Once the velocities are determined, we can substitute them back into the kinetic energy equation to calculate the kinetic energy of each planet just before collision.
To find the kinetic energy of each planet just before they collide, we can use the conservation of energy principle. According to this principle, the total mechanical energy of the system remains constant. Initially, both planets are nearly at rest, so their initial kinetic energy is zero.
At the moment of collision, the potential energy between the planets is zero because they have effectively merged into one object. Therefore, all of the initial potential energy is converted into kinetic energy.
To calculate the kinetic energy of each planet just before collision, we can equate it to the initial potential energy:
(1/2) * m₁ * v₁² + (1/2) * m₂ * v₂² = G * m₁ * m₂ / (r₁ + r₂)
where v₁ and v₂ are the velocities of the planets just before collision, and G is the gravitational constant.
Given the values m₁ = 2.00 × 10²⁴ kg, m₂ = 8.00 × 10²⁴ kg, r₁ = 3.00 × 10⁶ m, r₂ = 5.00 × 10⁶ m, and G = 6.67 × 10⁻¹¹ N m²/kg², we can solve the equation to find the velocities.
Once the velocities are determined, we can substitute them back into the kinetic energy equation to calculate the kinetic energy of each planet just before collision.
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Question 2. [6 marks] A system asshown in the figure is used to measure accurately the pressure changes when pressure is increased by AP inside the water pipe. When the height difference reaches Ah = 70 mm, what is the change in pipe pressure? Water Pipe Glycerin, SG= 1.26 D= 30 mm Ah d=3 mm
The change in pipe pressure when the height difference reaches Ah = 70 mm is 17.3 kPa.
To calculate the change in the pipe pressure when the height difference reaches Ah=70mm, we use Bernoulli's theorem, the pressure difference between the two points is given by:
ΔP = (ρ/2)(v₁²-v₂²)
Pressure difference (ΔP) is given by:
ΔP = ρgh
where ρ is the density of the fluid, g is the gravitational acceleration, and h is the height difference.
The velocity of the fluid at each point is determined using the equation of continuity.
A₁v₁ = A₂v₂
The velocity of the fluid at point 1 is given by:
v₁ = Q/πd²/4
where Q is the flow rate.
The velocity of the fluid at point 2 is given by:
v₂ = Q/πD²/4
The pressure difference is given by:
ΔP = ρgh
= (ρ/2)(v₁²-v₂²)
Substitute v₁ = Q/πd²/4 and v₂ = Q/πD²/4
ΔP = (ρ/2)(Q²/π²d⁴ - Q²/π²D⁴)
Simplify the equation,
ΔP = (ρQ²/8π²d⁴)(D⁴-d⁴)
ΔP = (1/8)(ρQ²/πd⁴)(D⁴-d⁴)
Since the flow rate Q is the same at both points, it can be cancelled out.
ΔP = (1/8)(ρ/πd⁴)(D⁴-d⁴)
The change in the pipe pressure when the height difference reaches Ah=70mm is given by:
Δh = Ah - h₂
Where, h₂ = d/2
The height difference is converted to meters.
Δh = 70/1000 - 30/1000 = 0.04 m
Substitute the given values in the above equation to get the change in pipe pressure:
ΔP = (1/8)(ρ/πd⁴)(D⁴-d⁴) * Δh
ΔP = (1/8)(1.26/π(30/1000)⁴)(3/1000)⁴) * 0.04
ΔP = 17.3 kPa
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pr Question 7 A child pulls on a wagon with a force of 75N if the wagon moves a total of 42mm in 3.9min what is the average power delivered by the child? O 16 W O 13 W O 20 W O 17 W
The average power delivered by the child is 13 W.
To calculate the average power delivered by the child, we need to use the formula: Power = Work / Time.
First, we need to calculate the work done by the child. Work is given by the formula: Work = Force x Distance. In this case, the force applied by the child is 75N, and the distance moved by the wagon is 42mm (or 0.042m). Therefore, the work done is Work = 75N x 0.042m = 3.15 J.
Next, we need to determine the time taken by the child. The question states that the wagon moved a total of 42mm in 3.9 minutes. To calculate the time in seconds, we convert minutes to seconds by multiplying by 60: Time = 3.9 min x 60 s/min = 234 s.
Now we can calculate the average power delivered by the child using the formula: Power = Work / Time. Substituting the values, we have Power = 3.15 J / 234 s = 0.01346... W. Rounding to the appropriate number of significant figures, the average power delivered by the child is 13 W.
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6. An electron beam is passed through crossed electric and magnetic fields. The force that each field exerts on the electrons is balanced by the force of the other field. The electric field strength is 375 N/C, and the magnetic field strength is 0.125 T. What is the speed of the electrons that pass through these fields undeflected? Enter your answer 7. Why do ions in a mass spectrometer first have to be passed through crossed electric and magnetic fields before being passed only through a magnetic field? Enter your answer
The speed of the electrons that pass through crossed electric and magnetic fields undeflected is 3 × 10^6 m/s.
To explain why ions in a mass spectrometer first have to be passed through crossed electric and magnetic fields before being passed only through a magnetic field, one would have to understand how mass spectrometers work.
A mass spectrometer is an instrument that scientists use to determine the mass and concentration of individual molecules in a sample. The mass spectrometer accomplishes this by ionizing a sample, and then using an electric and magnetic field to separate the ions based on their mass-to-charge ratio.
Ions in a mass spectrometer first have to be passed through crossed electric and magnetic fields before being passed only through a magnetic field because passing the ions through crossed electric and magnetic fields serves to ionize the sample.
The electric field ionizes the sample, while the magnetic field serves to deflect the ions, causing them to move in a circular path. This deflection is proportional to the mass-to-charge ratio of the ions.
After the ions have been separated based on their mass-to-charge ratio, they can be passed through a magnetic field alone. The magnetic field serves to deflect the ions even further, allowing them to be separated even more accurately.
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Problem 2: Three 0,300 kg masses are placed at the corners of a right triangle as shown below. The sides of the triangle are of lengths a- 0,400 m, b =0.300 m, and c= 0.500 m. Calculate the magnitude and direction of the gravitational force acting on mg (the mass on the lower right corner) due to the other 2 masses only. (10 points) G = 6.67x10-11 N m2/kg? mo b TO
The gravitational force acting on mass 'mg' due to the other two masses only is approximately 0.5788 N and 24.78° from the horizontal, respectively.
