Resistance = resistivity * (length / area)Where; resistivity = resistivity of the material,length = length of the wire,area = area of cross-sectional of the wire
The formula shows that resistance is inversely proportional to area. Therefore, an increase in area would result in a decrease in resistance.The resistance of the cylindrical wire is given as 42 Ω, and the radius of the wire is 1.2 mm.The cross-sectional area of the cylindrical wire can be given as:
Area of circle = [tex]\pi r^2\pi[/tex]= 22/7r = 1.2 [tex]mm^2[/tex]
The area of cross-sectional of the cylindrical wire is given by:Area = [tex]πr^2[/tex]
Area = 22/7[tex](1.2)^2[/tex]
Area = 4.523 [tex]mm^2[/tex]
The cross-sectional area of the wire with the square cross-sectional area of sides 3.1 mm is given as; Area = [tex]a^2[/tex]
Area = [tex](3.1)^2[/tex]
Area = 9.61[tex]mm^2[/tex]
The resistivity of the material in both cases is the same; therefore, it is a constant. Hence, we can equate the two formulas;R₁ = R₂(l₁ / A₁)(A₂ / l₂)
We know that R₁ = 42 Ω,l₁ = l₂ = 4.2 m,A₁ = 4.523[tex]mm^2[/tex],A₂ = 9.61[tex]mm^2[/tex]
R₂ = R₁ (A₁ / A₂)R₂ = 42(4.523 / 9.61)R₂ = 19.78 Ω
Therefore, the resistance of the wire having square cross-sectional area is 19.78 Ω.
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A block of a clear, glass-ike material sits on a table surrounded by normal air (you may assume r=1.00 in air). A beam of light is incident on the block at an angle of 40.8 degrees. Within the block, the beam is observed to be at an angle of 22 8 degrees from the normal. What is the speed of light in this material? The answer appropriately rounded, will be in the form (X)x 10 m/s. Enter the number (X) rounded to two decimal places
The speed of light in a material can be determined using the relation:
n1 sin(θ1) = n2 sin(θ2),
where n1 = 1 in air (since it is given that r = 1.00 in air) and θ1 = 40.8 degrees (the angle of incidence).
The angle of refraction, θ2, is given as 22.8 degrees.
To find the refractive index, n2, we use:
n2 = n1 sin(θ1)/ sin(θ2)
n2 = sin(40.8)/sin(22.8)
= 1.6 (rounded to one decimal place)
The speed of light in the material can be found using:
v = c/n2, where c is the speed of light in vacuum
v = c/1.6 = 1.875x10^8 m/s (rounded to two decimal places)
Therefore, the speed of light in the material is 1.88 x 10^8 m/s (rounded to two decimal places).
Answer: 1.88
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The magnetic field is 1.50uT at a distance 42.6 cm away from a long, straight wire. At what distance is it 0.150mT ? 4.26×10 2
cm Previous Tries the middle of the straight cord, in the plane of the two wires. Tries 2/10 Previous Tries
The magnetic field strength of [tex]0.150 \mu T[/tex] is achieved at a distance of approximately 13.48 cm from the long, straight wire.
The magnetic field generated by a long, straight wire decreases with distance according to the inverse square law. This means that as the distance from the wire increases, the magnetic field strength decreases.
For calculating distance at which the magnetic field strength is [tex]0.150 \mu T[/tex], a proportion is set using the given information. Denote the distance from the wire where the field strength is[tex]0.150 \mu T[/tex] as x.
According to the inverse square law, the magnetic field strength (B) is inversely proportional to the square of the distance (r) from the wire. Therefore, following proportion can be set as:
[tex](B_1/B_2) = (r_2^2/r_1^2)[/tex]
Plugging in the given values,
[tex](1.50 \mu T/0.150 \mu T) = (42.6 cm)^2/x^2[/tex]
Simplifying the proportion:
[tex]10 = (42.6 cm)^2/x^2[/tex]
For finding x, rearrange the equation:
[tex]x^2 = (42.6 cm)^2/10\\x^2 = 181.476 cm^2[/tex]
Taking the square root of both sides,
x ≈ 13.48 cm
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An LRC circuit reaches resonance at frequency 8.92 Hz. If the resistor has resistance 138Ω and the capacitor has capacitance 3.7μF, what is the inductance of the inductor? A. 3400H B. 340H C. 8.6×10 −5
H D. 86H
The inductance of the inductor is the option is D) 86H.
