This is a problem based on the logic and interpretation of the variables. From the measured data taken
what is collected by the two individuals is expressed as,
- NED reference system: (x, t)
- PAM reference system: (x ', t')
From the reference system we know that ν is the speed of PAM (the other reference system) as a measurement by NED.
Then ν' is the speed of NED (from the other system of the reference) as a measurement by PAM.
In the context of Special Relativity, v' represents the relative velocity of Ned as observed from Pam's reference frame. This velocity takes into account the motion of both Ned and Pam and can be computed using the principles of Conservation of Momentum.
Explanation:The symbol v' can be interpreted as the velocity of Ned as measured from Pam's frame of reference. This concept forms the basis of Special Relativity as proposed by Einstein, where observations are taken from different frames of reference, in this case, Pam and Ned. Relative velocity, like v', is the velocity of an object (in this case, Ned) as observed from a particular frame of reference (in this case, Pam's), and it can change depending on who is making the observation. It takes into account the motion of both Ned and Pam and describes how fast Ned is moving and in what direction from Pam's perspective.
For example, if Pam and Ned were moving towards each other, the relative velocity v' would be the sum of their individual speeds as observed from Pam's perspective. If they were moving in the same direction, v' would be the difference in their individual speeds. Also, Pam's velocity in Ned's frame can be defined as -v'. This negative sign indicates they are moving in opposite directions.
To compute v', you would need to understand the principle of Conservation of Momentum, represented by equations defining momentum conservation in the x and y directions. Using this principle, you can solve for V.
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8. A gas is contained in a horizontal piston-cylinder apparatus at a pressure of 350 kPa and a volume of 0.02 m3 . Determine the work done by the piston on the gas if the cylinder volume is increased to 0.15 m3 through heating. Assume the pressure of the
Answer:
45500 J
Explanation:
Pressure, P =350 kPa = 350 x 1000 Pa
V1 = 0.02 m^3
V2 = 0.15 m^3
Work done by the piston
W = Pressure x increase in volume
W = P x (V2 - V1)
W = 350 x 1000 (0.15 - 0.02)
W = 45500 J
Thus, the work done is 45500 J.
Final answer:
The piston performs 45500 Joules of work on the gas when the volume of the gas in the piston-cylinder apparatus increases from 0.02 m³ to 0.15 m³ at a constant pressure of 350 kPa.
Explanation:
To determine the work done by the piston on the gas when the cylinder volume increases from 0.02 m³ to 0.15 m³ at a constant pressure of 350 kPa, we can use the formula for work done during a quasi-static process in thermodynamics, which is W = PΔV, where W is the work done by the gas, P is the constant pressure, and ΔV is the change in volume.
Given:
P = 350 kPa = 350000 Pa (since 1 kPa = 1000 Pa)
ΔV = 0.15 m³ - 0.02 m³ = 0.13 m³
We can now calculate the work done:
W = PΔV
W = 350000 Pa × 0.13 m³
W = 45500 J
Therefore, the piston performs 45500 Joules of work on the gas when the volume increases to 0.15 m³.
The colors of the stars in the sky range from red to blue. Assuming that the color indicates the frequency at which the star radiates the maximum amount of electromagnetic energy, estimate the surface temperature of red, yellow, white, and blue stars.
A) Estimate the surface temperature of red star. Assume that red color corresponds to wavelengths of approximately 650 nm.B) Estimate the surface temperature of yellow star. Assume that yellow color corresponds to wavelengths of approximately 570 nm.C) Estimate the surface temperature of blue star. Assume that blue color corresponds to wavelengths of approximately 470 nmD) Estimate the surface temperature of white star. Since green is in the middle of the visible spectrum, choose 520 nm wavelength for white star.
Answer:
a) 4458K b) 5048K, c) 6166K, d) 5573K
Explanation:
The temperature of the stars and many very hot objects can be estimated using the Wien displacement law
[tex]\lambda_{max}[/tex] T = 2,898 10⁻³ [m K]
T = 2,898 10⁻³ / [tex]\lambda_{max}[/tex]
a) indicate that the wavelength is
Lam = 650 nm (1 m / 109 nm) = 650 10⁻⁹ m
Lam = 6.50 10⁻⁷ m
T = 2,898 10⁻³ / 6.50 10⁻⁷
T = 4,458 10³ K
T = 4458K
b) lam = 570 nm = 5.70 10⁻⁷ m
T = 2,898 10⁻³ / 5.70 10⁻⁷
T = 5084K
c) lam = 470 nm = 4.70 10⁻⁷ m
T = 2,898 10⁻³ / 4.7 10⁻⁷
T = 6166K
d) lam = 520 nm = 5.20 10⁻⁷ m
T = 2,898 10⁻³ / 5.20 10⁻⁷
T = 5573K
A ) the surface temperature of red star is about 4500 K
B ) the surface temperature of yellow star is about 5100 K
C ) the surface temperature of blue star is about 6200 K
D ) the surface temperature of white star is about 5600 K
[tex]\texttt{ }[/tex]
Further explanationLet's recall the Wien's Displacement Law as follows:
[tex]\boxed {\lambda_{max}\ T = 2.898 \times 10^{-3} \texttt{ m.K}}[/tex]
where:
λ_max = the wavelength of the maximum radiation energy ( m )
T = surface temperature of the star ( K )
Let us now tackle the problem!
[tex]\texttt{ }[/tex]
Given:
wavelength of red light = λ_r = 650 nm = 650 × 10⁻⁹ m
wavelength of yellow light = λ_y = 570 nm = 570 × 10⁻⁹ m
wavelength of blue light = λ_b = 470 nm = 470 × 10⁻⁹ m
wavelength of white light = λ_w = 520 nm = 520 × 10⁻⁹ m
Asked:
A ) the surface temperature of red star = T_r = ?
B ) the surface temperature of yellow star = T_y = ?
C ) the surface temperature of blue star = T_b = ?
D ) the surface temperature of white star = T_w = ?
