Answer:
work done is -150 kJ
Explanation:
given data
volume v1 = 2 m³
pressure p1 = 100 kPa
pressure p2 = 200 kPa
internal energy = 10 kJ
heat is transferred = 150 kJ
solution
we know from 1st law of thermodynamic is
Q = du +W ............1
put here value and we get
-140 = 10 + W
W = -150 kJ
as here work done is -ve so we can say work is being done on system
Final answer:
The work done by the gas during the compression where 2 m³ of an ideal gas is compressed from 100 kPa to 200 kPa, with an internal energy increase of 10 kJ, and 150 kJ of heat transferred to the surroundings, is -160 kJ.
Explanation:
The student has asked how much work was done by the gas during a compression process in which 2 m³ of an ideal gas is compressed from 100 kPa to 200 kPa, the internal energy increases by 10 kJ, and 150 kJ of heat is transferred to the surroundings. To find the work done by the gas, we can use the first law of thermodynamics, which states that the change in internal energy (ΔU) is equal to the heat added to the system (Q) minus the work done by the system (W). The formula is ΔU = Q - W.
In this scenario, we have ΔU as +10 kJ (because the internal energy increases) and Q as -150 kJ (because heat is transferred to the surroundings, meaning it is leaving the system, thus it's a negative value). Plugging these values into the first law of thermodynamics gives us:
10 kJ = -150 kJ - W
When we rearrange the equation to solve for W, it becomes:
W = -150 kJ - 10 kJ
W = -160 kJ
Since work done by the system is a negative value in this case, it indicates that 160 kJ of work has been done on the gas by the surroundings during the compression. Thus, the work done by the gas itself is -160 kJ.
A pressure cooker cooks a lot faster than an ordinary pan by maintaining a higher pressure and temperature inside. the lid of a pressure cooker is well sealed, and steam can escape only through an opening in the middle of the lid. a separate metal piece, the petcock, sits on top of this opening and prevents steam from escaping until the pressure force overcomes the weight of the petcock. the periodic escape of the steam in this manner prevents any potentially dangerous pressure buildup and keeps the pressure inside at a constant value. determine the mass of the petcock of a pressure cooker whose operation pressure is 100 kpa gauge and has an opening cross-sectional area of 4 mm2. assume an atmospheric pressure of 101 kpa.
A pressure cooker cooks a lot faster than an ordinary pan by maintaining a higher pressure and temperature inside. The mass of the petcock of the pressure cooker is approximate [tex]40.8\ gm[/tex].
The pressure force on the petcock is the difference between the pressure inside the cooker and the atmospheric pressure, multiplied by the cross-sectional area of the opening:
Pressure force = (Pressure inside - Atmospheric pressure) * Opening area
Given that the operating pressure is 100 kPa gauge and the atmospheric pressure is 101 kPa,
Pressure inside[tex]= (100+ 101) \times 1000 = 201000\ Pa[/tex]
Atmospheric pressure [tex]= 101 \times 1000 = 101000\ Pa[/tex]
Now, calculate the pressure force:
Pressure force[tex]= (201000\ Pa - 101000\ Pa) \times 4\ mm^2[/tex]
Pressure force [tex]= 100000\ Pa \times 4 \times 10^{-6} m^2[/tex]
Pressure force [tex]= 0.4\ N[/tex]
The weight of the petcock is equal to the force of gravity acting on it:
Weight = mass × gravitational acceleration
[tex]Weight = mass \times 9.8 m/s^2\\m \times 9.8 = 0.4 \\m = 0.4 / 9.8 \\m = 0.0408\ kg[/tex]
So, the mass of the petcock of the pressure cooker is approximate [tex]40.8\ gm[/tex].
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To find the mass of the petcock, we calculate the force exerted by the steam using the given pressure and area, then equate it to the weight of the petcock. This gives us a mass of approximately 0.082 kg.
To determine the mass of the petcock in a pressure cooker, we need to understand the pressure dynamics and forces at play. The pressure cooker operates at a gauge pressure of [tex]100 kPa,[/tex] and the cross-sectional area of the opening through which steam escapes is given as [tex]4 mm^2[/tex].
First, let's convert the cross-sectional area from [tex]mm^2[/tex] to [tex]m^2[/tex]:
[tex]4 mm^2 = 4 \times 10^{-6} m^2[/tex]
The force exerted by the steam on the petcock can be calculated using the pressure-force relationship: [tex]F = PA[/tex]
Here, P is the absolute pressure inside the cooker, which is the sum of the gauge pressure and the atmospheric pressure:
[tex]P = 100 kPa (gauge) + 101 kPa (atmospheric) = 201 kPa[/tex]
The force is then:
[tex]F = P \times A = 201,000 Pa \times 4 \times 10^{-6} m^2 = 0.804 N[/tex]
The force exerted by the petcock due to its weight is [tex]F = mg[/tex], where m is the mass and g is the acceleration due to gravity ([tex]9.81 m/s^2[/tex]).
Setting the force exerted by the steam equal to the weight of the petcock gives us:
[tex]mg = 0.804 N[/tex]
Therefore, the mass of the petcock is:
[tex]m = F/g = 0.804 N / 9.81 m/s^2 \approx 0.082 kg[/tex]
Thus, the mass of the petcock is approximately [tex]0.082 kg[/tex].
A device expends 130 kJ of energy while pressurizing 10 kg of water initially at 17oC. The isentropic efficiency of the device is 50%. Inefficiencies are represented by a heat loss from the device casing. What is most nearly the final temperature of the water?
Answer:
T = 19°C
Explanation:
The solved solution is in the attach document.
Answer:
T2 = 19°C
Explanation:
See the attachment below.
A chamber fitted with a piston can be controlled to keep the pressure in the chamber constant as the piston moves up and down to increase or decrease the chamber volume. The chamber contains an ideal gas at 296 K and 1.00 atm.What is the work done on the gas as the piston compresses it from 1.00 L to 0.633 L ?
Express your answer with the appropriate units.
W =
J
Answer:
W = 37.2J
Explanation:
See attachment below.
You stand 17.5 m from a wall holding a tennis ball. You throw the tennis ball at the wall at an angle of 22.5∘ from the ground with an initial speed of 24.5 m/s. At what height above its initial position does the tennis ball hit the wall? Ignore any effects of air resistance.
The height of the ball would be 4.32 m
Explanation:
Given-
Distance from the ball, s = 17.5 m
Angle of projection, θ = 22.5°
Initial speed, u = 24.5 m/s
Height, h = ?
Let t be the time taken.