Given data:Resonance frequency f = 8.92 HzResistance R = 138 ΩCapacitance C = 3.7 μFWe need to find out the inductance L of the inductor. At resonance frequency, the capacitive reactance Xc = Inductive reactance XlThus, we can write;Xc = XlOr, 1 / (2πfC) = 2πfLor, L = 1 / (4π²f²C)Now, putting the values of f and C;L = 1 / (4π² × 8.92² × 3.7 × 10⁻⁶)≈ 86H.
Thus, the correct option is D) 86H.Note:In an LRC circuit, L stands for inductor or coil, R stands for resistor and C stands for the capacitor.
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A battery-operated car utilizes a 12.0 V system. Find the charge (in C) the batteries must be able to move in order to accelerate the 790 kg car from rest to 25.0 m/s, make it climb a 2.10 ✕ 10^2 m high hill, and then cause it to travel at a constant 25.0 m/s by exerting a 4.20 ✕ 10^2 N force for an hour.
The charge the batteries must be able to move in order to accelerate the 790 kg car from rest to 25.0 m/s, make it climb a 2.10 ✕ 10^2 m high hill, and then cause it to travel at a constant 25.0 m/s by exerting a 4.20 ✕ 10^2 N force for an hour is 2.3 x 10^5 C.
The work done by the battery-powered car is obtained from adding the potential and kinetic energy needed to overcome frictional forces.
W= ∆PE + ∆KE + W_friction
(1)Initial potential energy is 0. ∆PE = mgh = (790 kg)(9.8 m/s²)(210 m) = 1.64 x 10^6 J
(2)Final kinetic energy is 0.5mv² = 0.5(790 kg)(25 m/s)² = 4.94 x 10^5 J. ∆KE = 4.94 x 10^5 J
(3)Power is force times velocity.
Power = (4.20 ✕ 10² N)(25 m/s) = 1.05 x 10^4 W
(4)Time is one hour or 3600 s.
(5)The total work is the sum of ∆PE, ∆KE, and work from friction. Work = ∆PE + ∆KE + W_friction = W
(6)Efficiency = work output/work input = (5)/(6)(7)
Power is equal to energy divided by time. P = E/t
(8)Current is power divided by voltage. P = IVI = P/V
(9)Charge is current times time. Q = ItCharge (Q) = Current (I) × time (t) = Power (P) / Voltage (V) × time (t)Charge = 1.05 x 10^4 W / 12.0 V × 3,600 s
Charge = 2.3 x 10^5 C
Therefore, the charge the batteries must be able to move in order to accelerate the 790 kg car from rest to 25.0 m/s, make it climb a 2.10 ✕ 10^2 m high hill, and then cause it to travel at a constant 25.0 m/s by exerting a 4.20 ✕ 10^2 N force for an hour is 2.3 x 10^5 C.
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The intensity of a certain sound wave is 5.42 W/m2. If its intensity is raised by 12.4 decibels, the new intensity (in W/m2)
The intensity of a sound wave is given as 5.42 W/m².
If its intensity is raised by 12.4 decibels, we are to find the new intensity of the sound wave in W/m².
Formula relating intensity and decibel is; dB = 10 log (I/I₀)⇒ I/I₀ = antilog (dB/10)Where, I₀ is the threshold of hearing. Sound intensity ratio in (dB) = 12.4So, new intensity = I = I₀ antilog (dB/10) = 1 x antilog (12.4/10)W/m².
Therefore, new intensity = 1.5 x 5.42 W/m² = 8.13 W/m².Hence, the new intensity (in W/m²) is 8.13 W/m².
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A converging lens has a focal length of 14.0 cm. Locate the images for object distances of (a) 40.0 cm, (b) 14.0 cm, and (c) 9.0 cm. For each case, state whether the image is real or virtual, upright or inverted, and find the magnification. Sketch a ray diagram for each case showing the 3 important rays.
a. For an object distance of 40.0 cm, the image formed by a converging lens with a focal length of 14.0 cm is real, inverted, and located beyond the focal point. The magnification can be determined using the lens formula and is less than 1.
b. For an object distance of 14.0 cm, the image formed by the lens is at infinity, resulting in a real, inverted, and highly magnified image.
c. For an object distance of 9.0 cm, the image formed by the lens is virtual, upright, and located on the same side as the object. The magnification is greater than 1.
a. When the object distance is 40.0 cm, the image formed by the converging lens is real, inverted, and located beyond the focal point. The magnification (m) can be determined using the lens formula:
1/f = 1/v - 1/u,
where f is the focal length, v is the image distance, and u is the object distance. By substituting the given values, we can solve for v and calculate the magnification.
b. For an object distance of 14.0 cm, the image formed by the lens is at infinity, resulting in a real, inverted, and highly magnified image. This occurs when the object is placed at the focal point of the lens. The magnification in this case can be calculated using the formula:
m = -v/u,
where v is the image distance and u is the object distance.
c. When the object distance is 9.0 cm, the image formed by the lens is virtual, upright, and located on the same side as the object. This occurs when the object is placed inside the focal point of the lens. The magnification can be calculated using the same formula as in case a. However, the magnification will be greater than 1, indicating an upright and enlarged image.
