Answer and Explanation:
This experiment is known as Lenz's tube.
The Lenz tube is an experiment that shows how you can brake a magnetic dipole that goes down a tube that conducts electric current. The magnet, when falling, along with its magnetic field, will generate variations in the magnetic field flux within the tube. These variations create an emf induced according to Faraday's Law:
[tex]\varepsilon =-\frac{d\phi_B}{dt}[/tex]
This emf induced on the surface of the tube generates a current within it according to Ohm's Law:
[tex]V=IR[/tex]
This emf and current oppose the flux change, therefore a field will be produced in such a direction that the magnet is repelled from below and is attracted from above. The magnitude of the flux at the bottom of the magnet increases from the point of view of the tube, and at the top it decreases. Therefore, two "magnets" are generated under and above the dipole, which repel it below and attract above. Finally, the dipole feels a force in the opposite direction to the direction of fall, therefore it falls with less speed.
Answer:
Check below for the answer and explanation
Explanation:
According to Faraday's law of electromagnetic induction, if a conductor is exposed to changing magnetic flux, an emf and hence a current is induced in the conductor. The strength of the induced emf is directly proportional to the rate of change of the magnetic flux.
Induced emf, [tex]e =-N\frac{d \phi}{dt}[/tex]
Induced current, I = e/R
In this example, as magnet is dropped down the aluminium pipe, the magnetic flux changes, and current is induced in the pipe.
According to Lenz's law, the direction of the induced current in the conductor opposes the direction of the magnetic flux that produces it.
Based on these stated laws, current is induced in this aluminium pipe and the direction of this induced current opposes the magnetic flux change. The magnetic field is repelled and falls slowly.
A spaceship is traveling toward the earth from the space colony on Asteroid 1040A. The ship is at the halfway point of the trip, passing Mars at a speed of 0.9c relative to the Mars frame of reference. At the same instant, a passenger on the spaceship receives a radio message from her boyfriend on 1040A and another from her sister on earth. According to the passenger on the ship, were these messages sent simultaneously or at different times? If at different times, which one was sent first? Explain your reason
Answer:
The message (signal) coming from the earth was sent first.
Explanation:
The radio messages reach Mars simultaneously, because the distance from Earth to Mars and that of from Mars to Asteroid is same. But the passenger in the spaceship is moving relative to Mars towards Earth and hence, the message from Earth reaches first.
According to passenger frame, the message (signal) coming from the Earth was sent first compared to message coming from Asteroid.
An insulated piston–cylinder device contains 0.05 m3 of saturated refrigerant- 134a vapor at 0.8-MPa pressure. The refrigerant is now allowed to expand in a reversible manner until the pressure drops to 0.4 MPa. Determine (a) the final temperature in the cylinder and (b) the work done by the refrigerant
The final temperature of the refrigerant in the piston-cylinder device can be determined via lookup and interpolation from standard tables, based on the final pressure of 0.4 MPa. The work done by the refrigerant as it expands and drops in pressure can be calculated via the first law of thermodynamics, specifically accounting for changes in internal energy as work done by the system.
Explanation:This is an example of a reversible adiabatic expansion process involving a refrigerant (refrigerant-134a) in a piston-cylinder device. The process follows the behavior of ideal gases, and so we can make use of the first law of thermodynamics and other gas laws to determine the final temperature and the work done by the refrigerant.
To find the final temperature, we incorporate the specifics of the refrigerant-134a, which is defined by specific tables found in thermodynamics textbooks, providing details of temperature at various pressures. Interpolation between table values may be necessary to find the exact temperature at 0.4 MPa. Generally, the temperature will fall as the refrigerant expands and the pressure lowers, as defined by the ideal gas law (pV=nRT).
For the work done by the refrigerant, we'd need to apply the first law of thermodynamics, which in this case can be simplified as ΔU = W because there's no heat transfer in an adiabatic process (dQ=0). Changes in the internal energy of the gas would translate directly into work done on the piston. We calculate work using the formula -P(ΔV), where the negative sign indicates work being done by the system.
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(a) The final temperature in the cylinder is approximately 18.0°C.
(b) The work done by the refrigerant during the expansion is approximately 7.72 kJ.
To solve this problem, we need to determine two things: the final temperature of the refrigerant-134a vapor and the work done by the refrigerant during the expansion.
Given that the process is reversible and the system is insulated, this suggests that the expansion process is isothermal for an ideal gas, but since refrigerant-134a is not an ideal gas, we will use the refrigerant tables to find the properties.
Given Data:
Initial volume [tex]\( V_1 \)[/tex] : 0.05 m³Initial pressure [tex]\( P_1 \)[/tex] : 0.8 MPaFinal pressure [tex]\( P_2 \)[/tex] : 0.4 MPaThe process is reversibleStep-by-Step Solution:
(a) Determine the Final Temperature in the Cylinder:
1. Find the Initial and Final States Using Refrigerant-134a Tables:
Initial State [tex](P1 = 0.8 MPa)[/tex]:Look up the refrigerant-134a property tables for [tex]\( P = 0.8 \)[/tex] MPa.
At [tex]\( P = 0.8 \)[/tex] MPa, the refrigerant-134a is in the saturated vapor region. The saturated temperature and properties at this pressure are:
Saturated temperature [tex]\( T_1 \): \( T_{\text{sat}}(0.8 \text{ MPa}) \approx 26.7^\circ \text{C} \)[/tex]Specific volume [tex]\( v_g \): \( v_{\text{g}}(0.8 \text{ MPa}) \approx 0.0769 \text{ m}^3/\text{kg} \)[/tex]Final State [tex](P2 = 0.4 MPa)[/tex] :Similarly, look up the refrigerant-134a property tables for [tex]\( P = 0.4 \)[/tex] MPa.
At [tex]\( P = 0.4 \)[/tex] MPa, the refrigerant-134a is also in the saturated vapor region. The properties at this pressure are:
Saturated temperature [tex]\( T_2 \)[/tex] : [tex]\( T_{\text{sat}}(0.4 \text{ MPa}) \approx 18.0^\circ \text{C} \)[/tex]Specific volume [tex]\( v_g \)[/tex] : [tex]\( v_{\text{g}}(0.4 \text{ MPa}) \approx 0.0917 \text{ m}^3/\text{kg} \)[/tex]The final temperature of the refrigerant-134a after the expansion, which is at 0.4 MPa, is approximately [tex]\( 18.0^\circ \text{C} \)[/tex].
