The description to the diagram and the concepts are as given below. The final angular speed of the disc-brick system is 235.8 rad/s. The kinetic energy of the system must increase to maintain the law of conservation of energy.
a) The description of the vector diagram for the angular momentum before and after placing the brick on the disc.
Before placing the brick on the disc:
The vector diagram for the angular momentum of the spinning disc consists of a vector representing the angular momentum, which is directed along the axis of rotation and has a magnitude given by the product of the moment of inertia and the angular speed. The magnitude of the vector is proportional to the length of the vector arrow.
After placing the brick on the disc:
After placing the brick on the edge of the disc, the angular momentum vector diagram will show an additional vector representing the angular momentum of the brick.
This vector will have a magnitude determined by the product of the moment of inertia of the brick and its angular speed. The direction of the vector will be the same as that of the disc's angular momentum vector.
b) The physics laws and concepts used to find the angular speed of the dise-brick system are the law of conservation of angular momentum, the moment of inertia, and the law of conservation of energy. The law of conservation of angular momentum states that angular momentum is conserved in a system in the absence of an external torque.
The moment of inertia of a rigid object depends on the distribution of mass in the object, relative to the axis of rotation. The moment of inertia for a solid disc is (1/2)MR².
The law of conservation of energy states that the energy of a system remains constant unless it is acted upon by a non-conservative force. In this case, the only non-conservative force acting on the system is the friction between the brick and the disc.
c) The initial angular momentum of the disc is given by:
L1 = Iω1
where I is the moment of inertia of the disc and ω1 is the initial angular speed of the disc.
L1 = (1/2)MR12ω1 = (1/2)(100)(1.6)²(25) = 4000 kg m²/s
The final angular momentum of the disc-brick system is:L2 = Iω2where ω2 is the final angular speed of the disc-brick system. The moment of inertia of the disc-brick system can be calculated as:I = (1/2)MR12 + MR22 = (1/2)(100)(1.6)² + (20)(1.6)² = 425.6 kg m²/sThe final angular momentum of the disc-brick system is:
L2 = Iω2L2 = (425.6)(ω2)
The law of conservation of angular momentum can be used to find the final angular speed of the disc-brick system.
L1 = L2Iω1 = (425.6)(ω2)ω2 = ω1I/I2ω2 = (25)(4000)/(425.6) = 235.8 rad/s
d) The kinetic energy of the system increases when the brick is placed on the disc. This is because the moment of inertia of the system increases, while the angular speed remains constant.
Therefore, the kinetic energy of the system must increase to maintain the law of conservation of energy.
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Current in a Loop uniform magnetic field, perpendicular to the plane of the coil, changes at a rate of 9.00E-3 T/s. Determine the current in A 35.0 cm diameter coil consists of 24 turns of circular copper wire 2.60 mm in diameter the loop Subrnit Answer Tries 0/12 Determine the rate at which thermal energy is produced.
The current flowing through the loop is approximately 0.992 Amperes. The rate of change of magnetic field is given as 9.00E-3 T/s. Therefore, the rate of change of magnetic flux is:
dΦ/dt = (9.00E-3 T/s) * 0.3848 m^2 = 3.4572E-3 Wb/s
The current in the loop can be determined by using Faraday's law of electromagnetic induction. According to the law, the induced electromotive force (emf) is equal to the rate of change of magnetic flux through the loop. The emf can be calculated as: ε = -N * dΦ/dt. where ε is the induced emf, N is the number of turns in the coil, and dΦ/dt is the rate of change of magnetic flux.The magnetic flux (Φ) through the loop is given by: Φ = B * A. where B is the magnetic field strength and A is the area of the loop.Given that the coil has a diameter of 35.0 cm and consists of 24 turns, we can calculate the area of the loop: A = π * (d/2)^2. where d is the diameter of the coil.
Substituting the values, we get: A = π * (0.35 m)^2 = 0.3848 m^2
The rate of change of magnetic field is given as 9.00E-3 T/s. Therefore, the rate of change of magnetic flux is:
dΦ/dt = (9.00E-3 T/s) * 0.3848 m^2 = 3.4572E-3 Wb/s
Now, we can calculate the induced emf:
ε = -N * dΦ/dt = -24 * 3.4572E-3 Wb/s = -0.08297 V/s
Since the coil is made of copper, which has low resistance, we can assume that the induced emf drives the current through the loop. Therefore, the current flowing through the loop is: I = ε / R
To calculate the resistance (R), we need the length (L) of the wire and its cross-sectional area (A_wire).The cross-sectional area of the wire can be calculated as:
A_wire = π * (d_wire/2)^2
Given that the wire diameter is 2.60 mm, we can calculate the cross-sectional area: A_wire = π * (2.60E-3 m/2)^2 = 5.3012E-6 m^2
The length of the wire can be calculated using the formula:
L = N * circumference
where N is the number of turns and the circumference can be calculated as: circumference = π * d
L = 24 * π * 0.35 m = 26.1799 m
Now we can calculate the resistance: R = ρ * L / A_wire
where ρ is the resistivity of copper (1.7E-8 Ω*m).
R = (1.7E-8 Ω*m) * (26.1799 m) / (5.3012E-6 m^2) = 8.3741E-2 Ω
Finally, we can calculate the current:
I = ε / R = (-0.08297 V/s) / (8.3741E-2 Ω) = -0.992 A
Therefore, the current flowing through the loop is approximately 0.992 Amperes.
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An undamped 1.92 kg horizontal spring oscillator has a spring constant of 21.4 N/m. While oscillating, it is found to have a speed of 2.56 m/s as it passes through its equilibrium position. What is its amplitude A of oscillation?
The amplitude of oscillation of an undamped 1.92 kg horizontal spring oscillator with a spring constant of 21.4 N/m and a speed of 2.56 m/s as it passes through its equilibrium position is 0.407 meters.
The amplitude of an oscillation is defined as the maximum displacement from the equilibrium position or mean position of the particle or object in oscillation.What is the formula for amplitude?The amplitude A of a particle in oscillation is given by:A = (2KE/mω2)1/2where KE is the kinetic energy of the particle,m is the mass of the particle, andω is the angular frequency of the oscillation.
The angular frequency is defined as the number of radians per second by which the object rotates or oscillates. It is usually represented by the symbol ω.What is the kinetic energy of the particle?The kinetic energy of the particle is given by:KE = 0.5mv2where m is the mass of the particle, andv is the velocity of the particle.