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A 3-phase electrical device connected as a Y circuit with each phase having a resistance of 25 ohms. The line voltage is 230 volts.
a. What is the phase current??
In a Y-connected circuit, the line voltage (V_line) is equal to the phase voltage (V_phase). Therefore, the line voltage is 230 volts. The phase current in the Y-connected circuit is 9.2 Amperes.
To calculate the phase current (I_phase), we need to use Ohm's Law. Ohm's Law states that the current (I) flowing through a resistor is equal to the voltage (V) across the resistor divided by the resistance (R).
In this case, the resistance of each phase is given as 25 ohms. Since the line voltage (V_line) is equal to the phase voltage (V_phase), we can use the line voltage in the calculation.
Using Ohm's Law: I_phase = V_phase / R_phase
Since V_line = V_phase, we can substitute the values: I_phase = V_line / R_phase
Substituting V_line = 230 volts and R_phase = 25 ohms, we get:
I_phase = 230 V / 25 Ω = 9.2 Amperes
Therefore, the phase current in the Y-connected circuit is 9.2 Amperes.
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A 68 kg skier approaches the foot of a hill with a speed of 15 m>s. The surface of this hill slopes up at 40.0° above the horizontal and has coefficients of static and kinetic friction of 0.75 and 0.25, respectively, with the skis. (a) Use energy conservation to find the maximum height above the foot of the hill that the skier will reach. (b) Will the skier remain at rest once she stops, or will she begin to slide down the hill? Prove your answer.
Final kinetic energy,Ek2 = 1/2 × m × v2²Ek2 = 1/2 × (68 kg) × (v2)²Ek2 = 34m²/s². The weight of the skier, mg = (68 kg)(9.8 m/s²)mg = 666.4 N. Therefore, the frictional force will be able to balance the weight of the skier and prevent her from sliding down the hill.
(a) Maximum height the skier will reach. The work-energy principle of physics states that the total work done on a system is equal to the change in its kinetic energy.
In other words, the work-energy principle says that the initial kinetic energy plus the work done on the system equals the final kinetic energy.
When a skier is skiing down a hill, he is losing gravitational potential energy and gaining kinetic energy. So, if we can determine the initial and final kinetic energies, we can find the maximum height reached by the skier.
Work done by frictional force, Wfriction = fs×m×g×cosθ×dwhere fs = 0.75 is the coefficient of static friction between skis and snow,m = 68 kg is the mass of the skier, g = 9.8 m/s² is the acceleration due to gravity,θ = 40.0° is the angle of the slope, d = L/sinθ is the length of the slope,L = vt = (15 m/s)(10 s) = 150 m is the length of the slope that the skier covers in 10 seconds. Wfriction = (0.75)(68 kg)(9.8 m/s²) cos 40° (150 m/sin 40°)W friction = 21917 J Initial kinetic energy,Ek1 = 1/2 × m × v1²Ek1 = 1/2 × (68 kg) × (15 m/s)²Ek1 = 15300 J
Conservation of energy states that the sum of initial kinetic energy and initial potential energy is equal to the sum of final kinetic energy and final potential energy, where potential energy comes in the form of gravitational potential energy when we deal with vertical motions. Mathematically, it can be written asInitial kinetic energy + Initial potential energy = Final kinetic energy + Final potential energySince the skier starts from rest, the initial kinetic energy is zero.
Hence, Initial potential energy at the foot of the hill = Final kinetic energy + Final potential energywhere potential energy is given bymgh where m is the mass of the object, g is the acceleration due to gravity, and h is the height of the object above some reference point (usually the ground).
Final kinetic energy,Ek2 = 1/2 × m × v2²Ek2 = 1/2 × (68 kg) × (v2)²Ek2 = 34m²/s²
Final potential energy at the maximum height h = Final potential energy at the foot of the hill + Work done by frictional force-mgh = 0 + Ek1 - Ek2 - Wfriction-mgh = (15300 J) - (34 m²/s²) - (21917 J)-mgh = -66617 Jh = 33.81 mTherefore, the maximum height that the skier will reach is 33.81 m.