Solution:
Part A) :[tex]T_r = ( 2.898 \times 10^{-3} ) \div \lambda_r[/tex]
[tex]T_r = ( 2.898 \times 10^{-3} ) \div ( 650 \times 10^{-9} )[/tex]
[tex]\boxed {T_r \approx 4500 \texttt{ K} }[/tex]
[tex]\texttt{ }[/tex]
Part B) :[tex]T_y = ( 2.898 \times 10^{-3} ) \div \lambda_y[/tex]
[tex]T_y = ( 2.898 \times 10^{-3} ) \div ( 570 \times 10^{-9} )[/tex]
[tex]\boxed {T_y \approx 5100 \texttt{ K} }[/tex]
[tex]\texttt{ }[/tex]
Part C) :[tex]T_b = ( 2.898 \times 10^{-3} ) \div \lambda_b[/tex]
[tex]T_b = ( 2.898 \times 10^{-3} ) \div ( 470 \times 10^{-9} )[/tex]
[tex]\boxed {T_b \approx 6200 \texttt{ K} }[/tex]
[tex]\texttt{ }[/tex]
Part D) :[tex]T_w = ( 2.898 \times 10^{-3} ) \div \lambda_w[/tex]
[tex]T_w = ( 2.898 \times 10^{-3} ) \div ( 520 \times 10^{-9} )[/tex]
[tex]\boxed {T_w \approx 5600 \texttt{ K} }[/tex]
[tex]\texttt{ }[/tex]
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Answer detailsGrade: High School
Subject: Mathematics
Chapter: Energy
An applied force of 122 N is exerted horizontally on an 28 kg box of dogs in Yulin. The coefficient of kinetic friction between the floor and the box is 0.35. If the box is initially at rest, what is the final kinetic energy after it has been moved 9.46 m across the floor?
Answer:
The final kinetic energy is 242 J.
Explanation:
Hi there!
According to the work-energy theorem, the total work done on the box is equal to its change in kinetic energy:
W = ΔKE
Where:
W = work done on the box.
ΔKE = change in kinetic energy (final KE - initial KE).
The only forces that do work in this case are the applied force and the friction force because the box moves only horizontally.
The equation of work is the following:
W = F · s
Where:
F = force.
s = traveled distance.
Then, the work done by the applied force is:
W = 122 N · 9.46 m = 1.15 × 10³ J
To calculate the work done by friction, we have to find the friction force:
Fr = N · μ
Where:
Fr = friction force.
N = normal force.
μ = coefficient of kinetic friction.
The box does not have a net vertical acceleration. It means that the sum of the vertical forces acting on the box is zero:
∑Fy = 0
In this case, the only vertical forces are the weight of the box and the normal force. Then:
Weight + N = 0
N = - Weight
The weight of the box is calculated as follows:
Weight = m · g
Where:
m = mass of the box.
g = acceleration due to gravity.
Then:
-Weight = N = 28 kg · 9.8 m/s² = 274.4 N
Now, we can calculate the friction force:
Fr = N · μ
Fr = 274.4 N · 0.35 = 96 N
The work done by the friction force will be:
W = Fr · s
W = 96 N · 9.46 m = 908 J
Since the work done by friction opposes to the sense of movement, the work is negative.
Now, we can calculate the total work done on the box:
W total = W applied forece + W friction force
W = 1.15 × 10³ J - 908 J = 242 J
Applying the work-energy theorem:
W = final KE - initial KE
Since the box is initially at rest the initial kinetic energy is zero. Then:
W = final KE - 0
W = final KE
Final KE = 242 J
The final kinetic energy is 242 J.
A playground merry-go-round has radius 2.80 m and moment of inertia 2400 kg⋅m2 about a vertical axle through its center, and it turns with negligible friction.A child applies an 20.0 N force tangentially to the edge of the merry-go-round for 25.0 s . If the merry-go-round is initially at rest, what is its angular speed after this 25.0 s interval?
Answer:
[tex]\omega_f = 0.602\ rad/s[/tex]
Explanation:
given,
radius of merry- go- round = 2.80 m
moment of inertia = I = 2400 kg⋅m²
child apply force tangentially = 20 N
for time = 25 s
angular speed after 25 speed = ?
initial angular speed of the merry go round = 0 rad/s
we know,
torque = I α.............(1)
α is angular acceleration
and also
τ = F.r........................(2)
computing equation (1) and (2)
F . r = I α
[tex]\alpha = \dfrac{\omega_f - \omega_i}{t}[/tex]
[tex]F . r =I \times \dfrac{\omega_f - \omega_i}{t}[/tex]
[tex]20 \times 2.89 =2400\times \dfrac{\omega_f -0}{25}[/tex]
[tex]\omega_f = 0.602\ rad/s[/tex]
the angular speed of merry-go-round after 25 second is equal to [tex]\omega_f = 0.602\ rad/s[/tex]
A rectangular coil of dimensions 5.40cm x 8.50cm consists of25 turns of wire. The coil carries a current of 15.0 mA.
a) Calculate the magnitude of its magnetic moment
b) Suppose a uniform magnetic field of magnitude of 0.350 T isapplied parallel to the plane of the loop. What is the magnitude ofthe torque acting on the loop?
Answer:
(a) Magnetic moment will be [tex]17.212\times 10^{-4}A-m^2[/tex]
(b) Torque will be [tex]6.024\times 10^{-4}N-m[/tex]
Explanation:
We have given dimension of the rectangular 5.4 cm × 8.5 cm
So area of the rectangular coil [tex]A=5.4\times 8.5=45.9cm^2=45.9\times 10^{-4}m^2[/tex]
Current is given as [tex]i=15mA=15\times 10^{-3}A[/tex]
Number of turns N = 25
(A) We know that magnetic moment is given by [tex]magnetic\ moment=NiA=25\times 45.9\times 10^{-4}\times 15\times 10^{-3}=17.212\times 10^{-4}A-m^2[/tex]
(b) Magnetic field is given as B = 0.350 T
We know that torque is given by [tex]\tau =BINA=0.350\times 15\times 10^{-3}\times 25\times 45.9\times 10^{-4}=6.024\times 10^{-4}N-m[/tex]
Final answer:
a) The magnitude of the magnetic moment is 0.0172 A·m². b) The magnitude of the torque on the loop is 0 N·m.
