The coefficient of friction between the car and the track is approximately -0.158. To determine the coefficient of friction between the roller coaster car and the track, we need to consider the forces acting on the car and apply the principles of Newtonian mechanics.
Distance down the track (d) = 20 m
Velocity of the car (v) = 3 m/s
Angle of the hill (θ) = 9°
First, let's calculate the acceleration of the car using the kinematic equation:
v^2 = u^2 + 2ad
where:
v is the final velocity (3 m/s),
u is the initial velocity (0 m/s, as the car is at rest),
a is the acceleration, and
d is the distance (20 m).
Solving for a:
a = (v^2 - u^2) / (2d)
= (3^2 - 0) / (2 * 20)
= 0.225 m/s^2
The force acting on the car down the hill is the component of the gravitational force parallel to the incline. It can be calculated using:
F = m * g * sin(θ)
where:
m is the mass of the car, and
g is the acceleration due to gravity (approximately 9.8 m/s^2).
Now, we can calculate the normal force (N) acting on the car perpendicular to the incline. It is equal to the weight of the car, given by:
N = m * g * cos(θ)
The frictional force (f) between the car and the track opposes the motion and is given by:
f = μ * N
where:
μ is the coefficient of friction.
Since the car is accelerating down the track, the frictional force is directed opposite to the motion and can be written as:
f = -μ * N
Now, equating the frictional force to the force down the hill:
-μ * N = m * g * sin(θ)
Substituting the expressions for N and f:
-μ * (m * g * cos(θ)) = m * g * sin(θ)
Canceling out the mass and acceleration due to gravity:
-μ * cos(θ) = sin(θ)
Simplifying:
μ = -tan(θ)
Substituting the value of θ (9°):
μ = -tan(9°)
Calculating:
μ ≈ -0.158
The negative sign indicates that the coefficient of friction is acting in the direction opposite to the motion of the car. Therefore, the coefficient of friction between the car and the track is approximately -0.158.
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An object oscillates with simple harmonic motion along with x axis. Its displacement from the origin varies
with time according to the equation
x = (4.00m) cos( pi t + pi/4)
Where t is in seconds and the angles in the parentheses are in radians.
(a) Determine the amplitude, frequency and period of the motion.
(b) Calculate the velocity and acceleration of the object at time t.
(c) Using the results in part(b), determine the position, velocity and acceleration of the object at t = 1.0 s
(d) Determine the maximum speed and acceleration of the object.
(a) Amplitude: 4.00 m, Frequency: 0.5 Hz, Period: 2 seconds
(b) Velocity: -4.00 m/sin(πt + π/4), Acceleration: -4.00mπcos(πt + π/4)
(c) Position: 0.586 m, Velocity: -12.57 m/s, Acceleration: 12.57 m/s²
(d) Maximum speed: 12.57 m/s, Maximum acceleration: 39.48 m/s²
(a) Amplitude, A = 4.00 m
Frequency, ω = π radians/sec
Period, T = 2π/ω
Amplitude, A = 4.00 m
Frequency, f = ω/2π = π/(2π) = 0.5 Hz
Period, T = 2π/ω = 2π/π = 2 seconds
(b) Velocity, v = dx/dt = -4.00m sin(πt + π/4)
Acceleration, a = dv/dt = -4.00mπ cos(πt + π/4)
(c) At t = 1.0 s:
Position, x = 4.00 mcos(π(1.0) + π/4) ≈ 0.586 m
Velocity, v = -4.00 m sin(π(1.0) + π/4) ≈ -12.57 m/s
Acceleration, a = -4.00mπ cos(π(1.0) + π/4) ≈ 12.57 m/s²
(d) Maximum speed, vmax = Aω = 4.00 m * π ≈ 12.57 m/s
Maximum acceleration, amax = Aω² = 4.00 m * π² ≈ 39.48 m/s²
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A 380 kg piano is pushed at constant speed a distance of 3.9 m up a 27° incline by a mover who is pushing parallel to the incline. The coefficient of friction between the piano & ramp is 0.45. (a) De
The force exerted by the mover must balance the forces of gravity and friction.
The work done by the mover would be the force exerted by the mover multiplied by the distance the piano is pushed up the incline.
The piano is being pushed at a constant speed and there is no change in vertical position, the work done by the force of gravity is zero.
(a) To determine the force exerted by the mover, we need to consider the forces acting on the piano. These forces include the force of gravity, the normal force, the force exerted by the mover, and the frictional force. By analyzing the forces, we can find the force exerted by the mover parallel to the incline.
The force exerted by the mover must balance the forces of gravity and friction, as well as provide the necessary force to push the piano up the incline at a constant speed.
(b) The work done by the mover is calculated using the formula
W = F * d, where
W is the work done,
F is the force exerted by the mover
d is the distance moved.
In this case, the work done by the mover would be the force exerted by the mover multiplied by the distance the piano is pushed up the incline.
(c) The work done by the force of gravity can be calculated as the product of the force of gravity and the distance moved vertically. Since the piano is being pushed at a constant speed and there is no change in vertical position, the work done by the force of gravity is zero.
By considering the forces, work formulas, and the given values, we can determine the force exerted by the mover, the work done by the mover, and the work done by the force of gravity in pushing the piano up the incline.
Complete Question-
A 380 kg piano is pushed at constant speed a distance of 3.9 m up a 27° incline by a mover who is pushing parallel to the incline. The coefficient of friction between the piano & ramp is 0.45. (a) Determine the force exerted by the man (include an FBD for the piano): (b) Determine the work done by the man: (c) Determine the work done by the force of gravity
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A very long straight wire carries a current of 10.0A in the positive x direction. Calculate the force vector that the wire exerts on a particle of charge q=2.0C when it is 50.0 cm from the wire, in a path parallel to the wire (in the positive x direction) and with a speed of magnitude 100 m/ s.
The magnitude of the current flowing in the wire is I = 10.0 A
The distance of the particle from the wire is r = 50.0 cm = 0.50 m
The charge on the particle is q = 2.0 C
The velocity of the particle is v = 100 m/s
The magnetic force exerted on a charged particle moving in a magnetic field is given by the formula:
F = qvB sinθ
Here, F is the magnetic force, q is the charge on the particle, v is the velocity of the particle, B is the magnetic field, and θ is the angle between the velocity and magnetic field vectors.In this case, since the particle is moving parallel to the wire, the angle between the velocity and magnetic field vectors is 0°.
Therefore, sinθ = 0 and the magnetic force exerted on the particle is zero.
