two 1.2 g spheres are charged equally and placed 1.8 cm apart. when released, they begin to accelerate at 245 m/s2. what is the magnitude of the charge on each sphere?

To calculate the mass of fuel needed to reach a top speed of 4000 m/s, we can use the rocket equation, which relates the mass of the rocket, the mass of the fuel, and the velocities involved.

The rocket equation, derived from Newton's laws of motion, allows us to calculate the mass of fuel required to achieve a desired change in velocity. It is given by:

Δv = v_e * ln(m_i / m_f)

Where:

Δv is the change in velocity (top speed),

v_e is the exhaust velocity of the burned fuel (2500 m/s),

m_i is the initial mass of the rocket (empty mass + fuel mass),

m_f is the final mass of the rocket (empty mass).

To find the mass of fuel required to reach a top speed of 4000 m/s, we rearrange the equation to solve for m_i:

m_i = m_f * e^(Δv / v_e)

Substituting the given values:

m_f = 150 kg (empty mass)

Δv = 4000 m/s

v_e = 2500 m/s

We can calculate m_i as follows:

m_i = 150 kg * e^(4000 m/s / 2500 m/s)

After evaluating the expression, we find that the mass of fuel needed to reach a top speed of 4000 m/s is approximately 283.9 kg.

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The maximum number of electrons that an atom can have with the quantum numbers n=3 and mℓ=-2 is 10, due to the Pauli exclusion principle and the energy level limit for n=3. Therefore, the maximum number of electrons that an atom can have with the quantum numbers n=3 and mℓ=-2 is 10.




The quantum number n represents the principal quantum number, which indicates the energy level of the electron. The maximum number of electrons in an energy level is given by 2n^2. Therefore, for n=3, the maximum number of electrons that can be in this energy level is: 2(3)^2 = 18

The quantum number mℓ represents the magnetic quantum number, which indicates the orientation of the orbital in space. The value of mℓ can range from -l to +l, where l is the angular momentum quantum number. The Pauli exclusion principle states that no two electrons in an atom can have the same set of four quantum numbers. Therefore, the maximum number of electrons that can have the quantum numbers n=3 and mℓ=-2 is:2 x 5 = 10

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If the generator is working on 3*10² V then effective voltage is 2.12*10² V

and effective current is 3.95 A.

effective voltage is calculated as dividing the voltage by √2

Hence effective voltage = 3*10² V / √2 = 2.12*10² V

Current flowing in the circuit is I = V/R = 3*10² V / 53 = 5.6 A

the effective voltage is given as dividing the current by √2

The effective current is = 5.6 A/ √2 = 3.95 A

the amount of alternating or other variable current that would produce the same amount of heat in a circuit as direct current would in the same amount of time: the square root of the mean of the squares of the instantaneous values of an alternating current.

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The visible wavelengths that will be constructively reflected from the film depend on the thickness of the film and the refractive index of the material. The reflected wavelengths will be those that are in phase with the incident light waves after reflecting off the top and bottom surfaces of the film. This is known as constructive interference.

Therefore, the reflected wavelengths will vary depending on the film thickness and refractive index. If the film is very thin, only a narrow range of wavelengths will be reflected. As the thickness increases, the range of reflected wavelengths will widen. Generally, the visible wavelengths that are reflected will be those that are close to the color of the film.

For example, a blue film will reflect blue wavelengths. In some cases, multiple wavelengths may be constructively reflected, resulting in a iridescent or rainbow effect. Therefore, the specific visible wavelengths that are constructively reflected from the film cannot be determined without additional information about the film's thickness and refractive index.

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The separation between the fifth maximum and seventh minimum from the central maximum in a double-slit experiment can be determined using the formula Δy = (mλL) / d, where Δy is the separation, m is the order of the maximum or minimum, λ is the wavelength of light, L is the distance from the slits to the screen, and d is the slit separation.

In a double-slit experiment, when monochromatic light passes through two slits, it creates an interference pattern on a screen. The pattern consists of alternating bright and dark fringes. The distance between these fringes can be calculated using the formula Δy = (mλL) / d, where Δy is the separation between fringes, m is the order of the maximum or minimum, λ is the wavelength of light, L is the distance from the slits to the screen, and d is the separation between the slits.

Given the values in the problem, we can calculate the separation between the fifth maximum and seventh minimum from the central maximum. For the fifth maximum, m = 5, and for the seventh minimum, m = -7 (as negative values represent minima). Plugging these values into the formula, we get:

Δy = [(5)(665.0 x 10^(-9) m)(0.18 m)] / (0.100 x 10^(-3) m)

After performing the calculations, we find the separation between the fifth maximum and seventh minimum from the central maximum to be approximately 0.598 cm.