Explanation:
a) To calculate the magnitude of the magnetic moment, we can use the formula μ = nIA, where μ is the magnetic moment, n is the number of turns, I is the current, and A is the area of the coil. In this case, n = 25, I = 15.0 mA = 0.015 A, and A = (5.40 cm)(8.50 cm) = 45.9 cm² = 0.00459 m². Plugging these values into the formula, we get μ = (25)(0.015 A)(0.00459 m²) = 0.0172 A·m².
b) To calculate the magnitude of the torque, we can use the formula τ = μBsinθ, where τ is the torque, μ is the magnetic moment, B is the magnetic field strength, and θ is the angle between μ and B. In this case, μ = 0.0172 A·m² (calculated in part a),
B = 0.350 T, and since the magnetic field is applied parallel to the plane of the loop, θ = 0°.
Plugging these values into the formula, we get τ = (0.0172 A·m²)(0.350 T)(sin 0°)
= 0 N·m.
006 10.0 points Two pucks of equal mass collide. One puck (puck A) is stationary before the collision. After the collision the puck that was initially stationary moves along in the same direction in which the puck that hit it (puck B) was initially moving. Puck B Puck A Which of the following statements is correct if the total energy of the system is conserved during the collision (elastic collision)? 1. There isn't enough information to answer the question. 2. Both pucks slide past the point of colli- sion. 3. The puck B remains at the point of colli- sion. 4. The puck B rebounds.
Answer: 3. The puck B remains at the point of collision.
Explanation:
Assuming no external forces acting during the collision, total momentum must be conserved.
The initial momentum is due only to puck B, as Puck A is at rest.
The final momentum is given by the sum of the momenta of both pucks, so we can write the following equation:
mA*viA = (mA * vfA) + (mB * vfB)
As mA = mB = m, we can simplify the former equation as follows:
viA = vfA + vfB (1)
Now, we also know, that the collision was an elastic collision, so total kinetic energy must be conserved too:
½ m viA²= ½ m vfA² + ½ m vfB²
Simplifying on both sides, we finally have:
viA² = vfA² + vfB² (2)
Now, if we square both sides of (1), we get:
viA² = (vfA + vfB)²= vfA² + 2* vfA * vfB +vfB² (3)
As the right side in (2) and (3) must be equal each other (as the left sides do), the only choice is that either vfA or vfB, be zero.
As we are told that puck A (initially stationary) after the collision, moves, the only possible choice is that puck B remain at rest in the point of collision, after the collision, exchanging his speed with puck A.
In an elastic collision where the total energy of the system is conserved, Puck B rebounds. This is because kinetic energy, along with momentum, is conserved in such a collision, causing the moving puck to rebound.
Explanation:Considering this scenario from the lens of physics, the principle of conservation of momentum and kinetic energy comes into play, which means the total momentum and kinetic energy before and after the collision should remain constant. This is consistent with the properties of an elastic collision. Both pucks have the same mass and initially, Puck B is in motion while Puck A is stationary. Hence, all of the initial energy and momentum are with Puck B.
Upon collision, the energy is transferred, causing Puck A to move in the same direction that Puck B was initially moving. The correct statement is that if the collision is elastic and the total energy of the system is conserved, 'Puck B rebounds'. This rebounding comes from the conservation of kinetic energy principle which holds in an elastic collision. That is, the total initial kinetic energy equals the total final kinetic energy.
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Two masses sit at the top of two frictionless inclined planes that have different angles. Which mass gets to the bottom first?
Answer:
Explanation:
Let the two inclined planes having angle of inclinations α and β.
The acceleration along the inclined plane acting on the body is gSinα and gSinβ.
If α > β
So, g Sinα > g Sinβ
So, more the inclination of the plane more be the acceleration of body and hence the time taken is less.
So, the body kept on the inclined whose inclination is more reaches at the bottom first.
The mass sitting on the plane inclined to a greater angle to the horizontal will reach the bottom first because it will experience greater acceleration.
Let the angle of inclination of the first mass to the horizontal = θLet the angle of inclination of the second mass to the horizontal = β
The net horizontal force on the masses is calculated as follows;
[tex]\Sigma F_x = 0\\\\mgsin(\theta) = ma\\\\gsin(\theta) = a\ \ \ or \ \ \ \\\\gsin(\beta ) = a[/tex]
Assuming the value of the angles of inclination of the plane is the following;
θ = 60⁰ and β = 30⁰a = gsin(60) = 0.866g
a = gsin(30) = 0.5g
Thus, we can conclude that the mass sitting on the plane inclined to a greater angle to the horizontal will reach the bottom first because it will experience greater acceleration.
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A 50-N crate is pulled up a 5-m inclined plane by a worker at constant velocity. If the plane is inclined at an angle of 37° to the horizontal and there exists a constant frictional force of 10 N between the crate and the surface, what is the force applied by the worker?
Answer:F=40.09 N
Explanation:
Given
weight of crate [tex]W=50 N[/tex]
Inclination [tex]\theta =37^{\circ}[/tex]
Frictional Force [tex]f=10 N[/tex]
as the crate is moving with constant velocity therefore net Force on crate is zero
[tex]F-50\sin (37)-f=0[/tex]
[tex]F=50\sin (37)+10[/tex]
[tex]F=30.09+10[/tex]
[tex]F=40.09 N[/tex]
Four students use different instruments to measure the length of the same pen. Which measurement implies the greatest precision?
a. 16.0 cm.
b. 0.160 m.
c. 0.00016 km.
d. Need more information.
e. 160.0 mm
Answer:
e. 160.0 mm
Explanation:
Precision is defined as the accuracy in measurement that the measuring instrument measure any given specimen. The instrument having the lowest least count will be more precise than the instrument with higher least count.
Also precision of the reading is given by the number of the significant figures in the given sample of reading.
Option (e) that is 160.0 has a total number of significant figure of 4, which is the largest total significant figures among the other options.
Also the measurement reads 160.0 mm which measure to the lowest possible measurement of the given pen. Thus this reading is more precise.
Hence the correct option is --- Option (e) 160.0 mm
You are lying in bed and want to shut your bedroom door. You have a bouncy "superball" and a blob of clay, both with the same mass. Which one would be more effective to throw at your door to close it?
a. The superball.
b. Neither will work.
c. The blob of clay.
d. Both the same.