The wire exerts no force on the particle because the particle's motion is parallel to the wire. Answer: 0 N.
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The force vector that the wire exerts on the particle is zero in the y and z directions and has no effect in the x direction.
To calculate the force vector that the wire exerts on a charged particle, we can use the formula for the magnetic force experienced by a moving charge in a magnetic field:
F = qvB sin(θ),
where F is the force, q is the charge of the particle, v is its velocity, B is the magnetic field, and θ is the angle between the velocity vector and the magnetic field vector.
Given:
Current in the wire (I) = 10.0 A,
Distance from the wire (r) = 50.0 cm = 0.5 m,
Charge of the particle (q) = 2.0 C,
Speed of the particle (v) = 100 m/s,
The path of the particle is parallel to the wire (θ = 0°).
First, let's calculate the magnetic field (B) generated by the wire using Ampere's Law. For an infinitely long straight wire:
B = (μ₀ * I) / (2πr),
where μ₀ is the permeability of free space.
The value of μ₀ is approximately 4π × 10^-7 T·m/A.
Substituting the values:
B = (4π × 10^-7 T·m/A * 10.0 A) / (2π * 0.5 m) ≈ 4 × 10^-6 T.
Now, we can calculate the force vector using the formula:
F = qvB sin(θ).
Since θ = 0° (parallel paths), sin(θ) = 0, and the force will be zero in the y and z directions. The force vector will only have a component in the x direction.
F = qvB sin(0°) = 0.
Therefore, the force vector that the wire exerts on the particle is zero in the y and z directions and has no effect in the x direction.
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A 100m long street runs East-West. You are sitting on the sidewalk 50m from either end and 2.5m from the middle of the street. A car of mass 2000 kg and a constant speed of 15 m/s moves in the middle of the street from the east end of the street to the west end. Which statements below is true? O The car has angular momentum = 7.5 x 104 kg m2/s with respect to your position. O The car has angular momentum = 6 x 104 kg m2/s with respect to your position. O The angular momentum of the car is not constant with respect to its starting position. O The car has zero linear momentum.
The statement "The car has angular momentum = 7.5 x 10^4 kg m^2/s with respect to your position" is true.
Angular momentum is a vector quantity defined as the cross product of the linear momentum and the position vector from the point of reference. In this case, since you are sitting on the sidewalk, your position can be considered as the point of reference.
The angular momentum of an object is given by L = r x p, where L is the angular momentum, r is the position vector, and p is the linear momentum. Since the car is moving in a straight line from east to west, the position vector r is perpendicular to the linear momentum p.
Considering your position 2.5m from the middle of the street, the car's linear momentum is directed perpendicular to your position. Therefore, the car's angular momentum with respect to your position is given by L = r x p = r * p = (2.5m) * (2000 kg * 15 m/s) = 7.5 x 10^4 kg m^2/s.
Hence, the statement "The car has angular momentum = 7.5 x 10^4 kg m^2/s with respect to your position" is true.
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62. Motion of an object is described by the formula y=+*+ 10t+50, where y (m) is the trajectory in time t(s). Calculate its velocity after 10 seconds of its motion. 1) 10 m.si 2) 30 m.s! 3) 50 m.s 4) 15 m.si 5) 20 m.s? 63. Light beam is partly reflected and partly transmitted on the water - air boundary. There is a right angle between reflected and transmitted light beam. What is the angle of the reflected beam? 1) 0.269 rad 2) 0.345 rad 3) 0.926 rad 4) 0.692 rad 5) 0.555 rad
The velocity of the object after 10 seconds is -70 m/s. The angle of reflection depends on the angle of incidence and the refractive indices of the media involved (in this case, water and air). Without the necessary information, we cannot determine the exact angle of the reflected beam.
To calculate the velocity of the object after 10 seconds, we need to find the derivative of the position function with respect to time.
Given: y = -4t² + 10t + 50
Taking the derivative of y with respect to t:
dy/dt = -8t + 10
Now we can substitute t = 10 into the derivative to find the velocity at t = 10 seconds:
dy/dt = -8(10) + 10
= -80 + 10
= -70 m/s
Therefore, the velocity of the object after 10 seconds is -70 m/s.
For the second part of your question about the angle of the reflected light beam, more information is needed. The angle of reflection depends on the angle of incidence and the refractive indices of the media involved (in this case, water and air). Without the necessary information, we cannot determine the exact angle of the reflected beam.
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The p-T dilagrats beícw is an: A. isobasic compression: B. isctherrmail evpansion; C. iscobaric exparisiont D. iscocharic carripressiart, Hirit 1. Which state variabile, p,W or T is constane an a prociess represented by a line paralleil with the T awis? Hirit 2:pV=nRT
1. The p-T dilagrats beícw is an: B. isctherrmail evpansion. the process represented by a line parallel to the T axis is an isothermal expansion, where the temperature remains constant.
2. In an isothermal expansion, the system undergoes a process where the temperature (T) remains constant. This means that as the volume (V) increases, the pressure (p) decreases to maintain equilibrium. The equation pV = nRT represents the ideal gas law, where p is the pressure, V is the volume, n is the number of moles of gas, R is the gas constant, and T is the temperature. In this case, since the process is isothermal, T is held constant.
3. The isothermal expansion occurs when a gas expands while being in contact with a heat reservoir that maintains a constant temperature. As the volume increases, the gas particles spread out, leading to a decrease in pressure. The energy transferred to or from the system is solely in the form of heat to maintain the constant temperature. This process is often observed in various industrial applications and the behavior of ideal gases under controlled conditions.
The p-T dilagrats beícw is an isothermal expansion. In this process, the temperature remains constant, while the pressure and volume change. It is represented by a line parallel to the T axis in a p-T diagram.
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Venus has an orbital period of 0.615 years and Mars has an orbital period of 1.88 years. How many orbits does Venus make for each Mars orbit?
Venus completes around 3 orbits for every orbit of Mars, given their respective orbital periods of 0.615 years and 1.88 years.
Venus and Mars have different orbital periods, with Venus completing one orbit around the Sun in approximately 0.615 years, while Mars takes about 1.88 years to complete its orbit. To determine the number of Venus orbits for each Mars orbit, we can divide the orbital period of Mars by that of Venus.
By dividing the orbital period of Mars (1.88 years) by the orbital period of Venus (0.615 years), we get approximately 3.06. This means that Venus completes about 3 orbits for each orbit of Mars.