(b)The skier will remain at rest once she stops since the coefficient of static friction between skis and snow is 0.75, which is greater than the coefficient of kinetic friction, 0.25.
When the skier stops, the force of friction between skis and snow will be the maximum value of static friction, which is given byfs × m × gfs × m × g = (0.75)(68 kg)(9.8 m/s²)fs × m × g = 477.48 N
The weight of the skier,mg = (68 kg)(9.8 m/s²)mg = 666.4 N
Therefore, the frictional force will be able to balance the weight of the skier and prevent her from sliding down the hill.
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A circuit connects battery to three light bulbs in parallel. In other words, all the light bulbs are in parallel with one another, and in parallel with the battery. What happens to the circuit if one of the light bulb burns out? Why? A. Total resistance increases, other bulbs get brighter B. Total resistance increases, other bulbs get dimmer C. Total resistance increases, brightness of other bulbs does not change D. All the bulbs go out E. Total resistance decreases, other bulbs get brighter F. Total resistance decreases, other bulbs get dimmer G. Total resistance decreases, brightness of other bulbs does not change
If one of the light bulb burns out, Total resistance increases, other bulbs get dimmer. The circuit would not be broken if one of the bulbs burns out. This is the effect of a parallel circuit when one component fails. Therefore. the correct answer is option B.
In a parallel circuit, each device operates independently. As a result, if one component fails, it does not cause the others to stop working. However, since the resistance of each bulb is fixed, the total resistance of the circuit decreases as bulbs are added.
When a bulb burns out, the resistance of the circuit rises, making the other bulbs dimmer. Because the current in a parallel circuit is divided among the components, the current flowing through each remaining bulb would decrease if one bulb burns out.
So, if one bulb fails, the voltage across it would drop, and it would get dimmer. That's why in parallel circuit the bulbs are installed in parallel to ensure that they function independently of each other. So, option B is the correct answer.
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An experimental bicycle wheel is place on a test stand so that it is free to turn on its axle. If a constant net torque of 7.5 N-m is applied to the tire for 1.5 seconds, the angular speed of the tire increases from 0 to 2 rev/min. The external torque is then removed, and the wheel is brought to rest by friction in its bearings in 175 s. a) Compute the moment of inertia of the wheel about the rotation rate. b) Compute the friction torque. c) Compute the total number of revolutions made by the wheel in the 175-second time interval.
Answer:
The total number of revolutions made by the wheel in the 175-second time interval is approximately 8.75 revolutions.
a) To compute the moment of inertia of the wheel about the rotation axis, we can use the equation:
Δθ = (1/2)αt^2
Where Δθ is the change in angle (in radians), α is the angular acceleration (in radians per second squared), and t is the time (in seconds).
Initial angular velocity, ω_i = 0 rev/min
Final angular velocity, ω_f = 2 rev/min
Time, t = 1.5 s
First, let's convert the angular velocities to radians per second:
ω_i = (0 rev/min) * (2π rad/rev) * (1 min/60 s) = 0 rad/s
ω_f = (2 rev/min) * (2π rad/rev) * (1 min/60 s) = (2π/30) rad/s
The angular acceleration can be calculated using the equation:
α = (ω_f - ω_i) / t
α = [(2π/30) rad/s - 0 rad/s] / 1.5 s = (2π/30) rad/s^2
Now, let's find the change in angle:
Δθ = (1/2) * (2π/30) rad/s^2 * (1.5 s)^2
Δθ = (π/30) rad
The moment of inertia (I) of the wheel can be determined using the equation:
Δθ = (1/2)αt^2 = (1/2) * (I * α) * t^2
Rearranging the equation:
I = (2Δθ) / (α * t^2)
Substituting the values:
I = (2 * π/30) rad / ((2π/30) rad/s^2 * (1.5 s)^2)
I = 2.222 kg·m^2
b) To compute the friction torque, we can use the equation:
τ_f = I * α
Substituting the values:
τ_f = (2.222 kg·m^2) * (2π/30) rad/s^2
τ_f ≈ 0.370 N·m
c) To compute the total number of revolutions made by the wheel in the 175-second time interval, we can use the equation:
Δθ = ω_avg * t
Where Δθ is the change in angle (in radians), ω_avg is the average angular velocity (in radians per second), and t is the time (in seconds).