Horizontal speed, [tex]u_{x}[/tex] = u cosθ
= 24.5 * cos 22.5°
= 24.5 * 0.924
= 22.64 m/s
Vertical velocity, [tex]u_{y}[/tex] = u sinθ
= 24.5 * sin 22.5°
= 24.5 * 0.383
= 9.38 m/s
We know,
[tex]x = u * cos (theta) * t[/tex]
[tex]17.5 = 22.64 * t\\\\t = 0.77s[/tex]
To calculate the height:
[tex]h = ut - \frac{1}{2}gt^2[/tex]
[tex]h = u sin (theta)t - \frac{1}{2} gt^2[/tex]
[tex]h = 9.38 * 0.77 - \frac{1}{2} * 9.8 * (0.77)^2\\ \\h = 7.22 - 2.90\\\\h = 4.32m\\[/tex]
Therefore, height of the ball would be 4.32 m
Atmospheric pressure is reported in a variety of units depending on local meteorological preferences. In many European countries the unit millibar (mbar) is preferred, in other countries the unit hectopascal (1 hPa = 1 mbar) is used, and in the United States inches of mercury (in Hg) is the commonly used unit. In most chemistry textbooks the units most commonly used are torr, mmHg, and atmospheres (atm). The unit atm is defined at sea level to be 1 atm = 760 mm Hg exactly. The density of mercury is 13.534 times that of water, if atmospheric pressure will support 769.6 mm Hg, what height of a water column would that same pressure support in mm?
Answer:
[tex]h_w=10415.7664\ mm[/tex] of water column.
Explanation:
Given:
density of mercury, [tex]S_m=13.534[/tex]
height of the mercury column supported by the atmosphere, [tex]h_m=769.6\ mm[/tex]
As we know that the equivalent pressure in terms of liquid column is given as:
[tex]P=\rho.g.h[/tex]
so,
[tex]S_m\times 1000\times g.h_m=\rho_w.g.h_w[/tex]
where:
[tex]g=[/tex] gravity
[tex]h_w=[/tex] height of water column
[tex]\rho_w=[/tex] density of water
[tex]13534\times 9.8\times 769.6=1000\times 9.8\times h_w[/tex]
[tex]h_w=10415.7664\ mm[/tex] of water column.
Final answer:
The atmospheric pressure that supports a 769.6 mm column of mercury will support a water column that is 13.6 times taller due to the density difference, resulting in a water column approximately 10,466.56 mm, or about 10.47 meters, tall.
Explanation:
When we talk about atmospheric pressure, we often use various units like millimeters of mercury (mmHg) or torr, which are equivalent to 1 atm of pressure, defined as exactly 760 mmHg. Since mercury is about 13.6 times denser than water, a column of mercury under atmospheric pressure is much shorter than a column of water under the same pressure. To find the height of a water column supported by a pressure of 769.6 mm Hg, we can set up a proportion using the densities of mercury and water. Since 1 atm supports a 760 mm column of mercury, and the density of mercury is 13.6 times that of water, the same pressure will support a water column that is 13.6 times taller.
The calculation is straightforward:
Height of mercury column (Hg): 769.6 mmDensity ratio (Hg:water): 13.6Height of water column = Height of mercury column × Density ratioHeight of water column = 769.6 mm × 13.6Height of water column = 10466.56 mmTherefore, the atmospheric pressure that supports a 769.6 mm Hg column will support a water column of approximately 10,466.56 mm, or about 10.47 meters tall.
A basketball player throws a chall -1 kg up with an initial speed of his hand at shoulder height = 2.15 m Le gravitational potential energy ber ground level the ball leves 50% .(a) Give the total mechanical energy of the ball E in terms of maximum height Am it reaches, the mass m, and the gravitational acceleration g.(b) What is the height, hm in meters?
Complete Question:
A basketball player tosses a basketball m=1kg straight up with an initial speed of v=7.5 m/s. He releases the ball at shoulder height h= 2.15m. Let gravitational potential energy be zero at ground level
a) Give the total mechanical energy of the ball E in terms of maximum height hn it reaches, the mass m, and the gravitational acceleration g.
b) What is the height, hn in meters?
Answer:
a) Energy = mghₙ
b) Height, hₙ = 5.02 m
Explanation:
a) Total energy in terms of maximum height
Let maximum height be hₙ
At maximum height, velocity, V=0
Total mechanical energy , E = mgh + 1/2 mV^2
Since V=0 at maximum height, the total energy in terms of maximum height becomes
Energy = mghₙ
b) Height, hₙ in meters
mghₙ = mgh + 1/2 mV^2
mghₙ = m(gh + 1/2 V^2)
Divide both sides by mg
hₙ = h + 0.5 (V^2)/g
h = 2.15m
g = 9.8 m/s^2
V = 7.5 m/s
hₙ = 2.15 + 0.5(7.5^2)/9.8
hₙ = 2.15 + 2.87
hₙ = 5.02 m
college physics 1, final exam 2015 a closed 2.0l container holds 3.0 mol of an idea gas. if 200j of heat is added, and no work is done, what is the chanhe in internal enegery of the system
Answer: The change in internal energy of the system is 200 Joules
Explanation:
According to first law of thermodynamics:
[tex]\Delta E=q+w[/tex]
[tex]\Delta E[/tex]=Change in internal energy
q = heat absorbed or released
w = work done or by the system
w = work done by the system=[tex]-P\Delta V=0[/tex]
q = +200J {Heat absorbed by the system is positive}
[tex]\Delta E=+200+0=+200J[/tex]
Thus the change in internal energy of the system is 200 Joules
Assume that the length of the magnet is much smaller than the separation between it and the charge. As a result of magnetic interaction (i.e., ignore pure Coulomb forces) between the charge and the bar magnet, the magnet will experience which of the following?
a. No torque at all
b. A torque only if one magnetic pole is slightly closer to the charge than the other
c. A torque due to the charge attracting the south pole of the magnet
d. A torque due to the charge attracting the north pole of the manget
Answer:
Assuming that the length of the magnet is much smaller than the separation between it and the charge. As a result of magnetic interaction (i.e., ignore pure Coulomb forces) between the charge and the bar magnet, the magnet will not experience any torque at all - option A
Explanation:
Assuming that the length of the magnet is much smaller than the separation between it and the charge. As a result of magnetic interaction (i.e., ignore pure Coulomb forces) between the charge and the bar magnet, the magnet will not experience any torque at all; the reason being that: no magnetic field is being produced by a charge that is static. Only a moving charge can produce a magnetic effect. And the magnet can not have any torque due to its own magnetic lines of force.
The magnet will experience No torque at all.
Ignoring of pure Coulomb forces:Here the length of the magnet should be less than the separation between it and the charge. Due to this there is magnetic interaction (i.e., ignore pure Coulomb forces) that lies between the charge and the bar magnet, the magnet should not experience any torque at all; the reason being that: no magnetic field should be generated via a charge i.e. here a moving charge can generate a magnetic effect. And the magnet can not have any torque because of its own magnetic lines of force.
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How much work does it take for an external agent to move a 45.0-nC charge from a point on the +x-axis, 3.40 cm from the origin to a point halfway between the 41.0-nC and 52.0-nC charges?
Answer:
The work done on the 45.0nC charge is 2.24×10^-3J. The detailed solution can be found in the attachment below.