(b) Determine the Work Done by the Refrigerant:
1. Calculate the Initial and Final Mass:
Using the specific volume [tex]\( v_g \)[/tex] to find the mass:
[tex]\[ m = \frac{V_1}{v_g (P_1)} \][/tex]
For [tex]\( P_1 = 0.8 \)[/tex] MPa:
[tex]\[ m = \frac{0.05 \text{ m}^3}{0.0769 \text{ m}^3/\text{kg}} \approx 0.650 \text{ kg} \][/tex]
For [tex]\( P_2 = 0.4 \)[/tex] MPa, verify if the mass is the same (which it is for an ideal gas in a closed system):
[tex]\[ V_2 = m \times v_g (P_2) = 0.650 \text{ kg} \times 0.0917 \text{ m}^3/\text{kg} \approx 0.0597 \text{ m}^3 \][/tex]
The new volume [tex]\( V_2 \)[/tex] can be verified as:
[tex]\[ V_2 = \text{initial volume} \times \frac{v_g (P_2)}{v_g (P_1)} \][/tex]
Which confirms our calculation.
2. Calculate the Work Done During Expansion:
For a reversible expansion in an insulated system (isoenthalpic process), the work done \( W \) can be approximated using:
[tex]\[ W = \int_{V_1}^{V_2} P \, dV \][/tex]
The work done for an ideal gas (but approximate here for refrigerants) can be simplified using:
[tex]\[ W = \text{P}_1 \times V_1 \ln \left( \frac{V_2}{V_1} \right) \][/tex]
For refrigerants, use specific volume:
[tex]\[ W = \text{P}_1 \times V_1 \left[ \frac{v_g (P_2)}{v_g (P_1)} - 1 \right] \][/tex]
Substituting:
[tex]\[ W = 0.8 \text{ MPa} \times 0.05 \text{ m}^3 \left( \frac{0.0917}{0.0769} - 1 \right) \][/tex]
[tex]\[ W = 0.8 \times 10^3 \text{ Pa} \times 0.05 \text{ m}^3 \left( 1.193 - 1 \right) \][/tex]
[tex]\[ W = 40 \text{ kJ} \times 0.193 \approx 7.72 \text{ kJ} \][/tex]
Choose the correct statement regarding a compound microscope being used to look at a mite. The eyepiece lens forms a virtual image of the mite. If the focal distance of the objective lens is shortened, then its magnification decreases. The converging objective lens forms a virtual image of the mite. If the focal distance of the objective lens is lengthened, then its magnification increases. The image formed by the objective lens should be located just inside the focal point of the eyepiece lens
Answer:
a) True. The image of the mite is virtual
e) True. The image must be within the focal length of the eyepiece len
Explanation:
Let's review the general characteristics of compound microscopes
Formed by two converging lenses
Magnification is
M = -L/fo 0.25/fe
Where fo is the focal length of the objective lens and fe is the focal length of the ocular lens, L is the tube length
Let's review the claims
a) True. The image of the mite is virtual
b) False. The effect is the opposite of the magnification equation
c) False. The objective lens forms a real image
d) False. As the seal distance increases the magnification decreases
e) True. The image must be within the focal length of the eyepiece len
A compound microscope uses an objective lens to create a real, inverted image larger than the object, and an eyepiece (ocular) to magnify this image further into a virtual image. The correct statements include that the eyepiece forms a virtual image, and the image from the objective lens should be within the eyepiece's focal length for further magnification.
Explanation:To understand how a compound microscope works, we analyze the function of its two lenses: the objective lens and the eyepiece. Initially, an object just beyond the objective lens's focal length (fobj) creates a real, inverted image that is larger than the object. This initial image acts as the object for the eyepiece lens, or ocular, which is placed within its own focal length (feye) to further magnify the image, effectively functioning as a magnifying glass. The resulting image is a virtual, larger, and further magnified version of the initial image, making it more comfortable for viewing as the eye is relaxed when looking at distant objects.
If we consider the statements provided, the correct statements are as follows:
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After watching a news story about a fire in a high rise apartment building, you and friend decide to design an emergency escape device from the top of a building. To avoid engine failure, your friend suggest a gravitational powered elevator. The design has a large, heavy turntable (a horizontal disk that is free to rotate about its center) on teh roof with a cable wound around its edge. The free end of the cable goes horizontally to the edge of the building roof, pases over a heavy vertical pulley, and then hangs straight down. A strong wire cage which can hold 5 people is then attached to the hanging end of the cable. When people enter the cage adn release it, the cable unrolls from the turntable lowering the people as safely to the ground. to see if the design is feasible you decide to calculate the acceleration of the fully loaded elevator to make sure it is much less than g. Your friend design has the radius of the turntable disk as 1.5 m and its mass as 2x that of the fully loaded elevator. The disk which serves as the vertical pulley has 1/4 the radius of the turntable and 1/16 its mass. In your physics book you find that the moment of inertia if a disk is 1/2 that of a ring.
Answer:
You have been hired as part of a research team consisting of ... Torque: After watching a news story about a fire in a high rise apartment building, you and your friend decide to design an emergency escape device from the top ... To avoid engine failure, your friend suggests a gravitational powered elevator.
Explanation:
Say you want to make a sling by swinging a mass M of 1.7 kg in a horizontal circle of radius 0.048 m, using a string of length 0.048 m. You wish the mass to have a kinetic energy of 14.0 Joules when released. How strong will the string need to be
Answer:
Tension in the string is equal to 58.33 N ( this will be the strength of the string )
Explanation:
We have given mass m = 1.7 kg
radius of the circle r = 0.48 m[tex]F=\frac{mv^2}{r}=\frac{1.7\times 4.05^2}{0.48}=58.33N[/tex]
Kinetic energy is given 14 J
Kinetic energy is equal to [tex]KE=\frac{1}{2}mv^2[/tex]
So [tex]\frac{1}{2}\times 1.7\times v^2=14[/tex]
[tex]v^2=16.47[/tex]
v = 4.05 m/sec
Centripetal force is equal to [tex]F=\frac{mv^2}{r}=\frac{1.7\times 4.05^2}{0.48}=58.33N[/tex]
So tension in the string will be equal to 58.33 N ( this will be the strength of the string )
Final answer:
The problem requires finding the tension in the string by using the given kinetic energy to calculate the velocity and then applying the centripetal force formula to find the required string strength.
Explanation:
The student question involves calculating the tension in a string when a mass is swung to obtain a certain kinetic energy. Considering the mass M has a kinetic energy of 14.0 Joules, we can use the relation for kinetic energy (KE) of a rotating body, which is KE = 1/2 m v^2, where 'm' is the mass and 'v' is the tangential velocity. From the given kinetic energy and mass, we can solve for v.
Once we have the velocity, we can use centripetal force formula, which is F = m v^2 / r, where 'm' is the mass, 'v' is the velocity, and 'r' is the radius. This formula will allow us to find the required strength of the string, which, in physics, is essentially the tension that the string must be able to withstand without breaking.
Note that the tension in the string will be equal to the centripetal force at the point of release when the mass is in horizontal circular motion.