The main answer is as follows:A right triangle has been depicted with sides a = 0.400 m, b = 0.300 m and c = 0.500 m, with three masses, each of 0.300 kg, placed at its corners.
Calculate the gravitational force acting on mass 'mg' located at the bottom right corner, with the other two masses as the only sources of the gravitational force.The magnitude and direction of the gravitational force acting on the mass are to be determined.
According to Newton's universal law of gravitation,F = (G m₁m₂)/r²Where,F = gravitational forceG = Universal Gravitational Constant, 6.67 × 10⁻¹¹ Nm²/kg²m₁, m₂ = mass of two bodies,r = distance between the centres of the two massesHere, the gravitational force acting on mass 'mg' is to be determined by the other two masses, each of 0.300 kg.Let us consider the gravitational force acting on 'mg' due to mass 'm1'.
The distance between masses 'mg' and 'm1' is the hypotenuse of the right triangle, c = 0.500 m.Since mass of 'mg' and 'm1' are equal, m = 0.300 kg each.
The gravitational force acting between them can be calculated as,
F₁ = G (0.300 × 0.300) / (0.500)²,
F₁ = 0.107 N (Approximately)
Similarly, the gravitational force acting on 'mg' due to mass 'm2' can be calculated as,
F₂ = G (0.300 × 0.300) / (0.300)²,
F₂ = 0.600 N (Approximately).
The direction of the gravitational force due to mass 'm1' acts on 'mg' towards the left, while the force due to mass 'm2' acts towards the bottom.Let us now calculate the resultant gravitational force on 'mg'.
For that, we can break the two gravitational forces acting on 'mg' into two components each, along the horizontal and vertical directions.F₁x = F₁ cos θ
0.107 × (0.4 / 0.5) = 0.0856 N,
F₂x = F₂ cos 45°
0.600 × 0.707 = 0.424 N (Approximately),
F₁y = F₁ sin θ
0.107 × (0.3 / 0.5) = 0.0642 N,
F₂y = F₂ sin 45°
0.600 × 0.707 = 0.424 N (Approximately).
The resultant gravitational force acting on mass 'mg' is given by,
Fres = (F₁x + F₂x)² + (F₁y + F₂y)²
Fres = √ ((0.0856 + 0.424)² + (0.0642 - 0.424)²)
Fres = √0.3348Fres = 0.5788 N (Approximately)
The direction of the resultant gravitational force acting on 'mg' makes an angle, θ with the horizontal, such that,
Tan θ = (F₁y + F₂y) / (F₁x + F₂x)
(0.0642 - 0.424) / (0.0856 + 0.424)θ = 24.78° (Approximately).
Therefore, the magnitude and direction of the gravitational force acting on 'mg' due to the other two masses only are approximately 0.5788 N and 24.78° from the horizontal, respectively.
Thus, the gravitational force acting on mass 'mg' due to the other two masses only is approximately 0.5788 N and 24.78° from the horizontal, respectively.
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Two toroidal solenoids are wound around the same form so that the magnetic field of one passes through the turns of the other. Solenoid 1 has 710 turns and solenoid 2 has 380 turns. When the current in solenold 1 IS 6.60 A , the average flux
through each turn of solenoid 2 is 4.00×10-2 Wb.
What is the mutual inductance of the pair of solenoids?
The current in solenoid 1 IS 6.60 A , the average flux through each turn of solenoid 2 is 4.00×10-2 Wb. the mutual inductance of the pair of solenoids is approximately 230.30 Wb-turns/A.
The mutual inductance (M) between the pair of solenoids can be calculated using the formula:
M = N2Φ2 / I1
where N2 is the number of turns in solenoid 2, Φ2 is the average flux through each turn of solenoid 2, and I1 is the current in solenoid 1.
Given:
N2 = 380 turns
Φ2 = 4.00×10-2 Wb
I1 = 6.60 A
Substituting these values into the formula, we get:
M = (380 turns)(4.00×10-2 Wb) / 6.60 A
Calculating this expression:
M = (1520 Wb-turns) / 6.60 A
M ≈ 230.30 Wb-turns/A
Therefore, the mutual inductance of the pair of solenoids is approximately 230.30 Wb-turns/A.
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A runner, jogging along a straight-line path, starts at a position 60.0 m east of a milestone marker and heads west. After a short time interval he is 27.2 m west of the mile marker. Choose east to be the positive x-direction. What is the runner's displacement from his starting point?
The runner's displacement from his starting point is -87.2 meters. The negative sign indicates that the runner has moved in the opposite direction from his initial position, westward in this case.
To calculate the runner's displacement from his starting point, we need to determine the net distance and direction he has traveled.
The runner starts 60.0 m east of the milestone marker, which we can assign a positive value in the x-direction. When he is 27.2 m west of the mile marker, we can assign this a negative value in the x-direction.
To find the displacement, we can subtract the final position from the initial position:
Displacement = Final position - Initial position
The initial position is 60.0 m in the positive x-direction, and the final position is 27.2 m in the negative x-direction.
Displacement = -27.2 m - 60.0 m
Displacement = -87.2 m
Therefore, the runner's displacement from his starting point is -87.2 meters. The negative sign indicates that the runner has moved in the opposite direction from his initial position, westward in this case.
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A 10 volt battery is connected to a 4 uF parallel plate capacitor and a 20 MQ resistor. The radius of the plates of the capacitor is 8 mm. Find the magnetic field inside the capacitor 2 mm away from the center of the capacitor 1 minute after the initial connection of the battery. Find the magnetic field 10 mm away from the center.
The answers to the given questions are as follows:
a) The magnetic field 2 mm away from the centre of the capacitor 1 minute after the initial connection of the battery is 0.5 × 10⁻⁷ T·m/A.
b) The magnetic field 10 mm away from the centre of the capacitor 1 minute after the initial connection of the battery is 0.1 × 10⁻⁷ T·m/A.
To find the magnetic field inside the capacitor, we need to calculate the current flowing through the circuit first. Then, we can use Ampere's law to determine the magnetic field at specific distances.
Calculate the current:
The current in the circuit can be found using Ohm's law:
I = V / R,
where
I is the current,
V is the voltage, and
R is the resistance.
Given:
V = 10 volts,
R = 20 MQ (megaohms)
R = 20 × 10⁶ Ω.
Substituting the given values into the formula, we get:
I = 10 V / 20 × 10⁶ Ω
I = 0.5 × 10⁶ A
I = 0.5 μA.