Explanation:
The Problem solution makes use of the potential energy relationship between the charges. This solution assumes the distance as shown in the diagram. For a different distance arrangement adjustments should be made appropriately.
The question in Physics pertains to the work needed by an external agent to move a charge within an electric field, and it involves applying the concept of electric potential energy. The work done is equal to the change in electric potential energy, which requires knowledge of the charges' positions and potentials.
Explanation:The question asks: How much work does it take for an external agent to move a 45.0-nC charge from a point on the +x-axis, 3.40 cm from the origin to a point halfway between the 41.0-nC and 52.0-nC charges? To answer this question, we would use the concept of electric potential energy in the electric field created by point charges. Work is required to move a charge within an electric field against electric forces. The work done by an external force to move a charge from one point to another is equal to the change in electric potential energy, which can be calculated from the initial and final electric potentials at the points in question.
To find the required work, we need to know the initial and final positions relative to other charges, and then we apply the electric potential energy formula. However, a complete solution would require additional specifics about the configuration and distances between the charges. Without these details, we cannot provide an exact numerical answer.
A running back with a mass of 86 kg and a velocity of 9 m/s (toward the right) collides with, and is held by, a 129-kg defensive tackle going in the opposite direction (toward the left). What is the velocity of the tackle before the collision for their velocity afterward to be zero
Final answer:
The velocity of the defensive tackle before the collision is -6 m/s (toward the left).
Explanation:
According to the law of conservation of momentum, the total momentum before the collision is equal to the total momentum after the collision. Since the two players stick together after the collision, their velocities will be equal but opposite in direction.
Let's assume that the velocity of the defensive tackle before the collision is v. The total momentum before the collision is given by:
m1 * v1 + m2 * v2 = (m1 + m2) * v
Where:
m1 = mass of the running back = 86 kg
v1 = velocity of the running back = 9 m/s (toward the right)
m2 = mass of the defensive tackle = 129 kg
v2 = velocity of the defensive tackle (to be determined)
Using the above equation, we can solve for v:
(86 kg * 9 m/s) + (129 kg * v2) = (86 kg + 129 kg) * 0
774 kg*m/s + 129 kg * v2 = 0 kg*m/s
v2 = -6 m/s
Therefore, the velocity of the defensive tackle before the collision is -6 m/s (toward the left).
Even though Alice visits the wishing well frequently and always tosses in a coin for good luck, none of her wishes have come true. As a result, she decides to change her strategy and make a more emphatic statement by throwing the coin downward into the well. If the water is 7.03 m below the point of release and she hears the splash 0.81 seconds later, determine the initial speed at which she threw the coin. (Take the speed of sound to be 343 m/s.)
Explanation:
The formula to calculate total time taken is as follows.
Total time = time to fall + time for sound
So, time for sound = [tex]\frac{distance}{velocity}[/tex]
= [tex]\frac{7.03}{343}[/tex]
= 0.0204 sec
Hence, time to fall is as follows.
(0.81 - 0.0204) sec
= 0.7896 sec
Now, we will calculate the time to fall as follows.
y = [tex]y_{o} + v_{o}yt + \frac{1}{2}at^{2}[/tex]
0 = [tex]h + v \times t - \frac{1}{2}gt^{2}[/tex]
0 = [tex]7.03 + v \times (0.81 - 0.0204) - 0.5 \times 9.81 \times(0.81 - 0.0204)^{2}[/tex]
= [tex]7.8196 - 0.5 \times 9.81 \times 0.623[/tex]
= 7.8196 - 3.058
= 4.7616 m/s
Therefore, she threw the coin at 4.76 m/s in the upward direction.
A loading car is at rest on a track forming an angle of 25◦ with the vertical when a force is applied to the cable attached at C. The gross weight of the car and its load is 5500 lb, and it acts at point G. Knowing the tension in the cable connected at C is 5000 lb, determine (a) the acceleration of the car, (b) the distance the car moves in 20 s, (c) the time it takes for the car to return to its original position if the cable breaks after 20 s.
Answer:
Check attachment for solution
Explanation:
The motion of the car along the inclined plane reduces the force required
to pull the car upwards.
The correct values are
(a) The acceleration of the car upwards is approximately 0.09 ft./s².
(b) The distance the car moves in 20 s. is approximately 18 ft.
(c) The time it takes the car to return to its original position is approximately 1.[tex]\underline{\overline {1}}[/tex] seconds.
Reasons:
(a) Component of the car's weight acting along the incline plane, [tex]W_\parallel[/tex] = W·sin(θ)
∴ [tex]W_\parallel[/tex] = 5500 lbf × cos(25°) ≈ 4984.69 lbf.
The force pulling the car upwards, F = T - [tex]W_\parallel[/tex]
Which gives;
F = 5,000 lbf - 4984.69lbf = 15.31 lbf
[tex]Mass \ of \ the \ car = \dfrac{5500}{32.174} \approx 170.95[/tex]
The mass of the car, m ≈ 170.95 lbf
[tex]Acceleration = \dfrac{Force}{Mass}[/tex]
[tex]Acceleration \ of \ the \ car = \dfrac{15.31}{170.95} \approx 0.09[/tex]
The acceleration of the car, a ≈ 0.09 ft./s².
(b) The distance the car moves is given by the kinematic equation of
motion, s = u·t + 0.5·a·t², derived from Newton Laws of motion.
Where;
u = The initial velocity of the car = 0 (the car is initially at rest)
t = The time taken = 20 seconds
a = The acceleration ≈ 0.09 ft./s²
∴ s ≈ 0 × 20 + 0.5 × 0.09 × 20² = 18
The distance the car moves, s ≈ 18 ft.
(c) If the cable breaks, we have;
Force acting downwards on the car = Weight of the car acting on the plane
∴ Force acting downwards on the car = [tex]W_\parallel[/tex] = 4984.69 lbf
Therefore;
[tex]Acceleration \ of \ the \ car downwards, \ a_d = \dfrac{W_\parallel}{m}[/tex]
Which gives;
[tex]a_d = \dfrac{4984.69 \ lbf}{170.95 \ lb} \approx 29.16 \ m/s^2[/tex]
The time it takes car to travel the 18 ft. back to its original position is given as follows;
s = u·t + 0.5·a·t²
The initial velocity, u= 0
Therefore;
[tex]t = \mathbf{\sqrt{\dfrac{2 \cdot s}{a} }}[/tex]
Which gives;
[tex]t = \sqrt{\dfrac{2 \times 18}{29.16} } \approx 1.\overline {1}[/tex]
The time it takes the car to return to its original position, t ≈ 1.[tex]\overline {1}[/tex] seconds
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The magnetic field between the poles of a magnet has magnitude 0.510 T. A circular loop of wire with radius 3.20 cm is placed between the poles so the field makes an angle of 22.0° with the plane of the loop. What is the magnetic flux through the loop?