Answer:
Choice A. The bouncy "superball" will exert approximately twice as much force than the blob of clay when tossed out at the same speed.
Explanation:
The momentum of an object is equal to the product of its mass and its velocity. The momentum of the system is conserved even if the collision is inelastic.
When the bouncy ball or the blob of clay hits the door, their momentum changes. Since momentum is conserved, the door would move in the opposite direction such that the total momentum stays at zero.
Let the mass of each object be [tex]m[/tex]. Suppose that both objects hit the door at a speed of [tex]v[/tex] in the same direction.
The bouncy ball will likely bounce back at about the same speed (in the opposite direction, away from the door.) The magnitude of the change in velocity will be at most [tex]2v[/tex]. The magnitude of the change in momentum will be at most [tex]2 \,m\cdot v[/tex].However, when the blob of clay hits the door, its shape would change (and it would potentially stick to the door.) In other words, its velocity becomes almost [tex]0[/tex] after the collision. The magnitude of the change in its momentum will only be around [tex]m \cdot v[/tex], which is only about [tex]\dfrac{1}{2}[/tex] the momentum change due to the bouncy ball.By Newton's Second Law, the net force on the door is proportion to the rate of change in its momentum. Assume that the two objects are in contact with the door for the same amount of time, the bouncy ball would exert about twice as much force on the door as the clay would. Hence it is "more effective" for closing the door.
The clay is more effective than the superball for shutting the door because upon impact the clay sticks to the door and transfers all of its momentum to it, while the superball bounces back and doesn't transfer all of its momentum.
Explanation:The most effective object to throw at your door to shut it would be c. The blob of clay. This is because of the principle of conservation of momentum. When the clay hits the door, it sticks to it, thus transferring all of its momentum to the door. This momentum is what causes the door to move and potentially close. On the other hand, when the superball hits the door, it bounces back, meaning not all of its momentum is transferred to the door. Hence, the clay, by virtue of its ability to stick and transfer its full momentum, would be more effective.
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Problem 12: A 20.0-m tall hollow aluminum flagpole is equivalent in strength to a solid cylinder 4.00 cm in diameter. A strong wind bends the pole much as a horizontal force of 1100 N exerted at the top would. How to the side does the top of the pole flex?
Answer:
The deformation in the pole due to force is 0.70 mm.
Explanation:
Given that,
Height = 20.0 m
Diameter = 4.00 cm
Force = 1100 N
We need to calculate the area
Using formula of area
[tex]A=\pi\times r^2[/tex]
[tex]A=\pi\times(2.00\times10^{-2})^2[/tex]
[tex]A=0.00125\ m^2[/tex]
[tex]A=1.25\times10^{-3}\ m^2[/tex]
We need to calculate the deformation
Using formula of deformation
[tex]\Delta x=\dfrac{1}{s}(\dfrac{F}{A}\times L)[/tex]
Where, s = shear modulus
F = force
l = length
A = area
Put the value into the formula
[tex]\Delta x=\dfrac{1}{2.5\times10^{10}}\times(\dfrac{1100}{1.25\times10^{-3}}\times 20.0)[/tex]
[tex]\Delta x=0.000704\ m[/tex]
[tex]\Delta x=7.04\times10^{-4}\ m[/tex]
[tex]\DElta x=0.70\ mm[/tex]
Hence, The deformation in the pole due to force is 0.70 mm.
A 191 191 kg sculpture hangs from a horizontal rod that serves as a pivot about which the sculpture can oscillate. The sculpture's moment of inertia with respect to the pivot is 17.2 17.2 kg·m2, and when it is swung at small amplitudes, it is found to oscillate at a frequency of 0.925 0.925 Hz. How far is the pivot from the sculpture's center of mass?
Answer:
r = 0.31 m
Explanation:
Given that,
Mass of the sculpture, m = 191 kg
The sculpture's moment of inertia with respect to the pivot is, [tex]I=17.2\ kg-m^2[/tex]
Frequency of oscillation, f = 0.925 Hz
Let r is the distance of the the pivot from the sculpture's center of mass. The frequency of oscillation is given by :
[tex]f=\dfrac{1}{2\pi}\sqrt{\dfrac{mgr}{I}}[/tex]
[tex]r=\dfrac{4\pi^2f^2I}{mg}[/tex]
[tex]r=\dfrac{4\pi^2\times 0.925^2\times 17.2}{191\times 9.8}[/tex]
r = 0.31 m
So, the pivot is 0.31 meters from the sculpture's center of mass. Hence, this is the required solution.
Moe is carrying and supporting a large crate by exerting 1000 N. He is walking at constant velocity across a level, horizontal floor. If he covers a distance of 10 meters, how much work does he do on the crate? Use g = 10m/s2 if needed. Ignore friction between Moe and the crate.
Answer:
he did not work on the create
Explanation:
Honestly I have no idea it makes a lot of sense to use the work equation so that was my first answer but for some reason on UT Quest it said that was the wrong and moe not doing any work on the create was the right answer
Final answer:
The work done by Moe on the crate is 10,000 J.
Explanation:
The work done by Moe on the crate can be calculated using the formula:
Work = Force x Distance x Cosine(theta)
Since Moe is exerting a force of 1000 N and the distance covered is 10 meters, we can plug these values into the formula:
Work = 1000 N x 10 m x Cosine(0°)
The angle theta is 0° because Moe is exerting a force in the same direction as the displacement.
Cosine(0°) is equal to 1, so the work done by Moe on the crate is:
Work = 1000 N x 10 m x 1 = 10,000 J
A rope is tied to a tree 4.5 feet from the ground and then run through a pulley hooked to a vehicle 33 feet from the tree. If a person stands at the tree and pulls ten feet of the rope (after all slack is taken up) how far will the vehicle move?
If a person pulls ten feet of the rope tied to a vehicle through a pulley, the vehicle will move the same distance, which is ten feet assuming ideal conditions with no slack or stretch in the system.
