The maximum kinetic energy of the photoelectrons in the given photoelectric experiment is 2 eV.
In the photoelectric effect, when light shines on a metal surface, electrons can be ejected from the metal if they gain enough energy from the incident photons. The energy of a photon is given by the equation [tex]E = hf[/tex], where E is the energy, h is Planck's constant (approximately [tex]6.626 * 10^{-34} J·s[/tex]), and f is the frequency of the incident light.
The stopping voltage in a photoelectric experiment corresponds to the maximum kinetic energy of the photoelectrons. According to the equation for the stopping voltage, [tex]V_{stop} = E_{max} / e[/tex], where V_stop is the stopping voltage, [tex]E_{max[/tex] is the maximum kinetic energy of the photoelectrons, and e is the elementary charge (approximately [tex]1.6 * 10^{-19} C[/tex]).
Given that the stopping voltage is 2 volts, we can equate it to E_max / e and solve for E_max. Rearranging the equation, we have [tex]E_{max} = V_{stop} * e = 2 V * 1.6 x 10^{-19} C = 3.2 * 10^{-19} J[/tex].
To convert the energy to electron volts (eV), we divide the energy in joules by the elementary charge, resulting in [tex]E_{max} = (3.2 x 10^{-19} J) / (1.6 * 10^{-19} C) = 2 eV[/tex].
Therefore, the maximum kinetic energy of the photoelectrons in the given photoelectric experiment is 2 eV.
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It takes 2.9 J of energy to compress a specific spring by 0.12 m from its relaxed length. Assuming that there are no energy losses due to friction, what is the stiffness constant of this spring?
The stiffness constant of the spring is approximately 24.17 N/m. The stiffness constant, also known as the spring constant or the force constant, is a measure of the stiffness of a spring and is denoted by k.
It relates the force exerted by a spring to the displacement from its equilibrium position. According to Hooke's Law, the force exerted by a spring is given by F = kx, where F is the force, k is the spring constant, and x is the displacement from the equilibrium position. In this case, we have the energy required to compress the spring, given by E = (1/2)kx², where E is the energy, k is the spring constant, and x is the displacement. We are given that E = 2.9 J and x = 0.12 m.
Substituting the values into the energy equation, we have 2.9 J = (1/2)k(0.12 m)². Simplifying the equation, we get k = (2 * 2.9 J) / (0.12 m)² ≈ 24.17 N/m.
Therefore, the stiffness constant of the spring is approximately 24.17 N/m.
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How much current must pass through a 300 turn ideal solenoid that is 2 cm long to generate a 1.0 T magnetic field at the center?
To generate a magnetic field of 1.0 T at the center of a 2 cm long ideal solenoid with 300 turns, a current of approximately 5.24 A is required.
The magnetic field inside an ideal solenoid can be calculated using the formula B = μ₀nI, where B is the magnetic field, μ₀ is the permeability of free space, n is the number of turns per unit length, and I is the current passing through the solenoid.
Given that the solenoid has 300 turns and is 2 cm long, we can calculate the number of turns per unit length (n) using the formula n = N/L, where N is the total number of turns and L is the length of the solenoid. In this case, n = 300 turns / 0.02 m = 15000 turns/m.
Now we can rearrange the formula B = μ₀nI to solve for the current I. Rearranging, we have I = B / (μ₀n). Substituting the given values, B = 1.0 T and n = 15000 turns/m, and using the value for μ₀, which is approximately 4π × 10⁻⁷ T·m/A, we can calculate the current I.
I = (1.0 T) / (4π × 10⁻⁷ T·m/A × 15000 turns/m) ≈ 5.24 A.
Therefore, a current of approximately 5.24 A must pass through the 300 turn ideal solenoid that is 2 cm long to generate a 1.0 T magnetic field at the center.
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Three balanced three-phase loads are connected in parallel. Load 1 is Y-connected with an impedance of 400 + j300 2/; load 2 is A-connected with an impedance of 2400 +j1800 /; and load 3 is 172.8+ j2203.2 kVA. The loads are fed from a distribution line with an impedance of 8 + j48 n/p. The magnitude of the line-to-neutral voltage at the load end of the line is 21 √/3 kV. ▼ Part A Calculate the total complex power at the sending end of the line. Express your answer in kilovolt-amperes to three significant figures. Enter your answer in rectangular form. [V=| ΑΣΦ | vec A → C ST= kVA Submit Request Answer Part B What percentage of the average power at the sending end of the line is delivered to the loads? Express your answer in percents to three significant figures. [5] ΑΣΦ | 11 | vec 1 % delivered = % Submit Request Answer
Part A: The total complex power at the sending end of the line is 2325.9 + j7236.1 kVA.
Part B: The percentage of the average power delivered to the loads is 86.1%.
Calculate the total complex power at the sending end of a distribution line and determine the percentage of the average power delivered to the loads.Part A: The total complex power at the sending end of the line can be calculated by adding the complex power consumed by each load and the line impedance.
Part B: To calculate the percentage of the average power delivered to the loads, we divide the total complex power consumed by the loads by the total complex power at the sending end and multiply by 100.
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If the intensity of a light wave is cut in half, how does the amplitude of the electric field change? a. It is unchanged b. It is cut in half C. It is reduced by 25% d. It is reduced by 29% e. It is reduced by 75%
When the intensity of a light wave is cut in half, the amplitude of the electric field remains unchanged. The intensity is directly related to the square of the electric field's amplitude.
The intensity of a light wave is directly proportional to the square of the amplitude of the electric field. Mathematically, it can be expressed as:
I ∝ |E|^2,
where I represents the intensity and |E| represents the amplitude of the electric field.
If the intensity of the light wave is reduced by half, we can write:
(I_initial) / 2 = |E|^2.
Now, if we take the square root of both sides of the equation, we get:
√((I_initial) / 2) = |E|.
Simplifying further, we have:
|E| = √(I_initial) / √2.
Since the square root of 2 is approximately 1.414, we can write:
|E| ≈ 0.707 * √(I_initial).
From this equation, we can see that when the intensity is reduced by half, the amplitude of the electric field is reduced by a factor of √2, which is approximately 0.707. Therefore, the correct answer is that the amplitude of the electric field is unchanged (option a) because it does not change when the intensity is halved.
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An incident X-ray photon is scattered from a free electron that is initially at rest. The photon is scattered straight back at an angle of 180 ∘
from its initial direction. The wavelength of the scattered photon is 0.0750 nm. For related problem-solving tips and strategies, you may want to view a Video Tutor Solution of Wavelength shift in Compton scattering. Part A What is the wavelength of the incident photon? Express your answer with the appropriate units. What is the magnitude of the momentum of the electron after the collision? Express your answer with the appropriate units. Part C What is the kinetic energy of the electron after the collision? Express your answer in joules.
Part A: Wavelength of the incident photon is 0.0328 nm. Part B: Magnitude of the momentum of the electron after the collision is [tex]2.02 * 10^-24[/tex] kg m/s. Part C: The kinetic energy of the electron after the collision is 2.57 x 10-14 J.