Answer:
1.52×10⁻³ Wb
Explanation:
Using
Φ = BAcosθ.......................... Equation
Where, Φ = magnetic Field, B = 0.510 T, A = cross sectional area of the loop, θ = angle between field and the plane of the loop
Given: B = 0.510 T, θ = 22°,
A = πr², Where r = radius of the circular loop = 3.20 cm = 0.032 m
A = 3.14(0.032²)
A = 3.215×10⁻³ m²
Substitute into equation 1
Ф = 0.510(3.215×10⁻³)cos22°
Ф = 0.510(3.215×10⁻³)(0.927)
Ф = 1.52×10⁻³ Wb
Hence the magnetic flux through the loop = 1.52×10⁻³ Wb
Final answer:
To calculate the magnetic flux through a loop, use the formula Φ = B * A * cos(θ) with the given magnetic field strength, loop's area, and angle. For a 0.510 T field and a 3.20 cm radius loop at 22°, the magnetic flux is 1.5 * 10⁻³ Wb.
Explanation:
The student asked about calculating the magnetic flux through a circular loop of wire placed in a magnetic field. To find the magnetic flux (Φ), we use the formula Φ = B * A * cos(θ), where B is the magnetic field strength, A is the area of the loop, and θ is the angle between the magnetic field and the normal to the loop's plane. Given the field's magnitude is 0.510 T, the radius of the loop is 3.20 cm (which gives an area A = π * r²), and the angle is 22.0°, the magnetic flux can be calculated.
The area A of the loop is A = π * (0.032 m)² = 3.2*10⁻³ m². Then, we apply the cosine of the angle, cos(22°) = 0.927. So the flux Φ = (0.510 T) * (3.2*10⁻³ m²) * 0.927 = 1.5 * 10⁻³ Wb (weber).
A 6.0-cm-diameter, 11-cm-long cylinder contains 100 mg of oxygen (O2) at a pressure less than 1 atm. The cap on one end of the cylinder is held in place only by the pressure of the air. One day when the atmospheric pressure is 100 kPa, it takes a 173 N force to pull the cap off.
Explanation:
The given data is as follows.
Mass of oxygen present = 100 mg = [tex]100 \times 10^{-3}[/tex] g
So, moles of oxygen present are calculated as follows.
n = [tex]\frac{100 \times 10^{-3}}{32}[/tex]
= [tex]3.125 \times 10^{-3}[/tex] moles
Diameter of cylinder = 6 cm = [tex]6 \times 10^{-2}[/tex] m
= 0.06 m
Now, we will calculate the cross sectional area (A) as follows.
A = [tex]\pi \times \frac{(0.06)^{2}}{4}[/tex]
= [tex]2.82 \times 10^{-3} m^{2}[/tex]
Length of tube = 11 cm = 0.11 m
Hence, volume (V) = [tex]2.82 \times 10^{-3} \times 0.11[/tex]
= [tex]3.11 \times 10^{-4} m^{3}[/tex]
Now, we assume that the inside pressure is P .
And, [tex]P_{atm}[/tex] = 100 kPa = 100000 Pa,
Pressure difference = 100000 - P
Hence, force required to open is as follows.
Force = Pressure difference × A
= [tex](100000 - P) \times 2.82 \times 10^{-3}[/tex]
We are given that force is 173 N.
Thus,
[tex](100000 - P) \times 2.82 \times 10^{-3}[/tex] = 173
Solving we get,
P = [tex]3.8650 \times 10^{4} Pa[/tex]
= 38.65 kPa
According to the ideal gas equation, PV = nRT
So, we will put the values into the above formula as follows.
PV = nRT
[tex]38.65 \times 3.11 \times 10^{-4} = 3.125 \times 10^{-3} \times 8.314 \times T[/tex]
T = 462.66 K
Thus, we can conclude that temperature of the gas is 462.66 K.
A Carnot engine receives 250 kJ·s−1 of heat from a heat-source reservoir at 525°C and rejects heat to a heat-sink reservoir at 50°C. What are the power developed and the heat rejected?
a. The quantity of heat rejected by the Carnot engine is equal to -101.2 kJ/s.
b. The power developed by the Carnot engine is equal to 148.8 kJ/s.
Given the following data:
Quantity of heat received = 250 kJ/sTemperature of heat-source = 525°CTemperature of heat rejected = 50°CConversion:
Temperature of heat-source = 525°C to Kelvin = 525 + 273 = 798K
Temperature of heat rejected = 50°C to Kelvin = 50 + 273 = 323K
To find the power developed and the heat rejected, we would use Carnot's equation:
[tex]-\frac{Q_R}{T_R} = \frac{Q_S}{T_S}[/tex]
Where:
[tex]Q_R[/tex] is the quantity of heat rejected.[tex]T_R[/tex] is the heat-sink temperature.[tex]T_S[/tex] is the heat-source temperature.[tex]Q_S[/tex] is the quantity of heat received.Making [tex]Q_R[/tex] the subject of formula, we have:
[tex]Q_R = -( \frac{Q_S}{T_S})T_R[/tex]
Substituting the given parameters into the formula, we have;
[tex]Q_R = -( \frac{250}{798}) \times 323\\\\Q_R = -( \frac{80750}{798})[/tex]
Quantity of heat rejected = -101.2 kJ/s
Now, we can determine the power developed by the Carnot engine:
[tex]P = -Q_S - Q_R\\\\P = -250 - (-101.2)\\\\P = -250 + 101.2[/tex]
Power, P = 148.8 kJ/s.
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The power developed by the Carnot engine is approximately 148.8 kilowatts. The heat rejected by the Carnot engine is approximately 101.2 kilowatts.
The Carnot efficiency (η) of a heat engine is given by the formula:
η = 1 - (T₁ ÷ T₂)
Heat received (Q(in)) = 250,000 J/s
Temperature of the heat-source reservoir (T(Hot)) = 798.15 K
Temperature of the heat-sink reservoir (T(Cold) = 323.15 K
The Carnot efficiency:
η = 1 - (T₁ ÷ T₂)
η = 1 - (323.15 ÷ 798.15 )
η = 0.5952
Therefore, The Carnot efficiency is 0.5952, which means the engine converts 59.52% of the heat received into useful work.
Power Developed:
P = η × Q(in)
P = 0.5952 × 250,000
P = 148,800 = 148.8 kW
Therefore, The power developed by the Carnot engine is approximately 148.8 kilowatts.
Heat Rejected:
Q(out) = Q(in) - P
Q(out) = 250,000- 148,800 = 101,200 J/s
Q(out) = 101.2 kW
Therefore, The heat rejected by the Carnot engine is approximately 101.2 kilowatts.
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A piston–cylinder device initially contains 1.4 kg of refrigerant-134a at 100 kPa and 20°C. Heat is now transferred to the refrigerant from a source at 150°C, and the piston, which is resting on a set of stops, starts moving when the pressure inside reaches 120 kPa. Heat transfer continues until the temperature reaches 80°C. Assuming the surroundings to be at 25°C and 100 kPa, determine (a) the work done, (b) the heat transfer, (c) the exergy destroyed, and (d) the second-law efficiency of this process.