Given data,Mass of the oscillator, m = 1.92 kgSpring constant, k = 21.4 N/mSpeed of the oscillator, v = 2.56 m/sThe formula for the amplitude of oscillation is:A = (2KE/mω2)1/2The formula for the angular frequency of the oscillation is:ω = (k/m)1/2The formula for the kinetic energy of the particle is:KE = 0.5mv2Substitute the given values in the above formulas to get the value of amplitude as follows:
ω = (k/m)1/2
ω = (21.4 N/m ÷ 1.92 kg)1/2ω = 3.27 rad/s
KE = 0.5mv2
KE = 0.5 × 1.92 kg × (2.56 m/s)2
KE = 5.19 J
Now,A = (2KE/mω2)1/2
A = (2 × 5.19 J ÷ 1.92 kg × (3.27 rad/s)2)1/2
A = 0.407 m
Therefore, the amplitude of oscillation is 0.407 meters.
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DETAILS SERPSE 10 9.1.P.002. A 2.91 kg particle has a velocity of (3.05 1 - 4.08 ) m/s. (a) Find its x and y components of momentum. Px = kg-m/s Py = kg-m/s (b) Find the magnitude and direction of its momentum. kg-m/s (clockwise from the +x axis) Read It Need Help?
The x and y components of momentum are, Px = 8.85 kg-m/s and Py = -11.90 kg-m/s and the magnitude of momentum is 15.17 kg-m/s and the direction of momentum is -52.92° clockwise from the +x axis.
A 2.91 kg particle has a velocity of (3.05i - 4.08j) m/s.
Given, Mass of the particle, m = 2.91 kg
The velocity of the particle,
v = 3.05i - 4.08j m/s
.The formula for momentum is:
P = m*v= 2.91*3.05i + 2.91*(-4.08)j= 8.8495i - 11.9028j
Hence, the x and y components of momentum are:
Px = 8.85 kg-m/sPy = -11.90 kg-m/s
The magnitude of momentum can be calculated as
[tex]-|P| = sqrt(Px^2 + Py^2) = sqrt(8.85^2 + (-11.90)^2) = 15.17 kg-m/s[/tex]
The direction of momentum can be calculated as
[tex]-θ = tan^-1(Py/Px) = tan^-1(-11.90/8.85) = -52.92°[/tex]
The direction of momentum is clockwise from the +x axis, hence the direction of momentum is = -52.92° clockwise from the +x axis.
Thus, the x and y components of momentum are, Px = 8.85 kg-m/s and Py = -11.90 kg-m/s. The magnitude of momentum is 15.17 kg-m/s and the direction of momentum is -52.92° clockwise from the +x axis.
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A projectile is fired with an initial speed of 49.6 m/s at an angle of 42.2° above the horizontal on a long flat firing range. Determine the direction of the motion of the projectile 1.20 s after firing
1.20 seconds after firing, the projectile is moving upward and also in the positive x-direction horizontally.
To determine the direction of motion of the projectile 1.20 seconds after firing, we need to consider the vertical and horizontal components of its motion separately.
First, let's analyze the vertical component of motion. The projectile experiences a downward acceleration due to gravity. The vertical velocity of the projectile can be calculated using the formula:
v_vertical = v_initial * sin(theta)
where v_initial is the initial speed of the projectile and theta is the launch angle. Plugging in the given values:
v_vertical = 49.6 m/s * sin(42.2°)
v_vertical ≈ 33.08 m/s (upward)
Since the vertical velocity component is positive, the projectile is moving in an upward direction.
Next, let's consider the horizontal component of motion. The horizontal velocity of the projectile remains constant throughout its flight, assuming no air resistance. The horizontal velocity can be calculated using the formula:
v_horizontal = v_initial * cos(theta)
Plugging in the given values:
v_horizontal = 49.6 m/s * cos(42.2°)
v_horizontal ≈ 37.81 m/s (horizontal)
The horizontal velocity component is positive, indicating motion in the positive x-direction.
Therefore, 1.20 seconds after firing, the projectile is moving upward and also in the positive x-direction horizontally.
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Spiders may lunostrands of the webs to give enhanced response at troquencies corresponding to the frequencies at which des table prey might strog Ort web has a typical diameter of 0.0020 mm and spidsk has a density of 1300 kg/m To give a resonance at 190 Hz to what tonsion must in sp der adjusta 12 cm long strand of ?
The necessary tension in the 12 cm long strand of spider web to achieve resonance at 190 Hz is approximately 0.119 N.
To calculate the necessary tension in a 12 cm long strand of spider web to achieve resonance at 190 Hz, we can use the formula for the fundamental frequency of a vibrating string:
f = (1/2L) * sqrt(T/μ)
Where f is the frequency, L is the length of the string, T is the tension, and μ is the linear mass density (mass per unit length) of the string.
Given that the strand of spider web has a typical diameter of 0.0020 mm, we can calculate its linear mass density (μ) using the formula:
μ = (π * (d/2)^2 * ρ) / L
Where d is the diameter of the strand and ρ is the density of the spider silk.
Converting the diameter to meters and using the given density of 1300 kg/m³, we can substitute the values into the equation for μ.
Next, we rearrange the equation for the fundamental frequency to solve for the tension T:
T = (f * 2L * sqrt(μ))²
Substituting the values of f (190 Hz) and L (12 cm) into the equation, along with the calculated value of μ, we can solve for T, which represents the tension required to achieve resonance at 190 Hz.
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All three bulbs are identical and so are the two batteries.
Compare the brightness of the bulbs.
A.
A greater than B greater than C
b.
A greater than C greater than B
c.
A greater than B equals C
d
A
All three bulbs are identical and so are the two batteries. Comparing the brightness of the bulbs willkll be D. A less than B equals C
How to explain the informationIf all three bulbs are identical and so are the two batteries, then all three bulbs will be equally bright. The brightness of a light bulb is determined by the amount of current flowing through it, and the current flowing through each bulb will be the same since they are all connected in parallel. Therefore, all three bulbs will be equally bright.
The statement "A less than B equals C" is not relevant to the question of the brightness of the bulbs. It is possible that A, B, and C are all equally bright, in which case A would be less than B and equal to C. However, it is also possible that A, B, and C are not all equally bright, in which case A might be less than B but brighter than C.