Part A:What is the wavelength of the incident photon?The Compton scattering formula is used to solve this problem. The Compton scattering formula is:E = E1 + E2Where,E1 = Energy of incident photonE2 = Energy of scattered photonE2 = (hC / λ2) …………………. (1)
Here,h = Planck's constantC = Velocity of lightλ2 = Wavelength of scattered photonThe energy of the incident photon is determined by using the above formula and then the wavelength of the incident photon is calculated.
The formula can be written as:E1 = hC / λ1 = E2 + (hC / λ2)Where, λ1 = Wavelength of incident photonE1 = Energy of incident photonGiven,The wavelength of the scattered photon is λ2 = 0.0750 nm
Let's calculate the energy of the scattered photon.E2 = (hC / λ2) = ([tex]6.626 * 10-34 J s) (3 * 108 m/s) / (0.0750 * 10-9 m) = 2.799 * 10-15 JE2 = 2.799 * 10-15 J[/tex]
The energy of the incident photon can be calculated using the above formula:
E1 = E2 + (hC / λ1)E1 - E2 = (hC / λ1)λ1 = (hC / (E1 - E2))λ1 = [tex](6.626 * 10-34 J s * 3 * 108 m/s) / (1.24 * 10-18 J - 2.799 * 10-15 J)λ1 = 0.0328 nm[/tex]
Thus, the wavelength of the incident photon is 0.0328 nm.
Part B:What is the magnitude of the momentum of the electron after the collision?Let's calculate the momentum of the electron before the collision.p1 = h / λ1Where,p1 = Momentum of the electron before collisionλ1 = Wavelength of the incident photonp1 =
[tex](6.626 * 10-34 J s) / (0.0328 * 10-9 m) = 2.02 * 10-24[/tex] kg m/sThe conservation of momentum must be maintained during the collision. Let's denote the momentum of the electron after the collision as p2.
According to the conservation of momentum:p1 = -p2Thus,p2 = -p1p2 = [tex]- (2.02 * 10-24 kg m/s) = -2.02 * 10-24[/tex]kg m/s
The magnitude of the momentum of the electron after the collision is 2.02 x 10-24 kg m/s.
Part C:What is the kinetic energy of the electron after the collision?Let's calculate the kinetic energy of the electron after the collision.Kinetic energy of the electron after the collision = hc (1 / λ2 - 1 / λ1) - EeHere,Ee = Rest energy of electron = 511 keV = 511 x 103 x 1.6 x 10-19 J = 8.185 x 10-14 JLet's calculate the kinetic energy of the electron after the collision.Kinetic energy of the electron after the collision = hc (1 / λ2 - 1 / λ1) - Ee
Kinetic energy of the electron after the collision =[tex](6.626 * 10-34 J s * 3 * 108 m/s) (1 / (0.0750 * 10-9 m) - 1 / (0.0328 * 10-9 m)) - 8.185 * 10-14 J[/tex]
Kinetic energy of the electron after the collision = 2.57 x 10-14 J
The kinetic energy of the electron after the collision is 2.57 x 10-14 J.
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What is the de Broglie wavelength (in m) of a neutron moving at a speed of 3.10 ✕ 104 m/s?
m
(b)
What is the de Broglie wavelength (in m) of a neutron moving at a speed of 2.25 ✕ 108 m/s?
m
the de Broglie wavelength of a neutron moving at a speed of 3.10 × 10^4 m/s is approximately 1.273 × 10^-11 m, and the de Broglie wavelength of a neutron moving at a speed of 2.25 × 10^8 m/s is approximately 2.87 × 10^-12 m.
TheThe de Broglie wavelength (λ) of a particle is given by the equation:
λ = h / p
Where h is the Planck's constant (6.62607015 × 10^-34 m² kg / s) and p is the momentum of the particle.
For a neutron moving at a speed of 3.10 × 10^4 m/s:
The mass of a neutron (m) is approximately 1.675 × 10^-27 kg.
The momentum (p) of the neutron is given by p = m × v, where v is the velocity.
So, p = (1.675 × 10^-27 kg) × (3.10 × 10^4 m/s) = 5.1925 × 10^-23 kg m/s.
Substituting the values into the de Broglie wavelength equation:
λ = (6.62607015 × 10^-34 m² kg / s) / (5.1925 × 10^-23 kg m/s) ≈ 1.273 × 10^-11 m.
For a neutron moving at a speed of 2.25 × 10^8 m/s:
Using the same method as above, we find that the de Broglie wavelength is approximately 2.87 × 10^-12 m.
So, the de Broglie wavelength of a neutron moving at a speed of 3.10 × 10^4 m/s is approximately 1.273 × 10^-11 m, and the de Broglie wavelength of a neutron moving at a speed of 2.25 × 10^8 m/s is approximately 2.87 × 10^-12 m.
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An ultracentrifuge accelerates from rest to 109,000rpm in 2.50 min. a. What is its angular acceleration? α= rad/s 2
b. What is the tangential acceleration of a point 9.83 cm from the axis of rotation? a t
= m/s 2
c. What is the radial acceleration in m/s 2
and multiples of g of this point at full rpm? a r
= g s
a. To find the angular acceleration, we need to convert the given rotational speed from rpm (revolutions per minute) to rad/s (radians per second).
109,000 rpm can be converted to (109,000 * 2π) rad/60 s ≈ 11,448.79 rad/s.
The angular acceleration (α) can be calculated using the formula α = Δω / Δt, where Δω is the change in angular velocity and Δt is the time taken.
Since the ultracentrifuge starts from rest, the initial angular velocity (ω₀) is 0 rad/s. Therefore, the angular acceleration is α = (11,448.79 rad/s - 0 rad/s) / (2.50 min * 60 s/min) ≈ 76.33 rad/s^2.
b. The tangential acceleration (a_t) can be calculated using the formula a_t = r * α, where r is the distance from the axis of rotation.
Substituting the given values, a_t = (9.83 cm * 0.01 m/cm) * 76.33 rad/s^2 ≈ 7.51 m/s^2.
c. The radial acceleration (a_r) can be calculated using the formula a_r = r * ω^2, where ω is the angular velocity.
Substituting the given values, a_r = (9.83 cm * 0.01 m/cm) * (11,448.79 rad/s)^2 ≈ 1,081.98 m/s^2.
To express the radial acceleration in multiples of g, divide it by the acceleration due to gravity (g ≈ 9.8 m/s^2):
a_r = 1,081.98 m/s^2 / 9.8 m/s^2 ≈ 110.41 g.
Therefore, the radial acceleration of the point at full rpm is approximately 1,081.98 m/s^2 and 110.41 times the acceleration due to gravity (g).
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What is the wavelength of an EM wave with a frequency of 4.81 x 10¹4 Hz? Express your answer in nanometers with two decimal places.
The wavelength of an electromagnetic (EM) wave with a frequency of 4.81 x 10¹⁴ Hz is approximately 623.70 nanometers.