Answer:
a) 0.504 kJ
b) 67.7 kJ
c) 14.9 kJ
d) 25.5%
Explanation:
note:
solution is attached in word form due to error in mathematical equation. futhermore i also attach Screenshot of solution in word because to different version of MS Office please find the attachment
A 7.35 H inductor with negligible resistance is placed in series with a 14.1 V battery, a 3.00 ? resistor, and a switch. The switch is closed at time t = 0 seconds.
(a) Calculate the initial current at t = 0 seconds.
(b) Calculate the current as time approaches infinity.
(c) Calculate the current at a time of 6.25 s.
(d) Determine how long it takes for the current to reach half of its maximum.
Answer:
(a). The initial current at t=0 is zero.
(b). The current as time approaches infinity is 4.7 A
(c). The current at a time of 6.25 s is 4.33 A.
(d). The time is 1.69 sec.
Explanation:
Given that,
Inductance = 7.35 H
Voltage = 14.1 V
Resistance= 3.00 ohm
(a). We need to calculate the initial current at t = 0
Using formula of current
[tex]I=(\dfrac{E}{R})(1-e^{\dfrac{-tR}{L}})[/tex]
Put the value into the formula
[tex]I=(\dfrac{E}{R})(1-e^{\dfrac{-0\timesR}{L}})[/tex]
[tex]I=(\dfrac{E}{R})(1-1)[/tex]
[tex]I=0[/tex]
(b). We need to calculate the current as time approaches infinity.
Using formula of current
[tex]I=(\dfrac{E}{R})(1-e^{\dfrac{-tR}{L}})[/tex]
Put the value into the formula
[tex]I=(\dfrac{14.1}{3.00})(1-e^{\dfrac{-\infty\times3.00}{7.35}})[/tex]
[tex]I=\dfrac{14.1}{3.00}(1-0)[/tex]
[tex]I=4.7\ A[/tex]
(c). We need to calculate the current at a time of 6.25 s
Using formula of current
[tex]I=(\dfrac{E}{R})(1-e^{\dfrac{-tR}{L}})[/tex]
Put the value into the formula
[tex]I=(\dfrac{14.1}{3.00})(1-e^{\dfrac{-6.25\times3.00}{7.35}})[/tex]
[tex]I=4.33\ A[/tex]
(d). We need to calculate the time
Using formula of current
[tex]I=(\dfrac{E}{R})(1-e^{\dfrac{-tR}{L}})[/tex]
Put the value into the formula
[tex]2.35=(\dfrac{14.1}{3.00})(1-e^{\dfrac{-t\times3.00}{7.35}})[/tex]
[tex]ln(0.5)=(\dfrac{-t\times3.00}{7.35}})[/tex]
[tex]t=\dfrac{(\ln(2)\times7.35)}{3.00}[/tex]
[tex]t=1.69\ s[/tex]
Hence, (a). The initial current at t=0 is zero.
(b). The current as time approaches infinity is 4.7 A
(c). The current at a time of 6.25 s is 4.33 A.
(d). The time is 1.69 sec.
A conducting sphere of radius R1 carries a charge Q. Another conducting sphere has a radius R2 = 3 4 R1, but carries the same charge. The spheres are far apart. What is the ratio E2 E1 of the electric field near the surface of the sphere with radius R2 to the field near the surface of the sphere with radius R1?
Answer:
The ratio of electric field is 16:9.
Explanation:
Given that,
Radius [tex]R_{2}=\dfrac{3}{4}R_{1}[/tex]
Charge = Q
We know that,
The electric field is directly proportional to the charge and inversely proportional to the square of the distance.
In mathematically term,
[tex]E=\dfrac{kQ}{R^2}[/tex]
Here, [tex]E\propto\dfrac{1}{R^2}[/tex]
We need to calculate the ratio of electric field
Using formula of electric field
[tex]\dfrac{E_{2}}{E_{1}}=\dfrac{R_{1}^2}{R_{2}^2}[/tex]
Put the value into the formula
[tex]\dfrac{E_{2}}{E_{1}}=\dfrac{(4R_{1})^2}{(3R_{1})^2}[/tex]
[tex]\dfrac{E_{2}}{E_{1}}=\dfrac{16}{9}[/tex]
Hence, The ratio of electric field is 16:9.
Final answer:
The ratio of the electric fields E2/E1 at the surface of two conducting spheres with radii R2 = 3/4R1 carrying the same charge is 16/9.
Explanation:
The question is asking for the ratio of the electric fields near the surface of two conducting spheres carrying the same charge Q but having different radii, R1 and R2 where R2 is three-fourths of R1. To find the electric field E near the surface of a conducting sphere, we use the formula:
E = kQ/[tex]r^{2}[/tex]
where k is Coulomb's constant, Q is the charge, and R is the radius of the sphere. Since the charge Q is the same on both spheres, we can calculate the ratio of the electric fields by plugging in the radii:
E2/E1 = (kQ/[tex]r2^{2}[/tex]) / (kQ/[tex]r1^{2}[/tex])
Simplifying further, since k is a constant it cancels out, along with Q, which is the same for both spheres, we get:
E2/E1 = ([tex]r1^{2}[/tex]) / ([tex]r2^{2}[/tex])
Substituting R2 = 3/4R1:
E2/E1 = [tex]r1^{2}[/tex] / (3/4 R1)[tex]{2}[/tex]
E2/E1 = 1 / (3/4)^2
E2/E1 = 1 / (9/16) = 16/9
Therefore, the ratio E2/E1 is 16/9.
A system of 1223 particles, each of which is either an electron or a proton, has a net charge of -5.328×10-17 C. How many protons are in this system (exactly)?
Answer:
Therefore the number of proton in the given system is 450.
Explanation:
Given that, a system has 1223 particles.
Let x number of proton be present in the system.
Then the number of electron is =(1223-x)
The charge of a proton is = 1.602×10⁻¹⁹ C
The charge of an electron = - 1.602×10⁻¹⁹ C
The charge of x protons is =( 1.6×10⁻¹⁹×x) C
The charge of (1223-x) electrons is = - 1.6×10⁻¹⁹ (1223-x) C
According to the problem,
(1.6×10⁻¹⁹×x) +{ - 1.6×10⁻¹⁹ (1223-x)}= -5.328×10⁻¹⁷
⇒1.6×10⁻¹⁹(x-1223+x)=-5.328×10⁻¹⁷
[tex]\Rightarrow (2x-1223)=\frac{-5.328\times 10^{-17}}{1.6\times 10^{-19}}[/tex]
⇒2x-1223= -333
⇒2x= -333+1223
⇒2x=900
[tex]\Rightarrow x=\frac{900}{2}[/tex]
⇒x=450
Therefore the number of proton is 450.