Therefore, the current in the circuit 0.5 μA.
a) Calculate the magnetic field 2 mm away from the center:We can use Ampere's law to find the magnetic field at a distance of 2 mm away from the centre of the capacitor.
Ampere's law states that the line integral of the magnetic field around a closed loop is proportional to the current passing through the loop.
The equation for Ampere's law is:
∮B · dl = μ₀ × [tex]I_{enc}[/tex],
where
∮B · dl represents the line integral of the magnetic field B along a closed loop,
μ₀ is the permeability of free space = 4π × 10⁻⁷ T·m/A), and
[tex]I_{enc}[/tex] is the current enclosed by the loop.
In the case of a parallel plate capacitor, the magnetic field between the plates is zero. Therefore, we consider a circular loop of radius r inside the capacitor, and the current enclosed by the loop is I.
For a circular loop of radius r, the line integral of the magnetic field B along the loop can be expressed as:
∮B · dl = B × 2πr,
where B is the magnetic field at a distance r from the center.
Using Ampere's law, we have:
B × 2πr = μ₀ × I.
Substituting the given values:
B × 2π(2 mm) = 4π × 10⁻⁷ T·m/A × 0.5 μA.
Simplifying:
B × 4π mm = 2π × 10⁻⁷ T·m/A.
B = (2π × 10⁻⁷ T·m/A) / (4π mm)
B = 0.5 × 10⁻⁷ T·m/A.
Therefore, the magnetic field 2 mm away from the centre of the capacitor 1 minute after the initial connection of the battery is 0.5 × 10⁻⁷ T·m/A.
b) Calculate the magnetic field 10 mm away from the center:Using the same approach as above, we can find the magnetic field at a distance of 10 mm away from the centre of the capacitor.
B × 2π(10 mm) = 4π × 10⁻⁷ T·m/A × 0.5 μA.
Simplifying:
B × 20π mm = 2π × 10⁻⁷ T·m/A.
B = (2π × 10⁻⁷ T·m/A) / (20π mm)
B = 0.1 × 10⁻⁷ T·m/A.
Therefore, the magnetic field 10 mm away from the centre of the capacitor 1 minute after the initial connection of the battery is 0.1 × 10⁻⁷ T·m/A.
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A propagating wave on a taut string of linear mass density u = 0.05 kg/m is represented by the wave function y(x,t) = 0.5 sin(kx - 12nt), where x and y are in X meters and t is in seconds. If the power associated to this wave is equal to 34.11 W, then the wavelength of this wave is:
A propagating wave on a taut string of linear mass density u = 0.05 kg/m is represented by the wave function y(x,t) = 0.5 sin(kx - 12nt), where x and y are in X meters and t is in seconds. If the power associated to this wave is equal to 34.11 W, the wavelength of the wave is approximately 0.066 meters or 66 millimeters.
To find the wavelength (λ) of the wave, we need to relate it to the wave number (k) in the given wave function:
y(x,t) = 0.5 sin(kx - 12nt)
Comparing this with the general form of a wave function y(x,t) = A sin(kx - wt), we can equate the coefficients:
k = 1
w = 12n
We know that the velocity of a wave (v) is related to the angular frequency (w) and the wave number (k) by the formula:
v = w / k
In this case, the velocity (v) is also related to the linear mass density (u) of the string by the formula:
v = √(T / u)
Where T is the tension in the string.
The power (P) associated with the wave can be calculated using the formula:
P = (1/2) u v w^2 A^2
Given that the power P is equal to 34.11 W, we can substitute the known values into the power formula:
34.11 = (1/2) (0.05) (√(T / 0.05)) (12n)^2 (0.5)^2
Simplifying this equation, we get:
34.11 = 0.025 √(T / 0.05) (12n)^2
Dividing both sides of the equation by 0.025, we have:
1364.4 = √(T / 0.05) (12n)^2
Squaring both sides of the equation, we get:
(1364.4)^2 = (T / 0.05) (12n)^2
Rearranging the equation to solve for T, we have:
T = (1364.4)^2 × 0.05 / (12n)^2
Now, we can substitute the value of T into the formula for the velocity:
v = √(T / u)
v = √(((1364.4)^2 × 0.05) / (12n)^2) / 0.05
v = (1364.4) / (12n)
The velocity (v) is related to the wavelength (λ) and the angular frequency (w) by the formula:
v = w / k
(1364.4) / (12n) = 12n / λ
Simplifying this equation, we get:
λ = (12n)^2 / (1364.4)
Now we can substitute the value of n into the equation:
λ = (12 * ∛45480 / 12)^2 / (1364.4)
Evaluating this expression, we find:
λ ≈ 0.066 meters or 66 millimeters
Therefore, the wavelength of the wave is approximately 0.066 meters or 66 millimeters.
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In the process of freezing of a mass m kg of a material whose latent heat of fusion is IF and its boiling temperature is f °C, the change in the entropy of the universe equals
The change in entropy of the universe in the process of freezing is zero. This result is consistent with the second law of thermodynamics, which states that in any real process, the entropy of the universe must either remain constant or increase. In the case of freezing, the decrease in entropy of the material is compensated by an equal increase in entropy of the surroundings, resulting in no net change in entropy of the universe.
In the process of freezing, the change in entropy of the universe can be determined by considering the entropy change of the material undergoing freezing and the entropy change of the surroundings.
1. Entropy change of the material undergoing freezing:
During the freezing process, the material undergoes a phase transition from a liquid to a solid state. The change in entropy of the material can be calculated using the formula:
ΔS_material = -m * L_f / T_f
where ΔS_material is the change in entropy of the material, m is the mass of the material, L_f is the latent heat of fusion, and T_f is the freezing temperature in Kelvin.
2. Entropy change of the surroundings:
During the freezing process, the surroundings gain heat from the material as it releases latent heat. The change in entropy of the surroundings can be calculated using the formula:
ΔS_surroundings = q / T_f
where ΔS_surroundings is the change in entropy of the surroundings, q is the heat gained by the surroundings, and T_f is the freezing temperature in Kelvin.
Since the material releases heat to the surroundings during freezing, the heat gained by the surroundings (q) is equal to the latent heat of fusion (L_f) multiplied by the mass of the material (m).
q = m * L_f
Substituting this into the equation for the entropy change of the surroundings:
ΔS_surroundings = (m * L_f) / T_f
3. Total change in entropy of the universe:
The total change in entropy of the universe is the sum of the entropy changes of the material and the surroundings:
ΔS_universe = ΔS_material + ΔS_surroundings
ΔS_universe = -m * L_f / T_f + (m * L_f) / T_f
Simplifying:
ΔS_universe = 0
Therefore, the change in entropy of the universe in the process of freezing is zero. This result is consistent with the second law of thermodynamics, which states that in any real process, the entropy of the universe must either remain constant or increase. In the case of freezing, the decrease in entropy of the material is compensated by an equal increase in entropy of the surroundings, resulting in no net change in entropy of the universe.