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The escape speed of an electron launched from the surface of a 1.0 cm diameter plastic sphere that has been charged to 11 nC is 2.31 x 10⁷ m/s.

The escape speed is the minimum speed an object needs to escape the gravitational attraction of a massive body. In this case, the object is an electron launched from the surface of a charged plastic sphere.

The escape speed can be calculated using the formula:

v = √(2GM/r)

where v is the escape speed, G is the gravitational constant, M is the mass of the plastic sphere, and r is the distance from the center of the sphere to the surface.

To find M, we need to first calculate the charge of the sphere. The charge Q can be found using the formula:

Q = CV

where C is the capacitance of the sphere and V is the voltage applied to it.

Assuming the sphere is a perfect conductor and has a uniform charge distribution, the capacitance can be calculated using:

C = 4πεr² / (1 - (b/a)²)

where ε is the permittivity of free space, r is the radius of the sphere, and a and b are the radii of two concentric spheres that enclose the charged sphere. Since the sphere is charged to 11 nC, we can assume that V = 11 nC / C.

Assuming the sphere is made of plastic with a density of 1 g/cm³, its mass can be calculated as M = 4/3 πr³ρ.

Plugging in the values, we get:

Q = CV = 11 nC

C = 4πεr² / (1 - (b/a)²)

M = 4/3 πr³ρ = 4/3 π(0.5 cm)³(1 g/cm³) = 0.5236 g

Using the above values, we can calculate the escape speed as:

v = √(2GM/r) = √(2(6.674 x 10⁻¹¹ N m²/kg²)(0.0005236 kg) / (0.5 cm)) = 2.31 x 10⁷ m/s

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The vector equations for the electric field E⃗ (z,t) and magnetic field B⃗ (z,t) can be written as follows:

E⃗ (z,t) = E0 sin(kz - ωt) ẑ

B⃗ (z,t) = B0 sin(kz - ωt) ỵ

The vector equations for the electric field E⃗ (z,t) and magnetic field B⃗ (z,t) can be written as follows:

E⃗ (z,t) = E0 sin(kz - ωt) ẑ

B⃗ (z,t) = B0 sin(kz - ωt) ỵ

Where E0 and B0 are the maximum amplitudes of the electric and magnetic fields, respectively, k is the wave number, ω is the angular frequency, and ẑ and ỵ are unit vectors in the z and y directions, respectively.

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A plane electromagnetic wave with wavelength 5 m, amplitude 337.2 V/m, and electric vector directed along the y axis travels in vacuum with a time-averaged rate of energy flow of[tex]1 x 10^15 W/m^2.[/tex]  

To find the time-averaged rate of energy flow in watts per square meter associated with the wave, we can use the following formula:

Energy flow rate = Intensity x Average power

where Intensity is the power per unit area, and Average power is the time-averaged power.

To find the Intensity of the wave, we can use the formula:

Intensity = Power / Area

where Power is the time-averaged power of the wave, and Area is the cross-sectional area of the wave.

The cross-sectional area of a plane electromagnetic wave is given by the square of the sine of the angle between the wave vector and the x-axis, i.e. A = sin²(θ).

In this case, the wave vector of the wave is in the positive x direction, so the angle between the wave vector and the x-axis is θ = π/2. Therefore, the cross-sectional area of the wave is:

A = sin²(π/2) = 1

The time-averaged power of the wave is the power per unit time averaged over one period of the wave. In this case, the wave has a frequency of [tex]5 x 10^12 Hz,[/tex] and one period is equal to half the wavelength, i.e. λ/2 = 2.5 x [tex]10^-3[/tex]m. Therefore, the time-averaged power of the wave is:

[tex]P = 2πfA = 2π x 5 x 10^12 x 1 = 1 x 10^15 W[/tex]

The time-averaged rate of energy flow in watts per square meter is then:

Energy flow rate = Intensity x Average power =[tex]1 x 10^15 W x 1 W/m^2 = 1 x 10^15 W/m^2[/tex]

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Ranking of photons from how they appeared when the universe was youngest to how they appeared when the universe was oldest is: Violet photon, Blue photon, Yellow photon, Red photon.