A commercial office building is to be supplied service at 208Y/120 V from the utility company 12.47 kV distribution feeder (12.47 kV line-to-line and 7.2 kV lineto-neutral). The estimated demand load is 85 kW at 0.9 lagging power factor. Determine the appropriate apparent power rating and voltage rating of the threephase, pad mounted transformer required to serve this load. The transformer is connected delta-grounded wye. Assume the load is continuous and allow a 25% factor for load growth.
Answer:
Apparent power rating is: 120 kVA
Apparent voltage rating is: 0.208 kV
Explanation:
Given demand load of commercial office building P = 85 kW @ pf = 0.9 lagging
Allow load growth of 25% = 0.25 * 85 = 21.25 kW
Maximum load is Pm = 85 + 21.25 = 106.25 @ pf = 0.9 lagging
Apparent power demand S = Pm/pf = 106.25/0.9 = 118.05 kVA
This apparent power should be meet by 3-phase pad mount transformer at secondary voltage of 208 V (L-L) and secondary should grounded star .
Apparent Power rating of 3-phase pad mounted transformer is ST = 120 kVA
Volatage rating of 3-phase pad mounted transformer is Delta - grounded star V1 : V2 = 12.47 : 0.208 kV
A standard door into a house rotates about a vertical axis through one side, as defined by the door's hinges. A uniform magnetic field is parallel to the ground and perpendicular to this axis. Through what angle must the door rotate so that the magnetic flux that passes through it decreases from its maximum value to 0.30 of its maximum value?
Answer:
The angle that the door must rotate is 70.5 graus
Explanation:
When the door rotates through and angel X, the magnetic flux that passes through the door decreases from its maximum value to 0.3 of its maximum value
This way,
X = 0.3 Xmax
X = B A cosX = 0.3 B A
or
cosX = 0.3
or
X = [tex]cos^{-1}[/tex] (0.3) = 70.5
X = 70.5 graus
A positive point charge q1 = +5.00 × 10−4C is held at a fixed position. A small object with mass 4.00×10−3kg and charge q2 = −3.00×10−4C is projected directly at q1. Ignore gravity. When q2 is 4.00m away, its speed is 800m/s. What is its speed when it is 0.200m from q1?
Answer:
Therefore the speed of q₂ is 1961.19 m/s when it is 0.200 m from from q₁.
Explanation:
Energy conservation law: In isolated system the amount of total energy remains constant.
The types of energy are
Kinetic energy.Potential energy.Kinetic energy [tex]=\frac{1}{2} mv^2[/tex]
Potential energy =[tex]\frac{Kq_1q_2}{d}[/tex]
Here, q₁= +5.00×10⁻⁴C
q₂=-3.00×10⁻⁴C
d= distance = 4.00 m
V = velocity = 800 m/s
Total energy(E) =Kinetic energy+Potential energy
[tex]=\frac{1}{2} mv^2[/tex]+ [tex]\frac{Kq_1q_2}{d}[/tex]
[tex]=\frac{1}{2} \times 4.00\times 10^{-3}\times(800)^2 +\frac{9\times10^9\times 5\times10^{-4}\times(-3\times10^{-4})}{4}[/tex]
=(1280-337.5)J
=942.5 J
Total energy of a system remains constant.
Therefore,
E [tex]=\frac{1}{2} mv^2[/tex] + [tex]\frac{Kq_1q_2}{d}[/tex]
[tex]\Rightarrow 942.5 = \frac{1}{2} \times 4 \times10^{-3} \times V^2 +\frac{9\times10^{9}\times5\times 10^{-4}\times(-3\times 10^{-4})}{0.2}[/tex]
[tex]\Rightarrow 942.5 = 2\times10^{-3}v^2 -6750[/tex]
[tex]\Rightarrow 2 \times10^{-3}\times v^2= 942.5+6750[/tex]
[tex]\Rightarrow v^2 = \frac{7692.5}{2\times 10^{-3}}[/tex]
[tex]\Rightarrow v= 1961.19[/tex] m/s
Therefore the speed of q₂ is 1961.19 m/s when it is 0.200 m from from q₁.
Suppose hydrogen and oxygen are diffusing through air. A small amount of each is released simultaneously. How much time passes before the hydrogen is 1.00 s ahead of the oxygen
Answer:
Hydrogen takes 0.391s to get to distance x
Explanation:
From the chromatography table:
[tex]D_H_2=6.4\times10^{-5}m^2/s\\D_O_2=1.8\times10^{-5}m^2/s\\[/tex]
Using the equation[tex]x_m_s=\sqrt(2Dt)[/tex]. This equation relates time to distance during diffusion
[tex]x_m_s[/tex],[tex]_O_2[/tex]=[tex]\sqrt[/tex][tex]2D_o_2[/tex][tex]t_o_2[/tex] and [tex]x_m_s[/tex],[tex]__H_2[/tex]=[tex]\sqrt[/tex][tex]2D_H__2[/tex][tex]t_H__2[/tex]
Let the distance traveled be denoted by x(same distance traveled by both gases).
Distance is same when difference between[tex]t_H__2[/tex] and [tex]t_O__2[/tex] is 1.0 seconds.
[tex]t_O__2=t_H___2[/tex][tex]+1.0s[/tex]
At equal distance=>
[tex]2D_O__2[/tex][tex]t_O__2[/tex]=[tex]2D_H__2[/tex][tex]t_H__2[/tex]
[tex]D_O_2[/tex][tex](t_H__2[/tex][tex]+1.0s)=D_H__2[/tex][tex]t_H__2[/tex]
Solving for hydrogen time:
[tex]t_H__2=(D_0__2)\div[/tex][tex](D_H__2[/tex]-[tex]D_O__2)[/tex][tex]\times1.0[/tex]
=[tex](1.8\times10^{-5}m^2/s)\div(6.4\times10^{-5}m^2/s-1.8\times10^{-5}m^2/s)\times1.0s[/tex]
=0.391s
Final answer:
To find the time before hydrogen is 1.00 s ahead of oxygen when both are diffusing through air, we use Graham's law of effusion. Hydrogen effuses four times faster than oxygen, so with calculations, we find that this time is approximately 2.33 seconds.
Explanation:
When hydrogen and oxygen are diffusing through air and are released simultaneously, we want to determine the time that passes before the hydrogen gas (H2) is 1.00 s ahead of the oxygen gas (O2). This concept involves diffusion rates in gases, which can be described using Graham's law of effusion. According to Graham's law, the rate of effusion for a gas is inversely proportional to the square root of its molar mass (M).
Given that hydrogen effuses four times as rapidly as oxygen, we can write the relationship between their rates as RH2 / RO2 = sqrt(MO2 / MH2). Knowing that the molar mass of hydrogen (MH2) is 2 g/mol and the molar mass of oxygen (MO2) is 32 g/mol, we can substitute these values into the equation to find the rate ratio.