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A levitating train is three cars long (150 m) and has a mass of 100 metric tons (1 metric ton = 1000 kg). The current in the superconducting wires is about 500 kA, and even though the traditional design calls for many small coils of wire, assume for this problem that there is a 150-m-long, straight wire carrying the current beneath the train. A perpendicular magnetic field on the track levitates the train. Find the magnitude of the magnetic field B needed to levitate the train.
The magnitude of the magnetic field needed to levitate the train is approximately 0.0131 N/(A·m). To find the magnitude of the magnetic field B needed to levitate the train, we can use the equation for the magnetic force on a current-carrying wire. which is given by F = BIL.
The force of attraction between a magnetic field and a current-carrying wire is given by the equation F = BIL, where F is the force, B is the magnetic field, I is the current, and L is the length of the wire. For the train to be levitated, this magnetic force must balance the force of gravity on the train.
The force of gravity on the train can be calculated using the equation F = mg, where m is the mass of the train and g is the acceleration due to gravity. Given that the mass of the train is 100 metric tons, which is equivalent to 100,000 kg, and the acceleration due to gravity is approximately 9.8 m/s², we can determine the force of gravity.
By setting the force of attraction equal to the force of gravity and rearranging the equation, we have BIL = mg. Plugging in the values for the train's length L (150 m), current I (500 kA = 500,000 A), and mass m (100,000 kg), we can solve for the magnetic field B. The magnitude of the magnetic field needed to levitate the train is approximately 0.0131 N/(A·m).
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10. An electron (charge -1.60 x 10-19 C and mass 9.11 x 10-31 kg) is initially at rest at the center of a uniformly charged ring of radius 3 mm and linear charge density ^ = -4.07 nC/m. The electron is nudged slightly and starts accelerating away from the ring along its central axis. Which of the following is closest to the electron's speed by the time it is very far from the ring? a) 5.0 x106 m/s d) 8.0 x 106 m/s c) 7.0 x 106 m/s b) 6.0 x 106 m/s e) 9.0 x 106 m/s
The electron is nudged slightly and starts accelerating away from the ring along its central axis. the electron's speed when it is very far from the ring is 0 m/s. None of the given options (a, b, c, d, or e) are closest to the correct answer.
To find the speed of the electron when it is very far from the ring, we can use the principle of conservation of energy.
The initial energy of the electron is entirely in the form of electric potential energy due to the interaction with the charged ring. As the electron moves away from the ring, this potential energy is converted into kinetic energy.
The electric potential energy between the electron and the ring is given by:
U = - (k * q * Q) / r,
where U is the electric potential energy, k is the Coulomb's constant (9 x 10^9 N·m^2/C^2), q is the charge of the electron (-1.60 x 10^-19 C), Q is the linear charge density of the ring (-4.07 x 10^-9 C/m), and r is the distance between the electron and the center of the ring.
The initial potential energy of the electron is:
U_initial = - (k * q * Q * r_initial) / r_initial,
where r_initial is the initial distance between the electron and the center of the ring. Since the electron is initially at the center of the ring, r_initial = 0.
The final kinetic energy of the electron when it is very far from the ring is:
K_final = (1/2) * m * v_final^2,
where K_final is the final kinetic energy, m is the mass of the electron (9.11 x 10^-31 kg), and v_final is the final velocity of the electron.
According to the conservation of energy, the initial potential energy is equal to the final kinetic energy:
U_initial = K_final.
Solving for v_final, we get:
v_final = sqrt((2 * U_initial) / m).
Substituting the values, we have:
v_final = sqrt((2 * (-(k * q * Q * r_initial) / r_initial)) / m).
Calculating the numerical value:
v_final = sqrt((2 * (-(9 x 10^9 N·m^2/C^2) * (-1.60 x 10^-19 C) * (-4.07 x 10^-9 C/m) * 0) / (9.11 x 10^-31 kg)).
v_final = sqrt(0) = 0 m/s.
Therefore, the electron's speed when it is very far from the ring is 0 m/s. None of the given options (a, b, c, d, or e) are closest to the correct answer.
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A series RLC circuit has components with the following values: L = 16.0 mH, C = 86.0 nF, R = 10.02, and AV = 100 V, with Av = AV max sin wt. max (a) Find the resonant frequency of the circuit. kHz
The resonant frequency of the circuit is approximately 135.8 kHz.
To find the resonant frequency of the series RLC circuit, we can use the formula:
f_res = 1 / (2π√(LC))
L = 16.0 mH = 16.0 x [tex]10^(-3)[/tex] H
C = 86.0 nF = 86.0 x [tex]10^(-9)[/tex]F
Plugging in the values:
f_res = 1 / (2π√(16.0 x[tex]10^(-3[/tex]) * 86.0 x [tex]10^(-9)))[/tex]
f_res = 1 / (2π√(1.376 x [tex]10^(-6)))[/tex] ≈ 1 / (2π x 0.001173) ≈ 1 / (0.007356) ≈ 135.8 kHz
The resonant frequency of a circuit refers to the frequency at which the impedance of the circuit is purely resistive, resulting in maximum current flow or minimum impedance.
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Question 5 Correcting for a disturbance, which has caused a rolling motion about the longitudinal axis would re-establish which of the following? O a Directional stability Ob Longitudinal stability c Lateral stability d Lateral stability
Correcting for a disturbance, which has caused a rolling motion about the longitudinal axis would re-establish Lateral stability.
What is stability? Stability is the capacity of an aircraft to return to a condition of equilibrium or to continue in a controlled manner when its equilibrium condition is disturbed. Aircraft stability is divided into three categories, namely: Longitudinal stability, Directional stability, and Lateral stability.
What is Longitudinal Stability? Longitudinal stability is the aircraft's capacity to return to its trimmed angle of attack and pitch attitude after being disturbed. The longitudinal axis is utilized to define it.
What is Directional Stability?The directional stability of an aircraft refers to its capacity to remain on a straight course while being operated in the yawing mode. The vertical axis is used to determine it.
What is Lateral Stability? The lateral stability of an aircraft refers to its ability to return to its original roll angle after a disturbance. The longitudinal axis is used to determine it.