A 20 kg box on a horizontal frictionless surface is moving to the right at a speed of 4.0 m/s. The box hits and remains attached to one end of a spring of negligible mass whose other end is attached to a wall. As a result, the spring compresses a maximum distance of 0.50 m, and the box then oscillates back and forth. (a) i. The spring does work on the box from the moment the box first hits the spring to the moment the spring first reaches its maximum compression. Indicate whether the work done by the spring is positive, negative, or zero. ____ Positive ____ Negative ____ Zero
Answer:
Work done by the spring is negative
Explanation:
We can answer this question by thinking what is the force acting on the box.
In fact, the force acting on the box is the restoring force of the spring, which is given by Hooke's Law:
[tex]F=-kx[/tex]
where
k is the spring constant
x is the displacement of the box with respect to the equilibrium position of the spring
The negative sign in the equation indicates that the direction of the force is always opposite to the direction of the displacement: so, whether the spring is compressed or stretched, the force applied by the spring on the box is towards the equilibrium position.
The work done by the restoring force is also given by
[tex]W=Fx cos \theta[/tex]
where
F is the restoring force
x is the displacement
[tex]\theta[/tex] is the angle between the direction of the force and the displacement
Here we know that the force is always opposite to the displacement, so
[tex]\theta=180^{\circ} \rightarrow cos \theta =-1[/tex]
Which means that the work done by the spring is always negative, since the direction of the restoring force is always opposite to the direction of motion.
The work done by the spring on the box as it compresses is negative, due to the force applied by the spring being in the opposite direction of the box's displacement.
Explanation:For the given problem, the work done by the spring on the box is negative. This is because the spring is exerting a force in the opposite direction to that of the box's motion, leading to a decrease in the kinetic energy of the box. According to the work-energy principle, if the force applied by the spring opposes the direction of motion, the work done is negative. When the spring compresses, it stores elastic potential energy, which is a conversion of the box's kinetic energy. The spring force acts to the left (assuming the right is the positive direction), while the displacement of the box due to that force is to the right, resulting in negative work done by the spring.
Calculate the magnitude of the magnetic force on a 270 m length of wire stretched between two towers and carrying a 150 A current. The Earth's magnetic field of 4.0×10−5 T makes an angle of 80 ∘ with the wire
Answer:
Force on the wire is equal to 15.95 N
Explanation:
We have given length of the wire l = 270 m
Current flowing in the wire i = 150 A
Magnetic field [tex]B=4\times 10^{-5}T[/tex]
Angle between magnetic field and wire [tex]\Theta =80^{\circ}[/tex]
We have to find the force on the wire
Force on current carrying conductor is equal to [tex]F=IBlsin\Theta[/tex]
So [tex]F=150\times 4\times 10^{-5}\times 270\times sin80^{\circ}=15.95N[/tex]
So force on the wire is equal to 15.95 N
Using the formula F = IlB sin(θ), with I = 150 A, l = 270 m, B = 4.0×10⁻⁵ T, and θ = 80°, the magnitude of the magnetic force on the wire is calculated to be approximately 158.76 Newtons.
Explanation:To calculate the magnitude of the magnetic force on the wire, we use the formula F = IlB sin(θ), where F represents the force, I is the current, l is the length of the wire, B is the magnetic field strength, and θ is the angle between the wire and the magnetic field. In this scenario, I = 150 A, l = 270 m, B = 4.0×10⁻⁵ T, and θ = 80°.
First, we calculate the sine of the angle:
sin(80°) ≈ 0.9848Plugging the values into the force equation gives:
F = (150 A) × (270 m) × (4.0×10⁻⁵ T) × 0.9848
F = 158.76 N (rounded to two decimal places)
Hence, the magnitude of the magnetic force on the wire is approximately 158.76 Newtons.
The sound tube experiment was performed in gas Carbon Dioxide at temperature 20 deg. C. The students partnering on the bench obtained for the slope of the straight line fitting of the experimental points the value 365.0. Compare the speed of sound following from that slope to the calculated speed of sound from the gas properties? For CO2, Cp/Cv = 1.289, and the mass of one mol CO2 is 0.044 kg. The sound tube length is 0.367 m. The additional necessary datum is given in the text.
Answer:
The speed of sound theoretically is 267.148 m/s which is clearly less than slope calculated speed 365.0 m/s
Explanation:
check the attached picture
A certain hydraulic system is designed to exert a force 100 times as large as the one put into it. (a) What must be the ratio of the area of the slave cylinder to the area of the master cylinder? (b) What must be the ratio of their diameters? (c) By what factor is the distance through which the output force moves reduced relative to the distance through which the input force moves? Assume
Answer:
A) 100
B) 10
C) 0.01
Explanation:
Let
Fs = force on slave cylinder
Fm = force on master cylinder
Given that the designed to exert a force 100 times as large as the one put into it. That is
Fs = 100 Fm
Using Pascal's law
Fs/As = Fm/Am
100Fm/As = Fm/Am
100/As = 1/Am
Cross multiply
As= 100Am
As/Am = 100
b) What must be the ratio of their diameters
Using their areas ratio, area of a cylinder is πr^2
A = πr^2 = π(D/2)^2
π(Ds/2)^2 ÷ π(Dm/2)^2 = 100
(Ds/2)^2 ÷ (Dm/2)^2 = 100
(Ds/Dm)^2 = 100
Ds/Dm = 10
(c) By what factor is the distance through which the output force moves reduced relative to the distance through which the input force moves? Assume no losses to friction
Let us consider the workdone at the input and at the output.
Work done = force × distance
Fs × Hs = Fm × Hm
100Fm × Hs = Fm × Hm
100Hs = Hm
100Hs/Hm = 1
Hs/Hm = 1/100
Hs/Hm = 0.01
As friends frequently do, Josh and John stand at either end of a very long, stationary skateboard, with Josh at the front and John at the rear. John then tosses a heavy ball toward Josh who, caught unawares, ducks so that the ball goes sailing over his head and lands on the ground. There is no friction between the skateboard and the ground. After the ball is thrown, which way, if at all, does the skateboard move
A.Backward
B.Forward
C.Neither
Answer:
B. Forward
Explanation:
The net force in the system is initially balanced and the system is in equilibrium.
1) As John ducks, two things happens. First, there is a sudden impulse from his end which will change the momentum of the system from zero to an amount Mv proportional to the impulse Ft, which will be directed away from his direction because,
2) the process of ducking pushes his center of mass forward, which also moves the center of mass of the whole system away from him. This two effect will cause the skateboard to move forward.