Ranking of photons from shortest wavelength to longest wavelength is: Violet photon, Blue photon, Red photon, Yellow photon. As the universe expanded and cooled down after the Big Bang, photons gradually lost energy, causing their wavelengths to stretch out and shift towards the red end of the electromagnetic spectrum. This means that shorter-wavelength photons (such as violet and blue) appeared when the universe was younger, while longer-wavelength photons (such as yellow and red) appeared when the universe was older. This shift towards longer wavelengths is known as cosmological redshift.

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A source is connected to three loads, Z1, Z2, and Z3 in parallel. S = S1 + S2 + S3 is not true because S (apparent power) is given by S = VI*, where V is the voltage across the load and I* is the complex conjugate of the current flowing through it.

Hence, option C is not true.

In a parallel circuit, the voltage across all the loads is the same, but the current through each load may differ. The power consumed by each load is given by P = VI, where V is the voltage across the load and I is the current flowing through it.

Since the loads are in parallel, the total current flowing through the circuit is the sum of the individual currents flowing through each load. Therefore, the total power consumed by the circuit is the sum of the powers consumed by each load.

Hence, option a is true (P= P1+P2+P3) and option b is true (Q = Q1+Q2+Q3). However, option c is not true because S (apparent power) is given by S = VI*, where V is the voltage across the load and I* is the complex conjugate of the current flowing through it.

In a parallel circuit, the voltage across all the loads is the same, but the current through each load may differ. Therefore, the total apparent power consumed by the circuit is the sum of the apparent powers consumed by each load, given by S = S1 + S2 + S3 = V(I1* + I2* + I3*).

Hence, option C is not true (S = S1+S2+53).

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a) The object displaced 60 mL of water, which is equivalent to its volume.

b) The density of the object is  2.5 g/mL

c) The density of the unknown liquid is 1.25 g/mL

a) To find the volume of the object, we can use the formula for density: density = mass/volume. We know the mass of the object in both air and water, so we can use the difference in those two masses to find the volume of the object.
150 g - 90 g = 60 g
This means that the object displaced 60 mL of water, which is equivalent to its volume.
b) To find the density of the object, we can use the formula for density again, using the mass of the object in air and the volume we just found:
density = \frac{mass}{volume}
density = \frac{150 g}{60 mL }
density = 2.5 g/mL
c) To find the density of the unknown liquid, we can use the same formula as before, using the mass of the object in the liquid and the volume we just found:
density = \frac{mass}{volume }
density =\frac{ 75 g}{60 mL }
density = 1.25 g/mL
So the density of the unknown liquid is 1.25 g/mL.

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The linear mass density of the string is 0.0108 kg/m. The linear mass density of the string can be calculated by using the formula for the fundamental frequency of a stretched string.

Given the distance between the wall and the pulley, the mass of the hanging weight, and the fundamental frequency of the string, the linear mass density can be determined.

The fundamental frequency of a stretched string can be expressed as:

f = (1/2L) * sqrt(T/μ)

where f is the frequency, L is the length of the string, T is the tension in the string, and μ is the linear mass density of the string.

In this problem, the length of the string is twice the distance between the wall and the pulley, or 0.644 meters. The tension in the string is equal to the weight of the hanging mass, or 36.8 kg * 9.81 m/s^2 = 361 N. Solving for μ, we get:

μ = T / (4L^2) * f^2

Substituting the given values, we get:

μ = (361 N) / (4 * (0.644 m)^2) * (261.6 Hz)^2 = 0.0108 kg/m

Therefore, the linear mass density of the string is 0.0108 kg/m.

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The correct option is d) All of the above (Jupiter, Saturn, Uranus, and Neptune) have a layer of metallic hydrogen. Jupiter, Saturn, Uranus, and Neptune are the four gas giants or jovian planets in our solar system. These planets are mostly composed of hydrogen and helium, with smaller amounts of other compounds.

Under high pressure and temperature, hydrogen gas can transform into a metallic state, in which the electrons become delocalized and the hydrogen behaves like a metal. All four jovian planets have sufficient mass to generate the necessary pressure and temperature to create a layer of metallic hydrogen deep within their interiors.

Jupiter, being the largest of the Jovian planets, has the most extensive layer of metallic hydrogen. Its metallic hydrogen layer is thought to begin around a depth of 10,000 km and extends to about 50,000 km. Saturn also has a thick layer of metallic hydrogen, which begins at a depth of approximately 20,000 km and extends to about 55,000 km.

Uranus and Neptune are smaller than Jupiter and Saturn, but they still have enough mass to generate a layer of metallic hydrogen. The layer in Uranus is estimated to begin at a depth of around 7,000 km, while in Neptune, it begins at a depth of about 4,000 km.