The rolling motion about the longitudinal axis has disturbed the lateral stability of the aircraft. Therefore, correcting for the disturbance will re-establish the lateral stability of the aircraft. Therefore, the answer is option d: Lateral stability. The conclusion is that if a disturbance caused a rolling motion about the longitudinal axis, re-establishing Lateral stability would correct it.
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A sinusoidal sound wave moves through a medium and is described by the displacement wave function
(x, t) = 2.19 cos(16.3x - 851t)
where s is in micrometers, x is in meters, and t is in seconds.
(a) Find the amplitude of this wave.
um
(b) Find the wavelength of this wave.
cm
(c) Find the speed of this wave.
(a) The amplitude of the sinusoidal sound wave is 2.19 μm.
(b) The wavelength is given by λ = 1/16.3 = 0.0613 m or 6.13 cm.
(c) The frequency is f = 851 Hz. S
The amplitude of a wave represents the maximum displacement of particles in the medium from their equilibrium position. In this case, the maximum displacement is given as 2.19 μm. Moving on to the wavelength, it can be determined by examining the coefficient of x in the displacement wave function, which is 16.3.
This coefficient represents the number of wavelengths that fit within a distance of 1 meter. Therefore, the wavelength is calculated as 1/16.3 = 0.0613 m or 6.13 cm. To find the speed of the wave, the formula v = λf is used, where v is the speed, λ is the wavelength, and f is the frequency. The frequency is obtained from the coefficient of t in the displacement wave function, which is 851. Substituting the values, the speed is calculated as (0.0613 m) × (851 Hz) = 52.15 m/s.
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A parallel-plate capacitor has a plate area of 0.2 m² and a plate separation of 0.1 mm. To obtain an electric field of 2.0 x 10^6 V/m between the plates, calculate the magnitude of the charge on each plate
The magnitude of the charge on each plate of the parallel-plate capacitor is approximately 4.0 x 10^-5 C.
The electric field between the plates of a parallel-plate capacitor can be calculated using the formula:
E = σ / ε₀
Where:
E is the electric-field,
σ is the surface charge density on the plates, and
ε₀ is the permittivity of free space.
The surface charge density can be defined as:
σ = Q / A
Where:
Q is the charge on each plate, and
A is the area of each plate.
Combining these equations, we can solve for the charge on each plate:
E = Q / (A * ε₀)
Rearranging the equation, we have:
Q = E * A * ε₀
Substituting the given values for the electric field (2.0 x 10^6 V/m), plate area (0.2 m²), and permittivity of free space (ε₀ ≈ 8.85 x 10^-12 C²/N·m²), we find that the magnitude of the charge on each plate is approximately 4.0 x 10^-5 C.
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Draw a ray diagram and answer the questions for each of the following situations: a) An object is 4.5 cm from a lens with a focal length of +2.5 cm. Which of the following apply to the image? behind t
The image formed by the lens is virtual, upright, and located 5.625 cm behind the lens.
To determine the characteristics of the image formed by the lens, we can use the lens formula:
1/f = 1/v - 1/u
where f is the focal length of the lens, v is the image distance from the lens, and u is the object distance from the lens.
Given:
f = +2.5 cm (positive for a converging lens)
u = -4.5 cm (negative because the object is in front of the lens)
Let's substitute the given values into the lens formula:
1/2.5 = 1/v - 1/-4.5
Simplifying this equation, we get:
0.4 = 1/v + 1/4.5
To further solve the equation, we can find a common denominator:
0.4 = (4.5 + v)/(4.5v)
Cross-multiplying, we have:
0.4 * 4.5v = 4.5 + v
1.8v = 4.5 + v
Bringing v terms to one side and constants to the other side:
1.8v - v = 4.5
0.8v = 4.5
v = 4.5 / 0.8
v = 5.625 cm
The positive value of v indicates that the image formed by the lens is on the same side as the object, which makes it a virtual image. Since the object is real and upright, the image will also be virtual and upright. The magnitude of the image distance is 5.625 cm, indicating that the image is located 5.625 cm behind the lens.
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Q. 137: Two lenses L₁ and L₂ are used to make a telescope. The larger lens L₁ is a convex lens with both surfaces having radius of curvature equal to 0.5 m. The smaller lens L₂ has two surfaces with radius of curvature 4 cm. Both the lenses are made of glass having refractive index 1.5. The two lenses are mounted in a tube with separation between them equal to 1 cm less than the sum of their focal length. (a) Find the position of the image formed by such a telescope for an object at a distance of 100 m from the objective lens L₁. (b) What is the size of the image if object is 1 m high? Do you think that lateral magnification is a useful way to characterize a telescope?
a) The image is 6.74 times larger than the object and is formed 6.74 times farther from the objective lens than the focal length.
b) The image is 6.74 times larger than the object and is formed 6.74 times farther from the objective lens than the focal length.
(a) Position of the image formed by such a telescope for an object at a distance of 100m from the objective lens L₁
The focal length of the convex lens L₁ can be obtained as follows:f = R/(n-1)
where R is the radius of curvature of the lens and n is the refractive index.
f = 0.5 m / (1.5 - 1) = 1 m
The distance between the two lenses is given as 1 cm less than the sum of their focal length. The focal length of the smaller lens L₂ is given as:
f₂ = R/(n-1) = 0.04m/(1.5-1) = 0.16 m
The distance between the lenses is given as (f₁ + f₂ - 0.01) = 1 + 0.16 - 0.01 = 1.15 m
Therefore, the magnification of the telescope is given by:
M = - v/u
where v is the image distance and u is the object distance.
u = -100 m, f₁ = 1 m, and f₂ = 0.16 m
Substituting in the formula,
M = - (f₁ + f₂ - d)/(f₂ * (f₁ + f₂ - d)/f₁ - d/u)
M = - (1.16 - 0.01)/((0.16 * (1.16 - 0.01))/1 - (-100)) = -6.74
We obtain a negative magnification because the image is inverted.
(b) Size of the image if object is 1m high
The height of the image is given by:
h₂ = M * h₁
where h₁ is the height of the objecth₁ = 1 m
Therefore, the height of the image is:
h₂ = -6.74 * 1 = -6.74 m
We obtain a negative height because the image is inverted.
Lateral magnification is a useful way to characterize a telescope as it provides information about the size and position of the image relative to the object. It helps to understand the quality of the image and how well the telescope is able to resolve details.