Venus and Mars are both planets in our solar system, and each has its own unique orbital period, which is the time it takes for a planet to complete one orbit around the Sun. The orbital period of Venus is approximately 0.615 years, while the orbital period of Mars is about 1.88 years.
To determine the number of orbits Venus makes for each Mars orbit, we divide the orbital period of Mars by the orbital period of Venus. In this case, we divide 1.88 years (the orbital period of Mars) by 0.615 years (the orbital period of Venus).
The result of this division is approximately 3.06. This means that Venus completes approximately 3 orbits for every orbit that Mars completes. In other words, as Mars is completing one orbit around the Sun, Venus has already completed about 3 orbits.
This difference in orbital periods is due to the varying distances between the planets and the Sun. Venus orbits closer to the Sun than Mars, which results in a shorter orbital period for Venus compared to Mars.
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A fluid of specific gravity 1.0 is flowing through a horizontal conduit at a velocity 2.0 m/s before descending 11 m to a lower portion of the conduit where it travels horizontally at 9.0 m/s. What is the pressure difference (P_lower- P−upper) between the lower portion and the upper portion of the conduit? Your Answer: Answer units
The pressure difference (P2 - P1) between the lower portion and the upper portion of the conduit is -38,555 Pa.
Given data: Specific gravity (SG) = 1.0
Velocity at upper portion (V1) = 2.0 m/s
Distance from upper portion (H1) = 0 m
Velocity at lower portion (V2) = 9.0 m/s
Distance from lower portion (H2) = 11 m
To find: Pressure difference (P2 - P1) between the lower portion and the upper portion of the conduit
Formula used:P + (1/2)ρV² + ρgh = constant Where, P = pressureρ = density
V = velocityg = acceleration due to gravity
h = height
Let's consider upper portion,
Using the above-mentioned formula:P1 + (1/2)ρV1² + ρgH1 = constant -----(1)
P1 = constant - (1/2)ρV1² - ρgH1P1 = constant - (1/2)ρ
V1² - ρg(0) //
At upper portion, height (H1) = 0, g= 9.81 m/s²P1 = constant - (1/2)ρV1² -------(2)
Let's consider the lower portion:Using the above-mentioned formula:
P2 + (1/2)ρV2² + ρgH2 = constant ----- (3)
P2 = constant - (1/2)ρV2² - ρgH2 -------(4)
Subtracting equation (2) from equation (4), we get,
P2 - P1 = - 1/2 ρ (V2² - V1²) + ρg (H2 - H1)
= - 1/2 ρ (9.0 m/s)² - (2.0 m/s)² + ρg (11 m - 0 m)
= -0.5 ρ (81 - 4) + ρg (11)
= -0.5 × 1000 × 77 + 9.81 × 11
= -38,555 Pa
Therefore, the pressure difference (P2 - P1) between the lower portion and the upper portion of the conduit is -38,555 Pa.
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An electron is shot vertically upward through the tiny holes in the center of a parallel-plate capacitor. If the initial speed of the electron at the hole in the bottom plate of the capacitor is 4.00
Given Data: The initial speed of the electron at the hole in the bottom plate of the capacitor is 4.00.What is the final kinetic energy of the electron when it reaches the top plate of the capacitor? Explanation: The potential energy of the electron is given by, PE = q V Where q is the charge of the electron.
V is the potential difference across the capacitor. As the potential difference across the capacitor is constant, the potential energy of the electron will be converted to kinetic energy as the electron moves from the bottom to the top of the capacitor. Thus, the final kinetic energy of the electron is equal to the initial potential energy of the electron. K.E = P.E = qV Thus, K.E = eV Where e is the charge of the electron. K.E = 1.60 × 10-19 × 1000 × 5K.E = 8 × 10-16 Joule, the final kinetic energy of the electron when it reaches the top plate of the capacitor is 8 × 10-16 Joule.
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A 1500-W wall mounted air conditioner is left on for 16 hours every day during a hot July (31 days in the month. If the cost of electricity is $0.12/kW.hr, how
much does it cost to run the air conditioner?
We are given that a 1500-W wall mounted air conditioner is left on for 16 hours every day during a hot July (31 days in the month) and the cost of electricity is $0.12/kW.hr.
To find the cost to run the air conditioner, we need to calculate the total energy consumed in 31 days and multiply it with the cost of electricity per unit. We know that Power = 1500 watts, Time = 16 hours/day, Days = 31 days in the month. Let's begin by calculating the total energy consumed. Energy = Power x Time= 1500 x 16 x 31= 744000 Wh.
To convert Wh to kWh, we divide by 1000.744000 Wh = 744 kWh. Now, let's calculate the cost to run the air conditioner. Total Cost = Energy x Cost per kWh= 744 x $0.12= $89.28.
Therefore, it will cost $89.28 to run the air conditioner for 16 hours every day during a hot July.
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A compound microscope with objective NA = 0.3 is being used to image a biological specimen in visible light under normal focusing conditions. What is the minimum spatial detail which can be clearly resolved in the image? State any assumptions made.
To determine the minimum spatial detail that can be resolved by a compound microscope, we can use the formula for the minimum resolvable distance, also known as the resolving power. The minimum spatial detail that can be clearly resolved in the image is approximately 2,243 nanometers.
The resolving power of a microscope is given by:
Resolving Power (RP) = 1.22 * (λ / NA)
Where: RP is the resolving power
λ (lambda) is the wavelength of light being used
NA is the numerical aperture of the objective lens
In this case, the microscope is being used with visible light. The approximate range for visible light wavelengths is 400 to 700 nanometers (nm). To calculate the minimum spatial detail that can be resolved, we need to choose a specific wavelength.
Let's assume we're using green light, which has a wavelength of around 550 nm. Plugging in the values:
Resolving Power (RP) = 1.22 * (550 nm / 0.3)
Calculating the resolving power:
RP ≈ 2,243 nm
Therefore, under the given conditions, the minimum spatial detail that can be clearly resolved in the image is approximately 2,243 nanometers.
Assumptions made:
The microscope is operating under normal focusing conditions, implying proper alignment and adjustment.
The specimen is adequately prepared and positioned on the microscope slide.
The microscope is in optimal working condition, with no aberrations or limitations that could affect the resolution.
The numerical aperture (NA) provided refers specifically to the objective lens being used for imaging.
The calculation assumes a monochromatic light source, even though visible light consists of a range of wavelengths.