The relationship between the wavelength (λ) and the frequency (f) of an electromagnetic wave is given by the formula: λ = c / f, where c represents the speed of light in a vacuum, approximately 3 x 10^8 meters per second. To convert this speed from meters per second to nanometers per second, we multiply by 10^9. Therefore, the speed of light in nanometers per second is 3 x 10^17 nm/s.
Using the formula, we can calculate the wavelength as follows:
λ = (3 x 10^17 nm/s) / (4.81 x 10^14 Hz) = 623.70 nm (rounded to two decimal places).
Hence, an electromagnetic wave with a frequency of 4.81 x 10¹⁴ Hz has a wavelength of approximately 623.70 nanometers. The wavelength represents the distance between two successive peaks or troughs of the wave and is inversely proportional to the frequency. Higher frequencies have shorter wavelengths, while lower frequencies have longer wavelengths.
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Rowan throws a marble from the second floor
of his house (initial height : 3m). The speed of
the marble as it leaves his hand is always 6m/s. Disregard air resistance. In each of the cases below, solve for the speed at which the marble hits the ground. (Make sure to use the
conservation of energy in your solution and NOT kinematics)
The marble will hit the ground with a speed of 6 m/s in all three cases. This is because the total mechanical energy of the marble is conserved.
The total mechanical energy of an object is the sum of its kinetic energy and its potential energy. The kinetic energy of an object is equal to half its mass multiplied by its velocity squared. The potential energy of an object is equal to its mass multiplied by the acceleration due to gravity multiplied by its height.
In the first case, the marble is thrown horizontally from a height of 3 m. The initial velocity of the marble is 6 m/s. The initial kinetic energy of the marble is equal to 1/2 * 0.005 * 36 = 0.9 J.
The initial potential energy of the marble is equal to 0.005 * 9.8 * 3 = 1.47 J. The total mechanical energy of the marble is equal to 0.9 + 1.47 = 2.37 J.
As the marble falls, its potential energy decreases and its kinetic energy increases. When the marble hits the ground, its potential energy is zero and its kinetic energy is equal to the total mechanical energy of the marble,
which is 2.37 J. This means that the velocity of the marble when it hits the ground is equal to the square root of 2.37 J / 0.005 kg, which is 6 m/s.
In the second and third cases, the marble is thrown at an angle. However, the total mechanical energy of the marble is still conserved. This means that the marble will still hit the ground with a speed of 6 m/s.
Here are some additional details about conservation of energy:
Conservation of energy is a law of physics that states that the total energy of an isolated system remains constant.Energy can be converted from one form to another, but it cannot be created or destroyed.Conservation of energy is a fundamental law of physics that has been tested and confirmed many times.Conservation of energy is a powerful tool that can be used to solve problems in physics and engineering. In this case, we used conservation of energy to solve for the speed of a marble as it hits the ground.To know more about velocity click here
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Convert using dimensional analysis
I) 18/5 kmph into m/s (velocity)
II) 5/18 m/s into kmph(velocity)
I) The velocity 18/5 kmph in m/s is 4 m/s.
II) The velocity 5/18 kmph in m/s is 20 kmph.
Dimensional Analysis is a mathematical process used to convert one unit to another. This is done by multiplying the original value with a ratio of equivalent units that is equal to 1. When using dimensional analysis, it is important to keep track of units and cancel out any units that are not needed.
The following is the solution to the conversion of kmph to m/s and vice versa using dimensional analysis.
I) 18/5 kmph into m/s (velocity)When converting kmph to m/s, we need to multiply by 1000/3600 which is equal to 5/18 since there are 1000 meters in one kilometer and 3600 seconds in one hour. Therefore,18/5 kmph x 1000 m/1 km x 1 hour/3600 s = 4 m/s (velocity). Thus, 18/5 kmph is equal to 4 m/s.
II) 5/18 m/s into kmph (velocity)When converting m/s to kmph, we need to multiply by 3600/1000 which is equal to 18/5 since there are 3600 seconds in one hour and 1000 meters in one kilometer. Therefore,5/18 m/s x 3600 s/1 hour x 1 km/1000 m = 20 kmph (velocity). Thus, 5/18 m/s is equal to 20 kmph.
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nswered ct Answer What is the total energy of an electron moving with a speed of 0.35c, (in keV)? 31.35 545.5032 margin of error +/- 1% 27
The total energy of an electron moving with a speed of 0.35c is approximately 31.35 keV, with a margin of error of +/- 1%.
To calculate the total energy of an electron, we can use the relativistic energy equation:
E = γmc²
where E represents energy, γ is the Lorentz factor, m is the rest mass of the electron, and c is the speed of light.
The Lorentz factor is given by:
[tex]\gamma = \frac{1}{\sqrt{1 - \left(\frac{v}{c}\right)^2}}[/tex]
where v is the velocity of the electron and c is the speed of light.
Given that the electron is moving with a speed of 0.35c, we can substitute this value into the equation to calculate the Lorentz factor. Then, by multiplying the Lorentz factor by the rest mass of the electron (m = 0.511 MeV/c²) and the square of the speed of light (c² = 299,792,458 m²/s²), we can find the total energy in joules.
Converting the energy from joules to kiloelectron volts (keV), we divide the energy value by the conversion factor 1 keV = 1.60218 x 10^-16 J. Performing the calculations, the total energy of the electron moving with a speed of 0.35c is approximately 31.35 keV, with a margin of error of +/- 1%.
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Why is it important to always turn the micrometer in the same direction when counting the fringes of a helium-neon (HeNe) laser beam operating at 632.8nm thats producing an interference pattern of bright and dark fringes?
It is important to always turn the micrometer in the same direction when counting the fringes of a HeNe laser beam's interference pattern to maintain consistency and accuracy in the fringe counting process. This ensures that the fringes are counted consistently and eliminates potential errors that could arise from alternating directions.
The interference pattern produced by a HeNe laser beam consists of alternating bright and dark fringes, and counting these fringes is a common method to measure small distances or wavelengths. When using a micrometer to measure the fringe spacing or count the fringes, it is crucial to maintain a consistent and systematic approach.
Turning the micrometer in the same direction ensures that the fringe counting process follows a consistent pattern. This helps eliminate errors that can occur if the direction is alternated. If the micrometer is turned in different directions for consecutive fringe counts, it can lead to confusion and inaccuracies in the counting process. It may result in miscounting or skipping fringes, leading to incorrect measurements or calculations.
By consistently turning the micrometer in the same direction, it becomes easier to keep track of the fringes and maintain a systematic approach. This consistency improves the reliability and precision of the measurements and allows for more accurate calculations based on the fringe count.
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A plane monochromatic electromagnetic wave is travelling in vacuum along the direction of Cartesian coordinates. The electric vector of the wave has the form E = (E0x cos(kz – wt), E0y cos(kz – wt − φ),0) where E0x and E0y are the x- and y-component of the field, and p is a constant 4 phase factor. Draw graphs of Ey versus Ex at the arbitrarily chosen origin z=0 in the xy-plane for the following values of E0x E0y and φ (a) E0x = 2E0y = E0 and φ = 0; Eox = 2E0y E0 = and φ = π
(b) E0x = E0y = E0 and φ = π/2 ; E0x = 2E0y = E0 and φ = -π/2 (c) E0x = 2E0y = E0 and φ = π/4 ; E0x = 2E0y = E0 and φ = -π/4
The graph of Ey versus Ex for (a) E0x = 2E0y = E0 and φ = 0 is a straight line with a positive slope of 2.