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12.1
Part A
What is the specific heat of a substance if 130 kJ of heat is needed to raise 9.1 kg of the substance from 18.0∘C to 37.2∘C?
Express your answer using two significant figures.
c = _________________ J/kg⋅C∘
Part B
How much heat is needed to melt 18.50 kg of silver that is initially at 15 ∘C? The melting point of silver is 961∘C, the heat of fusion is 88 kJ/kg, the specific heat is 230 J/kg⋅C∘.
Express your answer to two significant figures and include the appropriate units.
Q =
The specific heat of the substance is approximately 502 J/(kg·°C). The heat needed to melt the silver is approximately 3.37 × 10^9 J.
Part A:
We can determine the specific heat of the substance by utilizing the following formula:
q = m * c * ΔT
q = heat energy (130 kJ)
m = mass of the substance (9.1 kg)
c = specific heat of the substance (to be determined)
ΔT = change in temperature (37.2°C - 18.0°C)
Rearranging the equation to solve for c:
c = q / (m * ΔT)
Substituting the given values:
c = 130 kJ / (9.1 kg * (37.2°C - 18.0°C))
Calculating the numerical value:
c ≈ 502 J/(kg·°C)
Part B:
To calculate the heat needed to melt the silver, we can use the formula:
Q = m * Lf
Q = heat energy needed
m = mass of the silver (18.50 kg)
Lf = heat of fusion (88 kJ/kg)
However, before melting, the silver needs to be heated from its initial temperature (15°C) to its melting point (961°C). The heat needed for this temperature change can be calculated using:
Q = m * c * ΔT
Q = heat energy needed
m = mass of the silver (18.50 kg)
c = specific heat of silver (230 J/(kg·°C))
ΔT = change in temperature (961°C - 15°C)
The total heat needed is the sum of the heat required for temperature change and the heat of fusion:
Q = (m * c * ΔT) + (m * Lf)
Substituting the given values:
Q = (18.50 kg * 230 J/(kg·°C) * (961°C - 15°C)) + (18.50 kg * 88 kJ/kg)
Calculating the numerical value:
Q ≈ 3.37 × 10^9 J
Therefore, the answers are:
Part A: The specific heat of the substance is approximately 502 J/(kg·°C).
Part B: The heat needed to melt the silver is approximately 3.37 × 10^9 J.
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Complete the following beta decays. Make sure to delete the "0" that appears in the pre-subscript position of the nuclide symbol before submitting your responses. 20F e +ve+ 239Npe" + vet 3H+ve+ 207 Bi et + 60 e + ve + Ni
Please note that the "vet" in the second decay is not a recognized symbol or notation for beta decay. If you provide more specific information or correct any errors.
Neutrinos are subatomic particles that are electrically neutral and have very low mass. They interact weakly with matter, making them difficult to detect. In beta decay, neutrinos are often emitted along with the electron or positron to conserve certain properties, such as lepton number and angular momentum.During beta decay, the neutrino is denoted as νe (electron neutrino) or νμ (muon neutrino), depending on the type of decay involved. For example, in the beta decay of a neutron (n → p + e- + νe), an electron and an electron neutrino are emitted.The presence of neutrinos in beta decay was initially postulated by Wolfgang Pauli in 1930 to account for the conservation of energy, momentum, and angular momentum. Neutrinos were eventually detected experimentally in the 1950s, confirming their existence.
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An evacuated tube uses an accelerating voltage of 40 kV to accelerate electrons to hit a copper plate and produce X-rays. a. How much potential energy does a single electron loose due to being accelerated through the 40 kV potential? Hint: what is the charge of a single electron? b. What would be the maximum speed of these electrons? Hint: Potential energy is converted into another form of energy and the mass of an electron is 9.11x10" kg.
a. A single electron loses 6.408 × 10⁻¹⁵ J of potential energy.
b. The maximum speed of the electrons is 8.9 × 10⁶ m/s.
a. The potential energy lost by a single electron can be calculated using the equation for electric potential energy:
ΔPE = qΔV, where ΔPE is the change in potential energy, q is the charge of the electron (1.6 × 10⁻¹⁹ C), and ΔV is the change in voltage (40,000 V). Plugging in the values,
we get ΔPE = (1.6 × 10⁻¹⁹ C) × (40,000 V)
= 6.4 × 10⁻¹⁵ J.
b. To determine the maximum speed of the electrons, we can equate the loss in potential energy to the gain in kinetic energy.
The kinetic energy of an electron is given by KE = ½mv²,
where m is the mass of the electron (9.1 × 10⁻³¹ kg) and v is the velocity. Equating ΔPE to KE, we have ΔPE = KE.
Rearranging the equation, we get
(1.6 × 10⁻¹⁹ C) × (40,000 V) = ½ × (9.1 × 10⁻³¹ kg) × v².
Solving for v, we find
v = √((2 × (1.6 × 10⁻¹⁹ C) × (40,000 V)) / (9.1 × 10⁻³¹ kg))
= 8.9 × 10⁶ m/s.
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The magnetic field of a plane EM wave is given by B= B0
cos(kz−ωt)ˆj. Indicate:
a) The direction of propagation of the wave
b) The direction of E.
The direction of propagation is k, the electric field is i, and the magnetic field is j.
a) The direction of propagation of the wave
The direction of propagation of an electromagnetic wave is perpendicular to both the electric field and the magnetic field. The magnetic field vector in your question is in the j-direction, so the direction of propagation is in the k-direction.
b) The direction of E
The electric field vector is perpendicular to the magnetic field vector and the direction of propagation. Since the magnetic field vector is in the j-direction, the electric field vector is in the i-direction.
Here is a diagram of the electromagnetic wave:
|
| E
|
\|/
k---
The direction of propagation is k, the electric field is i, and the magnetic field is j.
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What is the focal length of 1.50 D reading glasses found on the rack in a pharmacy? Submit Answer Incorrect. Tries 2/40 Previous Tries
The focal length of 1.50 D reading glasses found on the rack in a pharmacy is 0.67 meters.
The focal length of a lens is a measure of its ability to converge or diverge light. It is commonly denoted by the symbol 'f'. In this case, we are given that the reading glasses have a power of 1.50 D. The power of a lens is the reciprocal of its focal length, so we can use the formula f = 1 / power to determine the focal length.
Substituting the given power of 1.50 D into the formula, we have f = 1 / 1.50. Simplifying this expression, we find that the focal length of the reading glasses is approximately 0.67 meters.