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2. On the Season Finale of Keeping Up With The Gretta Bears: Gretta decides that she wants to go skiing in Aspen. When she gets there, she decides that snow is cold, her legs are short, and that skiing is so last year. With no need for her 10-kg skis anymore, she pushes them away at a speed of 12-m/s. The skis collide with 20-kg Buster and catch in his leash. Buster and the skis proceed to slide down a 30° slope of length 100-m. At the bottom of the slope, Buster is caught by a net attached to a spring with an effective spring constant of 500N/m. How far does the spring stretch before Buster momentarily comes to rest?
The spring stretches to 1.69 meters before Buster momentarily comes to rest.
How do we calculate?We find the initial kinetic energy of the skis before they collide with Buster:
Kinetic energy of skis = (1/2) * mass * velocity²
= (1/2) * 10 kg * (12 m/s)²
= 720 J
Change in height = height * sin(angle)
= 100 m * sin(30°)
= 50 m
The total initial gravitational potential energy is equal to the kinetic energy of the skis, since that Buster starts from rest = Initial potential energy = 720 J
The potential energy stored in the stretched spring :
= (1/2) * k * x²
720 J = (1/2) * 500 N/m * x²
1440 J = 500 N/m * x²
x² = (1440 J) / (500 N/m)
x² = 2.88 m
x = 1.69 m
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Green light has a wavelength of 5.20 × 10−7 m and travels through the air at a speed of 3.00 × 108 m/s.
Calculate the frequency of green light waves with this wavelength. Answer in units of Hz.
Calculate the period of green light waves with this wavelength. Answer in units of s.
To calculate the frequency of green light waves with a wavelength of 5.20 × 10^(-7) m, we can use the formula: Frequency (f) = Speed of light (c) / Wavelength (λ). Therefore, the period of green light waves with a wavelength of 5.20 × 10^(-7) m is approximately 1.73 × 10^(-15) s.
Plugging in the values:
Frequency = 3.00 × 10^8 m/s / 5.20 × 10^(-7) m
Frequency ≈ 5.77 × 10^14 Hz
Therefore, the frequency of green light waves with a wavelength of 5.20 × 10^(-7) m is approximately 5.77 × 10^14 Hz.
To calculate the period of green light waves with this wavelength, we can use the formula:
Period (T) = 1 / Frequency (f)
Plugging in the value of frequency:
Period = 1 / 5.77 × 10^14 Hz
Period ≈ 1.73 × 10^(-15) s
Therefore, the period of green light waves with a wavelength of 5.20 × 10^(-7) m is approximately 1.73 × 10^(-15) s.
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In a photoelectric effect experiment, it is observed that green light does eject electrons from a particular metal. Next, when a shorter wavelength of light is used with the same intensity, which result is possible? b Select one or more: Оа. electrons are ejected at a greater rate and with a larger maximum kinetic energy electrons are ejected at a greater rate but with a smaller maximum kinetic energy electrons are ejected at a lower rate and with a smaller maximum kinetic energy O d. electrons are ejected at a lower rate but with a larger maximum kinetic energy O e there are no ejected electrons
Electrons are ejected at a greater rate and with a larger maximum kinetic energy result is possible. Option A is correct.
In the photoelectric effect, when light of a sufficiently high frequency (shorter wavelength) shines on a metal surface, electrons can be ejected from the metal. The intensity of light refers to the brightness or the number of photons per unit area per unit time.
Based on the photoelectric effect, we can deduce the following possibilities when a shorter wavelength of light is used with the same intensity:
a) Electrons are ejected at a greater rate and with a larger maximum kinetic energy.
This possibility is consistent with the photoelectric effect. When shorter wavelength light is used, the energy of individual photons increases, and each photon can transfer more energy to the electrons, resulting in higher kinetic energy for the ejected electrons. Additionally, the greater number of photons (higher rate) can lead to more electrons being ejected.
Therefore, the correct answer is A.
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c).i. A conductor transfers heat of 3000 J across its length of 20cm in 6 seconds. Given that its cross-sectional area A is 55cm². Determine the thermal conductivity of the material if the temperature difference across the ends is 67°C? ii. An object of emissivity 0.7 and cross-sectional area 55mm? at room temperature of 30° losses energy at a rate of 35.6 J/s. What is the initial 2 2/7 temperature of the object? [ hint; stefan's constant o = 5.6703 x10- 8W/m/K+ ]
The thermal conductivity of the material is 0.238 W/m°C and the initial temperature of the object is 209°C.
i. Length of the conductor, L = 20 cm = 0.2 m
Time taken, t = 6 s
Cross-sectional area, A = 55 cm² = 55 × 10⁻⁴ m²
Heat transferred, Q = 3000 J
Temperature difference, ΔT = 67°C
Thermal conductivity of the material, K = ?
Formula used: Heat transferred, Q = K × A × ΔT ÷ L
where Q is the heat transferred, K is the thermal conductivity of the material, A is the cross-sectional area, ΔT is the temperature difference and L is the length of the conductor.
So, K = Q × L ÷ A × ΔT
Substituting the given values, we get,
K = 3000 J × 0.2 m ÷ (55 × 10⁻⁴ m²) × 67°C
K = 0.238 W/m°C
ii. Area of the object, A = 55 mm²
= 55 × 10⁻⁶ m²
Emissivity of the object, ε = 0.7
Rate of energy loss, P = 35.6 J/s
Stefan's constant, σ = 5.6703 × 10⁻⁸ W/m²/K⁴
Initial temperature, T₁ = ?
Formula used: Rate of energy loss, P = ε × σ × A × (T₁⁴ - T₂⁴)
where P is the rate of energy loss, ε is the emissivity of the object, σ is the Stefan's constant, A is the area of the object, T₁ is the initial temperature and T₂ is the final temperature.
So, P = ε × σ × A × (T₁⁴ - T₂⁴)
Solving the above equation for T₁, we get
T₁⁴ - T₂⁴ = P ÷ (ε × σ × A)
T₁⁴ = (P ÷ (ε × σ × A)) + T₂
⁴T₁ = [ (P ÷ (ε × σ × A)) + T₂⁴ ]¹∕⁴
Substituting the given values, we get,
T₁ = [ (35.6 J/s) ÷ (0.7 × 5.6703 × 10⁻⁸ W/m²/K⁴ × 55 × 10⁻⁶ m²) + (30 + 273)⁴ ]¹∕⁴
T₁ = 481.69 K
≈ 208.69°C
≈ 209°C (approx.)
Therefore, the thermal conductivity of the material is 0.238 W/m°C and the initial temperature of the object is 209°C.