What is the relationship between the frequency (f) and wavelength (λ) of an electromagnetic wave?(a) For E0x = 2E0y = E0 and φ = 0, the graph of Ey versus Ex will be a straight line passing through the origin with a positive slope of 2.
(b) For E0x = E0y = E0 and φ = π/2, the graph of Ey versus Ex will be a straight line passing through the origin with a negative slope of -1.
(c) For E0x = 2E0y = E0 and φ = π/4, the graph of Ey versus Ex will be a curve that forms an ellipse in the first quadrant.
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Escaping from a tomb raid gone wrong, Lara Croft (m = 61.0 kg) swings across an alligator-infested river from a 9.30-m-long vine. If her speed at the bottom of the swing is 6.10 m/s and she makes it safely across the river, what is the minimum breaking strength of the vine? N
To find the minimum breaking strength of vine, we can use conservation of mechanical energy. The initial mechanical energy at highest point of the swing is equal to final mechanical energy at bottom of swing.
By considering the gravitational potential energy and the kinetic energy of Lara Croft, we can determine the minimum breaking strength of the vine. At the highest point of the swing, the vine's length is fully extended, and Lara Croft has only gravitational potential energy. At the bottom of the swing, when her speed is given as 6.10 m/s, she has both kinetic energy and gravitational potential energy. The gravitational potential energy at the highest point is equal to the kinetic energy at the bottom of the swing.
Using the equation for gravitational potential energy (PE = mgh) and the equation for kinetic energy (KE = 1/2mv^2), we can equate the two energies and solve for the breaking strength of the vine. The breaking strength will be the force required to stop Lara Croft's motion and bring her to a halt at the bottom of the swing.
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1) A metallic square loop (8cmx8cm in size) has a resistance of 0.2W. When a magnetic field is applied perpendicular to the loop it has an induced current of 250mA clockwise. a) Is the magnetic field strength increasing or decreasing? b) At what rate (in Ts)?
When a magnetic field is applied perpendicular to the loop it has an induced current of 250mA clockwise, The magnetic field strength is decreasing.
When a magnetic field is applied perpendicular to the metallic square loop, it induces an electromotive force (emf) in the loop, which in turn drives a current. According to Lenz's law, the induced current opposes the change in magnetic flux. Since the induced current is clockwise, it means it creates a magnetic field opposing the applied magnetic field.
The emf induced in the loop can be calculated using Faraday's law: emf = -dΦ/dt, where dΦ/dt represents the rate of change of magnetic flux. Given that the loop has a resistance of 0.2 Ω and an induced current of 250 mA (0.25 A), we can use Ohm's law, V = IR, to find the induced emf. V = (0.25 A) * (0.2 Ω) = 0.05 V.
Rearranging the equation, we find that dΦ/dt = -0.05 V/Ts. Therefore, the rate of change of the magnetic field strength is 0.05 T/s.
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8. What direction would you have to look to see
the sun rise or set on the following dates and
locations?
a) Bakersfield, December 21 – set
b) London, England, December 21 – rise
c) Santarem, Brazil, June 21 – set
d) Equator, March 21 – rise
e) North Pole, December 21 – rise
For the following dates and locations considering the Earth's axial tilt, we need to look
a) Bakersfield, December 21 – set
towards the southwestb) London, England, December 21 – rise
towards the southeastc) Santarem, Brazil, June 21 – set
towards the northwest to seed) Equator, March 21 – rise
towards the easte) North Pole, December 21 – rise
We would not be able to see the sunrise.The angle between the Earth's rotational axis and its orbital plane around the Sun is referred to as the Earth's axial tilt, also known as obliquity. The shifting of the seasons and fluctuations in the length of daylight throughout the year are caused by this tilt.
We must take into account the Earth's axial tilt and the Sun's corresponding positions in order to determine which way to look to watch the sun rise or set on particular dates and locations. Following are the tips for where to look for each situation:
a) Bakersfield, December 21 - set:
The winter solstice takes place on December 21 in the Northern Hemisphere, and Bakersfield is in that Hemisphere. The Sun sets in the southwest during the winter solstice. As a result, to observe the sunset on December 21 in Bakersfield, you would need to look southwest.
b) London, England, December 21 - rise:
The winter solstice occurs on December 21 in London, England, which is in the Northern Hemisphere. The Sun rises at this hour in a southeasterly direction. In order to observe the sunrise on December 21 in London, you would therefore need to look in that direction.
c) Santarem, Brazil, June 21 - set:
The winter solstice takes place in the Southern Hemisphere on June 21. Brazil's Santarem is a city in the Southern Hemisphere. In the Southern Hemisphere, the Sun sets in the northwest during the winter solstice. So, in order to witness the sunset in Santarem on June 21, you would need to gaze to the northwest.
d) Equator, March 21 - rise:
The equinox takes place on March 21, and no matter which hemisphere you are in, the Sun rises in the east. The Sun rises straight in the east at the equator, which is located at latitude 0 degrees. Therefore, to watch the sunrise on March 21 in the Equator, you would need to face east.
e) North Pole, December 21 - rise:
The polar night, a phenomenon at the North Pole, takes place on December 21. There is no sunrise because the Sun is still below the horizon. So, on December 21, you wouldn't be able to witness the sunrise at the North Pole.
Therefore, For the following dates and locations considering the Earth's axial tilt, we need to look
a) Bakersfield, December 21 – set
towards the southwestb) London, England, December 21 – rise
towards the southeastc) Santarem, Brazil, June 21 – set
towards the northwest to seed) Equator, March 21 – rise
towards the easte) North Pole, December 21 – rise
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A free electron has a kinetic energy 11.2eV and is incident on a potential energy barrier of U =32.8eV and width w=0.072nm. What is the probability for the electron to penetrate this barrier (in %)?
The probability for the electron to penetrate the potential energy barrier is approximately 48.33%. The probability of an electron penetrating a potential energy barrier can be determined using the concept of quantum tunneling. The transmission coefficient, denoted as T, represents the probability of the electron passing through the barrier.
The transmission coefficient can be calculated using the following formula:
T =[tex]e^(-2kw),[/tex]
where:
k is the wave number,
w is the width of the potential energy barrier.
The wave number (k) can be calculated using the equation:
k = [tex]\sqrt((2m(E - U)) / h^2),[/tex]
where:
m is the mass of the electron,
E is the kinetic energy of the electron,
U is the potential energy of the barrier,
h is the Planck's constant.
Given:
Kinetic energy of the electron (E) = 11.2 eV,
Potential energy of the barrier (U) = 32.8 eV,
Width of the barrier (w) = 0.072 nm.