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An RLC series circuit has a 3 Q resistor, a 354 mH inductor, and a 17.7 uF capacitor. If this is connected to a 178 Volt power supply, what will the rms current be at 362 Hz? Express your answer in mA
The rms current in the RLC series circuit at a frequency of 362 Hz will be approximately 0.358 A. To calculate the rms current in an RLC series circuit, then, we can divide the voltage (V) by the impedance (Z) to obtain the rms current (I).
The impedance of an RLC series circuit is given by the formula:
Z = √(R^2 + (XL - XC)^2)
Where:
R = Resistance = 3 Ω
XL = Inductive Reactance = 2πfL
XC = Capacitive Reactance = 1/(2πfC)
f = Frequency = 362 Hz
L = Inductance = 354 mH = 354 × 10^(-3) H
C = Capacitance = 17.7 μF = 17.7 × 10^(-6) F
Let's calculate the values:
XL = 2πfL = 2π(362)(354 × 10^(-3)) ≈ 1.421 Ω
XC = 1/(2πfC) = 1/(2π(362)(17.7 × 10^(-6))) ≈ 498.52 Ω
Now we can calculate the impedance:
Z = √(R^2 + (XL - XC)^2)
= √(3^2 + (1.421 - 498.52)^2)
≈ √(9 + 247507.408)
≈ √247516.408
≈ 497.51 Ω
Finally, we can calculate the rms current:
I = V / Z
= 178 / 497.51
≈ 0.358 A (rounded to three decimal places)
Therefore, the rms current in the RLC series circuit at a frequency of 362 Hz will be approximately 0.358 A.
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Question 2 1 pts Two particles are launched sequentially. Particle 1 is launched with speed 0.767c to the east. Particle 2 is launched with speed 0.506c to the north but at time 10.7ms later. After the second particle is launched, what is the speed of particle 2 as seen by particle 1 (as a fraction of c)?
The speed of particle 2 as seen by particle 1, after the second particle is launched, is approximately 0.662c.
To determine the speed of particle 2 as seen by particle 1, we need to apply the relativistic velocity addition formula. Let's denote the speed of particle 1 as v₁ and the speed of particle 2 as v₂.
The velocity addition formula is given by:
v = (v₁ + v₂) / (1 + (v₁ * v₂) / c²)
v₁ = 0.767c (speed of particle 1)
v₂ = 0.506c (speed of particle 2)
Using the formula, we can calculate the relative velocity:
v = (0.767c + 0.506c) / (1 + (0.767c * 0.506c) / c²)
= (1.273c) / (1 + 0.388462c² / c²)
= 1.273c / (1 + 0.388462)
≈ 0.662
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Several experiments are performed with light. Which of the following observations is not consistent with the wave model of light? a) The light can travel through a vacuum. b) The speed of the light is less in water than in air. c) The light can exhibit interference patterns when travelling through small openings. d) The beam of light travels in a straight line. e) The light can be simultaneously reflected and transmitted at certain interfaces.
Light has been a matter of extensive research, and experiments have led to various hypotheses regarding the nature of light. The two most notable hypotheses are the wave model and the particle model of light.
These models explain the behavior of light concerning the properties of waves and particles, respectively. Here are the observations for each model:a) Wave model: The light can travel through a vacuum.b) Wave model: The speed of the light is less in water than in air.c) Wave model
e) Wave model: The light can be simultaneously reflected and transmitted at certain interfaces.None of the observations contradicts the wave model of light. In fact, all the above observations are consistent with the wave model of light.The correct answer is d) The beam of light travels in a straight line. This observation is consistent with the particle model of light.
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A proton starts moving from rest in an electric field of magnitude 6.5x105 V/m. The field points in the positive
X-direction, and under the influence of the field, the proton moves 0.25 m in that direction.
a. What is the change in the proton's electric potential as a result of the displacement?
b. What is the change in the proton's electric potential energy due to the displacement?
c. What is the speed of the proton after it has moved 0.25 m, beginning from rest?
The magnitude of electric field that proton is subjected to is 6.5×10^5 V/m. Therefore, electric potential of proton at initial position is E₀ = 0. As proton moves in electric field by a distance d = 0.25 m in the direction of the field, its electric potential changes by an amount ΔV.
Proton, being a charged particle, is subjected to electric field when placed in the vicinity of another charged particle. The electric field exerts force on proton, causing it to move in a certain direction. In this question, proton is placed in an electric field of magnitude 6.5x10^5 V/m that points in positive X-direction. The proton moves 0.25 m in the direction of the field due to the influence of the field.The change in the proton's electric potential as a result of displacement is given by V = E x d, where V is change in the electric potential energy of proton, E is the electric field, and d is the displacement of the proton.
Initially, proton's electric potential is 0, as it is at rest, and as it moves by a distance of 0.25 m, its electric potential changes by an amount ΔV = V - E₀ = E x d = 6.5 x 10⁵ V/m x 0.25 m = 1.6 x 10^5 V. Therefore, change in electric potential of proton is 1.6 x 10^5 V.Using the equation, ΔPE = qΔV, we can calculate the change in electric potential energy of proton. Here, q is the charge of proton which is equal to 1.6 x 10⁻¹⁹ C. Hence, ΔPE = 1.6 x 10⁻¹⁹ C x 1.6 x 10^5 V = 2.56 x 10⁻¹⁴ J.
Therefore, change in electric potential energy of proton is 2.56 x 10⁻¹⁴ J.Finally, using the equation, v = √2KE/m, where KE is kinetic energy and m is mass, we can obtain the speed of proton after it has moved by 0.25 m. As proton starts from rest, KE = 0 initially. Therefore, KE = ΔPE = 2.56 x 10⁻¹⁴ J. Mass of proton is 1.67 x 10⁻²⁷ kg. Using these values, we can calculate the speed of proton which is 5.01 x 10⁶ m/s.
Therefore, the change in the proton's electric potential due to displacement is 1.6 x 10^5 V, and change in the proton's electric potential energy due to displacement is 2.56 x 10⁻¹⁴ J. The speed of proton after moving 0.25 m from rest in electric field of magnitude 6.5 x 10⁵ V/m is 5.01 x 10⁶ m/s.
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A bowling ball of mass 6.75 kg is rolling at 2.52 m/s along a level surface. (a) Calculate the ball's translational kinetic energy. (b) Calculate the ball's rotational kinetic energy. 23] (c) Calculate the ball's total kinetic energy. ] (d) How much work would have to be done on the ball to bring it to rest?