Explanation:The question is asking about how far a vehicle moves when a rope attached to it and run through a pulley is pulled a certain distance. This scenario can be understood using the principles of distance and leverage as applied in physics. When you pull a rope through a pulley, the movement or distance covered by the object attached to the rope is equivalent to the length of the rope pulled.
In this case, if a person pulls ten feet of the rope, the vehicle will also move ten feet. It's important to note that this is applicable under ideal conditions where the rope and pulley do not stretch or bend and the there is no slack in the system.
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You drop a rock off a bridge. When the rock has fallen 4 m, you drop a second rock. As the two rocks continue to fall, what happens to their velocities?
a. Both increase at the same rate.
b. The velocity of the first rock increases faster than the velocity of the second.
c. The velocity of the second rock increases faster than the velocity of the first.
d. Both velocities stay constant.
Answer:
option A.
Explanation:
The correct answer is option A.
Two rocks are off a bridge first rock is fallen 4 when the second rock is dropped.
Both the rock is dropped under the effect of acceleration due to gravity so, the rate of change of the velocity for both the rock particle will be the same.
Hence, the first rock will reach ground earlier than the second rock because the rate of change of both the rock is at the same rate.
At the time when the two rocks should continue to fall so their velocities should be increased.
The correct answer is option A.
Velocity:When two rocks are off a bridge so here first rock is fallen 4 at the time when the second rock should be fallen. Both the rock should be fallen under the impact of acceleration because of gravity due to which the rate of change of the velocity for both the rock particle should be similar.
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A 3 kg steel ball falls down vertically and strikes a floor with a speed of 12 m/s. It bounces off upward with the same speed. If the ball is in contact with the floor for 0.12 s, what is the magnitude of the average force exerted on the ball by the floor?
Answer:
600N
Explanation:
If the ball bounces off upward with the same speed, the velocities before and after are equal and in opposite directions. That means the floor must have caused a momentum impact to change its direction.
By the law of momentum conservation:
[tex]mv + \Delta P_f = mV[/tex]
where m = 3 kg is the ball mass. v = -12 m/s is the velocity right before the impact. V = 12m/s is the velocity right after the impact. ΔP_f is the momentum caused by the floor.
[tex]\Delta P_f = m(V-v) = 3(12 - (-12)) = 3*24 = 72kgm/s[/tex]
Then the average force exerted during the 0.12s impact is
[tex]F = \frac{\Delta P_f}{\Delta t} = \frac{72}{0.12} = 600N[/tex]
A 5 kg ball takes 13.3 seconds for one revolution around the circle. What's the magnitude of the angular velocity of this motion?
Answer: 0.47 rad/sec
Explanation:
By definition, the angular velocity is the rate of change of the angle traveled with time, so we can state the following:
ω = ∆θ/ ∆t
Now, we are told that in 13.3 sec, the ball completes one revolution around the circle, which means that, by definition of angle, it has rotated 2 π rad (an arc of 2πr over the radius r), so we can find ω as follows:
ω = 2 π / 13.3 rad/sec = 0.47 rad/sec
Answer:
0.472rad/s
Explanation:
Angular velocity = 2πf where f = frequency and frequency is the number of revolution per second and 2π represent a cycle of revolution. The mass of the body was 5kg, the time taken to complete a cycle was 13.3 s.
Frequency = 1/period where period is the time it takes to complete a revolution.
F = 1/13.3 = 0.075hz
Angular velocity = 2* 3.142* 0.075 = 0.472rad/s
A conducting sphere of radius r1= 0.38m has a total charge of Q=.75 uC. A second uncharged conducting sphere of radius r2= 0.28m is then connected to the first by a thin conducting wire. The spheres are separated by a very large distance to their size. What is the total charge on sphere two, Q2, in C?
Answer:
The Q₂ is 0.318 μC
Explanation:
The charge flows is the same on both, then:
[tex]V_{1} =\frac{kQ_{1} }{r_{1} } \\V_{2} =\frac{kQ_{2} }{r_{2} } \\Q_{2} =Q-Q_{1} \\\frac{kQ_{1} }{r_{1} } =\frac{k*(Q-Q_{1}) }{r_{2} } \\Q_{1} =\frac{\frac{Q}{r_{2} } }{(1/r_{1})+(1/r_{2}) }[/tex]
But:
[tex]\frac{1}{r_{1} } +\frac{1}{r_{2} }=\frac{1}{0.38} +\frac{1}{0.28} =6.2[/tex]
Q = = 0.75 μC
Replacing:
[tex]Q_{1} =\frac{\frac{0.75}{0.28} }{6.2} =0.432\mu C[/tex]
The Q₂ is equal:
Q₂ = 0.75 - 0.432 = 0.318 μC
The second conducting sphere, once connected and then disconnected from the first, ends up with the same charge as the first sphere, 0.75 µC or 0.75 x 10^-6 C.
Explanation:When two conducting spheres are connected by a thin conducting wire, the charge distributes itself evenly across both spheres, assuming both spheres are identical in size. In the case of spheres with different radii, the amount of charge on each sphere once they are separated again will still be proportional to the original amount. Since the two spheres in the question are described to be separated by a large distance relative to their size, the thin wire connecting them would create an equipotential surface, allowing the charge to redistribute.
The total charge Q is conserved in the system, thus the charge on the second sphere Q2 after disconnecting the wire would be the same as the initial total charge Q since it was not charged before. Therefore, the total charge on sphere two, Q2, will also be 0.75 μC or 0.75 x 10^{-6} C.
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Light is incident along the normal to face AB of a glass prism of refractive index 1.54. Find αmax, the largest value the angle α can have without any light being refracted out of the prism at face AC if the prism is immersed in water (with index of refraction 1.33). Express your answer in degrees. Ignore any reflections from the surface BC.
To solve this problem it is necessary to use the concepts related to Snell's law.