First, we need to convert the given energies from electron volts (eV) to joules (J). The conversion factor is 1 eV = 1.6 x [tex]10^(-19)[/tex] J.
E = 11.2 eV * (1.6 x [tex]10^(-19)[/tex]J/eV) = 1.792 x[tex]10^(-18[/tex]) J,
U = 32.8 eV * (1.6 x [tex]10^(-19)[/tex]J/eV) = 5.248 x [tex]10^(-18[/tex]) J.
Next, we calculate the wave number:
k = sqrt((2 * 9.11 x [tex]10^(-31[/tex]) kg * (1.792 x [tex]10^(-18)[/tex]J - 5.248 x [tex]10^(-18)[/tex]J)) / (6.626 x 1[tex]0^(-34[/tex]) J·[tex]s)^2[/tex]).
Plugging in the values and performing the calculation, we find:
k ≈ 2.589 x [tex]10^10 m^(-1[/tex]).
Finally, we calculate the transmission coefficient:
T = e^(-2 * (2.589 x [tex]10^10 m^(-1))[/tex] * (0.072 x [tex]10^(-9[/tex]) m)).
Plugging in the values and evaluating the expression, we find:
T ≈ 0.4833.
To convert the transmission coefficient to a percentage, we multiply by 100:
[tex]T_{percentage[/tex] ≈ 0.4833 * 100 ≈ 48.33%.
Therefore, the probability for the electron to penetrate the potential energy barrier is approximately 48.33%.
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What is the rest energy, E 0
, of an object with a mass of 1.00 g? 3.00×10 5
J 3.00×10 11
J 9.00×10 13
J 9.00×10 16
J
The rest energy, E₀ of an object with a mass of 1.00 g is[tex]9.00 * 10^13[/tex] J.Option C[tex]; 9.00*10^(13)[/tex]J is the correct option.
Rest energy, E₀ is the energy possessed by a body due to its rest mass or invariant mass. To determine the rest energy, E₀ of an object with a mass of 1.00 g, we use Einstein’s mass-energy relation,[tex]E = mc^2[/tex], where E represents the energy, m is the mass and c represents the speed of light.
Energy is a fundamental idea in physics that describes a system's capacity for work or effect production. Kinetic energy (energy of motion), potential energy (energy stored as a result of position or configuration), thermal energy (energy related to temperature), chemical energy (energy held in chemical bonds), and electromagnetic energy (energy carried by electromagnetic waves) are just a few examples of the various forms it can take.
The law of energy conservation states that energy can only be changed from one form to another and cannot be created or destroyed. The comprehension and study of energy transfer and transformation in a variety of disciplines, such as physics, engineering, and environmental science, are based on this idea.
Substituting the known values in the above formula, we get;E₀ =[tex]mc^2E₀[/tex] = (1.00 g)[tex](3.00 × [tex]10^8[/tex] m/s)^2[/tex] E₀ = (1.00 × [tex]10^-3[/tex] kg)(9.00 ×[tex]10^(16) m^2/s^2[/tex])
E₀ = 9.00 × [tex]10^(13)[/tex] J
Therefore, the rest energy, E₀ of an object with a mass of 1.00 g is[tex]9.00 * 10^13[/tex] J.Option C[tex]; 9.00*10^(13)[/tex]J is the correct option.
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Find the speed parameter (β) of a particle that takes 2.0 y longer than light to travel a distance of 6.0 ly. (Hint: One light-year is about 6 trillion miles).
To find the speed parameter (β) of a particle that takes 2.0 years longer than light to travel a distance of 6.0 light-years, we can use the formula:
Δt = Δt₀ / √(1 - β²)
Where:
Δt is the time taken by the particle (2.0 years)
Δt₀ is the time taken by light (which we need to calculate)
β is the speed parameter we're looking for
We know that light travels at the speed of light, which is approximately 6 trillion miles per year. So, the distance traveled by light can be calculated as:
d₀ = c * Δt₀
= (6 trillion miles/year) * Δt₀
Since the particle takes 2.0 years longer than light to travel the distance of 6.0 light-years, we have:
6.0 light-years = Δt₀ + 2.0 years
Simplifying this equation, we find:
Δt₀ = 6.0 light-years - 2.0 years
Now, we can substitute the values into the time dilation formula:
2.0 years = (6.0 light-years - 2.0 years) / √(1 - β²)
Rearranging the equation, we have:
√(1 - β²) = (6.0 light-years - 2.0 years) / 2.0 years
Squaring both sides of the equation:
1 - β² = [(6.0 light-years - 2.0 years) / 2.0 years]²
Simplifying and solving for β:
β² = 1 - [(6.0 light-years - 2.0 years) / 2.0 years]²
β ≈ √[1 - ((6.0 light-years - 2.0 years) / 2.0 years)²]
Since 1 light-year is about 6 trillion miles, we can convert the result to miles per year to obtain the speed parameter in appropriate units.
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Consider two sinusoidal waves traveling along a string, modeled as y1x,t=0.4sin(3x+4t) and y2x,t=0.8sin2x-3t. What is the height of the resultant wave formed by the interference of the two waves at the position x = 1.2 m at time t = 1.2 s?
The height of the resultant wave formed by the interference of the two waves at the position x = 1.2 m and time t = 1.2 s is approximately -0.48.
The height of the resultant wave, we need to add the heights of the two individual waves at the given position and time.
That y1(x, t) = 0.4sin(3x + 4t) and y2(x, t) = 0.8sin(2x - 3t), we can substitute the values of x = 1.2 m and t = 1.2 s into each equation.
For y1(1.2, 1.2), we have:
y1(1.2, 1.2) = 0.4sin(3(1.2) + 4(1.2))
y1(1.2, 1.2) = 0.4sin(3.6 + 4.8)
y1(1.2, 1.2) = 0.4sin(8.4)
y1(1.2, 1.2) ≈ 0.4(0.978)
y1(1.2, 1.2) ≈ 0.3912
For y2(1.2, 1.2), we have:
y2(1.2, 1.2) = 0.8sin(2(1.2) - 3(1.2))
y2(1.2, 1.2) = 0.8sin(2.4 - 3.6)
y2(1.2, 1.2) = 0.8sin(-1.2)
y2(1.2, 1.2) ≈ 0.8(-0.932)
y2(1.2, 1.2) ≈ -0.7456
The height of the resultant wave, we add the heights of y1(1.2, 1.2) and y2(1.2, 1.2):
resultant wave height = y1(1.2, 1.2) + y2(1.2, 1.2)
resultant wave height ≈ 0.3912 + (-0.7456)
resultant wave height ≈ -0.3544
Therefore, the height of the resultant wave formed by the interference of the two waves at x = 1.2 m and t = 1.2 s is approximately -0.3544, which can be rounded to -0.35.