In this scenario, a bowling ball with a mass of 6.75 kg is rolling at a speed of 2.52 m/s along a level surface.
The task is to calculate the ball's translational kinetic energy (Part a), rotational kinetic energy (Part b), total kinetic energy (Part c), and the amount of work required to bring the ball to rest (Part d).
Part a: The translational kinetic energy of the ball can be calculated using the equation KE_trans = (1/2) * m * v², where KE_trans is the translational kinetic energy, m is the mass of the ball, and v is its velocity.
Part b: The rotational kinetic energy of the ball can be determined using the equation KE_rot = (1/2) * I * ω², where KE_rot is the rotational kinetic energy, I is the moment of inertia of the ball, and ω is its angular velocity. For a solid sphere, the moment of inertia is given by I = (2/5) * m * r², where r is the radius of the ball.
Part c: The total kinetic energy of the ball is the sum of its translational and rotational kinetic energies: KE_total = KE_trans + KE_rot.
Part d: To bring the ball to rest, work must be done to remove its kinetic energy. The work required can be calculated as W = KE_total. Therefore, the work done on the ball to bring it to rest is equal to its total kinetic energy.
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According to Lenz's law,
the induced current in a circuit must flow in such a direction to oppose the magnetic flux.
the induced current in a circuit must flow in such a direction to oppose the change in magnetic flux.
the induced current in a circuit must flow in such a direction to enhance the change in magnetic flux.
the induced current in a circuit must flow in such a direction to enhance the magnetic flux.
There is no such law, the prof made it up specifically to fool gullible students that did not study.
Lenz's law is a basic principle of electromagnetism that specifies the direction of induced current that is produced by a change in magnetic field. According to Lenz's law, the direction of the induced current in a circuit must flow in such a way as to oppose the change in magnetic flux.
In other words, the induced current should flow in such a way that it produces a magnetic field that opposes the change in magnetic field that produced the current. This concept is based on the conservation of energy and the principle of electromagnetic induction.
Lenz's law is an important principle that has many practical applications, especially in the design of electrical machines and devices.
For example, Lenz's law is used in the design of transformers, which are devices that convert electrical energy from one voltage level to another by using the principles of electromagnetic induction.
Lenz's law is also used in the design of electric motors, which are devices that convert electrical energy into mechanical energy by using the principles of electromagnetic induction.
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Ignoring the motion of the sun within the Milky Way, calculate the total kinetic energy of the earth as it goes around the sun and rotates around its own axis. Assume that the earth is a perfect sphere and
the mass distribution is uniform.
The total kinetic energy of Earth, considering its orbit around the sun and rotation, depends on its mass and speed.
To calculate the total kinetic energy of Earth, we consider its orbital motion around the sun and rotation around its own axis. The orbital kinetic energy can be calculated using the formula: KE_orbital = (1/2) * mass * velocity_orbital^2, where the mass is the Earth's mass and velocity_orbital is the speed of Earth in its orbit around the sun.
For the rotational kinetic energy, we use the formula: KE_rotational = (1/2) * moment_of_inertia * angular_velocity^2, where the moment_of_inertia is specific to the Earth's shape (a uniform sphere) and
angular_velocity is the rotational speed of Earth. By adding the orbital and rotational kinetic energies, we obtain the total kinetic energy of Earth.
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a particle with a mass of 1.00 × 10−20 kg is oscillating with simple harmonic motion with a period of 1.00 × 10−5 s and a maximum speed of 1.00 × 103 m/s. calculate (a) the angular frequency and (b) the maximum displacement of the particle.
The angular frequency of the particle is 2π × 10^5 rad/s, and the maximum displacement is approximately 0.005 meters.
(a) The angular frequency (ω) can be calculated using the formula ω = 2π/T, where T is the period of oscillation.
Given:
Mass of the particle (m) = 1.00 × 10^(-20) kg
Period of oscillation (T) = 1.00 × 10^(-5) s
Using the formula, we have:
ω = 2π/T = 2π/(1.00 × 10^(-5)) = 2π × 10^5 rad/s
Therefore, the angular frequency is 2π × 10^5 rad/s.
(b) The maximum displacement (A) of the particle can be determined using the formula A = vmax/ω, where vmax is the maximum speed of the particle.
Given:
Maximum speed of the particle (vmax) = 1.00 × 10^3 m/s
Angular frequency (ω) = 2π × 10^5 rad/s
Using the formula, we have:
A = vmax/ω = (1.00 × 10^3)/(2π × 10^5) ≈ 0.005 m
Therefore, the maximum displacement of the particle is approximately 0.005 meters.
The angular frequency of the particle is 2π × 10^5 rad/s, and the maximum displacement is approximately 0.005 meters.
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1. An 8-m-long double pipe heat exchanger is constructed of 4 -std. type M and 3 std type M copper tubing. It is used to cool unused engine oil. The exchanger takes water into the annulus at 10 ∘ C at a rate of 2.Ykg/s, which exits at 10.7 ∘ C, and oil into the pipe at 140 ∘ C at a rate of 0.2 kg/s. Determine the expected outlet temperature of the oil. Assume counter flow.
The expected outlet temperature of oil is 48.24°C.
Given Data:
Length of heat exchanger, L = 8 m
Mass flow rate of water, mw = 2.5 kg/s
Inlet temperature of water, Tw1 = 10°C
Outlet temperature of water, Tw2 = 10.7°C
Mass flow rate of oil, mo = 0.2 kg/s
Inlet temperature of oil, To1 = 140°C (T1)
Type of copper tube, Std. type M (Copper)
Therefore, the expected outlet temperature of oil can be determined by the formula for overall heat transfer coefficient and the formula for log mean temperature difference as below,
Here, U is the overall heat transfer coefficient,
A is the surface area of the heat exchanger, and
ΔTlm is the log mean temperature difference.
On solving the above equation we can determine ΔTlm.
Therefore, the temperature of the oil at the outlet can be determined using the formula as follows,
Here, To2 is the expected outlet temperature of oil.
Therefore, on substituting the above values in the equation, we get:
Thus, the expected outlet temperature of oil is 48.24°C.
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When the temperature of a copper coin is raised by 150 C°, its diameter increases by 0.26%. To two significant figures, give the percent increase in (a) the area of a face, (b) the thickness, (c) the volume, and (d) the mass of the coin. (e) Calculate the coefficient of linear
expansion of the coin.