A soap bubble (n = 1.28) having a wall thickness of 116 nm is floating in air. (a) What is the wavelength of the visible light that is most strongly reflected? nm (b) Explain how a bubble of different thickness could also strongly reflect light of this same wavelength. This answer has not been graded yet. (c) Find the two smallest film thicknesses larger than the one given that can produce strongly reflected light of this same wavelength. nm (smaller thickness) nm (larger thickness)
Answer:
Explanation:
a , b )
The problem is based on interference in thin films
formula for constructive interference
2μ t = ( 2n+ 1 ) λ / 2 , μ is refractive index of layer, t is thickness and λ is wavelength of light.
n is called the order of fringe . If we place n= 0 , 1 , 2 etc , the thickness also changes . So constructive interference is possible at more than one thickness .
Put the value of λ = 116 nm . μ = 1.28 , t = 116 nm in the given equation
2 x 1.28 x 116 x 2 = ( 2n+ 1 ) λ
593.92 = ( 2n+ 1 ) λ
when n = 0
λ = 593.92 nm .
This falls in visible range .
c )
2μ t = ( 2n+ 1 ) λ / 2
Put λ = 593.92 nm , n = 1
2 x 1.28 t₁ = 3 x 593.92 / 2
t₁ = 348 nm .
Put n = 2
2 x 1.28 t₂ = 5 x 593.92 / 2
t₂ = 580 nm .
We've seen that stout tendons in the legs of hopping kangaroos store energy. When a kangaroo lands, much of the kinetic energy of motion is converted to elastic energy as the tendons stretch, returning to kinetic energy when the kangaroo again leaves the ground. If a hopping kangaroo increases its speed, it spends more time in the air with each bounce, but the contact time with the ground stays approximately the same. Explain why you would expect this to be the case
Answer:
Check the explanation
Explanation:
So far there’s an increases in the speed of the kangaroo, then the tendons will stretch more thereby enabling them to store more energy. For this reason, they will have a additional time in the air propelled by greater spring energy. In contact with the ground, it will turn out to be like a spring in simple harmonic motion. There will be increases in their agility rate in hopping the amplitude of the oscillation, but that does not in any way affect the time, or period in contact with the ground.
Kangaroos convert kinetic energy to elastic potential energy during landing which is immediately converted back to kinetic energy for the next leap. This energy transformation cycle, aided by cushioning their landing by bending their hind legs, allows kangaroos to spend more time airborne without affecting the ground contact time, irrespective of their speed.
Explanation:The phenomenon in question about kangaroo jumping is rooted in physics and biomechanics. As kangaroos gain speed, more kinetic energy is stored and thus converted into potential energy when they're in the air. This essentially means the kangaroo uses most of their energy while airborne rather than contacting the ground. Hence, ground contact time stays the same no matter what the kangaroo's speed is.
Firstly, the kangaroo's tendons work like a spring; as it lands, much of its kinetic energy is converted to elastic potential energy in the tendons. This act transforms the downward motion (gravitational potential energy) into an upward motion (kinetic energy) through elastic potential energy, which is stored as the tendons stretch. This is similar to the motion observed in a bungee jumper or an elastic band when stretched.
Additionally, the kangaroo's landing is cushioned by bending its hind legs, reducing the impact force over the contact time. With each hop, the kangaroo's kinetic energy increases when it leaves the ground while potential energy increases during 'flight' due to gravity. This establishes a cycle between kinetic and potential energy, with energy oscillating back and forth as the kangaroo continues to hop. Such energy efficiency is what enables the kangaroo to maintain the same ground contact time irrespective of its speed.
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A thin rod of length 1.4 m and mass 140 g is suspended freely from one end. It is pulled to one side and then allowed to swing like a pendulum, passing through its lowest position with angular speed 1.09 rad/s. Neglecting friction and air resistance, find (a) the rod's kinetic energy at its lowest position and (b) how far above that position the center of mass rises.
Answer:
a The kinetic energy is [tex]KE = 0.0543 J[/tex]
b The height of the center of mass above that position is [tex]h = 1.372 \ m[/tex]
Explanation:
From the question we are told that
The length of the rod is [tex]L = 1.4m[/tex]
The mass of the rod [tex]m = 140 = \frac{140}{1000} = 0.140 \ kg[/tex]
The angular speed at the lowest point is [tex]w = 1.09 \ rad/s[/tex]
Generally moment of inertia of the rod about an axis that passes through its one end is
[tex]I = \frac{mL^2}{3}[/tex]
Substituting values
[tex]I = \frac{(0.140) (1.4)^2}{3}[/tex]
[tex]I = 0.0915 \ kg \cdot m^2[/tex]
Generally the kinetic energy rod is mathematically represented as
[tex]KE = \frac{1}{2} Iw^2[/tex]
[tex]KE = \frac{1}{2} (0.0915) (1.09)^2[/tex]
[tex]KE = 0.0543 J[/tex]
From the law of conservation of energy
The kinetic energy of the rod during motion = The potential energy of the rod at the highest point
Therefore
[tex]KE = PE = mgh[/tex]
[tex]0.0543 = mgh[/tex]
[tex]h = \frac{0.0543}{9.8 * 0.140}[/tex]
[tex]h = 1.372 \ m[/tex]
Answer:
a) Kr = 0.0543 J
b) Δy = 0.0396 m
Explanation:
a) Given
L = 1.4 m
m = 140 g = 0.14 kg
ω = 1.09 rad/s
Kr = ?
We have to get the rotational inertia as follows
I = Icm + m*d²
⇒ I = (m*L²/12) + (m*(L/2)²)
⇒ I = (0.14 kg*(1.4 m)²/12) + (0.14 kg*(1.4 m/2)²)
⇒ I = 0.09146 kg*m²
Then, we apply the formula
Kr = 0.5*I*ω²
⇒ Kr = 0.5*(0.09146 kg*m²)*(1.09 rad/s)²
⇒ Kr = 0.0543 J
b) We apply the following principle
Ei = Ef
Where the initial point is the lowest position and the final point is at the maximum height that its center of mass can achieve, then we have
Ki + Ui = Kf + Uf
we know that ωf = 0 ⇒ Kf = 0
⇒ Ki + Ui = Uf
⇒ Uf - Ui = Ki
⇒ m*g*yf - m*g*yi = Ki
⇒ m*g*(yf - yi) = Ki
⇒ m*g*Δy = Ki
⇒ Δy = Ki/(m*g)
where
Ki = Kr = 0.0543 J
g = 9.81 m/s²
⇒ Δy = (0.0543 J)/(0.14 kg*9.81 m/s²)
⇒ Δy = 0.0396 m
An astronaut is being tested in a centrifuge. The centrifuge has a radius of 5.20 m and, in starting, rotates according to θ = 0.170t2, where t is in seconds and θ is in radians. When t = 4.70 s, what are the magnitudes of the astronaut's (a) angular velocity, (b) linear velocity, (c) tangential acceleration, and (d) radial acceleration?