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The celestial sphere is a useful model with the Earth at the center, and the sphere of the sky, constellations revolving around it from east to west. In ancient times, people thought that thi was actually the case. Now we know that this only a perception caused by our view of the horizon of a spherical Earth, spinning on its own axis from west to east. Run NAAP app. Then click lab 3. The rotating sky. Click the Rotating sky Explorer, a simula window shows up. For the following questions, use the above simulation launched. Under "star patterns" turn on three constellations, Under location, enter in New York City (40.4 N,73.6 W). Start the animati (you can adjust the speed if you want). 1) From New York City, which constellation is always above the horizon? Always below the hafrizon? Rises and sets below the horizon each day? (final reminder: no one word answer! You answers must be in the form of "A constellation that is always above the horizon from New Yor city is...") 2) From the North Pole (Under location, enter 90 N ), are there constellations that rise above and set below the horizon each day? 3) From the equator (Under location, enter 0N), are there any constellations that are always above the horizon or always below the horizon? 4) At latitudes where Orion rises and sets, in which direction does it set? Does Orion always set in the same direction?
From New York City, a constellation that is always above the horizon is Ursa Major (also known as the Big Dipper) and a constellation that is always below the horizon is Crux (also known as the Southern Cross).
A constellation that rises and sets below the horizon each day is Canis Major (also known as the Great Dog).2) From the North Pole (Under location, enter 90 N), no constellations rise above and set below the horizon each day. All the stars, including the circumpolar constellations, rotate around the North Star, Polaris.3) From the equator (Under location, enter 0N), there are no constellations that are always above or below the horizon.
At latitudes where Orion rises and sets, it sets in the west. Orion does not always set in the same direction; its setting direction changes over the course of a year because of the Earth's orbit around the Sun and the apparent motion of the stars in the sky.
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A solid sphere (I = 2MR2/5) rolls without slipping down a plane inclined at 29◦ relative to horizontal. What type of friction acts and what is the coefficient of friction?
When a solid sphere rolls without slipping down an inclined plane, both static friction and kinetic friction can act.
Initially, as the sphere starts rolling, static friction provides the necessary torque to initiate rolling motion. The magnitude of static friction is given by fs ≤μ sNsN, where μ s is the coefficient of static friction and N is the normal force. The static friction acts in the direction opposite to the motion.
Once the sphere is in motion, kinetic friction comes into play to maintain the rolling motion. The magnitude of kinetic friction is given by f k = kN, where μ k is the coefficient of kinetic friction.
To determine the coefficient of friction, we need additional information such as the materials involved or any given values. Without specific data, we cannot provide an exact coefficient of friction.
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An amoeba is 0.302 cm away from the 0.297 cm focal length objective lens of a microscope. (See the image. Due to the nature of this problem, do not use rounded intermediate values) Where is the image formed by the objective lens? (Enter the image distance in cm.) cm (b) What is this image's magnification? (c) An eyepiece with a 2.00 cm focal length is placed 19.4 cm from the objective. Where is the final image? (Enter the image distance in cm.) cm (d) What magnification is produced by the eyepiece? (e) What is the overall magnification?
The overall magnification is -0.493.
To find the missing values, let's go step by step:
(a) To determine the image distance formed by the objective lens, we can use the lens formula:
1/f = 1/d_o + 1/d_i
where f is the focal length of the lens, d_o is the object distance, and d_i is the image distance.
Given:
f = 0.297 cm
d_o = -0.302 cm (negative because the object is placed in front of the lens)
Substituting the values into the lens formula:
1/0.297 = 1/(-0.302) + 1/d_i
Solving for d_i, we get:
1/d_i = 1/0.297 - 1/(-0.302)
1/d_i = 3.367003367003367 - (-3.311258278145695)
1/d_i = 6.678261645148062
d_i = 1/6.678261645148062
d_i = 0.149 cm
Therefore, the image formed by the objective lens is located at a distance of 0.149 cm from the lens.
(b) The magnification produced by the objective lens can be calculated using the magnification formula:
Magnification = -d_i/d_o
Substituting the values:
Magnification = -0.149 cm / -0.302 cm
Magnification = 0.493
The magnification of the image formed by the objective lens is 0.493.
(c) Now let's calculate the image distance formed by the eyepiece lens. Since the objective and eyepiece lenses are considered in combination, we can use the lens formula again:
1/f_total = 1/f_eyepiece - 1/d_image
Given:
f_eyepiece = 2.00 cm
d_image (distance from objective lens to the final image) = 19.4 cm
Substituting the values:
1/f_total = 1/2.00 - 1/19.4
Solving for 1/f_total:
1/f_total = 0.5 - 0.05154639175257732
1/f_total = 0.4484536082474227
f_total = 1/0.4484536082474227
f_total = 2.230434782608696 cm
The focal length of the combined system is 2.230434782608696 cm.
To find the image distance formed by the eyepiece, we can use the lens formula once more:
1/f_total = 1/d_object - 1/d_final_image
Given:
f_total = 2.230434782608696 cm
d_object (distance from the eyepiece lens to the objective lens) = 19.4 cm
Substituting the values:
1/2.230434782608696 = 1/19.4 - 1/d_final_image
Solving for 1/d_final_image:
1/d_final_image = 0.05154639175257732
d_final_image = 1/0.05154639175257732
d_final_image = 19.4 cm
Therefore, the final image is formed at a distance of 19.4 cm from the eyepiece lens.
(d) The magnification produced by the eyepiece lens can be calculated using the magnification formula:
Magnification_eyepiece = -d_final_image/d_object
Substituting the values:
Magnification_eyepiece = -19.4 cm / 19.4 cm
Magnification_eyepiece = -1
The magnification of the image formed
by the eyepiece lens is -1.
(e) The overall magnification is the product of the magnifications produced by the objective lens and the eyepiece lens:
Overall Magnification = Magnification_objective x Magnification_eyepiece
Overall Magnification = 0.493 x -1
Overall Magnification = -0.493
Therefore, the overall magnification is -0.493.
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A mass of 2.9 kg is observed to be in SHM with an angular frequency of 3.19 rad/s. The amplitude of the SHM is seen to decrease over time and careful measurement shows this is due to a damping coefficient of 0.35 N/m. How long will it take for the amplitude of the oscillations to halve?
Give your solution to 3 s.f.
The amplitude of the oscillations will halve in approximately 6.85 seconds.
In damped harmonic motion, the amplitude of the oscillations decreases exponentially with time. The time it takes for the amplitude to halve is given by the formula:
t = (1 / λ) * ln(2)
where λ is the damping coefficient divided by the mass. In this case, λ = 0.35 N/m / 2.9 kg = 0.1207 s⁻¹. Substituting this value into the formula, we get:
t = (1 / 0.1207) * ln(2) ≈ 6.85 seconds (rounded to 3 significant figures).
Therefore, it will take approximately 6.85 seconds for the amplitude of the oscillations to halve.
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Determine the position of Fermi energy level (EF) at T = 310 K if m*h = 6m*e for an intrinsic Semiconductor with a band gap of 0.7 eV ?
The position of Fermi energy level (EF) at T = 310 K if m*h = 6m*e for an intrinsic Semiconductor with a band gap of 0.7 eV is 0.0349 eV.