Since hydrogen is four times faster, and we want hydrogen to be 1.00 s ahead of the oxygen, we can use the ratio to calculate how long it would take for oxygen to travel the same distance. This time can then be added to 1.00 s to find the total elapsed time. Here's a step-by-step approach to calculate this:
Calculate the square root of the ratio of the molar masses: sqrt(32/2) = sqrt(16) = 4.
The rate of hydrogen is therefore four times the rate of oxygen: RH2 = 4 × RO2.
If we let t be the time for oxygen to effuse, hydrogen will effuse in t/4 time.
To be 1.00 s ahead, we want t/4 = t - 1.00.
Solving for t gives us t = 4/3 seconds (approximately 1.33 s).
This is the time it would take for oxygen to cover the same distance that hydrogen covers in 1/3 second.
Thus, the total time before hydrogen is 1.00 s ahead of the oxygen is approximately 1.33 s (the time for oxygen) + 1.00 s = 2.33 seconds.
This concept is particularly useful in analytical chemistry, specifically in techniques like gas chromatography, where differences in the rate of diffusion of gases are used to separate and identify components in a mixture.
What is the energy in the spark produced by discharging the second capacitor? 1. The same as the discharge spark of the first capacitor 2. More energetic than the discharge spark of the first capacitor 3. Less energetic than the discharge spark of the first capacitor
Complete Question
The two isolated parallel plate capacitors be- low, one with plate separation d and the other with D > d, have the same plate area A and
are given the same charge Q.
What is the energy in the spark produced by discharging the second capacitor?
1. The same as the discharge spark of the first capacitor
2. More energetic than the discharge spark of the first capacitor
3. Less energetic than the discharge spark of the first capacitor
Answer:
The correct option is 2
Explanation:
The formula for the energy stored in the capacitor is
[tex]U = \frac{Q^2}{2C}[/tex]
And generally the formula for finding the capacitance of a capacitor is
[tex]C = \frac{\epsilon_oA}{d}[/tex]
We can denote the capacitance of the first capacitor as [tex]C_1 = \frac{\epsilon_oA}{d}[/tex]
and denote the capacitance of the second capacitor as [tex]C_2 = \frac{\epsilon_oA}{D}[/tex]
Looking at this formula we can see that C varies inversely with d
as D > d it means that [tex]C_1 > C_2[/tex]
Since the charge is constant
[tex]U\ \alpha\ \frac{1}{C}[/tex] i.e U varies inversely with C
So [tex]C_1 > C_2[/tex] => [tex]U_2 >U_1[/tex]
This means that the energy of spark would be more for capacitor two compared to capacitor one
The correct option is 2
The energy in the spark produced by discharging a capacitor can vary between different capacitors based on their capacitance and potential difference.
When discharging a capacitor, the energy stored in the capacitor is released as a spark, which can be compared between different capacitors.
In this case, if the second capacitor discharges, the spark produced may have varying energy levels compared to the spark produced by the first capacitor, depending on the capacitance and potential difference.
The energy in the spark produced by discharging the second capacitor can be calculated using relevant formulas relating to capacitance, potential difference, and energy stored.
A 1000 kg automobile is traveling at an initial speed of 20 m/s. It is brought to a complete stop in 5 s over a distance of 50 m. What is the work done in stopping the automobile
Answer:
W = -2*10⁵ J
Explanation:
Assuming no friction present, we can find the work done by an external force stopping the car, applying the work-energy theorem.This theorem says that the total work done on one object by an external net force, is equal to the change in the kinetic energy of the object.If the automobile is brought to a complete stop, we can find the change of the kinetic energy as follows:[tex]\Delta K = K_{f} - K_{0} = 0 - \frac{1}{2} * m* v_{0} ^{2} \\\\ \Delta K = -\frac{1}{2}*1000kg*(20 m/s)^{2} = -200000 J= -2e5 J[/tex]
So, the total work done in stopping the automobile, is -2*10⁵ J. The minus sign stems from the fact that the force and the displacement have opposite directions.Given values:
Mass, m = 1000 kgInitial speed, v = 20 m/sDistance, d = 50 mTime, t = 5 sAs we know,
→ [tex]\Delta K = K_f - K_0[/tex]
[tex]= 0-\frac{1}{2}mv_2^2[/tex]
By substituting the values,
[tex]= - \frac{1}{2}\times 1000\times (20)^2[/tex]
[tex]= - 500\times 400[/tex]
[tex]= -200000 \ J[/tex]
[tex]= -2\times 10^5 \ J[/tex]
Thus the above answer is right.
Learn more about speed here:
https://brainly.com/question/16794794
A particle is uncharged and is thrown vertically upward from ground level with a speed of 26.4 m/s. As a result, it attains a maximum height h. The particle is then given a positive charge +q and reaches the same maximum height h when thrown vertically upward with a speed of 28.8 m/s. The electric potential at the height h exceeds the electric potential at ground level. Finally, the particle is given a negative charge -q. Ignoring air resistance, determine the speed with which the negatively charged particle must be thrown vertically upward, so that it attains exactly the maximum height h. In all three situations, be sure to include the effect of gravity.
Answer:
[tex]23.76 \ m/s[/tex]
Explanation:
Energy Conversions
This is an example where the mechanical energy is not conserved since an external force is acting and distorting the original balance between kinetic and potential gravitational energy.
Let's start with the first event, the particle being thrown upwards with an initial speed vo. The initial mechanical energy at zero height is only kinetic:
[tex]\displaystyle M=\frac{mv_o^2}{2}[/tex]
When the particle reaches its maximum height, the mechanical energy is only potential gravitational:
M'=mgh
Equating both:
[tex]\displaystyle \frac{mv_o^2}{2}=mgh[/tex]
Simplifying by m and solving for h
[tex]\displaystyle h=\frac{v_o^2}{2g}=\frac{26.4^2}{2\cdot 9.8}=35.56\ m[/tex]
The particle is then given a positive charge and we know it reaches the same maximum height when the initial speed is 28.8 m/s. The initial kinetic energy was not totally converted to potential gravitational energy. The charge that was given to the particle and the electric potential present changed the energy balance by introducing a new member into the equation. The final energy at maximum height is
[tex]M'=mgh+U[/tex]
Where U is the electric energy the particle has when reached the maximum height. Equating the initial and final energies we have
[tex]\displaystyle \frac{mv_o'^2}{2}=mgh+U[/tex]
Simplifying by m and solving for U
[tex]\displaystyle U/m=\frac{v_o'^2}{2}-gh=\frac{28.8^2}{2}-9.8\cdot 35.56[/tex]
[tex]U/m=66.232\ J/Kg[/tex]
This energy makes the particle have an additional force downwards that brakes it until it stops. When the charge is negative, the new electrical force will be directed upwards in such a way that the particle will reach the same maximum height with less initial speed v''o. The new equilibrium equation will be
[tex]\displaystyle \frac{mv_o''^2}{2}=mgh-U[/tex]
Simplifying by m and solving for v''o
[tex]\displaystyle \frac{v_o''^2}{2}=gh-U/m[/tex]
[tex]\displaystyle v_o''=\sqrt{2(gh-U/m)}=\sqrt{2(9.8\cdot 35.56 -66.232)}=23.76\ m/s[/tex]
[tex]\boxed{v_o''=23.76 \ m/s}[/tex]
Final answer:
To find the speed of a negatively charged particle reaching height h, consider gravitational potential energy, kinetic energy, and work done against or by the electric field. A negative charge requires less initial kinetic energy due to electric field assistance, but exact speed calculation necessitates specific values for mass, charge, and field strength.