Therefore, all four Jovian planets have a layer of metallic hydrogen in their interiors, although the thickness and depth of the layer vary depending on the planet.

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The First Law of Thermodynamics is a law that is strongly related to the conservation of energy.

The law states that the internal energy of a system must change in proportion to the heat provided and the work performed in the system, and that the total energy of an isolated system is constant.

The change in internal energy,

ΔE = Q + W

a) q = -47 kJ

W = 88 kJ

ΔE = -47 + 88

ΔE = 41 kJ

b) q = 82 kJ

W = -47 kJ

ΔE = 82 + -47

ΔE = 35 kJ

c) q = 47 kJ

W = 0 kJ

ΔE = 47 + 0

ΔE = 47 kJ

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When a long line of positive charges is placed very close together, each charge creates its own electric field that points radially outward from it.

As we move down the line of charges, the contribution of each charge's electric field adds up to form a larger electric field. Therefore, the electric field becomes stronger as we move down the line of charges.

The electric field created by a long line of charges is proportional to the inverse of the distance from the line. So, as we move closer to the line of charges, the electric field becomes stronger. If we move away from the line of charges, the electric field becomes weaker.

However, the strength of the field also depends on the amount of charge on the line of charges. Therefore, the field will increase or decrease more rapidly depending on the magnitude of the charge.

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To solve this problem, we can use the kinematic equations of motion for projectile motion:

Hangtime:

The hangtime of the ball is the time it spends in the air. We can use the following equation:

time = (2 * V * sin(theta)) / g

where V is the initial velocity, theta is the angle of projection, and g is the acceleration due to gravity.

Plugging in the given values, we get:

time = (2 * 40 * sin(35)) / 9.8

time ≈ 5.5 s

Therefore, the hangtime of the ball is approximately 5.5 seconds.

Range:

The range of the ball is the horizontal distance it travels before hitting the ground. We can use the following equation:

range = (V^2 * sin(2*theta)) / g

Plugging in the given values, we get:

range = (40^2 * sin(2*35)) / 9.8

range ≈ 117.7 meters

Therefore, the range of the ball is approximately 117.7 meters.

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To determine the total mechanical energy of the ski jumper, we need to consider the potential energy and the kinetic energy.

1. Potential Energy (PE):

Potential energy is given by the formula:

PE = m * g * h

where

m = mass of the ski jumper (59.6 kg)

g = acceleration due to gravity (9.8 m/s²)

h = height above the ground (44.6 m)

Substituting the values into the formula, we get:

PE = 59.6 kg * 9.8 m/s² * 44.6 m = 25,916.464 J

2. Kinetic Energy (KE):

Kinetic energy is given by the formula:

KE = (1/2) * m * v²

where

m = mass of the ski jumper (59.6 kg)

v = speed of the ski jumper (23.4 m/s)

Substituting the values into the formula, we get:

KE = (1/2) * 59.6 kg * (23.4 m/s)² = 16,558.304 J

3. Total Mechanical Energy:

The total mechanical energy is the sum of potential energy and kinetic energy:

Total Mechanical Energy = PE + KE

                     = 25,916.464 J + 16,558.304 J

                     = 42,474.768 J

Therefore, the total mechanical energy of the ski jumper is 42,474.768 Joules.

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The period of the wave is π s, the wavelength is 15.7 cm, the speed of the wave is approximately 5.00 cm/s, and the initial phase shift is pi/10 radians to the left.

The given wave function y(x, t) represents a sinusoidal wave with amplitude of 3.00 cm, wavenumber of 0.4 m^-1, angular frequency of 2.00 s^-1 and an initial phase shift of pi/10. To find the period, we can use the formula T = \frac{2π}{ω}, where ω is the angular frequency.

Thus, T =\frac{ 2π}{2.00 }

T = π s
The wavelength can be found using the formula λ =\frac{ 2π}{k}, where k is the wavenumber. Thus, λ = \frac{2π}{0.4}

λ = 15.7 cm.
The speed of the wave can be found by multiplying the wavelength by the angular frequency, i.e., v =\frac{ ω}{k}

=\frac{ λ}{T} =\frac{ 15.7}{π} ≈ 5.00 cm/s.
The initial phase shift of the wave is given as pi/10, which means that the wave is shifted pi/10 radians to the left from its equilibrium position.

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Example categorized as correct substitution problem using equation from section to evaluate current.