(a) The percent increase in the area of a face is approximately 0.52%.
(b) The percent increase in the thickness is approximately 0.26%.
(c) The percent increase in the volume is approximately 0.78%.
(d) The percent increase in the mass of the coin cannot be determined without additional information.
(e) The coefficient of linear expansion of the coin is approximately 1.73 x 10^-5 C^-1.
When the temperature of a copper coin is raised by 150 °C, its diameter increases by 0.26%. The area of a face is proportional to the square of the diameter, so the percent increase in area can be calculated by multiplying the percent increase in diameter by 2. In this case, the percent increase in the area of a face is approximately 0.52%.
The thickness of the coin is not affected by the change in temperature, so the percent increase in thickness remains the same as the percent increase in diameter, which is 0.26%.
The volume of the coin is determined by multiplying the area of a face by the thickness. Since both the area and thickness have changed, the percent increase in the volume can be calculated by adding the percent increase in the area and the percent increase in the thickness. In this case, the percent increase in the volume is approximately 0.78%.
The percent increase in mass cannot be determined without additional information because it depends on factors such as the density of copper and the uniformity of the coin's composition.
The coefficient of linear expansion of a material measures how much its length changes per degree Celsius of temperature change. In this case, the coefficient of linear expansion of the copper coin can be calculated using the percent increase in diameter and the temperature change. The coefficient of linear expansion is approximately 1.73 x 10^-5 C^-1.
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Problem 2 (10 points) Earth has a radius of 6.38 x 106m. Its mass is 5.98 x 1024 kg. Ignoring the atmosphere, if we fire a projectile from a mountain top fast enough that it will orbit just over the surface of the planet, how fast would you have to fire it for this to happen? If instead you wanted to fire the projectile so that it escapes from Earth's' gravitational pull, what initial velocity would you need?
To achieve a circular orbit just over the surface of the planet, the projectile must have a specific velocity.
Using the equation for circular motion, v² = GM / r, where G is the gravitational constant, M is the mass of the Earth, and r is the radius of the Earth, we can calculate the required velocity.
Substituting the given values into the equation, we have v² = (6.67 x 10^-11 Nm²/kg² x 5.98 x 10^24 kg) / (6.38 x 10^6 m)². Simplifying this expression yields v² = 398600.5 m²/s². Taking the square root of both sides, we find that v ≈ 6301.9 m/s.
Therefore, in order for the projectile to orbit just over the surface of the planet, it needs to be fired with an initial velocity of approximately 6301.9 m/s.
If, on the other hand, we want the projectile to escape from the Earth's gravitational pull, we need to determine the escape velocity. The escape velocity is the speed required for an object to overcome the gravitational force and break free from the planet's gravitational field.
Using the escape velocity formula v = √(2GM / r), where G, M, and r are the same as before, we can calculate the escape velocity. Substituting the values into the equation, we have v = √(2 x 6.67 x 10^-11 Nm²/kg² x 5.98 x 10^24 kg / 6.38 x 10^6 m). Simplifying this expression, we find that v ≈ 11186 m/s.
Hence, to escape from the Earth's gravitational pull, the projectile must be fired with an initial velocity of approximately 11186 m/s.
In summary, to orbit just over the surface of the planet, the projectile needs an initial velocity of 6301.9 m/s, while to escape from the Earth's gravitational pull, it requires an initial velocity of 11186 m/s.
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A
car engina buns 7 kg fuel at 1,648 K and rejects energy to the
radiator and the exhaust at an average temperature of 543k. if the
fuel provides 34296 kJ/kg whaf is the max amount of work the engine
The maximum amount of work the engine can do is 76.68 kJ.
The maximum amount of work that can be done by the engine is given as;
Wmax = Qin(1- T2/T1)
where T2 = lower temperature
T1 = higher temperature
mf = 7 kg (mass of fuel burned)
hf = 34296 kJ/kg (specific enthalpy of fuel)
h1 = 34296 kJ/kg (specific enthalpy of fuel at high temperature)
h2 = 136 kJ/kg (specific enthalpy of fuel at low temperature)
T1 = 1648 K (higher temperature)
T2 = 543 K (lower temperature)
Substituting the values in the equation, we get;
Qin = mf × hf= 7 kg × 34296 kJ/kg = 240072 kJ
Qout = m (h1-h2)= 7 kg (34296-136) kJ/kg= 240052 kJ
W = Qin - Qout= 240072 - 240052= 20 kJ
Maximum work done by the engine,
Wmax = Qin(1- T2/T1)= 240072 (1- 543/1648)= 76680 J = 76.68 kJ∴
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Two vectors 10N and 8N on bearing 285° and N70°E
respectively, act on a body. Find the resultant force
and direction of motion of the body using the triangle
of vectors.
The resultant force is 12.6N at a bearing of 3°W of N. The direction of motion of the body is the same as the direction of the resultant force, which is 3°W of N.
A triangle of vectors can be used to solve vector addition problems, such as determining the resultant force and direction of motion of a body acted upon by two or more vectors.
Let's use this method to solve the given problem: Two vectors, 10N and 8N, act on a body on bearings 285° and N70°E respectively.
Using the triangle of vectors, we can determine the resultant force and direction of motion of the body.
1. Draw a diagram to scale, showing the two vectors and their respective bearings.
2. Begin by drawing the first vector, 10N, from the origin at bearing 285°.
3. Draw the second vector, 8N, from the end of the first vector at bearing N70°E.
4. Draw the third vector, the resultant force, from the origin to the end of the second vector.
5. Use a protractor and ruler to measure the magnitude and bearing of the resultant force.
The diagram is shown below: Triangle of vectors diagram using the two vectors 10N and 8N, with bearings 285° and N70°E respectively.
The third vector, the resultant force, is drawn from the origin to the end of the second vector.
The magnitude and bearing of the resultant force are found using a protractor and ruler.
6. Measure the magnitude of the resultant force using the ruler.
In this case, the magnitude is approximately 12.6N.
7. Measure the bearing of the resultant force using the protractor.
In this case, the bearing is approximately 3°W of N.
Therefore, the resultant force is 12.6N at a bearing of 3°W of N.
The direction of motion of the body is the same as the direction of the resultant force, which is 3°W of N.
Therefore, the body will move in this direction.