Explanation:
To determine the speed with which the negatively charged particle must be thrown upward to reach the same maximum height, h, we need to take into account the change in potential energy due to gravity, the kinetic energy due to the particle's movement, and the work done against the electric field.
For all scenarios, potential energy due to height (mg), kinetic energy (½mv²), and work against the electric field (qEh) are relevant.
Considering a positive electric potential at height h means for a positively charged particle, work done against the electric field is positive, requiring more kinetic energy (hence, higher speed) to reach the same height.
For a negatively charged particle in an upward positive field, the work done by the field assists the particle in reaching the height, so less initial kinetic energy (lower speed) is required.
To find the exact speed for the negatively charged particle, we equate the total energy at ground level to the total energy at height h, considering the negative charge's interaction with the electric field.
Without specific values for mass, charge, and electric field strength, a precise number cannot be given, though the process involves calculating and equating these energy values before and after.
You have built a device that measures the temperature outside and displays it on a dial as a measure of how far away from room temperature outside is. The way the dial works is that a needle with a charged ball on the end is placed between two charged parallel plates. The strength of the uniform electric field between the plates is proportional to the outside temperature. Given that the charged ball on the needle has a charge of?
Answer:
m=33.734 grams
E=41435.95 N/C
Explanation:
The detailed explanation of Answer is given in the attached file.
Use the worked example above to help you solve this problem. A wire carries a current of 21.8 A from west to east. Assume that at this location the magnetic field of Earth is horizontal and directed from south to north and that it has a magnitude of 5.00 10-5 T. (a) Find the magnitude and direction of the magnetic force on a 38.1 m length of wire. N
Answer:
Themagnitude of the force is 0.0415N and is directed vertically upwards. The solution to this problem uses the relationship between the Force experienced by a conductor in a magnetic field, the current flowing through the conductor, the length of the conductor and the magnitude of the electric field vector.
Mathematically this can be expressed as
F = I × L ×B
Where F = Force in newtons N
I = current in ampres A
L = length of the conductor in meters (m)
B = magnetic field vector in T
Explanation:
The calculation can be found in the attachment below.
Thedirection of the force can be found by the application of the Fleming's right hand rule. Which states that hold out the right hand with the index finger pointing in the direction of the magnetic field and the thumb pointing in the direction of the current in the conductor, then the direction which the middle finger points is the direction of the force exerted on the conductor. By applying this the direction is vertically upwards.
The magnitude of the magnetic force on a 38.1 m length of wire carrying a current of 21.8 A in a magnetic field with a strength of 5.00 x 10^-5 T is 4.153 x 10^-2 N, and the direction of the force is upward.
Explanation:To calculate the magnitude and direction of the magnetic force on a current-carrying wire in a magnetic field, you can use the formula F = ILB sin(θ), where F is the magnetic force, I is the current in the wire, L is the length of the wire within the magnetic field, B is the magnetic field strength, and θ is the angle between the direction of the current and the direction of the magnetic field.
In the given problem, we have I = 21.8 A (current), L = 38.1 m (length of wire), and B = 5.00 x 10-5 T (magnetic field strength). Since the wire carries current from west to east and the Earth's magnetic field is directed from south to north, the angle between the direction of the current and the Earth's magnetic field is 90° (sin(90°) = 1). Thus, using the formula:
F = (21.8 A) x (38.1 m) x (5.00 x 10-5 T) = 4.153 x 10-2 N
The direction of the force can be determined using the right-hand rule, which gives us the direction of the magnetic force as upward, perpendicular to the plane formed by the current and the magnetic field directions.
A galvanometer coil having a resistance of 20 Ω and a full-scale deflection at 1.0 mA is connected in series with a 4980 Ω resistance to build a voltmeter. What is the maximum voltage that this voltmeter can read?
Answer:
5 V
Explanation:
The maximum voltage the voltmeter can read will be the voltage drop across the 20 Ω resistance and the voltage drop across the 4980 Ω resistance.
V' = Ir +IR.................... equation 1
Where V' = Maximum voltage the voltmeter can read, I = current, r = resistance of the galvanometer coil, R = The resistance connected in series to the galvanometer.
Given: I = 1 mA = 0.001 A, r = 20Ω, R = 4980Ω
Substitute into equation 1
V' = 20(0.001)+4980(0.001)
V' = 0.02+4.98
V' = 5 V
Answer:
Explanation:
E = IR + Ir
Where,
I = current
= 1 mA
= 0.001 A
R = 4980 Ω
Internal resistance, r = 20 Ω
Maximum voltage, E = 0.001 × 4980 + 0.001 × 20
= 4.98 + 0.02
= 5 V
A 2.40 kg snowball is fired from a cliff 7.69 m high. The snowball's initial velocity is 13.0 m/s, directed 49.0° above the horizontal. (a) How much work is done on the snowball by the gravitational force during its flight to the flat ground below the cliff? (b) What is the change in the gravitational potential energy of the snowball-Earth system during the flight? (c) If that gravitational potential energy is taken to be zero at the height of the cliff, what is its value when the snowball reaches the ground?
Answer:
a) W = 180.87 J , b) ΔU = -180.87 J , c) ΔU = -180.87 J
Explanation:
a) Work is defined as
W = F .ds
Where bold indicates vectors, we can write the scalar product
W = F s cos θ
Where the angle is between force and displacement.
The force of gravity is the weight of the body, which is directed downwards and the displacement thickens the tip of the cliff at the bottom, so that it is directed downwards, therefore the angle is zero degrees
W = [tex]F_{g}[/tex] y
W = m g y
For this problem we must fix a reference system, from the statement it is established that the system is placed at the base of the cliff, so that final height is zero and the initial height (y₀ = 7.69m)
W = 2.40 9.8 (7.69-0)
W = 180.87 J
b) The potential energy is
U = mg y
The change in potential energy,
ΔU = [tex]U_{f}[/tex]- U₀
ΔU = mg ([tex]y_{f}[/tex]- y₀)
ΔU = 2.4 9.8 (0 -7.69)
ΔU = -180.87 J
c) in this case we change the reference system to the height of the cliffs, for this configuration
y₀ = 0
[tex]y_{f}[/tex] = -7.69 m
ΔU = 2.4 9.8 (-7.69 -0)
ΔU = -180.87 J