Snell's law establishes that reflection is subject to
[tex]n_1sin\theta_1 = n_2sin\theta_2[/tex]
Where,
[tex]\theta =[/tex] Angle between the normal surface at the point of contact
n = Indices of refraction for corresponding media
The total internal reflection would then be given by
[tex]n_1 sin\theta_1 = n_2sin\theta_2[/tex]
[tex](1.54) sin\theta_1 = (1.33)sin(90)[/tex]
[tex]sin\theta_1 = \frac{1.33}{1.54}[/tex]
[tex]\theta = sin^{-1}(\frac{1.33}{1.54})[/tex]
[tex]\theta = 59.72\°[/tex]
Therefore the [tex]\alpha_{max}[/tex] would be equal to
[tex]\alpha = 90\°-\theta[/tex]
[tex]\alpha = 90-59.72[/tex]
[tex]\alpha = 30.27\°[/tex]
Therefore the largest value of the angle α is 30.27°
The largest value the angle α can have without any light being refracted out of the prism at face AC is 30.27°.
How to calculate the angle?From the information given, the total internal reflection would be:
1.54sinb = (1.33) sin90°
sin b = (1.33 sin90° / 1.54)
b = 59.72°
Therefore, the value of the angle will be:
= 90° - 59.72°
= 30.27°
In conclusion, the correct option is 30.27°.
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What impulse occurs when an average force of 7.0 N is exerted on a cart for 2.5 s ?
Express your answer to two significant figures and include the appropriate units.
Answer:[tex]1.7\times 10[/tex]
Explanation:
Given
Force [tex]F=7 N[/tex]
time interval [tex]t=2.5 s[/tex]
Impulse is given by [tex]=Force \times time\ interval\ for\ applied\ force [/tex]
[tex]Impulse=7\times 2.5=17.5[/tex]
For two significant Figure
[tex]Impulse=1.7\times 10[/tex]
Three masses (3 kg, 5 kg, and 7 kg) are located in the xy-plane at the origin, (2.3 m, 0), and (0, 1.5 m), respectively.
A) Determine the center of mass of the system.
B) A 6 kg mass is added to the system. This four-mass system has a new center of mass at the origin. What is the location of the 6 kg mass?
Answer:
a) C.M [tex]=(\bar x, \bar y)=(0.767,0.7)m[/tex]
b) [tex](x_4,y_4)=(-1.917,-1.75)m[/tex]
Explanation:
The center of mass "represent the unique point in an object or system which can be used to describe the system's response to external forces and torques"
The center of mass on a two dimensional plane is defined with the following formulas:
[tex]\bar x =\frac{\sum_{i=1}^N m_i x_i}{M}[/tex]
[tex]\bar y =\frac{\sum_{i=1}^N m_i y_i}{M}[/tex]
Where M represent the sum of all the masses on the system.
And the center of mass C.M [tex]=(\bar x, \bar y)[/tex]
Part a
[tex]m_1= 3 kg, m_2=5kg,m_3=7kg[/tex] represent the masses.
[tex](x_1,y_1)=(0,0),(x_2,y_2)=(2.3,0),(x_3,y_3)=(0,1.5)[/tex] represent the coordinates for the masses with the units on meters.
So we have everything in order to find the center of mass, if we begin with the x coordinate we have:
[tex]\bar x =\frac{(3kg*0m)+(5kg*2.3m)+(7kg*0m)}{3kg+5kg+7kg}=0.767m[/tex]
[tex]\bar y =\frac{(3kg*0m)+(5kg*0m)+(7kg*1.5m)}{3kg+5kg+7kg}=0.7m[/tex]
C.M [tex]=(\bar x, \bar y)=(0.767,0.7)m[/tex]
Part b
For this case we have an additional mass [tex]m_4=6kg[/tex] and we know that the resulting new center of mass it at the origin C.M [tex]=(\bar x, \bar y)=(0,0)m[/tex] and we want to find the location for this new particle. Let the coordinates for this new particle given by (a,b)
[tex]\bar x =\frac{(3kg*0m)+(5kg*2.3m)+(7kg*0m)+(6kg*a)}{3kg+5kg+7kg+6kg}=0m[/tex]
If we solve for a we got:
[tex](3kg*0m)+(5kg*2.3m)+(7kg*0m)+(6kg*a)=0[/tex]
[tex]a=-\frac{(5kg*2.3m)}{6kg}=-1.917m[/tex]
[tex]\bar y =\frac{(3kg*0m)+(5kg*0m)+(7kg*1.5m)+(6kg*b)}{3kg+5kg+7kg+6kg}=0m[/tex]
[tex](3kg*0m)+(5kg*0m)+(7kg*1.5m)+(6kg*b)=0[/tex]
And solving for b we got:
[tex]b=-\frac{(7kg*1.5m)}{6kg}=-1.75m[/tex]
So the coordinates for this new particle are:
[tex](x_4,y_4)=(-1.917,-1.75)m[/tex]
A 200-Ω resistor is connected in series with a 10-µF capacitor and a 60-Hz, 120-V (rms) line voltage. If electrical energy costs 5.0¢ per kWh, how much does it cost to leave this circuit connected for 24 hours?
Answer:
Cost to leave this circuit connected for 24 hours is $ 3.12.
Explanation:
We know that,
[tex]\mathrm{X}_{\mathrm{c}}=\frac{1}{2 \pi \mathrm{fc}}[/tex]
f = frequency (60 Hz)
c= capacitor (10 µF = [tex]10^-6[/tex])
[tex]\mathrm{X}_{\mathrm{c}}=\text { Capacitive reactance }[/tex]
Substitute the given values
[tex]\mathrm{X}_{\mathrm{c}}=\frac{1}{2 \times 3.14 \times 10 \times 10^{-6} \times 60}[/tex]
[tex]\mathrm{X}_{\mathrm{c}}=\frac{1}{3.768 \times 10^{-3}}[/tex]
[tex]\mathrm{x}_{\mathrm{c}}=265.39 \Omega[/tex]
Given that, R = 200 Ω
[tex]X^{2}=R^{2}+X c^{2}[/tex]
[tex]X^{2}=200^{2}+265.39^{2}[/tex]
[tex]X^{2}=40000+70431.85[/tex]
[tex]X^{2}=110431.825[/tex]
[tex]x=\sqrt{110431.825}[/tex]
X = 332.31 Ω
[tex]\text { Current }(I)=\frac{V}{R}[/tex]
[tex]\text { Current }(I)=\frac{120}{332.31}[/tex]
Current (I) = 0.361 amps
“Real power” is only consumed in the resistor,
[tex]\mathrm{I}^{2} \mathrm{R}=0.361^{2} \times 200[/tex]
[tex]\mathrm{I}^{2} \mathrm{R}=0.1303 \times 200[/tex]
[tex]\mathrm{I}^{2} \mathrm{R}=26.06 \mathrm{Watts} \sim 26 \mathrm{watts}[/tex]
In one hour 26 watt hours are used.