The position of Fermi energy level (EF) at T = 310 K if m*h = 6m*e for an intrinsic Semiconductor with a band gap of 0.7 eV can be found using the equation shown below;[tex]E_F = [E_c + E_v]/2 + kT/2ln[(N_v/N_c)^1/2exp(-E_g/2kT)][/tex]
The Fermi level, commonly referred to as the Fermi energy level, is a crucial idea in solid-state physics that characterises the system's highest occupied energy state at zero degrees Celsius. It stands for the energy level at which a system in thermal equilibrium has a 50% chance of detecting an electron. The behaviour of electrons in a material can be predicted using the Fermi energy level as a reference point. In metals, the valence band, which houses the occupied electron states, is where the Fermi energy level is located.
Given that E_g = 0.7 eV (Band Gap), and k = [tex]8.617 * 10^-5 eV/K[/tex] (Boltzmann constant).
Also, m_h = 6m_e (Given relationship)We know that for intrinsic semiconductors at 310K, N_v = N_c, where N_v and N_c are respectively the effective densities of states for holes and electrons. Thus, ln[(N_v/N_c)] = 0
Then substituting the values in the equation:
[tex]E_F = [E_c + E_v]/2 + kT/2ln[(N_v/N_c)^1/2exp(-E_g/2kT)][/tex]= [tex][0 + 0]/2 + (8.617 x 10^-5 K)(310 K)/2ln[(1)^1/2exp(-0.7 eV/2(8.617 x 10^-5 eV/K)(310 K)][/tex]= [tex](8.617 x 10^-5 K)(310 K)/2ln[exp(-0.7 eV/2(8.617 x 10^-5 eV/K)(310 K)]E_F = 0.0349 eV[/tex]
Therefore, the position of Fermi energy level (EF) at T = 310 K if m*h = 6m*e for an intrinsic Semiconductor with a band gap of 0.7 eV is 0.0349 eV.
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A toaster is rated to use 1200 W when the voltage is 120 V. When the voltage is reduced, the power goes down to 500 W. What is the new voltage, assuming the resistance of the toaster is unchanged?
a) 57.5 V
b) 67.5 V
c) 77.5 V
d) 87.5 V
e) 97.5 V
The new voltage, when the power is reduced to 500 W, is approximately 67.5 volts. Option (b) is the correct answer. To find the new voltage, we can use the formula for power: P = V^2 / R
where:
- P is the power (in watts)
- V is the voltage (in volts)
- R is the resistance (in ohms)
- Power at the original voltage (P₁) = 1200 W
- Original voltage (V₁) = 120 V
- Power at the new voltage (P₂) = 500 W
Using the formula for power, we can write two equations:
P₁ = V₁^2 / R -----(1)
P₂ = V₂^2 / R -----(2)
Dividing equation (2) by equation (1), we get:
P₂ / P₁ = (V₂^2 / R) / (V₁^2 / R)
Simplifying, the resistance cancels out:
P₂ / P₁ = (V₂^2) / (V₁^2)
Now, we can solve for the new voltage (V₂):
V₂^2 = (P₂ / P₁) * V₁^2
Taking the square root of both sides:
V₂ = √((P₂ / P₁) * V₁^2)
Substituting the given values:
V₂ = √((500 W / 1200 W) * (120 V)^2)
Calculating the value, we have:
V₂ ≈ 67.5 V
Therefore, the new voltage, when the power is reduced to 500 W, is approximately 67.5 volts. Option (b) is the correct answer.
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2.4 kV single phase circuit feeds a load of 100 kW at a lagging power factor and load current 50 A. If it desired to improve power factor determine the following [3 Marks] a) The uncorrected power factor and reactive power of the load b) The new corrected p.f after installing a shunt capacitor bank with rating of 33.5 kVAr c) Total current drawn from the supply after p.f. correction
Uncorrected power factor: 0.833, Reactive power of the load: 32,080 VAR, New corrected power factor: 0.9998. Total current drawn from the supply after power factor correction: 41.68 A
What is the power factor and reactive power of the load, and what is the corrected power factor and total current drawn after installing a shunt capacitor bank?To determine the uncorrected power factor and reactive power of the load, we can use the following formulas:
a) The uncorrected power factor (cos φ) can be calculated using the formula:
cos φ = P / (V x I)
Where:
P = Load power in watts (100 kW)
V = Voltage in volts (2.4 kV = 2400 V)
I = Load current in amperes (50 A)
Plugging in the values, we get:
cos φ = 100,000 / (2400 x 50)
cos φ ≈ 0.833
The uncorrected power factor is approximately 0.833.
b) The reactive power (Q) of the load can be calculated using the formula:
Q = sqrt(Qc^2 - P^2)
Where:
Qc = Apparent power of the load in volt-amperes reactive (VAR)
P = Load power in watts (100 kW)
Given that the shunt capacitor bank rating is 33.5 kVAr (kilovolt-amperes reactive), we have:
Qc = 33.5 kVAr = 33,500 VAR
Plugging in the values, we get:
Q = sqrt((33,500)^2 - (100,000)^2)
Q ≈ 32,080 VAR
The reactive power of the load is approximately 32,080 VAR.
c) To calculate the new corrected power factor, we can use the formula:
cos φ' = sqrt(cos^2 φ + (Q / (V x I))^2)
Where:
cos φ' = New corrected power factor
cos φ = Uncorrected power factor (0.833)
Q = Reactive power of the load (32,080 VAR)
V = Voltage in volts (2.4 kV = 2400 V)
I = Load current in amperes (50 A)
Plugging in the values, we get:
cos φ' = sqrt((0.833)^2 + (32,080 / (2400 x 50))^2)
cos φ' ≈ 0.9998
The new corrected power factor is approximately 0.9998.
d) Finally, to determine the total current drawn from the supply after power factor correction, we can use the formula:
I' = P / (V x cos φ')
Where:
I' = Total current drawn from the supply after power factor correction
P = Load power in watts (100 kW)
V = Voltage in volts (2.4 kV = 2400 V)
cos φ' = New corrected power factor (0.9998)
Plugging in the values, we get:
I' = 100,000 / (2400 x 0.9998)
I' ≈ 41.68 A
The total current drawn from the supply after power factor correction is approximately 41.68 A.
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how does electromagnetism applied in headphones? Can i get detail explanation
Electromagnetism is applied in headphones through the use of a coil of wire and a permanent magnet. When an audio signal is passed through the coil of wire, it creates a varying magnetic field.
This magnetic field interacts with the permanent magnet, causing the coil to vibrate back and forth. These vibrations generate sound waves that are then transmitted to your ears as audio. The strength and frequency of the electrical signal determine the amplitude and pitch of the sound produced. This electromagnetism principle is used in both dynamic and planar magnetic headphones to convert electrical signals into sound.
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Calculate all currents with nodal analysis. Check the balance of power. Data: R₁=402, R₂=82, R3-24 02, U₁1-48 V, U₁2-24 V, Is-2 A. Usl R₁ Is ↑) U₁2₂ R₂ R₂
If R₁ = 402 ΩR₂ = 82 ΩR₃ = 2402 ΩU₁1 = 48 VU₁2 = 24 VIs = 2 A. The balance of power is P = Ps = 8.8758 W = 96 W.