Time, t = 175 s
First, let's calculate the average angular velocity:
ω_avg = (ω_i + ω_f) / 2 = (0 rad/s + (2π/30) rad/s) / 2 = (π/30) rad/s
Now, we can find the change in angle:
Δθ = (π/30) rad/s * 175 s
Δθ = 175π/30 rad ≈ 18.333π rad
To calculate the number of revolutions, we divide the change in angle by 2π:
Number of revolutions = (175π/30 rad) / (2π rad/rev) ≈ 8.75 rev
Therefore, the total number of revolutions made by the wheel in the 175-second time interval is approximately 8.75 revolutions.
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A parallel beam of monoenergetic photons emerged from a source when the shielding was removed for a short time. The photon energy hv and the total fluence o of photons are known. (a) Write a formula from which one can calculate the absorbed dose in air in rad from hv, expressed in MeV, and p, expressed in cm-². (b) Write a formula for calculating the exposure in R.
(a) Formula from which one can calculate the absorbed dose in the air in rad from hv, expressed in MeV, and p is [tex]D = (0.877 * o * hv) / p[/tex]. (b) the formula for calculating the exposure in R is [tex]X = (0.87 * o *hv)[/tex].
(a)These formulas allow for the calculation of radiation effects in different units. To calculate the absorbed dose in the air in rad (D), expressed in MeV and cm², the formula can be written as:
[tex]D = (0.877 * o * hv) / p[/tex]
Where o represents the total fluence of photons and hv represents the energy of photons in MeV. p is the area in [tex]cm^2[/tex] over which the radiation is spread.
(b)For calculating the exposure in R (X), the formula can be expressed as:
[tex]X = (0.87 * o *hv)[/tex]
Again, o represents the total fluence of photons and hv represents the energy of photons in MeV.
These formulas provide a means to quantify the absorbed dose and exposure to radiation in the air, allowing for a better understanding and assessment of radiation effects.
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A circular loop of wire with a radius 7.932 cm is placed in a magnetic field such that it induces an EMF of 3.9 V in the cir- cular wire loop. If the cross-sectional diame- ter of the wire is 0.329 mm, and the wire is made of a material which has a resistivity of 1.5 × 10⁻⁶ Nm, how much power is dissipated in the wire loop? Answer in units of W.
Radius of the circular loop, r = 7.932 cm Cross-sectional diameter of the wire, d = 0.329 mm Resistivity of the material, ρ = 1.5 × 10⁻⁶ Nm EMF induced in the circular wire loop, E = 3.9 V
We can find out the current in the circular loop of wire using the formula,
EMF = I × R where I is the current flowing through the wire and R is the resistance of the wire. R = ρl / A Diameter of the wire, d = 0.329 mm Radius of the wire, r' = 0.329 / 2 = 0.1645 mm Area of cross-section of the wire, A = πr'² = π(0.1645 × 10⁻³ m)² = 2.133 × 10⁻⁷ m² Length of the wire, l = 2πr = 2π(7.932 × 10⁻² m) = 0.4986 m
Resistance of the wire, R = (1.5 × 10⁻⁶ Nm × 0.4986 m) / 2.133 × 10⁻⁷ m² = 35.108 ΩI = E / R = 3.9 V / 35.108 Ω = 0.111 A
The magnetic field, B = E / A = 3.9 V / 2.133 × 10⁻⁷ m² = 1.829 × 10⁴ T
Power, P = I²R = (0.111 A)² × 35.108 Ω = 0.0436 W
Therefore, the power dissipated in the wire loop is 0.0436 W.
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A car travels in a straight line along a road. Its distance x from a stop sign is given as a function of time t by the equation x=1.4t²−8.8t³ (SI units). Calculate the distance of the car when it achieves its maximum speed in the positive x direction.
The distance traveled by the car when it achieves its maximum speed in the positive x direction is approximately 0.0016 kilometers.
Distance function: x = 1.4t² - 8.8t³
To determine the distance when the car achieves its maximum speed, we need to find the point where the velocity is maximum. The velocity is the first derivative of the distance function with respect to time.
By taking the derivative of the distance function with respect to time, we can find the rate of change of distance over time.
dx/dt = 2.8t - 26.4t²
To find the maximum speed, we need to find the point where the velocity is equal to zero:
2.8t - 26.4t² = 0
Simplifying the equation, we have:
t(2.8 - 26.4t) = 0
This equation has two solutions: t = 0 and t = 0.1061 seconds. Since we are interested in the time when the car achieves maximum speed, we consider t = 0.1061 seconds.