Energy used in 54 hours = 26 × 24 = 624 watt hours
E = 0.624 kilowatt hours
Cost = (5)(0.624) = 3.12
A physics class conducting a research project on projectile motion constructs a device that can launch a cricket ball. The launching device is designed so that the ball can be launched at ground level with an initial velocity of 28 m/ s at an angle of 30° to the horizontal. Calculate the horizontal component of the velocity of the ball:a. initiallyb. after 1.0 sc. after 2.0 s
Answer:
Explanation:
initial velocity, u = 28 m/s
Angle of projection, θ = 30°
The acceleration in horizontal direction is zero, so the horizontal component of velocity is constant.
Horizontal component of velocity, u cos θ = 28 x Cos 30 = 24.25 m/s
At t = 2 sec, the horizontal component of velocity = 24.25 m/s
At t = 3 sec, the horizontal component of velocity = 24.25 m/s
In this exercise we have to use the knowledge about oblique launch to calculate the components of velocity for each case, so we have that:
For all times we will find a velocity equal to 24.25 m/s
organizing the information given in the statement we have that:
initial velocity, u = 28 m/sAngle of projection, θ = 30°The acceleration in horizontal direction is zerovelocity is constant.Knowing that the component can be written as:
[tex]u cos \theta = 28 * Cos 30 = 24.25 m/s[/tex]
So as the formula does not depend on time we have that for any value it will have a constant velocity.
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Consider the amideanion.What is the central atom? Enter its chemical symbol.How many lone pairs are around the central atom?What is the ideal angle between the nitrogen-hydrogen bonds?Compared to the ideal angle, you would expect the actual angle between the nitrogen-hydrogen bonds to be ...
Answer:
a) The central atom of the amide ion is nitrogen
b) (NH2)-
c) There are two lone pairs around the nitrogen atom
d) The ideal angle between nitrogen hydrogen bonds is 109.5° C, typical of a tetrahedral electron density arrangement
e) I would expect the nitrogen-hydrogen bond angles in the amide ion to be less than 109.5 ° because unbonded pairs repel bonded pairs much more than other bonded pairs do. So the bonds in this ion would be pushed closer together than normal
Sometime around 2022, astronomers at the European Southern Observatory hope to begin using the E-ELT(European Extremely Large Telescope), which is planned to have a primary mirror 42 m in diameter. Let us assume that the light it focuses has a wavelength of 600 nm. (1 light-year = 9.461×1015 m) Note: Jupiter's Diameter dj=1.43×108 m 1) What is the most distant Jupiter-sized planet the telescope could resolve, assuming it operates at the diffraction limit? (Express your answer to two significant figures.)
Answer:
[tex]8.2\times 10^{15}\ m[/tex]
Explanation:
[tex]\lambda[/tex] = Wavelength = 600 nm
d = Diameter of mirror = 42 m
D = Distance of object
x = Diameter of Jupiter = [tex]1.43\times 10^8\ m[/tex]
Angular resoulution is given by
[tex]\Delta\theta=1.22\frac{\lambda}{d}\\\Rightarrow \Delta\theta=1.22\frac{600\times 10^{-9}}{42}\\\Rightarrow \Delta\theta=1.74286\times 10^{-8}\ rad[/tex]
We also have the relation
[tex]\Delta\theta\approx=\frac{x}{D}\\\Rightarrow D\approx\frac{x}{\Delta\theta}\\\Rightarrow D\approx\frac{1.43\times 10^8}{1.74286\times 10^{-8}}\\\Rightarrow D\approx 8.2049\times 10^{15}\ m[/tex]
The most distant Jupiter-sized planet the telescope could resolve is [tex]8.2\times 10^{15}\ m[/tex]
A heating coil inside an electric kettle delivers 2.2 kW of electrical power to the water in the kettle. How long will it take to raise the temperature of 0.50 kg of water from 30.0° C to 72.0° C
Answer:
0.04s
Explanation:
Specific heat of water c = 4.186J/g.C
The heat energy it would take to heat up 0.5 kg of water from 30C to 72 C is
[tex]E = mc\Delta T = 0.5 * 4.186 * (72 - 30) = 87.9 J[/tex]
If the power of the electric kettle is 2.2kW (or 2200W) and suppose the work efficiency is 100%, then the time it takes to transfer that power is
[tex] t = \frac{E}{P} = \frac{87.9}{2200} = 0.04 s[/tex]
The auditory canal behaves like a resonant tube to aid in hearing. One end terminated at the eardrum, while the other opens to the outside. Typically, the canal is about 2.4 cm long. At which frequency would it resonate in its first harmonic?
4.2 kHz
3.6 kHz
2.9 kHz
5.7 kHz
Answer:
3.6 kHz
Explanation:
The pipes behave like a closed pipe . The end open is the end of the air canal outside the ear and the closed end is the eardrum.
The first harmonic will be as seen in the figure attached.
The length of the first harmonic will be λ/4.
λ/4=2.4 cm
λ=2.4 * 4=9.6 cm 0.096 m
Speed of Sound- 344 m/s(in air)
velocity(v) * Time Period(T) = Wavelength (λ)
Also, Time Period(T)= \frac{\textrm{1}}{\textrm{Frequency(f)}}
\frac{\textrm{Velocity}}{\textrm{Wavelength}}=\frac{\textrm{1}}{\textrm{Time Period}} =Frequency
Plugging in the values into the equation,
Frequency = [tex]\frac{344}{0.096}[/tex] Hz
= 3583.3 Hz≈3600 Hz= 3.6 kHz
Frequency= 3.6 kHz
Answer:
3.6 kHz
Explanation:
The auditory canal is a closed pipe because it has one closed end, the end terminated at the eardrum.