Therefore, the focal length of the 1.50 D reading glasses found on the rack in the pharmacy is 0.67 meters.
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A source emitting a sound at 300 Hz is moving toward an observer at 25 m/s. The air temperature
is 15° C. Determine the frequency detected by the observer?
The frequency detected by the observer is approximately 324.53 Hz.
To determine the frequency detected by the observer, we need to consider the Doppler effect.
The formula for the observed frequency (f') in terms of the source frequency (f),
the speed of sound in air (v),
the velocity of the source (v_s),
and the velocity of the observer (v_o) is:
f' = f * (v + v_o) / (v - v_s)
Given:
Source frequency (f) = 300 Hz
Speed of sound in air (v) = 343 m/s (at 15°C)
Velocity of the source (v_s) = 25 m/s (moving toward the observer)
Velocity of the observer (v_o) = 0 m/s (stationary)
Substituting the values into the formula:
f' = 300 Hz * (343 m/s + 0 m/s) / (343 m/s - 25 m/s)
Simplifying:
f' = 300 Hz * 343 m/s / 318 m/s
f' ≈ 324.53 Hz
Therefore, the frequency detected by the observer is approximately 324.53 Hz.
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(e) Compare the advantages and disadvantages of wind and hydroelectric power with respect to the following; reliability of the primary energy source, environmental impact and geographical suitability. In your discussion give examples of countries where either wind or hydroelectric power generation is a good idea.
Wind and hydroelectric power have distinct advantages and disadvantages regarding the reliability of the primary energy source, environmental impact, and geographical suitability. Wind power relies on wind availability, which can vary, while hydroelectric power depends on water resources and is generally more reliable. Wind power has minimal environmental impact, while hydroelectric power can have significant ecological consequences. Geographical suitability varies, with wind power suitable in regions with consistent wind patterns and hydroelectric power feasible in areas with rivers and suitable topography. Examples of countries where wind power is prominent include Denmark and Germany, while Norway and Canada excel in hydroelectric power generation.
The reliability of the primary energy source is an important factor when comparing wind and hydroelectric power. Wind power relies on the availability of wind, which can fluctuate in intensity and consistency. This variability introduces challenges in maintaining a stable power supply, as the generation of electricity is directly dependent on wind conditions. In contrast, hydroelectric power depends on water resources, which can be managed through reservoirs and dams. This allows for greater control and predictability in power generation, making hydroelectric power more reliable.
When considering environmental impact, wind power has certain advantages. Wind turbines produce clean energy and have minimal greenhouse gas emissions. They also have a smaller land use footprint compared to large-scale hydroelectric projects. However, wind turbines can have visual and noise impacts, and their installation may affect local bird populations. On the other hand, hydroelectric power, while also a clean energy source, can have significant environmental consequences. The construction of large dams and reservoirs can lead to the loss of natural habitats, alteration of river ecosystems, and displacement of communities.
Geographical suitability plays a crucial role in determining the feasibility of wind and hydroelectric power generation. Wind power requires consistent wind patterns to generate electricity efficiently. Coastal regions and areas with high wind speeds are well-suited for wind power installations. Countries like Denmark and Germany have successfully harnessed wind power due to their favorable geographical conditions. Hydroelectric power, on the other hand, relies on rivers and suitable topography. Countries with abundant water resources and mountainous terrain, such as Norway and Canada, have leveraged hydroelectric power as a significant energy source.
In conclusion, wind power and hydroelectric power have distinct advantages and disadvantages. Wind power depends on wind availability, has minimal environmental impact, and is suitable for areas with consistent wind patterns. Hydroelectric power, while more reliable, can have notable ecological and social consequences and requires suitable water resources and topography. Countries like Denmark and Germany have embraced wind power, while Norway and Canada have harnessed the potential of hydroelectric power. The choice between wind and hydroelectric power depends on various factors, including the specific geographical conditions and the trade-offs between reliability, environmental impact, and resource availability.
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What is the unit vector in the direction of the vector A = A = i (58, -50, -61) cm?
Your drone sits at the origin of your chosen coordinate system, (0, 0, 0) m. You fly it from there in the same direction as the direction of a vector (39, 17, −28) for a distance of 8 m, where it hovers. From there you make the drone go in the same direction as the direction of a vector (-15, 27, 69) for a distance of 6 m, where it again hovers. What are its coordinates now?
The drone's coordinates after the two flights are (27.6, 18.2, 31.2) m.
The unit vector in the direction of vector A is:
u = A / |A| = (58/115, -50/115, -61/115)
Your drone sits at the origin of your chosen coordinate system, (0, 0, 0) m. You fly it from there in the same direction as the direction of a vector (39, 17, −28) for a distance of 8 m, where it hovers. From there you make the drone go in the same direction as the direction of a vector (-15, 27, 69) for a distance of 6 m, where it again hovers. What are its coordinates now
The drone's coordinates after the first 8 m flight are:
(0 + 8 * 39/115, 0 + 8 * 17/115, 0 - 8 * 28/115) = (31.2, 1.4, -22.4) m
The drone's coordinates after the second 6 m flight are:
(31.2 + 6 * (-15)/115, 1.4 + 6 * 27/115, -22.4 + 6 * 69/115) = (27.6, 18.2, 31.2) m
Therefore, the drone's coordinates after the two flights are (27.6, 18.2, 31.2) m.
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Light that has a 600-nm wavelength is incident upon two narrow slits that are separated by 0.550 mm. An interference pattern from the slits is projected onto a screen that is 2.70 m away. What is the separation distance Dy on the screen of the first bright fringe from the central bright fringe? m D1 = What is the separation distance Daz on the screen of the second dark fringe from the central bright fringe? m Da =
The distance between the two slits is given by d = 0.550 mm = 0.00055 m Wavelength of light is given by λ = 600 nm = 6.0 x 10^-7 m The distance from the slits to the screen is given by L = 2.70 m.
To calculate the distance between two bright fringes (Dy), we use the formula: y = (mλL)/d Where m is the order of the fringe, λ is the wavelength of the light, L is the distance from the slits to the screen, and d is the distance between the slits.
y = (1 × 6.0 x 10^-7 × 2.70)/0.00055= 2.94 x 10^-3 m Dy = 2.94 x 10^-3 m The distance between the central maximum and the second minimum of the diffraction pattern is given by y = To calculate the distance between the first and second minimum (Daz), we use the formula:
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A 12kg hanging sculpture is suspended by a 95-cm-long, 6.0g steel wire. When the wind blows hard, the wire hums at its fundamental frequency. What is the frequency of the hum?