Answer:
A) angular velocity; ω = 1.598 rad/s
B) linear velocity;V = 8.31 m/s
C) Tangential Acceleration;a_t = 1.768 m/s²
D) Radial Acceleration;a_r = 13.28 m/s²
Explanation:
We are given that;
Radius; r = 5.2m
Time;t = 4.7 sec
θ = 0.170t²
Thus, angular acceleration would be the second derivative of θ which is d²θ/dt²
Thus,α = d²θ/dt² = 0.34 rad/s²
A) Formula for angular velocity is;
ω = αt
Where α is angular acceleration and t is time.
Thus;ω = 0.34 x 4.7
ω = 1.598 rad/s
b) formula for linear velocity is given by; V = ωr
We have ω = 1.598 rad/s and r = 5.2m
Thus; V = 1.598 x 5.2
V = 8.31 m/s
c) formula for tangential acceleration is;
a_t = αr
a_t = 0.34 x 5.2
a_t = 1.768 m/s²
d) formula for radial acceleration is;
a_r = rω²
a_r = 5.2 x 1.598²
a_r = 13.28 m/s²
To find the magnitudes of the astronaut's angular velocity, linear velocity, tangential acceleration, and radial acceleration, differentiate the angular position equation, multiply the radius and the angular velocity to find the linear velocity, and use the rate of change of linear velocity to find the tangential acceleration. The radial acceleration is the product of the angular velocity and the linear velocity.
Explanation:The angular velocity can be found by differentiating the angular position equation with respect to time. The linear velocity is equal to the product of the radius and the angular velocity. The tangential acceleration is equal to the rate of change of linear velocity, while the radial acceleration is equal to the product of the angular velocity and the linear velocity.
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Problem 24.3 The assembly is made from a steel hemisphere, rho st = 7. 80 Mg/m3 , and an aluminum cylinder, rho al = 2. 70 Mg/m3 . If the height of the cylinder is h = 180 mm, determine the location z of the mass center of the assembly.
Given:
[tex]\rho_s = 7.8 \ Mg/m^3[/tex][tex]\rho_a = 2.70 \ Mg/m^3[/tex]Height of cylinder, [tex]h = 180 \ mm[/tex]Now,
The mass of the steel hemisphere will be:
→ [tex]m_h = \rho_s\times \frac{2}{3} \pi r^2[/tex]
By putting the values, we get
[tex]= 7.8\times 10^3\times \frac{2}{3} \pi (0.16)^2[/tex]
[tex]= 66.9 \ kg[/tex]
and,
The mass of aluminum cylinder will be:
→ [tex]m_c = \rho_a \times \pi r^2 h[/tex]
[tex]= 2.7\times 10^3\times \pi (0.08)^2 (0.18)[/tex]
[tex]= 9.7 \ kg[/tex]
Now,
The mass center of steel hemisphere will be:
→ [tex]z_1 = r - \frac{3r}{8}[/tex]
[tex]= 0.16-(3\times \frac{0.16}{8} )[/tex]
[tex]= 0.1 \ m[/tex]
The mass center of aluminum hemisphere will be:
→ [tex]z_2 = r+\frac{h}{2}[/tex]
[tex]= 0.16+\frac{0.18}{2}[/tex]
[tex]= 0.25 \ m[/tex]
hence,
The center of mass will be:
→ [tex]Z = \frac{m_h z_1 +z_2 m_c}{m_s+m_c}[/tex]
By putting the values, we get
[tex]= \frac{66.9\times 0.1+9.76\times 0.25}{66.9+9.76}[/tex]
[tex]= 0.12 \ m[/tex]
Thus the above answer is right.
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To find the location (z) of the mass center of a steel hemisphere and an aluminum cylinder assembly, we first calculate the mass of each part using the given densities and geometric properties. We then use a formula to calculate 'z' based on the mass and z-coordinate of the center of mass of each part. The center of mass assumes the symmetric mass distributions.
Explanation:To determine the location z of the mass center of the assembly, we first need to calculate the mass of each part of the assembly using their given densities and geometrical properties.
The mass of the steel hemisphere (mSt) is calculated as density times the volume. The volume of the hemisphere can be calculated using the formula 2/3*Pi*r^3, where r is the radius of the hemisphere.
The mass of the aluminum cylinder (mAl) is calculated the same way, as the product of the cylinder's density and volume. The volume of a cylinder is given by the formula Pi*r^2*h, where r is the radius and h is the height of the cylinder, which is given as 180 mm or 0.12 m.
Once we have these masses, we then calculate the mass center z of the assembly, which is given by the formula z = (mSt * zSt + mAl * zAl) / (mSt + mAl), where zSt and zAl are the z-coordinates of the center of the mass of the steel hemisphere and the aluminum cylinder respectively.
Since the mass of each body acts as if it were at the center of the body, we can assume that the z-coordinate of the hemisphere (zSt) is at its geometric center, whereas for the cylinder (zAl), it would be at h/2 from the bottom end.
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Two monatomic gases, helium and neon, are mixed in a sealed container and brought into thermal equilibrium at temperature T . If the molar mass of helium is 4.0 g/mol and the molar mass of neon is 20.2 g/mol , then _______.
A. all the atoms have the same average speed
B. the average speed of the neon atoms is greater than the average speed of the helium atoms
C. the average speed of the helium atoms is greater than the average speed of the neon atoms
D. the atoms diffuse from high temperature to low temperature
E. all the atoms have exactly the same velocity.
In a mixture of helium and neon gases at thermal equilibrium, the average speed of helium atoms will be greater than the average speed of neon atoms.
Explanation:In a mixture of two gases at thermal equilibrium, the average speed of the atoms will depend on their respective molar masses. The average speed of an atom can be calculated using the root mean square speed formula, v = sqrt(3kT/m), where v is the average speed, k is the Boltzmann constant, T is the temperature in Kelvin, and m is the molar mass of the atom. In this case, helium has a smaller molar mass than neon, so according to the formula, the average speed of helium atoms will be greater than the average speed of neon atoms.
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The average speed of helium atoms is higher than that of neon atoms because the molar mass of helium is much smaller than that of neon. At the same temperature, lighter molecules move faster. Thus, the correct answer is C.
To determine the average speeds of helium and neon atoms in a mixture at thermal equilibrium at temperature T, we need to consider the relationship between temperature, mass, and molecular speed.