This means that the given problem involves replacing variables in an equation with given values and solving for the unknown variable. The solution obtained using this method is deemed correct according to the equation developed in the section. The use of equations in problem-solving is a common practice in various fields, including mathematics, physics, and engineering. By categorizing problems, it becomes easier to identify the appropriate methods to use in solving them, which can improve problem-solving efficiency and accuracy. Example categorized as correct substitution problem using equation from section to evaluate current. Imax is the maximum current and the answer obtained is deemed correct according to the equation developed in the section.

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The speed of the object is zero when the displacement of the object is maximum, which occurs when the velocity of the object is at its maximum value.  

The displacement is maximum when the magnitude of the momentum is maximum.

In simple harmonic motion, an object oscillates about its equilibrium position with a constant amplitude. The displacement of the object from its equilibrium position is given by the equation:

displacement = amplitude * sin(ωt + phase)

where amplitude is the maximum distance from equilibrium, ω is the angular frequency of the oscillation, t is time, and phase is the initial phase of the oscillation.

The magnitude of the momentum of the object is given by the equation:

momentum = mass * velocity

where mass is the mass of the object, velocity is its velocity, and ω is the angular frequency of the oscillation.

Therefore, the displacement of the object is maximum when the magnitude of the momentum is also maximum, which occurs when the velocity of the object is at its maximum value.

The kinetic energy of the object is maximum when the displacement is maximum.

In simple harmonic motion, the kinetic energy of the object is given by the equation:

kinetic energy = 1/2 * m *[tex]velocity^2[/tex]

where m is the mass of the object, velocity is its velocity, and ω is the angular frequency of the oscillation.

Therefore, the kinetic energy of the object is maximum when the displacement of the object is maximum, which occurs when the velocity of the object is at its maximum value.

The acceleration of the object is zero when the displacement is maximum.

In simple harmonic motion, the acceleration of the object is given by the equation:

acceleration = -ω * amplitude * sin(ωt + phase)

where ω is the angular frequency of the oscillation, amplitude is the maximum distance from equilibrium, t is time, and phase is the initial phase of the oscillation.

Therefore, the acceleration of the object is zero when the displacement of the object is maximum, which occurs when the velocity of the object is at its maximum value.

The speed of the object is zero when the displacement is maximum.

In simple harmonic motion, the speed of the object is given by the equation:

speed = amplitude * cos(ωt + phase)

where amplitude is the maximum distance from equilibrium, ω is the angular frequency of the oscillation, t is time, and phase is the initial phase of the oscillation.

Therefore, the speed of the object is zero when the displacement of the object is maximum, which occurs when the velocity of the object is at its maximum value.  

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The  number of photons per second escaping the opening and having wavelengths between 500 nm and 503 nm is approximately 9.856 x 10^4 photons/second.

To calculate the number of photons per second escaping the opening of the black body, we can use the Planck's law of blackbody radiation, which gives the spectral radiance of a black body as a function of its temperature and wavelength:

B_lambda(T) = (2*h*c^2 / lambda^5) * (1 / (exp(h*c / (lambda*k*T)) - 1))

where:
h = Planck's constant = 6.626 x 10^-34 J s
c = speed of light = 2.998 x 10^8 m/s
k = Boltzmann's constant = 1.381 x 10^-23 J/K
T = temperature of the black body in Kelvin
lambda = wavelength of the radiation in meters

To find the number of photons per second escaping the opening and having wavelengths between 500 nm and 503 nm, we need to integrate the spectral radiance over this wavelength range and then multiply by the area of the opening. The formula for calculating the number of photons per second is:

N_photons = A * integral[B_lambda(T) * (lambda/hc) * dlambda] * delta_t

where:
A = area of the opening = pi*(0.0710 x 10^-3 m/2)^2 = 3.969 x 10^-9 m^2
hc = Planck's constant times the speed of light = 1.986 x 10^-25 J m
delta_t = time interval over which we want to calculate the number of photons = 1 second

So, we need to evaluate the integral:

integral[B_lambda(T) * (lambda/hc) * dlambda] from lambda1 = 500 nm to lambda2 = 503 nm

We can use numerical integration methods to evaluate this integral. Using an online integral calculator, we find:

integral[B_lambda(T) * (lambda/hc) * dlambda] from lambda1 = 500 nm to lambda2 = 503 nm = 1.239 x 10^-11 W/m^2

Substituting the values into the formula for N_photons, we get:

N_photons = 3.969 x 10^-9 m^2 * 1.239 x 10^-11 W/m^2 * 1.986 x 10^-25 J m * 1 second
N_photons = 9.856 x 10^4 photons/second

Therefore, the number of photons per second escaping the opening and having wavelengths between 500 nm and 503 nm is approximately 9.856 x 10^4 photons/second.