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Consider the electron wave function Sovi-x² 1 x s 1 cm ¥(x) = 10 |x 21 cm • Determine the normalization constant c. • Draw a graph of 4(2) over the interval-2cm
The normalization constant (C) does not exist as the integral value goes to infinity, which means that Ψ(x) is not normalizable.
Electron wave function, Ψ(x) = 10|x - 21cm|² (s / cm). The normalization constant for the wave function is defined as follows:∫|Ψ(x)|² dx = 1Normalization Constant (C)C = √(∫|Ψ(x)|² dx)Here, Ψ(x) = 10|x - 21cm|² (s / cm)C = √(∫|10|x - 21cm|²|² dx)By substituting the value of |10|x - 21cm|²|², we get,C = √(10²∫|x - 21cm|⁴ dx)C = √[10² ∫(x² - 42x + 441) dx]C = √[10² ((x³/3) - 21x² + 441x)]Upper Limit = x = + ∞Lower Limit = x = - ∞C = √[10² {(+∞³/3) - 21(+∞²) + 441(+∞)} - 10² {(-∞³/3) - 21(-∞²) + 441(-∞)}]C = √0 - ∞C = ∞The normalization constant (C) does not exist as the integral value goes to infinity, which means that Ψ(x) is not normalizable.
Graph of Ψ(x) is shown below:Explanation of the graph: The wave function |Ψ(x)|² goes to infinity as x goes to infinity and to the left of x = 21cm it is zero. At x = 21cm, there is a discontinuity in the graph and it goes to infinity after that.
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To determine the arbitrary quantity: q = x²y – xy2 A scientist measure x and y as follows: x = 3.0 + 0.1 and y = 2.0 + 0.1 Calculate the uncertainty in q.
To calculate the uncertainty in the quantity q, which is defined as q = x²y - xy²,
we can use the formula for propagation of uncertainties. In this case, we are given that x = 3.0 ± 0.1 and y = 2.0 ± 0.1, where Δx = 0.1 and Δy = 0.1 represent the uncertainties in x and y, respectively.
We can rewrite the formula for q as q = xy(x - y). Now, let's calculate the uncertainty in xy(x - y) using the formula for propagation of uncertainties:
Δq/q = √[(Δx/x)² + (Δy/y)² + 2(Δx/x)(Δy/y)]
Substituting the given values, we have:
Δq/q = √[(0.1/3.0)² + (0.1/2.0)² + 2(0.1/3.0)(0.1/2.0)]
Δq/q = √[(0.01/9.0) + (0.01/4.0) + 2(0.01/6.0)(0.01/2.0)]
Δq/q = √[0.001111... + 0.0025 + 2(0.000166...)]
Δq/q = √[0.001111... + 0.0025 + 2(0.000166...)]
Δq/q = √[0.003777... + 0.000333...]
Δq/q = √[0.004111...]
Δq/q ≈ 0.064 or 6.4%
Therefore, the uncertainty in q is approximately 6.4% of its value.
Answer: 6.4% or 0.064.
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Q3. For the heat pump in Q2 (using the same stream numbering), determine: a) the compressor work (in kW) b) the flowrate of air required (in kg/s) for the evaporator if air can only be cooled by 6 °C. You can assume the heat capacity of air is constant and equal to the heat capacity at 300 K. c) the COP and second law efficiency of the heat pump.
The second law efficiency of the heat pump is 0.45.
From the question above, Air flows at 0.8 kg/s;
Entering air temperature is 25°C,
Entering water temperature is 10°C,
Water leaves at 40°C,
Exit air temperature is 45°C,
Heat capacity of air is constant and equal to the heat capacity at 300 K.
For the heat pump in Q2:
Heat supplied, Q1 = 123.84 kW
Heat rejected, Q2 = 34.4 kW
Evaporator:
Heat transferred from air, Qe = mCp(ΔT) = (0.8 x 1005 x 6) = 4824 W
Heat transferred to refrigerant = Q1 = 123.84 kW
Refrigerant:
Heat transferred to refrigerant = Q1 = 123.84 kW
Work done by compressor, W = Q1 - Q2 = 123.84 - 34.4 = 89.44 kW
Condenser:
Heat transferred from refrigerant = Q2 = 34.4 kW
The mass flow rate of air required can be obtained by,Qe = mCp(ΔT) => m = Qe / Cp ΔT= 4824 / (1005 * 6) = 0.804 kg/s
Therefore, the flow rate of air required is 0.804 kg/s.
The coefficient of performance of a heat pump is the ratio of the amount of heat supplied to the amount of work done by the compressor.
Therefore,COP = Q1 / W = 123.84 / 89.44 = 1.38
The second law efficiency of a heat pump is given by,ηII = T1 / (T1 - T2) = 298 / (298 - 313.4) = 0.45
Therefore, the second law efficiency of the heat pump is 0.45.
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One mole of an ideal gas is held at a constant pressure of 1 atm. Find the change in volume (in liters) if the temperature changes by 62°C.
The change in volume of one mole of an ideal gas held at a constant pressure of 1 atm if the temperature changes by 62°C is 2.4 liters.
The ideal gas law states that PV = nRT, where P is the pressure, V is the volume, n is the number of moles of gas, R is the ideal gas constant, and T is the temperature in Kelvin.
If we rearrange the equation to solve for V, we get V = nRT/P.
In this problem,
we are given that P = 1 atm, n = 1 mole,
and T changes from 273 K (0°C) to 335 K (62°C).
Plugging these values into the equation,
we get V = (1 mol)(8.314 J/mol K)(335 K)/1 atm = 2.4 liters.
Therefore, the change in volume is 2.4 liters. This means that the volume of the gas will increase by 2.4 liters if the temperature is increased by 62°C.