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Two equal-mass hockey pucks undergo a glancing collision. Puck 1 is initially at rest and is struck by puck 2 travelling at a velocity of 13 m/s [E]. Puck 1 travels at an angle of [E 18 N] with velocity of 20 m/s . what is the velocity and direction of puck 2
Two equal mass hockey pucks are undergoing a glancing collision. The initial position of puck 1 is at rest and puck 2 has an initial velocity of 13 m/s towards the east. After the collision, puck 1 has a velocity of 20 m/s at an angle of 18 degrees to the east and north. We are supposed to determine the final velocity and direction of puck 2.
After the collision, the two pucks separate at angles to each other. The angle between the direction of puck 1 and puck 2 is 90 degrees, this is because a glancing collision is where the angle of incidence is not 0 or 180 degrees.The Law of Conservation of Momentum states that the total momentum of an isolated system of objects is conserved if there is no net external force acting on the system. That is, the total momentum before the collision is equal to the total momentum after the collision.
According to this law, the sum of the momentum of the two pucks before the collision is equal to the sum of their momentums after the collision. We can then write the following equation:
(m1 * v1) + (m2 * v2) = (m1 * vf1) + (m2 * vf2)
Where m is the mass of the puck, v is its initial velocity, and vf is its final velocity. We are given that the two pucks are of equal mass, therefore m1 = m2.
Substituting the values, we get:
(m1 * 0) + (m2 * 13 m/s) = (m1 * 20 m/s * cos 18) + (m2 * vf2)
Since the pucks are equal in mass, we can simplify the above equation as:
13 m/s = 20 m/s * cos 18 + vf2
The final velocity of puck 2 can be found by solving for vf2, giving:
vf2 = 13 m/s - 20 m/s * cos 18 vf2 = -4.24 m/s
The negative sign indicates that the final velocity of puck 2 is in the opposite direction to its initial velocity. Therefore, the final velocity and direction of puck 2 are: 4.24 m/s to the west.
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To fit a contact lens to a patient's eye, a keratometer can be used to measure the curvature of the cornea-the front surface of the eye. This instrument places an illuminated object of known size at a known distance p from the cornea, which then reflects some light from the object, forming an image of it. The magnification M of the image is measured by using a small viewing telescope that allows a comparison of the image formed by the cornea with a second calibrated image projected into the field of view by a prism arrangement. Determine the radius of curvature of the cornea when p=34.0 cm and M=0.0180.
The radius of curvature of the cornea is 7.53 mm.
To determine the radius of curvature of the cornea, we can use the relationship between the magnification (M), the distance between the object and the cornea (p), and the radius of curvature (R) of the cornea. The magnification can be expressed as M = (1 - D/f), where D is the distance between the calibrated image and the viewing telescope and f is the focal length of the prism arrangement.
Given that M = 0.0180, we can substitute this value into the magnification equation. By rearranging the equation, we can solve for D/f.Next, we need to consider the geometry of the system. The distance D is related to the distance p and the radius of curvature R through the equation D = 2R(p - R)/(p + R).By substituting the known values of M = 0.0180 and p = 34.0 cm into the equation, we can solve for D/f. Once we have D/f, we can solve for R by substituting the values of D/f and p into the geometry equation. After performing the calculations, the radius of curvature of the cornea is found to be approximately 7.53 mm.
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Write the complete decay equation for the given mucide in the computeXw notation Mater to the periodic table for vares of 2 decay of a naturally occurrin e isotope of tum reponible for some of our poure to begund nation
Alpha particle (4/2 He) + Thorium (Z/90 Th) ⟶ Radium (Z/88 Ra) + Alpha particle (4/2 He)
The complete decay equation for the given isotope of thorium (Th) undergoing alpha decay and producing a nuclide of radium (Ra) can be represented in the computeXw notation as follows:
α(4/2 He) + (Z/90 Th) ⟶ (Z/88 Ra) + α(4/2 He)
In this equation, α represents an alpha particle, which consists of 4 units of atomic mass and 2 units of atomic charge (helium nucleus), and (Z/90 Th) represents the parent thorium nucleus with atomic number Z = 90. The resulting nuclide is (Z/88 Ra), the daughter radium nucleus with atomic number Z = 88. The alpha particle is also emitted in the decay process, as represented by α(4/2 He).
Hence, the decay equation for the given isotope can be written as:
Alpha particle (4/2 He) + Thorium (Z/90 Th) ⟶ Radium (Z/88 Ra) + Alpha particle (4/2 He)
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How far from a wire carrying a current of 5 Amps is a second, parallel wire with a a current of 10 Amps, if the Magnetic Force of wire 1 on wire 2 is 3.6 x 10-2 N and each wire is 36 meters long. Include a picture and all 3 vectors on both wires,
If the Magnetic Force of wire 1 on wire 2 is 3.6 x 10-2 N and each wire is 36 meters long then, the two parallel wires must be 2 meters apart from each other.
The formula to calculate the magnetic force between two parallel conductors is given as : F = µI₁I₂l / 2πd
where
F is the magnetic force
µ is the permeability of free space, µ = 4π x 10-7 TmA-1
I₁ is the current flowing in the first conductor
I₂ is the current flowing in the second conductor
l is the length of the conductors
d is the distance between the conductors
In the given problem, we have :
I₁ = 5 Amps ; I₂ = 10 Amps ; F = 3.6 x 10-2 N ; l = 36 meters
The value of permeability of free space, µ = 4π x 10-7 TmA-1
We can rearrange the above formula to find the value of d as : d = µI₁I₂l / 2πF
Substituting the given values, we get, d= 2m
Therefore, the two parallel wires must be 2 meters apart from each other.
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What is the activity (in Bq) of a sample of Cs-137 if 31.6 years
ago it was recorded to have an activity of 9932.8 Bq.
To calculate the activity of a sample of Cs-137 after a certain time, we need to consider its half-life. Cs-137 has a half-life of 30.17 years. The activity of the Cs-137 sample is approximately 6437.2 Bq.
Given that the Cs-137 sample had an initial activity of 9932.8 Bq 31.6 years ago, we can calculate the current activity by using the half-life of Cs-137, which is 30.17 years.
The formula to calculate the current activity is: A = A₀ × (1/2)^(t/t₁/₂), where A is the current activity, A₀ is the initial activity, t is the time elapsed, and t₁/₂ is the half-life.