To calculate the frequency of the hum produced by the steel wire, we can use the formula for the fundamental frequency of a vibrating string.
The formula mentioned below:
f = (1 / (2L)) * sqrt(T / μ)
Where f is the frequency, L is the length of the string, T is the tension in the string, and μ is the linear mass density of the string.
First, we need to calculate the linear mass density of the steel wire. Linear mass density (μ) is defined as the mass per unit length. In this case, the wire has a mass of 6.0 grams and a length of 95 cm, so the linear mass density is:
μ = (mass / length) = (6.0 g / 95 cm)
Next, we need to calculate the tension in the wire. The tension is equal to the weight of the hanging sculpture, which is given as 12 kg. Therefore, the tension is:
T = weight = mass * gravity = (12 kg) * (9.8 m/s^2)
Substituting the values into the formula, we have:
f = (1 / (2 * 0.95 m)) * sqrt((12 kg * 9.8 m/s^2) / (6.0 g / 0.95 m))
Evaluating the expression, we find:
f ≈ 20.3 Hz
Therefore, the frequency of the hum produced by the steel wire is approximately 20.3 Hz.
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Problem 59. Extra Credit (10 pts) Find the voltage difference between two points that are a distance \( r_{1} \) and \( r_{2} \) from an infinitely) long a wire with constant charge/length \( \lambda
The voltage difference between two points at distances \( r_{1} \) and \( r_{2} \) from an infinitely long wire with a constant charge per unit length \( \lambda \) is given by \( V = \frac{{\lambda}}{{2\pi\epsilon_{0}}} \ln \left(\frac{{r_{2}}}{{r_{1}}}\right) \).
To calculate the voltage difference between two points at distances \( r_{1} \) and \( r_{2} \) from an infinitely long wire with a constant charge per unit length \( \lambda \), we can use the formula for the electric potential due to a line charge.
The formula for the voltage difference \( V \) is \( V = \frac{{\lambda}}{{4\pi\epsilon_{0}}} \ln \left(\frac{{r_{2}}}{{r_{1}}}\right) \), where \( \epsilon_{0} \) is the permittivity of free space.
In this case, however, we have a constant charge per unit length \( \lambda \) instead of a line charge density \( \rho \). To account for this, we need to divide \( \lambda \) by \( 2\pi \) to adjust the formula accordingly.
Therefore, the correct formula for the voltage difference is \( V = \frac{{\lambda}}{{2\pi\epsilon_{0}}} \ln \left(\frac{{r_{2}}}{{r_{1}}}\right) \).
This formula tells us that the voltage difference between two points is directly proportional to the natural logarithm of the ratio of the distances \( r_{2} \) and \( r_{1} \). As the distances increase, the voltage difference also increases logarithmically.
In conclusion, the voltage difference between two points at distances \( r_{1} \) and \( r_{2} \) from an infinitely long wire with a constant charge per unit length \( \lambda \) is given by the formula \( V = \frac{{\lambda}}{{2\pi\epsilon_{0}}} \ln \left(\frac{{r_{2}}}{{r_{1}}}\right) \).
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At a site where the Earth's magnetic field has a magnitude of 0.42 gauss (where 1 gauss = 1.00 X 104 T) and points to the north, 680 below the horizontal, a high-voltage pover line 153 m in length
carries a current or TEA.
Determine the magnitude and direction of the magnetic force exerted on this wire, if the orientation of the vire and hence the current is as follove
horizontally toward the south
The magnitude of the magnetic force is 3.99 TEA and its direction is upward.
Magnitude of Earth's magnetic field, |B|=0.42 G=0.42 × 10⁻⁴ T
Angle between direction of Earth's magnetic field and horizontal plane, θ = 680
Length of power line, l = 153 m
Current flowing through the power line, I = TEA
We know that the magnetic force (F) exerted on a current-carrying conductor placed in a magnetic field is given by the formula
F = BIl sinθ,where B is the magnitude of magnetic field, l is the length of the conductor, I is the current flowing through the conductor, θ is the angle between the direction of the magnetic field and the direction of the conductor, and sinθ is the sine of the angle between the magnetic field and the conductor. Here, F is perpendicular to both magnetic field and current direction.
So, magnitude of magnetic force exerted on the power line is given by:
F = BIl sinθ = (0.42 × 10⁻⁴ T) × TEA × 153 m × sin 680F = 3.99 TEA
Now, the direction of magnetic force can be determined using the right-hand rule. Hold your right hand such that the fingers point in the direction of the current and then curl your fingers toward the direction of the magnetic field. The thumb points in the direction of the magnetic force. Here, the current is flowing horizontally toward the south. So, the direction of magnetic force is upward, that is, perpendicular to both the direction of current and magnetic field.
So, the magnitude of the magnetic force is 3.99 TEA and its direction is upward.
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Suppose a truck with mass m = 2200 kg has a head-on collision with a subcompact car of mass m = 1100 kg a) At the collision, a truck exerts a force of 2 9 10 N on the subcompact car. If the absolute value of the acceleration experienced by the truck and the subcompact car is called as Atruck and Acar, respectively, then find the relationship between track and Gear b) At the time of a head-on collision, each vehicle has an initial speed of 15 m/s and they are moving in opposite directions (one in +x direction and the other in x direction). The two cars crash into each other and become entangled. What is the final velocity? c) What is the velocity change for the truck: What is the velocity change for the car:
The relationship between the acceleration of the truck and the car can be found using the equation F = ma, where F is the force, m is the mass, and a is the acceleration.
The final velocity of the entangled vehicles can be found using the conservation of momentum principle. The velocity change for each vehicle can be found by subtracting the final velocity from the initial velocity.
a) Using F = ma, we get the relationship Acar = 2Atruck. This means that the subcompact car experiences twice the acceleration of the truck during the collision.
b) Using conservation of momentum, we can find the final velocity of the entangled vehicles. The total momentum of the system before the collision is zero, since the vehicles are moving in opposite directions with equal speed. Therefore, the total momentum after the collision must also be zero. We can use this principle to find the final velocity, which is zero.
c) Using the equation v_f = v_i + at, where v_f is the final velocity, v_i is the initial velocity, a is the acceleration, and t is the time, we can find the velocity change for each vehicle.
The velocity change for the truck is -15 m/s, since it was moving in the opposite direction and came to a complete stop after the collision.
The velocity change for the car is +15 m/s, since it was also moving in the opposite direction and came to a complete stop after the collision.
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