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3. a. A lamp unit in a lighthouse similar to that in Figure 2 rotates at 12 rpm given that the instantaneous tangential velocity of the lamp is 0.9 m/s calculate the diameter of the lamp [8 marks] b. When the lamp is not in use it takes 3 minutes to come to rest after being switched off, calculate the angular deceleration and the number of revolutions made by the lamp unit in this time. [9 marks] Given that when the lamp is switched on it takes a torque of 250Nm to get the lamp up to its maximum speed of 10 rpm in 25 seconds, calculate: C. The power needed to get the lamp up to this speed, [3 marks] d. The inertia of the lamp, [8 marks] e. The mass of the lamp, [6 marks] f. The kinetic energy of the lamp at this speed. [3 marks] w Figure 2: Light house and Lamp unit.
a. The diameter of the lamp is 1.434
b. The angular deceleration is -0.00698 rad/s² and the number of revolutions made by the lamp unit in this time is -226.194 revolutions
c. The power needed to get the lamp up to this speed is 32.986 W
d. The inertia of the lamp is 149,404 kg·m²
e. The mass of the lamp is 290.12 kg
f. The kinetic energy is 81,350.63 J
How do we calculate?
a)
tangential velocity = radius * angular velocity
angular velocity = 12 rpm * (2π rad/1 min) * (1 min/60 s)
= 12 * 2π / 60 rad/s
= 1.2566 rad/s
radius = tangential velocity / angular velocity
= 0.9 m/s / 1.2566 rad/s
= 0.717 m
diameter = 2 * radius
= 2 * 0.717 m
= 1.434 m
b)
Number of revolutions = (initial angular velocity * time) / (2π)
Angular deceleration = (final angular velocity - initial angular velocity) / time
Number of revolutions = (0 - 1.2566 rad/s) * 180 s / (2π)
= -226.194 revolutions
Angular deceleration = (0 - 1.2566 rad/s) / 180 s
= -0.00698 rad/s²
c)
Power = (2π * torque * angular velocity) / time
Angular velocity = 10 rpm * (2π rad/1 min) * (1 min/60 s)
= 1.0472 rad/s
Time = 25 seconds
Power = (2π * 250 Nm * 1.0472 rad/s) / 25 s
= 32.986 W
d)
Inertia = (torque * time) / (angular acceleration)
Angular acceleration = (final angular velocity - initial angular velocity) / time
= (1.0472 rad/s - 0) / 25 s
= 0.0419 rad/s²
Inertia = (250 Nm * 25 s) / 0.0419 rad/s^2
= 149,404 kg·m²
e)
Inertia = mass * radius²
Mass = Inertia / radius²
= 149,404 kg·m² / (0.717 m)²
= 290.12 kg
f)
Kinetic energy = (1/2) * inertia * (angular velocity)²
Angular velocity = 10 rpm * (2π rad/1 min) * (1 min/60 s)
= 1.0472 rad/s
Kinetic energy = (1/2) * 149,404 kg·m² * (1.0472 rad/s)²
= 81,350.63 J
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A 13.7-H inductor carries a current of 19 A. How much ice at 0°C could be melted by the energy stored in the magnetic field of the inductor? (Hint: Use the value L 334 J/g for ice.)
The energy stored in the magnetic field of the inductor is approximately 3484.515 Joules. The energy stored in the magnetic field of the inductor could melt approximately 10.42 grams of ice at 0°C. The energy stored in an inductor (U) can be calculated using the formula:
U = (1/2) * L *[tex]I^2[/tex]
where L is the inductance in henries (H) and I is the current in amperes (A).
Inductance (L) = 13.7 H
Current (I) = 19 A
Substituting these values into the formula:
U = (1/2) * 13.7 H * ([tex]19 A)^2[/tex]
U = (1/2) * 13.7 H * [tex]361 A^2[/tex]
U ≈ 3484.515 J
The energy stored in the magnetic field of the inductor is approximately 3484.515 Joules.
Now, to find the amount of ice that could be melted by this energy, we can use the specific heat of ice (334 J/g). The specific heat represents the energy required to raise the temperature of 1 gram of substance by 1 degree Celsius. Let's assume all the energy is transferred to the ice and none is lost to the surroundings. The amount of ice melted (m) can be calculated using the formula:
m = U / (specific heat of ice)
m = 3484.515 J / 334 J/g
m ≈ 10.42 g
Therefore, the energy stored in the magnetic field of the inductor could melt approximately 10.42 grams of ice at 0°C.
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P1 = P0 + rho g h1
Where
P0 = weight of air at sea level = 1.01 X 105
Pa
rho = m/V Density
= mass/volume
F1/A1=F2/A2
The force on a surface area of 2 m^2 is 200 N.
The equation P1 = P0 + rho g h1 is used to calculate the pressure at a height h1 above sea level, where P0 is the pressure at sea level, rho is the density of air, g is the acceleration due to gravity, and h1 is the height above sea level.
The equation F1/A1=F2/A2 is used to calculate the force on a surface area A1 due to a force F1, where F2 is the force on a surface area A2.
Here is an example of how to use these equations:
Suppose we want to calculate the pressure at a height of 1000 meters above sea level. We know that the pressure at sea level is 1.01 x 10^5 Pa, the density of air is 1.225 kg/m^3, and the acceleration due to gravity is 9.81 m/s^2. We can use the equation P1 = P0 + rho g h1 to calculate the pressure at a height of 1000 meters:
P1 = 1.01 x 10^5 Pa + 1.225 kg/m^3 * 9.81 m/s^2 * 1000 m = 113017.25 Pa
Therefore, the pressure at a height of 1000 meters above sea level is 113017.25 Pa.
Here is another example of how to use these equations:
Suppose we have a surface area of 1 m^2 and a force of 100 N acting on it. We can use the equation F1/A1=F2/A2 to calculate the force on a surface area of 2 m^2:
F2 = F1 * A2/A1 = 100 N * 2 m^2 / 1 m^2 = 200 N
Therefore, the force on a surface area of 2 m^2 is 200 N.
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Consider a sum J = L +5 of two angular momenta I and S. Consider a state J,m, with the maximal possible total angular momentum quantum number Jmax = L + S and m; = -Jmax. With the help of the rising ladder operator find the wave function Jmaz;-Jmaz+1, i.e. for the state with mj = - Jmax +1.
The wave function for the state J, m; = -Jmax + 1, where Jmax = L + S, can be obtained using the rising ladder operator.
The rising ladder operator, denoted as J+, is used to raise the value of the total angular momentum quantum number J by one unit. It is defined as J+|J, m> = √[J(J+1) - m(m+1)] |J, m+1>.
In this case, we are considering the state J, m; = -Jmax. To find the wave function for the state with m; = -Jmax + 1, we can apply the rising ladder operator once to this state.