Substituting the values into the formula, we have:
A = 9932.8 Bq × (1/2)^(31.6/30.17)
Calculating this expression, we find that the current activity of the Cs-137 sample is approximately 6437.2 Bq.
Therefore, the activity of the Cs-137 sample, 31.6 years after it was recorded to have an activity of 9932.8 Bq, is approximately 6437.2 Bq.
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2. Describe what happens when a transverse wave travels from a low density medium to a high density medium. (3 marks)
When a transverse wave travels from a low density medium to a high density medium, it undergoes reflection and inversion of the wave.
When a wave travels from one medium to another medium, the wave undergoes a change in its speed and direction of propagation. It also undergoes reflection and inversion, if there is a boundary present between the two media. The direction of propagation changes at the boundary surface of two media due to the variation of refractive indices of two media. The wave inversion occurs at the boundary surface of two media. So, when a transverse wave travels from a low density medium to a high density medium, it undergoes reflection and inversion of the wave.The inversion of the wave is when the wave goes from an upside-down position to a right-side-up position.
This is what happens when the wave goes from a lower density medium to a higher density medium. When the wave hits the boundary between the two media, it is reflected back in the opposite direction, with the same frequency and wavelength. The speed of the wave is determined by the medium through which it is traveling, so when the wave hits the boundary, it slows down as it enters the higher density medium.
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A salad spinner has an internal 0.15-m radius spinning basket that spins at 26 rad/s to remove water from salad
greens. The basket has a rotational inertia of 0.1 kg-m?. To stop the basket, a piece of rubber is pressed against the outer edge of the basket, slowing it through friction. If
rubber is pressed into the outer edge with a force of 5 N, and the coefficient of kinetic friction between the rubber and the basket is 0.35, how long does it take for
the basket to stop?
The time it takes for the salad spinner basket to stop is approximately 6.19 seconds.
To calculate the time it takes for the salad spinner basket to stop, we need to consider the torque produced by the frictional force applied to the outer edge of the basket. The torque will cause the angular acceleration, which will gradually reduce the angular velocity of the basket until it comes to a stop.
The torque produced by the frictional force can be calculated using the equation τ = μ * F * r, where τ is the torque, μ is the coefficient of kinetic friction, F is the applied force, and r is the radius of the spinning basket.
The radius of the basket is 0.15 m, the coefficient of kinetic friction is 0.35, and the force applied is 5 N, we can calculate the torque as follows: τ = 0.35 * 5 N * 0.15 m.
Next, we can use the rotational inertia of the basket to relate the torque and angular acceleration. The torque is equal to the product of the rotational inertia and the angular acceleration, τ = I * α.
Rearranging the equation, we have α = τ / I.
Plugging in the values, α = (0.35 * 5 N * 0.15 m) / 0.1 kg-m².
Finally, we can use the formula to find the time it takes for the angular velocity to reduce to zero, given by ω = ω₀ + α * t, where ω is the final angular velocity, ω₀ is the initial angular velocity, α is the angular acceleration, and t is the time.
Since the final angular velocity is zero, we have 0 = 26 rad/s + (0.35 * 5 N * 0.15 m) / 0.1 kg-m² * t.
Solving for t, we find t = -26 rad/s / [(0.35 * 5 N * 0.15 m) / 0.1 kg-m²]. Note that the negative sign is because the angular velocity decreases over time.
Calculating the value, we get t ≈ -6.19 s. Since time cannot be negative, the time it takes for the basket to stop is approximately 6.19 seconds.
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A 1kg ball is fired from a cannon. What is the change in the
ball’s kinetic energy when it accelerates form 4.0 m/s2
to 8 m/s2?"
The change in the ball's kinetic energy when it accelerates from 4.0 m/s^2 to 8 m/s^2 is 64 Joules.
To calculate the change in kinetic energy, we need to determine the initial and final kinetic energies and then find the difference between them.
The formula for kinetic energy is given by:
Kinetic Energy = [tex](1/2) * mass * velocity^2[/tex]
Mass of the ball (m) = 1 kg
Initial acceleration (a₁) = 4.0 m/s²
Final acceleration (a₂) = 8 m/s²
Let's calculate the initial and final velocities using the formula of accelerated motion:
v = u + a * t
For initial velocity:
u = 0 (assuming the ball starts from rest)
a = a₁ = 4.0 m/s²
t = 1 second (arbitrary time interval for convenience)
Using the formula, we find:
v₁ = u + a₁ * t
v₁ = 0 + 4.0 * 1
v₁ = 4.0 m/s
For final velocity:
u = v₁ (the initial velocity is the final velocity from the previous calculation)
a = a₂ = 8 m/s²
t = 1 second (again, an arbitrary time interval for convenience)
Using the formula, we find:
v₂ = u + a₂ * t
v₂ = 4.0 + 8 * 1
v₂ = 12.0 m/s
Now, we can calculate the initial and final kinetic energies using the formula mentioned earlier:
Initial Kinetic Energy (KE₁) = (1/2) * m * v₁^2
KE₁ = (1/2) * 1 * 4.0^2
KE₁ = 8.0 J (Joules)
Final Kinetic Energy (KE₂) = (1/2) * m * v₂^2
KE₂ = (1/2) * 1 * 12.0^2
KE₂ = 72.0 J (Joules)
Finally, we can determine the change in kinetic energy:
Change in Kinetic Energy = KE₂ - KE₁
Change in Kinetic Energy = 72.0 J - 8.0 J
Change in Kinetic Energy = 64.0 J (Joules)
Therefore, the change in the ball's kinetic energy when it accelerates from 4.0 m/s² to 8 m/s² is 64.0 Joules.
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Consider a person traveling a distance of 300 km (with respect to the ground) in a relativistic car on a straight highway. Assume event A is when the car has gone 0 km of distance and event B is when the car has reached its destination. You only need to draw one diagram for parts e-g. Case 1: The car is traveling at a speed of 4.32 x108 km/hr. (a) Determine the velocity of the person in SR Units. (b) Determine the distance (with respect to the earth) traveled in SR units (c) Determine the time for the trip as measured by someone on the earth. (d) Determine the car's space-time interval. (e) Carefully draw and label a spacetime diagram for the car with respect to a person on the ground using the graph paper provided and a straight edge. (Note: this should not be a two- observer diagram) Make the diagram as accurate as possible. Make the diagram big enough to read and big enough to add another worldline. (f) When does a person on the ground see the car reach its destination. Draw a labeled worldline to support your answer. Case 2: If the car instead accelerated from rest to reach point B. (g) Draw a possible worldline for the car using a dashed line ("---") on your spacetime the diagram in part e). Considering Cases 1 and 2: (h) In which case(s) does a clock attached to the car measure proper time? Explain briefly. (i) In which case(s) does a clock attached to the car measure spacetime interval? Explain briefly. (j) In which case(s) does a clock attached to the car measure coordinate time? Explain
In both cases, the clock attached to the car measures coordinate time, which is the time measured by a single clock in a given frame of reference.