The length of the first harmonic of a closed pipe is given as;
L = λ/4 -------------------- (i)
where L = Length
and λ = wavelength
2.4 = λ/4
λ = 2.4 x 4 = 9.6 cm
Also, v = fλ ------------------ (ii)
where v = speed of sound in air = 344 m/s
f = frequency of wave in Hertz
f = v/λ ------------------ (iii)
convert 9.6 cm to m = 0.096 m
substitute for λ and v in (iii)
[tex]f = \frac{344}{0.096} = 3583.33[/tex]
3583.33 Hz = 3600 Hz = 3.6 kHz
Suppose that a simple pendulum consists of a small 81 g bob at the end of a cord of negligible mass. If the angle θ between the cord and the vertical is given by θ = (0.068 rad) cos[(9.2 rad/s) t + φ], what are (a) the pendulum's length and (b) its maximum kinetic energy?
Answer:
(a) 0.115 m
(b) 2.08 x 10^-5 J
Explanation:
mass of bob, m = 81 g = 0.081 kg
The equation of oscillation is given by
θ = 0.068 Cos {9.2 t + Ф}
Now by comparison
The angular velocity
ω = 9.2 rad/s
(a) [tex]\omega^{2} =\frac{g}{L}[/tex]
where, L be the length of the pendulum
[tex]L =\frac{g}{\omega ^{2}}[/tex]
[tex]L =\frac{9.8}{9.2 \times 9.2}[/tex]
L = 0.115 m
(b) A = L Sinθ
A = 0.115 x Sin 0.068
A = 7.8 x 10^-3 m
Maximum kinetic energy
K = 0.5 x mω²A²
K = 0.5 x 0.081 x 9.2 x 9.2 x 7.8 x 7.8 x 10^-6
K = 2.08 x 10^-5 J
At a certain location, Earth's magnetic field of 34 µT is horizontal and directed due north. Suppose the net field is zero exactly 8.1 cm above a long, straight, horizontal wire that carries a constant current. What are (a) the magnitude of the current and (b) the angle between the current direction and due north?
Answer:
a) I = 13.77 A
b) 0 ° or to the East
Explanation:
Part a
The magnetic field by properties would be 0 at the radius on this case r =8.1 cm.Analyzing the situation the wirde would produce a magnetic field equals in magnitude to the magnetic field on Earth by with the inverse direction.
The formula for the magnetic field due to a wire with current is:
[tex] B = \frac{\mu_0 I}{2 \pi r} [/tex]
In order to have a value of 0 for the magnetic field at the radius then we need to have this balance
B (r=8.1) = B (Earth)
Replacing:
[tex] B = \frac{\mu_0 I}{2 \pi r)}= B_{Earth} [/tex]
Solving from I, from the last equation we got:
[tex] I = \frac{2 \pi r B_{earth}}{\mu_0} [/tex]
[tex] I=\frac{2 \pi 0.081 m (34 x 10^{-6} T)}{4 \pi x 10^{-7} Tm/A}[/tex] = 13.77 A
Part b
We can use the right hand rule for this case.
The magnetic field of the wire would point to the South, because the magnetic field of the earth given points to the North. Based on this the current need's to flow from West to East in order to create a magnetic field pointing to the south, because the current would be perpendicular to the magnetic field created.
A mass of 0.56 kg is attached to a spring and set into oscillation on a horizontal frictionless surface. The simple harmonic motion of the mass is described by x(t) = (0.42 m)cos[(6 rad/s)t]. Determine the following. (a) amplitude of oscillation for the oscillating mass m (b) force constant for the spring N/m (c) position of the mass after it has been oscillating for one half a period m (d) position of the mass one-third of a period after it has been released m (e) time it takes the mass to get to the position x = −0.10 m after it has been released
Answer:
(a) 0.42 m
(b) 20.16 N/m
(c) - 0.42 m
(d) - 0.21 m
(e) 17.3 s
Solution:
As per the question:
Mass, m = 0.56 kg
x(t) = (0.42 m)cos[cos(6 rad/s)t]
Now,
The general eqn is:
[tex]x(t) = Acos\omega t[/tex]
where
A = Amplitude
[tex]\omega[/tex] = angular frequency
t = time
Now, on comparing the given eqn with the general eqn:
(a) The amplitude of oscillation:
A = 0.42 m
(b) Spring constant k is given by:
[tex]\omega = \sqrt{k}{m}[/tex]
[tex]\omega^{2} = \frac{k}{m}[/tex]
Thus
[tex]k = m\omega^{2} = 0.56\times 6^{2} = 20.16\ N/m[/tex]
(c) Position after one half period:
[tex]x(t) = 0.42cos\pi = - 0.42\ m[/tex]
(d) After one third of the period:
[tex]x(t) = 0.42cos(\frac{2\pi}{3}) = - 0.21\ m[/tex]
(e) Time taken to get at x = - 0.10 m:
[tex]-0.10 = 0.42cos6t[/tex]
[tex]6t = co^{- 1} \frac{- 0.10}{0.42}[/tex]
t = 17.3 s
The amplitude of oscillation is 0.42 m. The force constant of the spring is approximately 0.03 N/m. The position of the mass after one half a period, one-third of a period, and at x = -0.10 m can be determined using the given equation x(t).
Explanation:The amplitude of oscillation is the maximum displacement from the equilibrium position. In this case, the amplitude is given as 0.42 m.
The force constant (k) of the spring can be determined using Hooke's Law, which states that the force exerted by a spring is proportional to the displacement from equilibrium. In this case, the force constant is calculated by dividing the mass (0.56 kg) by the square of the angular frequency (6 rad/s) squared, which gives a force constant of approximately 0.03 N/m.
The position of the mass after it has been oscillating for one half a period can be found by substituting the value of time (T/2) into the equation x(t), which gives a position of approximately -0.42 m.
The position of the mass one-third of a period after it has been released can be determined by substituting the value of time (T/3) into the equation x(t), which gives a position of approximately 0.33 m.
The time it takes the mass to get to the position x = -0.10 m after it has been released can be found by rearranging the equation x(t) and solving for time. The time is approximately 0.14 seconds.
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