The average kinetic energy per atom at a given temperature T is the same for both helium and neon. This can be expressed as:
[tex]\frac{1}{2} m \langle v^2 \rangle = \frac{3}{2} k_B T[/tex]
where,
[tex]k_B[/tex]= Boltzmann constant
[tex]T[/tex]= temperature
[tex]m[/tex]= molar mass of the gas
Since both gases have the same average kinetic energy, the differences in their masses will influence their average speeds. Specifically, the equation for the root-mean-square speed (v_{rms}) of a gas is:
[tex]v_{\text{rms}} = \sqrt{\frac{3 k_B T}{m}}[/tex]
Given:
Molar mass of helium (He) =[tex]4.0 g/mol[/tex]
Molar mass of neon (Ne) = [tex]20.2 g/mol[/tex]
We see that helium has a much smaller molar mass compared to neon. Therefore, for the same temperature T:
[tex]v_{rms, He} > v_{rms, Ne}[/tex]
This means the average speed of helium atoms is greater than that of neon atoms. Thus, the correct answer is:
C. the average speed of the helium atoms is greater than the average speed of the neon atoms.
The mass of a particular eagle is twice that of a hunted pigeon. Suppose the pigeon is flying north at v i , 2 = 17.3 vi,2=17.3 m/s when the eagle swoops down, grabs the pigeon, and flies off. At the instant right before the attack, the eagle is flying toward the pigeon at an angle θ = 39.9 θ=39.9 ° below the horizontal and a speed of v i , 1 = 33.7 vi,1=33.7 m/s. What is the speed of the eagle immediately after it catches its prey?
The speed of the eagle immediately after catching the pigeon is [tex]$19.0$[/tex] m/s.
To solve this problem, we need to apply the principle of conservation of momentum, which states that the total momentum of a closed system remains constant before and after an interaction.
Given information:
- Mass of the pigeon = [tex]$m_2$[/tex]
- Mass of the eagle = [tex]$2m_2$[/tex] (twice the mass of the pigeon)
- Initial velocity of the pigeon, [tex]$\vec{v}_{i,2} = 17.3 m/s[/tex] (northward)
- Initial velocity of the eagle, [tex]$\vec{v}_{i,1} = 33.7 m/s[/tex] at an angle [tex]$\theta = 39.9^\circ$[/tex] below the horizontal
We need to find the final velocity of the eagle after catching the pigeon, [tex]$\vec{v}_f$[/tex].
Step 1: Resolve the initial velocity vectors into components.
For the pigeon:
[tex]$\vec{v}_{i,2} = (0, 17.3) m/s[/tex]
For the eagle:
[tex]$\vec{v}_{i,1} = (33.7 \cos 39.9^\circ, -33.7 \sin 39.9^\circ) m/s[/tex]
[tex]$\vec{v}_{i,1} = (22.8, -25.4) m/s[/tex]
Step 2: Calculate the initial total momentum of the system.
Initial total momentum, [tex]$\vec{p}_i = m_2 \vec{v}_{i,2} + (2m_2) \vec{v}_{i,1}$[/tex]
[tex]$\vec{p}_i = m_2 (0, 17.3) + 2m_2 (22.8, -25.4)$[/tex]
[tex]$\vec{p}_i = m_2 (45.6, -33.8) kg⋅m/s[/tex]
Step 3: Calculate the final total momentum of the system.
Since momentum is conserved, the final total momentum is equal to the initial total momentum.
[tex]$\vec{p}_f = \vec{p}_i = m_2 (45.6, -33.8) kg⋅m/s[/tex]
Step 4: Calculate the final velocity of the combined system (eagle + pigeon).
Let [tex]$\vec{v}_f = (v_{f,x}, v_{f,y})$[/tex] be the final velocity of the combined system.
Total final momentum = [tex]$(m_2 + 2m_2) \vec{v}_f = 3m_2 \vec{v}_f$[/tex]
[tex]3m_2 \vec{v}_f = m_2 (45.6, -33.8)$$\vec{v}_f = \left(\frac{45.6}{3}, -\frac{33.8}{3}\right)$ m/s\\$\vec{v}_f = (15.2, -11.3)$ m/s[/tex]
Step 5: Calculate the speed of the eagle after catching the pigeon.
Speed = [tex]$\sqrt{v_{f,x}^2 + v_{f,y}^2}$[/tex]
Speed = [tex]$\sqrt{15.2^2 + (-11.3)^2} m/s[/tex]
Speed = [tex]$19.0 m/s[/tex]
Consider an experiment in which slow neutrons of momentum ¯hk are scattered by a diatomic molecule; suppose that the molecule is aligned along the y axis, with one atom at y = b and the other at y = −b. The beam of neutrons is directed in the zb direction. Assume the atoms to be infinitely heavy so that they remain fixed throughout the experiment. The potential due to the atoms as seen by the neutrons can be represented by a delta function, so: V (~r) = a[δ(x)δ(y − b)δ(z) + δ(x)δ(y + b)δ(z)] (a) Calculate the scattering amplitude, and differential cross section, in the first order Born approximation. (b) In what ways does the quantum result differ from what one would expect classically?
Answer:
Check the explanation
Explanation:
When we have an object in periodic motion, the amplitude will be the maximum displacement from equilibrium. Take for example, when there’s a back and forth movement of a pendulum through its equilibrium point (straight down), then swings to a highest distance away from the center. This distance will be represented as the amplitude, A. The full range of the pendulum has a magnitude of 2A.
position = amplitude x sine function(angular frequency x time + phase difference)
x = A sin(ωt + ϕ)
x = displacement (m)
A = amplitude (m)
ω = angular frequency (radians/s)
t = time (s)
ϕ = phase shift (radians)
Kindly check the attached image below to see the step by step explanation to the question above.
Problem 3: An Nd:YAG laser operates in a pulsed mode, with an energy of 100mJ (millimoles) per pulse, and a pulse repetition rate of 10Hz. Light can be emitted at 1065 nm, 532 nm, or 355 nm. (a) Each pulse lasts for 1ns, and in between pulses, no light is emitted. What is the instantaneous laser power during each pulse
Given Information:
Energy of laser pulses = E = 100 mJ = 100×10⁻³ Joules
Time = t = 1 ns = 1×10⁻⁹ seconds
Required Information:
Instantaneous power = P = ?
Answer:
[tex]Instantaneous \: Power = 100 \: Mwatt[/tex]
Explanation:
The instantaneous power is the power dissipated at any instant of time whereas the average power is the power dissipated over a given time interval.
The instantaneous laser power during each pulse is given by
[tex]Instantaneous \: Power = \frac{E}{t}[/tex]
Where E is the energy of the laser pulses and t is the time that each pulse lasts.
[tex]Instantaneous \: Power = \frac{100\times10^{-3}}{1\times10^{-9}}[/tex]
[tex]Instantaneous \: Power = 1\times10^{8} \: watt[/tex]
or
[tex]Instantaneous \: Power = 100 \: Mwatt[/tex]
Therefore, the instantaneous power of each pulse is 100 Mwatt.