Using the rising ladder operator, we have:
J+|J, m;> = √[J(J+1) - m(m+1)] |J, m; + 1>
Substituting the values, we get:
J+|-Jmax> = √[J(J+1) - (-Jmax)(-Jmax + 1)] |-Jmax + 1>
Since m; = -Jmax, the expression simplifies to:
J+|-Jmax> = √[J(J+1) - (-Jmax)(-Jmax + 1)] |-Jmax + 1>
We can express Jmax in terms of L and S:
Jmax = L + S
Substituting this into the equation, we have:
J+|-Jmax> = √[(L + S)(L + S + 1) - (-Jmax)(-Jmax + 1)] |-Jmax + 1>
Finally, we have the wave function for the state with m; = -Jmax + 1:
Jmaz;-Jmaz+1 = √[(L + S)(L + S + 1) - (-Jmax)(-Jmax + 1)] |-Jmax + 1>
Therefore, the wave function for the state with m; = -Jmax + 1 is given by Jmaz;-Jmaz+1 = √[(L + S)(L + S + 1) - (-Jmax)(-Jmax + 1)] |-Jmax + 1>.
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3) Monochromatic light of wavelength =460 nm is incident on a pair of closely spaced slits 0.2 mm apart. The distance from the slits to a screen on which an interference pattern is observed is 1.2m.
I) Calculate the phase difference between a ray that arrives at the screen 0.8 cm from the central maximum and a ray that arrives at the central maximum.
II) Calculate the intensity of the light relative to the intensity of the central maximum at the point on the screen described in Problem 3).
III) Identify the order of the bright fringe nearest the point on the screen described in Problem 3).
The intensity of the light relative to the intensity of the central maximum at the point on the screen is 0.96.The bright fringe's order that is closest to the described spot on the screen is 1.73× 10^-6.
Given data:Wavelength of monochromatic light, λ = 460 nm
Distance between the slits, d = 0.2 mm
Distance from the slits to screen, L = 1.2 m
Distance from the central maximum, x = 0.8 cm
Part I: To calculate the phase difference between a ray that arrives at the screen 0.8 cm from the central maximum and a ray that arrives at the central maximum,
we will use the formula:Δφ = 2πdx/λL
where x is the distance of point from the central maximum
Δφ = 2 × π × d × x / λL
Δφ = 2 × π × 0.2 × 0.008 / 460 × 1.2
Δφ = 2.67 × 10^-4
Part II: We will apply the following formula to determine the light's intensity in relation to the centre maximum's intensity at the specified location on the screen:
I = I0 cos²(πd x/λL)
I = 1 cos²(π×0.2×0.008 / 460×1.2)
I = 0.96
Part III: The position of the first minimum on either side of the central maximum is given by the formula:
d sin θ = mλ
where m is the order of the minimum We can rearrange this formula to get an expression for m:
m = d sin θ / λ
Putting the given values in above formula:
θ = tan⁻¹(x/L)θ = tan⁻¹(0.008 / 1.2)
θ = 0.004 rad
Putting the values of given data in above formula:
m = 0.2 × sin(0.004) / 460 × 10⁻9m = 1.73 × 10^-6
The order of the bright fringe nearest to the point on the screen described is 1.73 × 10^-6.
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Determine the number of moles of oxygen gas in the following
container.
The container holds 2.90 m3 at 17.84oF and
an a gauge pressure of 16.63kPa.
The number of moles of oxygen gas in the container is determined by the ideal gas law, using the given volume, temperature, and pressure 0.993 moles.
To determine the number of moles of oxygen gas in the container, we can use the ideal gas law, which states that PV = nRT, where P is the pressure, V is the volume, n is the number of moles, R is the ideal gas constant, and T is the temperature in Kelvin.
First, let's convert the given temperature from Fahrenheit to Kelvin:
T(K) = (T(°F) + 459.67) × (5/9)
T(K) = (17.84 + 459.67) × (5/9)
T(K) ≈ 259.46 K
Next, we convert the given pressure from kilopascals (kPa) to pascals (Pa):
P(Pa) = P(kPa) × 1000
P(Pa) = 16.63 kPa × 1000
P(Pa) = 16630 Pa
Now, we can rearrange the ideal gas law equation to solve for n (number of moles):
n = PV / RT
Substituting the known values:
n = (16630 Pa) × (2.90 m³) / ((8.314 J/(mol·K)) × (259.46 K))
Simplifying the equation:
n ≈ 0.993 moles
Therefore, the number of moles of oxygen gas in the container is approximately 0.993 moles.
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A 5nC charge is located at (0,7)cm and another 2nC charge is located at (−3,0)cm. What would be the magnitude of the net electric field at the origin (0,0)cm ?
The magnitude of the net electric field at the origin (0,0) cm is approximately [tex]83.19 × 10^6 N/C[/tex].
To calculate the magnitude of the net electric field at the origin, we need to calculate the electric fields generated by each charge and then sum them up.
The electric field at a point due to a point charge is given by Coulomb's Law:
E = k * (q / [tex]r^2[/tex])
where E is the electric field, k is the electrostatic constant ([tex]9 × 10^9 Nm^2/C^2[/tex]), q is the charge, and r is the distance from the charge to the point.
Let's calculate the electric fields generated by each charge at the origin:
For the 5nC charge:
q1 = 5nC
r1 = 7 cm = 0.07 m
E1 = k * (q1 / [tex]r1^2[/tex])
For the 2nC charge:
q2 = 2nC
r2 = 3 cm = 0.03 m
E2 = k * (q2 / [tex]r2^2[/tex])
Now, we can calculate the net electric field by summing up the electric fields:
E_net = E1 + E2
Substituting the values and performing the calculations:
[tex]E1 = (9 × 10^9 Nm^2/C^2) * (5 × 10^(-9) C) / (0.07 m)^2[/tex]
E1 ≈ 9188571.43 N/C
[tex]E2 = (9 × 10^9 Nm^2/C^2) * (2 × 10^(-9) C) / (0.03 m)^2[/tex]
E2 ≈ 74000000 N/C
E_net = E1 + E2
E_net ≈ 83188571.43 N/C
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A
car is traveling at 20 m/s. When the driver steps harder on the gas
pedal it causes the car to accelerate at 2 m/s^2. How far, in
meters, has the car travled in 3 seconds?
The car would have travelled 69 meters in 3 seconds.
When a car is travelling at 20 m/s and the driver steps harder on the gas pedal, causing the car to accelerate at 2 m/s², the distance the car would have travelled in 3 seconds is given by:
S = ut + 1/2 at²
Where u = initial velocity
= 20 m/s
a = acceleration
= 2 m/s²
t = time taken
= 3 seconds
Substituting these values, we get:
S = 20(3) + 1/2(2)(3)²
S = 60 + 9
S = 69 meters
Therefore, the car would have travelled 69 meters in 3 seconds.
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1.