Now, we can calculate the distance by substituting this value of t into the distance function:
x = 1.4(0.1061)² - 8.8(0.1061)³
x ≈ 0.0016 kilometers
Therefore, the distance traveled by the car when it achieves its maximum speed in the positive x direction is approximately 0.0016 kilometers.
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A 4.0-kg mass attached to a spring oscillates in simple harmonic motion according to the expression e(t) = (15cm) cos (rad|s) + (7/3)rad). The time required for the mass to undergo two complete oscillations is: (a) 10.1 s (b) 5.03 s (c) 2.51 s (d) 1.26 s The maximum acceleration of the mass is: (a) 0.75 m/s2 (b) 3.75 m/s2 (c) 5.00 m/s2 (d) 25.0 m/s2
The value of the dielectric constant of the unknown material is approximately 1.037.
To calculate the value of the dielectric constant of the unknown material, we can use the concept of capacitance and the parallel plate capacitor equation.
The capacitance of a parallel plate capacitor is given by the formula:
C = (ε₀ * εr * A) / d
where C is the capacitance, ε₀ is the permittivity of free space (8.85 x 10^-12 F/m), εr is the relative permittivity (dielectric constant) of the material between the plates, A is the area of each plate, and d is the distance (gap) between the plates.
C = 95 pF = 95 x 10^-12 F
A = 110 cm^2 = 110 x 10^-4 m^2
d = 3.25 mm = 3.25 x 10^-3 m
We need to find the dielectric constant εr of the unknown material.
We can rearrange the formula to solve for εr:
εr = (C * d) / (ε₀ * A)
Substituting the given values:
εr = (95 x 10^-12 F * 3.25 x 10^-3 m) / (8.85 x 10^-12 F/m * 110 x 10^-4 m^2)
εr ≈ 1.037
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A single-phase 50-kVA, 2400/240-volt, 60-Hz distribution transformer is used as a stepdown transformer. The feeder (the line connected between the source and the primary terminal of the transformer) has the series impedance of (1.0 + j2.0) ohms. The equivalent series winding impedance of the transformer is (1.0 + j2.5) ohms. The transformer is delivering the rated power to the load at 0.8 power factor lagging at the rated secondary voltage. Neglect the transformer exciting current. (a) Replace all circuit elements with perunit values. (b) Find the per-unit voltage and the actual voltage at the transformer primary terminals. (c) Find the per-unit voltage and the actual voltage at the sending end of the feeder. (d) Find the real and reactive power delivered to the sending end of the feeder.
A single-phase 50-kVA, 2400/240-volt, 60-Hz distribution transformer is used as a stepdown transformer. The feeder (the line connected between the source and the primary terminal of the transformer) has the series impedance of (1.0 + j2.0) ohms. The equivalent series winding impedance of the transformer is (1.0 + j2.5) ohms.(a)Feeder impedance: 0.004167 + 0.008333 j ,Transformer impedance: 0.004167 + 0.009375 j(b) actual voltage at the primary terminals is 2400 volts.(c)The actual voltage at the sending end of the feeder is 2394.4 volts.(d) The real and reactive power delivered to the sending end of the feeder are 49.833 kVA and 33.125 kVA, respectively.
(a) To replace all circuit elements with per-unit values, we need to choose a base. In this case, we will choose the transformer's rated kVA as the base. This means that the transformer's rated voltage and current will be 1 per unit. The feeder's impedance and the transformer's equivalent series impedance can then be converted to per-unit values by dividing them by the transformer's rated voltage. The resulting per-unit values are:
Feeder impedance: 0.004167 + 0.008333 j
Transformer impedance: 0.004167 + 0.009375 j
(b) The per-unit voltage at the transformer primary terminals is equal to the transformer's turns ratio times the per-unit voltage at the secondary terminals. The turns ratio is given by the ratio of the transformer's rated voltages, which in this case is 2400/240 = 10. So the per-unit voltage at the primary terminals is 10 times the per-unit voltage at the secondary terminals, which is 1.0. This means that the actual voltage at the primary terminals is 2400 volts.
(c) The per-unit voltage at the sending end of the feeder is equal to the per-unit voltage at the transformer primary terminals minus the per-unit impedance of the feeder times the per-unit current flowing through the feeder. The per-unit current flowing through the feeder is equal to the real power delivered to the load divided by the transformer's rated voltage. The real power delivered to the load is 50 kVA, and the transformer's rated voltage is 2400 volts. So the per-unit current flowing through the feeder is 0.208333. This means that the per-unit voltage at the sending end of the feeder is 1.0 - 0.004167 ×0.208333 = 0.995833. This means that the actual voltage at the sending end of the feeder is 2394.4 volts.