It’s mid-afternoon on a lovely, sunny day; it’s 60°F, and the sun is 60° above the horizon. Rays from the sun strike the still surface of a shallow pond that is 20 cm deep. The rays of sun cast a shadow of a stick that is completely submerged, and stuck in the sandy bottom of the pond. If 10 cm of the stick is above the sand, what is the length of the shadow?
Answer:
The correct answer is 5.77 cm
Explanation:
Solution
From the question given, let us recall the following,
A sunny day = 60°F and
The sun above the horizon is = 60°
The surface of a shallow pond is = 20 cm deep
The stick above sand = 10 cm
The next step is to find the length of the shadow
Now,
let CD = stick
BC= Length of shadow
Thus,
CD/BC = Tan 60°
BC = CD/Tan 60°
= 10/√3 = 5.77 cm
Therefore, the length of the shadow is 5.77 cm
What If? The coil and applied magnetic field remain the same, but the circuit providing the current in the coil is now changed. The new circuit has an emf of e m f = 20.0 V, and this allows a mass of 51.0 g added to the right side to balance the system. What is the value of the resistance R (in Ω)?
Answer:
Using equations
R will be 1.25 Kilo ohm
To get the value of resistance, R, we need to use Ohm's law which is R = V/I', where I' is the current generated when the coil balances with the added mass. The exact value of R depends on parameters related to the coil and the magnetic field.
Explanation:The question is asking for the value of the resistance R in a given circuit, when the circuit produces a current which generates a balance with an added mass through a coil in a magnetic field. To find the value of R, we need to use Ohm's law, which expresses the relationship between voltage (V), current (I), and resistance (R) as V=IR.
Here, the electromotive force or emf can be treated as the voltage in the circuit. In this case, emf = 20.0 V. When this coil creates a balance with an added 51.0 g mass, an equivalent current will be generated, let's denote it by I'
Using Ohm's law, we can solve for R by rearranging the formula to R = V/I'. The exact value of I' and thus R will, however, depend on additional factors involving the parameters of the coil and magnetic field which are not provided in the question. The law used here, Lenz's law, is a manifestation of the conservation of energy, dictating that the current induced in a circuit due to a change in the magnetic field will create a magnetic field that opposes the initial changing magnetic field.
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how is velocity different from speed
Answer: velocity has a direction, while speed is the distance travelled by an object.
Explanation:
Answer:
Velocity includes Displacement instead of distance.
Explanation:
Velocity's formula is change in position divided(displacement) by change in time(Delta x/Delta t). Whereas speed is distance over change in time(d/Delta t).
A charged capacitor is connected to an ideal inductor to form an LC circuit with a frequency of oscillation f = 1.6 Hz. At time t = 0 the capacitor is fully charged. At a given instant later the charge on the capacitor is measured to be 3.0 μC and the current in the circuit is equal to 75 μA. What is the maximum charge of the capacitor?
Answer:
[tex]8.0\mu C[/tex]
Explanation:
We are given that
[tex]f=1.6 Hz[/tex]
[tex]q=3.0\mu C=3.0\times 10^{-6} C[/tex]
[tex]1\mu C=10^{-6} C[/tex]
Current,I=[tex]75\mu A=75\times 10^{-6} A[/tex]
[tex]1\mu A=10^{-6} A[/tex]
We have to find the maximum charge of the capacitor.
Charge on the capacitor,[tex]q=q_0cos\omega t[/tex]
[tex]\omega=2\pi f=2\pi\times 1.6=3.2\pi rad/s[/tex]
[tex]3\times 10^{-6}=q_0cos3.2\pi t[/tex]....(1)
[tex]I=\frac{dq}{dt}=-q_0\omega sin\omega t[/tex]
[tex]75\times 10^{-6}=-q_0(3.2\pi)sin3.2\pi t[/tex]....(2)
Equation (2) divided by equation (1)
[tex]-3.2\pi tan3.2\pi t=\frac{75\times 10^{-6}}{3\times 10^{-6}}=25[/tex]
[tex]tan3.2\pi t=-\frac{25}{3.2\pi}=-2.488[/tex]
[tex]3.2\pi t=tan^{-1}(-2.488)=-1.188rad[/tex]
[tex]q_0=\frac{q}{cos\omega t}=\frac{3\times 10^{-6}}{cos(-1.188)}=8.0\times 10^{-6}=8\mu C[/tex]
Hence, the maximum charge of the capacitor=[tex]8.0\mu C[/tex]
Aspartic acid is a polypeptide side chain found in proteins. The pKa of aspartic acid is 3.86. If this polypeptide were in an aqueous solution with a pH of 7, the side chain would have what charge? a) negative b) positive c) neutral d) there is no way to know
Answer: a) Negative
Explanation: According to the question: The pKa of aspartic acid is 3.86.
For acidic amino acids,
pH > pKa
When side chains are negatively charged, amino acid will be acidic
pH < pKa
That is, when side chains are uncharged, amino acid will be neutral
For aspartic acid, when this polypeptide were in an aqueous solution with a pH of 7
pH (7.0) > pKa (3.86)
Therefore the chains are negatively charged
Final answer:
In an aqueous solution at pH 7, the aspartic acid side chain would have a (a)negative charge because the pH of the environment is higher than the pKa of aspartic acid (3.86).
Explanation:
The question relates to the charge of the aspartic acid side chain in an aqueous solution at pH 7, given that the pKa of aspartic acid is 3.86. The pKa value represents the pH at which half of the aspartic acid side chains are deprotonated (negative charge) and half remain protonated (neutral). When the pH of the environment is higher than the pKa (as is the case here, pH 7 > pKa 3.86), the majority of the aspartic acid side chains will be deprotonated, thus carrying a negative charge. Consequently, in an aqueous solution at pH 7, the aspartic acid side chain would have (a)negative charge.
A 13.6- resistor, an 11.9-μF capacitor, and a 19.1-mH inductor are connected in series with a 117-V generator.
(a) At what frequency is the current a maximum?
(b) What is the maximum value of the RMS current?
Note: The ac current and voltage are RMS values and power is an average value unless indicated otherwise.
Answer:
Explanation:
Given the following information,
Resistor of resistance R = 13.6Ω
Capacitor of capacitance C = 11.9-μF
C = 11.9 × 10^ -6 F
Inductor of inductance L = 19.1-mH
L = 19.1 ×10^-3 H
All this connected in series to a generator that generates Vrms= 117V
Vo = Vrms√2 = 117√2
Vo = 165.463V
a. Frequency for maximum current?