Given that,Distance traveled by the car = 300 km = 3 × 10² km
Speed of the car = 4.32 × 10⁸ km/hr
Case 1:
(a) Velocity of the person in SR Units
The velocity of the car in SI unit = (4.32 × 10⁸ × 1000) / 3600 m/s = 120,000 m/s
The velocity of the person = 0 m/s
Relative velocity = v/c = (120,000 / 3 × 10⁸) = 0.4 SR Units
(b) Distance (with respect to the earth) traveled in SR units
Proper distance = L = 300 km = 3 × 10² km
Proper distance / Length contraction factor L' = L / γ = (3 × 10²) / (1 - 0.4²) = 365.8537 km
Distance traveled in SR Units = L' / (c x T) = 365.8537 / (3 × 10⁸ x 0.4) = 3.0496 SR Units
(c) Time for the trip as measured by someone on the earth
Time interval, T = L' / v = 365.8537 / 120000 = 0.003048 SR Units
Time measured by someone on Earth = T' = T / γ = 0.004807 SR Units
(d) Car's space-time interval
The spacetime interval, ΔS² = Δt² - Δx²
where Δt = TΔx = v x TT = 0.003048 SR Units
Δx = 120000 × 0.003048 = 365.76 km
ΔS² = (0.003048)² - (365.76)² = - 133,104.0799 SR Units²
(e) Spacetime diagramCase 2:If the car instead accelerated from rest to reach point B.(g) The possible worldline for the car using a dashed line ("---")Considering Cases 1 and 2:(h) In which case(s) does a clock attached to the car measure proper time? Explain briefly.In Case 2, as the car is accelerating from rest, it is under the influence of an external force and a non-inertial frame of reference.
Thus, the clock attached to the car does not measure proper time in Case 2.In Case 1, the clock attached to the car measures proper time as the car is traveling at a constant speed. Thus, the time interval measured by the clock attached to the car is the same as the time measured by someone on Earth.(i) In which case(s) does a clock attached to the car measure spacetime interval?
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71. Determine the potencial energy of an 10 kg object after 10 seconds of its free fall (without air resistance) from the height 1 km. 1) 52J 2) 50 kJ 3) 48 MJ 4) 54 kJ ) 5) 46 kJ 78. A basketball floats in a swimming pool. The ball has a mass of 0.5 kg and a diameter of 22 cm. What part of the volume of the ball is under the water level? (expess in percentage) 1) 8.97% 2) 7.54% 3) 5.56% 4) 9.54% 5) 6.12 %
The potential energy of the 10 kg object after 10 seconds of free fall from a height of 1 km is approximately 49.0 kJ.
1. The potential energy of an object can be calculated using the formula PE = mgh, where m is the mass, g is the acceleration due to gravity, and h is the height. In this case, the mass of the object is 10 kg, the height is 1 km (which is equal to 1000 meters), and the acceleration due to gravity is approximately 9.8 m/s². Substituting these values into the formula, we get PE = 10 kg × 9.8 m/s² × 1000 m = 98,000 J. However, since the answer choices are given in different units, we convert Joules to MegaJoules by dividing by 1,000,000. Therefore, the potential energy of the object is 98,000 J ÷ 1,000,000 = 0.098 MJ. Rounding to the nearest whole number, the potential energy is approximately 48 MJ.
2. The object's potential energy is determined by its mass, the acceleration due to gravity, and the height from which it falls. Using the formula PE = mgh, we multiply the mass of 10 kg by the acceleration due to gravity of 9.8 m/s² and the height of 1000 meters. The result is 98,000 Joules. To convert this value to MegaJoules, we divide by 1,000,000, giving us 0.098 MJ. Rounded to the nearest whole number, the potential energy is approximately 48 MJ.
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Review. The cosmic background radiation is blackbody radiation from a source at a temperature of 2.73K. (b) In what part of the electromagnetic spectrum is the peak of the distribution?
The peak of the distribution of the cosmic background radiation is in the microwave part of the electromagnetic spectrum. The frequency falls within the microwave region of the electromagnetic spectrum, indicating that the cosmic background radiation has its peak emission in that specific range.
The peak wavelength or frequency of blackbody radiation can be determined using Wien's displacement law, which states that the wavelength of the peak emission is inversely proportional to the temperature of the blackbody.
The formula for Wien's displacement law is:
λ_peak = b/T
where λ_peak is the peak wavelength, T is the temperature of the blackbody, and b is Wien's displacement constant, which is approximately equal to 2.898 × 10^(-3) m·K.
Substituting the given temperature T = 2.73 K into the formula, we can calculate the peak wavelength:
λ_peak = (2.898 × 10^(-3) m·K) / 2.73 K
≈ 1.06 × 10^(-3) m
To determine the corresponding region of the electromagnetic spectrum, we can use the relationship between wavelength and frequency:
c = λ · ν
where c is the speed of light (approximately 3.00 × 10^8 m/s), λ is the wavelength, and ν is the frequency.
Rearranging the equation, we get:
ν = c / λ
Substituting the calculated peak wavelength into the equation and solving for the frequency, we find:
ν = (3.00 × 10^8 m/s) / (1.06 × 10^(-3) m)
≈ 2.83 × 10^11 Hz
The frequency obtained corresponds to the microwave region of the electromagnetic spectrum.
The peak of the distribution of the cosmic background radiation, which is blackbody radiation from a source at a temperature of 2.73 K, is in the microwave part of the electromagnetic spectrum. This result is obtained by applying Wien's displacement law, which relates the peak wavelength of blackbody radiation to the temperature of the source.
The peak wavelength is determined to be approximately 1.06 × 10^(-3) m, which corresponds to a frequency of approximately 2.83 × 10^11 Hz. The frequency falls within the microwave region of the electromagnetic spectrum, indicating that the cosmic background radiation has its peak emission in that specific range.
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