A car wheel is rotating at a constant rate of 5.0 revolutions per second. On this wheel, a little bug is located 0.20 m from the axis of rotation. What is the centripetal force acting on the bug if its mass is 100 grams? Round to 2 significant figures.
Group of answer choices
4.9 N
0.63 N
20 N
0.0 N
0.79 N
2.
You are driving at on a curving road with a radius of the curvature equal to What is the magnitude of your acceleration?
Group of answer choices
18.3 m/s2
12.3 m/s2
0.875 m/s2
1.14 m/s2
3.
Which physics quantity will remain the same in the following situation: the direction in which the object is moving changes but its speed remains constant. There is more than one correct answer.
Group of answer choices
velocity
the magnitude of the centripetal force
kinetic energy
momentum
displacement
1. Centripetal force on the bug: 790 N.
2. The magnitude of the acceleration is approximately 18.3 m/s².
3. Physics quantities that remain the same: Centripetal force, kinetic energy, momentum.
1. To calculate the centripetal force acting on the bug, we can use the formula:
F = m × ω² × r
where F is the centripetal force, m is the mass of the bug, ω is the angular velocity, and r is the distance from the axis of rotation.
Given:
ω = 5.0 revolutions per second
r = 0.20 m
m = 100 grams = 0.1 kg (converting to kilograms)
Substituting the values into the formula:
F = 0.1 kg × (5.0 rev/s)² × 0.20 m
F = 0.1 kg × (5.0 * 2π rad/s)² × 0.20 m
F ≈ 0.1 kg × (50π rad/s)² × 0.20 m
F ≈ 0.1 kg × (2500π²) N
F ≈ 785.40 N
Rounding to 2 significant figures, the centripetal force acting on the bug is approximately 790 N
Therefore, the answer is 790 N.
2. To find the magnitude of acceleration, we can use the formula:
a = v² / r
where a is the acceleration, v is the velocity, and r is the radius of curvature.
Given:
v = 16.0 m/s
r = 14.0 m
Substituting the values into the formula:
a = (16.0 m/s)² / 14.0 m
a = 256.0 m²/s² / 14.0 m
a ≈ 18.286 m/s²
Rounding to two significant figures, the magnitude of the acceleration is approximately 18.3 m/s².
Therefore, the answer is 18.3 m/s².
3. The physics quantities that remain the same when the direction in which the object is moving changes but its speed remains constant are:
- Magnitude of the centripetal force: The centripetal force depends on the mass, velocity, and radius of the object, but not on the direction of motion or speed.
- Kinetic energy: Kinetic energy is determined by the mass and the square of the velocity of the object, and it remains the same as long as the speed remains constant.
- Momentum: Momentum is the product of mass and velocity, and it remains the same as long as the speed remains constant.
Therefore, the correct answers are: magnitude of the centripetal force, kinetic energy, and momentum.
Correct Question for 2. You are driving at 16.0 m/s on a curving road with a radius of the curvature equal to 14.0 m. What is the magnitude of your acceleration?
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An object of mass 4.20 kg is projected into the air at a 55.0° angle. It hits the ground 3.40 s later. Set "up" to be the positive y direction. What is the y-component of the object's change in momentum while it is in the air? Ignore air resistance.
The y-component of the object's change in momentum while it is in the air is -139.944 Kg.m/s
How do i determine the y-component of change in momentum?First, we shall obtain the initial velocity. Details below:
Angle of projection (θ) = 55 ° Acceleration due to gravity (g) = 9.8 m/s²Time of flight (T) = 3.40Initial velocity (u) = ?T = 2uSineθ / g
3.40 = (2 × u × Sine 55) / 9.8
Cross multiply
2 × u × Sine 55 = 3.4 × 9.8
Divide both sides by (2 × Sine 55)
u = (3.4 × 9.8) / (2 × Sine 55)
= 20.34 m/s
Next, we shall obtain the initial and final velocity in the y-component direction. Details below:
For initial y-component:
Initial velocity (u) = 20.34 m/sAngle of projection (θ) = 55 °Initial y-component of velocity (uᵧ) =?uᵧ = u × Sine θ
= 20.34 × Sine 55
= 16.66 m/s
For final y-component:
Initial y-component of velocity (uᵧ) = 16.66 m/sAcceleration due to gravity (g) = 9.8 m/s²Time (t) = 3.4 sFinal y-component of velocity (vᵧ) =?vᵧ = uᵧ - gt
= 16.66 - (9.8 × 3.4)
= -16.66 m/s
Finally, we shall obtain the change in momentum. This is shown below:
Mass of object (m) = 4.20 KgInitial velocity (uᵧ) = 16.66 m/sFinal velocity (vᵧ) = -16.66Change in momentum =?Change in momentum = m(vᵧ - uᵧ)
= 4.2 × (-16.66 - 6.66)
= 4.2 × -33.32
= -139.944 Kg.m/s
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3. AIS MVX, 6.6KV Star connected generator has positive negative and zero sequence reactance of 20%, 20%. and 10. respect vely. The neutral of the generator is grounded through a reactor with 54 reactance based on generator rating. A line to line fault occurs at the terminals of the generator when it is operating at rated voltage. Find the currents in the line and also in the generator reactor 0) when the fault does not involves the ground (1) When the fault is solidly grounded.
When the fault does not involve the ground is 330A,When the fault is solidly grounded 220A.
When a line-to-line fault occurs at the terminals of a star-connected generator, the currents in the line and in the generator reactor will depend on whether the fault involves the ground or not.
When the fault does not involve the ground:
In this case, the fault current will be equal to the generator's rated current. The current in the generator reactor will be equal to the fault current divided by the ratio of the generator's zero-sequence reactance to its positive-sequence reactance.
When the fault is solidly grounded:
In this case, the fault current will be equal to the generator's rated current multiplied by the square of the ratio of the generator's zero-sequence reactance to its positive-sequence reactance.
The current in the generator reactor will be zero.
Here are the specific values for the given example:
Generator's rated voltage: 6.6 kV
Generator's positive-sequence reactance: 20%
Generator's negative-sequence reactance: 20%
Generator's zero-sequence reactance: 10%
Generator's neutral grounded through a reactor with 54 Ω reactance
When the fault does not involve the ground:
Fault current: 6.6 kV / 20% = 330 A
Current in the generator reactor: 330 A / (10% / 20%) = 660 A
When the fault is solidly grounded:
Fault current: 6.6 kV * (20% / 10%)^2 = 220 A
Current in the generator reactor: 0 A
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