Current flowing through R1, I1 can be calculated using Ohm's law as follows:
I1 = (U1 - U2) / R1 = (48 - 24) / 402 = 0.06 A
Current flowing through R2, I2 can be calculated using Ohm's law as follows:
I2 = U2 / R2 = 24 / 82 = 0.2927 A
The current through R3, I3 can be calculated by nodal analysis.
I3 = (U2 - 0) / R3 + (U2 - U1) / R2 = (24 - 0) / 2402 + (24 - 48) / 82 = 0.0199 A
The total current leaving the node is the sum of the three currents.
Is = I1 + I2 + I3 = 0.06 + 0.2927 + 0.0199 = 0.3726 A
The total power in the circuit is given by the sum of the power dissipated by each resistor.
P1 = I1² R1 = 0.06² x 402 = 1.4488 WP2 = I2² R2 = 0.2927² x 82 = 7.3343 WP3 = I3² R3 = 0.0199² x 2402 = 0.0927 W
The total power in the circuit is:
P = P1 + P2 + P3 = 1.4488 + 7.3343 + 0.0927 = 8.8758 W
The power supplied by the source is: Ps = Is U1 = 2 x 48 = 96 W
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1/ Calculate the strength of the electric current passing through a conductor, assuming that the value of the electric charge passing through 180, in a time of one minute. C equals?
2/A copper wire with a cross-sectional area of 10 mm2, carries a current of magnitude A 45. Calculate the density of the current passing through the wire?
3/An electrical device marked, 200 V 100W. What is the intensity of the electric current in it?
4/When measuring the value of the voltage drop on a resistor whose value is 100, it was found that the value of the voltage 50v, what is the value of the current flowing through the resistor?
5/ When measuring the value of the voltage drop on a resistor whose value is 100, it was found that the value of the voltage 50v, what is the value of the current flowing through the resistor?
6/ When measuring the value of the voltage drop on a resistor whose value is 100, it was found that the value of the voltage 50v, what is the value of the current flowing through the resistor?
7/ Calculate the electrical resistance of an aluminum tube of length 20 cm and cross-sectional area of 10-4 m2. Then calculate the electrical resistance of a glass tube of the same dimensions?
8/ A copper wire of length 1.5 m and cross-sectional area of 0.6 mm2 has a voltage of 0.9 V. Calculate the current through the wire.?
1) The strength of the electric current is 3 A, 2) The density of the current is 4.5 A/mm², 3) The intensity of the electric current is 0.5 A, 4) The value of the current is 0.5 A, 7) The electrical resistance of the aluminum tube is 2 x 10^-3 Ω, and the electrical resistance of the glass tube is 8 x [tex]10^7[/tex]Ω, 8) The current is 1.5 A.
1) The strength of the electric current passing through the conductor is 3 A.
To calculate the electric current, we use the equation:
Current (I) = Charge (Q) / Time (t)
Given that the charge passing through is 180 C and the time is 1 minute (60 seconds), we can substitute these values into the equation:
I = 180 C / 60 s = 3 A
Therefore, the strength of the electric current passing through the conductor is 3 A.
2) The density of the current passing through the copper wire is 4.5 A/mm².
The current density (J) is defined as the current passing through a unit cross-sectional area of a conductor. It is calculated using the equation:
J = I / A
where I is the current magnitude and A is the cross-sectional area.
Given that the current magnitude is 45 A and the cross-sectional area is 10 mm² (or 0.01 cm²), we can substitute these values into the equation:
J = 45 A / 0.01 cm² = 4.5 A/mm²
Therefore, the density of the current passing through the copper wire is 4.5 A/mm².
3) The intensity of the electric current in the device is 0.5 A.
The intensity of the electric current (I) can be calculated using the equation:
I = Power (P) / Voltage (V)
Given that the power is 100 W and the voltage is 200 V, we can substitute these values into the equation:
I = 100 W / 200 V = 0.5 A
Therefore, the intensity of the electric current in the device is 0.5 A.
4) The value of the current flowing through the resistor is 0.5 A.
The current flowing through a resistor can be determined using Ohm's Law:
I = V / R
Given that the voltage drop is 50 V and the resistance is 100 Ω, we can substitute these values into the equation:
I = 50 V / 100 Ω = 0.5 A
Therefore, the value of the current flowing through the resistor is 0.5 A.
(Note: Questions 5 and 6 appear to be duplicate questions. Please provide a different question for one of them.)
7) The electrical resistance of the aluminum tube is 2 x [tex]10^-3[/tex] Ω, and the electrical resistance of the glass tube is 8 x [tex]10^7[/tex] Ω.
The electrical resistance (R) of a conductor can be calculated using the equation:
R = (ρ * L) / A
where ρ is the resistivity of the material, L is the length of the conductor, and A is the cross-sectional area.
For the aluminum tube, given that its length is 20 cm (or 0.2 m) and the cross-sectional area is [tex]10^-4[/tex] m², and the resistivity of aluminum is approximately 2.65 x [tex]10^-8[/tex] Ω∙m, we can substitute these values into the equation:
R = (2.65 x [tex]10^-8[/tex] Ω∙m * 0.2 m) / [tex]10^-4[/tex] m² = 2 x [tex]10^-3[/tex] Ω
For the glass tube, the resistivity of glass is much higher, typically in the range of [tex]10^{10}[/tex] to [tex]10^{14}[/tex] Ω∙m. Assuming a value of 10^12 Ω∙m, we can calculate the resistance using the same formula:
R = ([tex]10^{12}[/tex] Ω∙m * 0.2 m) /
[tex]10^-4[/tex] m² = 8 x [tex]10^7[/tex] Ω
Therefore, the electrical resistance of the aluminum tube is 2 x [tex]10^-3[/tex] Ω, and the electrical resistance of the glass tube is 8 x [tex]10^7[/tex] Ω.
8) The current through the copper wire is 1.5 A.
Using Ohm's Law, we can determine the current (I) in a wire using the equation:
I = V / R
Given that the length of the wire is 1.5 m, the cross-sectional area is 0.6 mm² (or 6 x [tex]10^-7[/tex] m²), and the voltage is 0.9 V, we need to calculate the resistance (R) of the wire first. The resistance can be calculated using the formula:
R = (ρ * L) / A
where ρ is the resistivity of copper (approximately 1.7 x [tex]10^-8[/tex] Ω∙m), L is the length of the wire, and A is the cross-sectional area.
Substituting the given values:
R = (1.7 x [tex]10^-8[/tex] Ω∙m * 1.5 m) / (6 x [tex]10^-7[/tex] m²) = 4.25 Ω
Now we can calculate the current:
I = 0.9 V / 4.25 Ω = 1.5 A
Therefore, the current through the copper wire is 1.5 A.
To learn more about electric current, click here: brainly.com/question/1100341
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