Maximum current occurs at resonance
I.e Xc = XL
At maximum current, the frequency is given as
f = 1/(2π√LC)
Then,
f = 1/(2π√(19.1×10^-3 × 11.9×10^-6)
f = 1/(2π√(2.2729×10^-7))
f = 1/(2π × 4.77 ×10^-4)
f = 333.83Hz
Then, the frequency is 333.83Hz.
b. Since we know the frequency,
Then, we need to find the capacitive and inductive reactance
Capacitive reactance
Xc = 1/2πfC
Xc = 1/(2π × 338.83 × 11.9×10^-6)
Xc = 1/ 0.024961
Xc = 40.1Ω
Also, Inductive reactance
XL = 2πfL
XL = 2π × 333.83 × 19.1×10^-3
XL = 40.1Ω
As expected, Xc=XL, resonance
Then, the impedance in AC circuit is given as
Z = √ (R² + (Xc—XL)²)
Z = √ 13.6² + (40.1-40.1)²)
Z = √13.6²
Z = 13.6 ohms
Then, using ohms las
V = IZ
Then, I = Vo/Z
Io = 165.46/13.6
Io = 12.17Amps
The current is 12.17 A
Answer:
a) Current is maximum at frequency, f₀ = 333.83 Hz
b) Maximum current = 12.17 A
Explanation:
Inductance, L = 19.1 mH = 19.1 * 10⁻³ H
Capacitance, C = 11.9 μF =11.9 * 10⁻⁶ F
a) Current is maximum at resonant frequency, f₀
[tex]f_{0} = \frac{1}{2\pi\sqrt{LC} }[/tex]
[tex]f_{0} = \frac{1}{2\pi\sqrt{11.9 * 10^{-6}* 19.1 * 10^{-3} } }[/tex]
[tex]f_{0} = 333.83 Hz[/tex]
b) Maximum value of the RMS current
[tex]V_{RMS} = 117 V\\V_{max} = \sqrt{2} V_{RMS}\\V_{max} = \sqrt{2} * 117\\V_{max} = 165.46 V[/tex]
[tex]I_{max} = \frac{V_{max} }{R} \\I_{max} = \frac{165.46}{13.6} \\I_{max} = 12.17 A[/tex]
How would you classify the wave?
Answer:
One way to categorize waves is on the basis of the direction of movement of the individual particles of the medium relative to the direction that the waves travel. Categorizing waves on this basis leads to three notable categories: transverse waves, longitudinal waves, and surface waves.
I've read about it but never seen one. The way I understand it, it's a coordinated physical motion executed by a great number of people, as in a large crowd at a sporting event, timed so that it appears to propagate from one end of the crowd to the opposite end.
I would classify it as a cooperative community activity, involving liberty, equality, and fraternity, executed for the common good.
A bucket of mass m is hanging from the free end of a rope whose other end is wrapped around a drum (radius R, mass M) that can rotate with negligible friction about a stationary horizontal axis. The drum is not a uniform cylinder and has unknown moment of inertia. When you release the bucket from rest, you find that it has a downward acceleration of magnitude a. What is the tension in the cable between the drum and the bucket
Final answer:
The tension in the cable connecting the drum to the bucket is equal to the mass of the bucket times the difference between the acceleration due to gravity and the bucket's downward acceleration.
Explanation:
To determine the tension in the cable between the drum and the bucket, we can apply Newton's second law to the hanging mass. The net force acting on the bucket is the difference between the weight of the bucket and the tension in the rope:
[tex]F_{net}[/tex] = mg - T
Since we know the bucket has a downward acceleration a, we can write Newton's second law as:
ma = mg - T
Where m is the mass of the bucket, g is the acceleration due to gravity, and T is the tension in the rope. We can rearrange the equation to solve for T:
T = mg - ma
T = m(g - a)
So the tension in the cable is equal to the mass of the bucket times the difference between the acceleration due to gravity and the downward acceleration of the bucket.
It's a hot and sunny day and you decide to go for a drive. When you open your car door, it's a lot hotter than outside. Why is that
An ambulance is traveling north at 48.4 m/s, approaching a car that is also traveling north at 28 m/s. The ambulance driver hears his siren at a frequency of 620 Hz. Ambulance 48.4 m/s 28 m/s Car What is the wavelength at any position in front of the ambulance for the sound from the ambulance’s siren? The velocity of sound in air is 343 m/s. Answer in units of m.
Answer:
Explanation:
For any point stationary in front of ambulance , the ambulance is approaching the point . In this way the case is similar to source of sound approaching the observer. The doppler's effect can be applied to know the apparent frequency.
velocity of sound V = 343 m /s
speed of source Vs = 48.4
observer is stationary.
apparent frequency = real frequency x V / ( V - Vs )
= 620 x 343 / ( 343 - 48.4 )
= 722 Hz approx.
Three children are riding on the edge of a merry‑go‑round that has a mass of 105 kg and a radius of 1.70 m . The merry‑go‑round is spinning at 22.0 rpm . The children have masses of 22.0 , 28.0 , and 33.0 kg . If the 28.0 kg child moves to the center of the merry‑go‑round, what is the new angular velocity in revolutions per minute? Ignore friction, and assume that the merry‑go‑round can be treated as a solid disk and the children as point masses.
Answer:
Explanation:
Given that,
Three children of masses and their position on the merry go round
M1 = 22kg
M2 = 28kg
M3 = 33kg
They are all initially riding at the edge of the merry go round
Then, R1 = R2 = R3 = R = 1.7m
Mass of Merry go round is
M =105kg
Radius of Merry go round.
R = 1.7m
Angular velocity of Merry go round
ωi = 22 rpm
If M2 = 28 is moves to center of the merry go round then R2 = 0, what is the new angular velocity ωf
Using conservation of angular momentum
Initial angular momentum when all the children are at the edge of the merry go round is equal to the final angular momentum when the second child moves to the center of the merry go round
Then,
L(initial) = L(final)
Ii•ωi = If•ωf
So we need to find the initial and final moment of inertia
NOTE: merry go round is treated as a solid disk then I= ½MR²
I(initial)=½MR²+M1•R²+M2•R²+M3•R²
I(initial) = ½MR² + R²(M1 + M2 + M3)
I(initial) = ½ × 105 × 1.7² + 1.7²(22 + 28 + 33)
I(initial) = 151.725 + 1.7²(83)
I(initial) = 391.595 kgm²
Final moment of inertial when R2 =0
I(final)=½MR²+M1•R²+M2•R2²+M3•R²
Since R2 = 0
I(final) = ½MR²+ M1•R² + M3•R²
I(final) = ½MR² + (M1 + M3)• R²
I(final)=½ × 105 × 1.7² + ( 22 +33)•1.7²
I(final) = 151.725 + 158.95
I(final) = 310.675 kgm²
Now, applying the conservation of angular momentum
L(initial) = L(final)
Ii•ωi = If•ωf
391.595 × 22 = 310.675 × ωf
Then,
ωf = 391.595 × 22 / 310.675
ωf = 27.73 rpm
So, the final angular momentum is 27.73 revolution per minute