(d) The real and reactive power delivered to the sending end of the feeder are equal to the real and reactive power delivered to the load. The real power delivered to the load is 50 kVA, and the reactive power delivered to the load is 33.333 kVA. This means that the real and reactive power delivered to the sending end of the feeder are 49.833 kVA and 33.125 kVA, respectively.
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1.The average geothermal gradient is about
degrees C/km.
2.A _texture is one in which layers occur that are produced by the preferred orientation of micas.
3. How deep would sedimentary rocks need to be buried to start becoming metamorphosed:
1.) The average geothermal gradient is about 25 degrees C/km.
2.) A schistose texture is one in which layers occur that are produced by the preferred orientation of micas.
3.) Sedimentary rocks would need to be buried at least 10 kilometers to start becoming metamorphosed.
1.) The average geothermal gradient is about 25 degrees C/km. Geothermal gradient refers to the rate of increase of temperature with depth in the Earth's interior. This rate varies depending on location, but the average rate is 25°C per kilometer of depth.
2.) A Schistose texture is one in which layers occur that are produced by the preferred orientation of micas. The schistose texture is the result of high pressure and temperature during metamorphism. During this process, micas (which are platy minerals) are forced to line up parallel to each other. This produces a layering or banding effect that is characteristic of schist.
3.) Sedimentary rocks would need to be buried at a depth of at least 10 kilometers to start becoming metamorphosed. This is because metamorphism requires high temperature and pressure, which are found at great depths in the Earth's interior. At this depth, the rocks would be subjected to high pressure from the overlying rocks and high temperature from the Earth's internal heat. This would cause them to undergo metamorphism and transform into a different type of rock. However, the exact depth required for metamorphism to occur depends on factors such as the composition of the rocks and the rate at which they are buried.
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Two identical, coherent rays of light interfere with each other. Separately, they each have an intensity of 30.5 W/m². What is the resulting intensity of the light if the phase shift between them is 1.15 radians? a. 61 W/m²
b. 42.96 W/m²
c. 25.6 W/m²
d. 51.19 W/m²
Two identical, coherent rays of light interfere with each other. Separately, they each have an intensity of 30.5 W/m².The resulting intensity of the light is approximately 88.827 W/m².So option b is correct.
The intensity of the light is calculated using the following formula:
Intensity = I₁ + I₂ + 2×I₁×I₂×cos(φ)
where:
I₁ and I₂ are the intensities of the two waves
phi is the phase difference between the two waves
In this case, I₁ = I₂ = 30.5 W/m² and phi = 1.15 radians. Plugging these values into the formula, we get:
Intensity = 30.5 W/m² + 30.5 W/m² + 2×30.5 W/m²×30.5 W/m²×cos(1.15 radians)
= 42.96 W/m²
Therefore option b is correct.
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Give an example where first the speed of the object increases, then emains constant for some time and then decrease.
H A man drags a 72-kg crate across the floor at a constant velocity by pulling on a strap attached to the bottom of the crate. The crate is tilted 25 ∘
above the horizontal, and the strap is inclined 61 ∘
above the horizontal. The center of gravity of the crate coincides with its geometrical center, as indicated in the drawing. Find the magnitude of the tension in the strap.
The problem involves calculating the tension in the strap used to pull a crate.
This tension is influenced by the weight of the crate, the angle at which the crate is tilted, and the angle of the strap from the horizontal. With known values, we can use fundamental physics equations to solve for the unknown tension. Let's break this down. The crate isn't accelerating, which means that the net force on it must be zero. Thus, the vertical component of the tension (T) in the strap must balance out the weight of the crate, and the horizontal component of the tension must balance the frictional force acting on the crate. Given the weight (W) of the crate is 72 kg * 9.8 m/s², the vertical component of the tension can be calculated as Tsin61° = Wsin25°. Solving for T gives us the tension in the strap.
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A rocket is launched from the Rocket Lab launch site at Mahia (latitude 39 south). Calculate the acceleration caused by centrifugal and Coriolis forces when it is travelling vertically at 5000 km/hour.
The acceleration caused by centrifugal and Coriolis forces when a rocket is traveling vertically at 5000 km/hour from the Rocket Lab launch site at Mahia (latitude 39° south) is approximately 0.079 m/s².
The centrifugal force and Coriolis force are the two components of the fictitious forces experienced by an object in a rotating reference frame. The centrifugal force acts outward from the axis of rotation, while the Coriolis force acts perpendicular to the object's velocity.
To calculate the acceleration caused by these forces, we need to consider the angular velocity and the latitude of the launch site. The angular velocity [tex](\( \omega \))[/tex] can be calculated using the rotational period of the Earth T:
[tex]\[ \omega = \frac{2\pi}{T} \][/tex]
The centrifugal acceleration [tex](\( a_c \))[/tex]can be calculated using the formula:
[tex]\[ a_c = \omega^2 \cdot R \][/tex]
where R is the distance from the axis of rotation (in this case, the radius of the Earth).
The Coriolis acceleration[tex](\( a_{\text{cor}} \))[/tex] can be calculated using the formula:
[tex]\[ a_{\text{cor}} = 2 \cdot \omega \cdot v \][/tex]
where v is the velocity of the rocket.
Given that the latitude is 39° south, we can determine the radius of the Earth R at that latitude using the formula:
[tex]\[ R = R_{\text{equator}} \cdot \cos(\text{latitude}) \][/tex]
Substituting the given values and performing the calculations, we find that the acceleration caused by centrifugal and Coriolis forces is approximately 0.079 m/s².
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Part A: Calculate the work done (in SI units) when 1 mole of gas expands from 5 dmº to 10 dm2 against a constant pressure of 1 atmosphere. Part B: A steam turbine is operating under the following conditions: steam to the turbine at 900°F and 120 psia, velocity – 250 ft/s; steam exiting at 700°F and 1 atm, velocity = 100 fts. Under these conditions, the enthalpy rate in and out are given as 1478.8 Btu/lb and 1383.2 Btu/lb as read from the steam tables, respectively. Calculate the rate at which work (in horsepower, hp) can be obtained from the turbine if the steam flow is 25,000 lb/h and the turbine operation is steady stat adiabatic.
Part A: the work done by 1 mole of gas is 0.5065 J. Part B: the rate at which work can be obtained from the turbine is 9286.36 hp.
Part A:Work done by an ideal gas is given by W = pΔV. Given:1 mole of gas expands from 5 dm3 to 10 dm3 against a constant pressure of 1 atmosphere.The pressure p = 1 atm The initial volume V1 = 5 dm³ = 5 x 10⁻³ m³The final volume V2 = 10 dm³ = 10 x 10⁻³ m³Therefore, the change in volume ΔV = V2 - V1= (10 x 10⁻³) - (5 x 10⁻³)= 5 x 10⁻³ m³ Now, work done by the gas,W = pΔV= (1 atm) x (5 x 10⁻³ m³)= 5 x 10⁻³ atm.m³ But, 1 atm.m³ = 101.3 J Therefore, W = (5 x 10⁻³) x 101.3= 0.5065 J Hence, the work done by 1 mole of gas is 0.5065 J.
Part B:Given:Mass flow rate of steam m = 25,000 lb/h Inlet steam conditions:Temperature T1 = 900 °FPressure P1 = 120 psiaEnthalpy h1 = 1478.8 Btu/lbExit steam conditions:Temperature T2 = 700 °FPressure P2 = 1 atmEnthalpy h2 = 1383.2 Btu/lbThe rate of work done is given by the expression, W = m (h1 - h2)In order to convert the units to SI units, we first need to convert the mass from lb/h to kg/s.1 lb = 0.4536 kg; 1 h = 3600 sTherefore, 1 lb/h = 0.4536/3600 kg/s = 1.26 x 10⁻⁴ kg/s Mass flow rate of steam m = 25,000 lb/h = 3.15 kg/s.
Therefore, the rate of work done isW = m (h1 - h2) = (3.15) (h1 - h2) Let's convert the enthalpies from Btu/lb to J/kg,1 Btu = 1055.06 J; 1 lb = 0.4536 kg Therefore, 1 Btu/lb = 2326 J/kgEnthalpy h1 = 1478.8 Btu/lb = 1478.8 x 2326 J/kg= 3.44 x 10⁶ J/kgEnthalpy h2 = 1383.2 Btu/lb = 1383.2 x 2326 J/kg= 3.22 x 10⁶ J/kgSubstituting the values in the equation,W = m (h1 - h2) = (3.15) (3.44 x 10⁶ - 3.22 x 10⁶)= 6.93 x 10⁶ J/s To convert the power from J/s to horsepower, we use the conversion 1 hp = 746 W. Power P = W/746= (6.93 x 10⁶) / 746= 9286.36 hp .
Therefore, the rate at which work can be obtained from the turbine is 9286.36 hp.
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