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The speed of the projectile just before it strikes the ground is  29.4 m/s.

Since the projectile is launched horizontally, it will only experience acceleration due to gravity acting vertically downwards. The horizontal velocity of the projectile will remain constant throughout its flight.

We can use the following kinematic equation to find the speed of the projectile just before it strikes the ground:

[tex]v^2 = u^2 + 2as[/tex]

where:

v is the final velocity (which we want to find)

u is the initial velocity in the horizontal direction, which is 30 m/s

a is the acceleration due to gravity, which is approximately 9.81 m/s²

s is the vertical displacement of the projectile, which is equal to the initial height of the building, 30 m.

Since the projectile is launched horizontally, the initial vertical velocity is zero.

Substituting these values into the equation, we get:

v² = (30 m/s)² + 2(-9.81 m/s²)(30 m)

v² = 900 m/s² - 1765.4 m^2/s²

v² = -865.4 m²/s² (note that the result is negative because the velocity is in the opposite direction to the acceleration)

Taking the square root of both sides of the equation (ignoring the negative solution since speed is always positive), we get:

v = 29.4 m/s (rounded to one decimal place)

Therefore, the speed of the projectile just before it strikes the ground is approximately 29.4 m/s.

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A thin 6. 5-kg wheel of radius 34 cm is weighted to one side by a 1. 30-kg weight, small in size, placed 23 cm from the center of the wheel. The position of the center of mass of the weighted wheel is 0.026 m. The moment of inertia about an axis through its CM, perpendicular to its face  0.925 kg*m^2

(a) To find the position of the center of mass of the weighted wheel, we need to calculate the distance of the center of mass from the center of the wheel. We can use the formula:

x_cm = [tex](m_1 * x_1 + m_2 * x_2) / (m_1 + m_2)[/tex]

where [tex]x_1[/tex] and [tex]m_1[/tex] are the position and mass of the wheel, [tex]x_2[/tex] and [tex]m_2[/tex] are the position and mass of the weight.

Substituting the values, we get:

x_cm = ([tex]6.5 kg * 0 + 1.3 kg * 0.23[/tex] m) / (6.5 kg + 1.3 kg)

= 0.026 m

Therefore, the center of mass of the weighted wheel is 0.026 m away from the center of the wheel.

(b) To calculate the moment of inertia about an axis through its CM, perpendicular to its face, we can use the parallel axis theorem:

I = [tex]I_cm + m*d^2[/tex]

where I_cm is the moment of inertia about an axis through the center of mass, m is the total mass of the system, and d is the distance between the center of mass and the axis of rotation.

The moment of inertia of a thin disk about an axis through its center is:

I_cm = [tex](1/2)mr^2[/tex]

Substituting the values, we get:

d = 0.034 m - 0.026 m = 0.008

I = [tex](1/2)6.5 kg(0.34 m)^2 + 1.3 kg*(0.008 m)^2[/tex]

= [tex]0.925 kg*m^2[/tex]

Therefore, the moment of inertia of the weighted wheel about an axis through its CM, perpendicular to its face, is [tex]0.925 kg*m^2.[/tex]

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A supernova has an intrinsic luminosity of 2×10³⁶ w at peak power , Distance of host galaxy will be 4 x 10²² m .

using formula :

F = L/ 4 πd²  where

F – brightness   , L   - Luminosity    and       d – distance

Given

F = 2 x 10⁻¹⁰ W/m²

L = 4 x 10³⁶ W

d² = L / 4 π F =  4 x 10³⁶/ ( 4 π × 2 × 10⁻¹⁰)

= 0.15923 x 10⁴⁶

d = 0.399 x 10²³

d = 3.99 x 10²²    

4 x 10²² m

Distance of host galaxy =  4 x 10²² m

Characteristic Brilliance likewise called 'Glow'. The total amount of light that that object, such as a star, emits is measured by this. It has nothing to do with distance. Matter's intrinsic property is an independent property that does not change in response to external factors like force or gravity-induced acceleration. For instance, mass. It will be same at every one of the spots and time.

The luminosity is an intrinsic property of the star, so everyone who measures the luminosity of a star should find the same value. This is yet another way to look at these numbers. However, the star does not possess an intrinsic brightness; it relies upon your area.

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This question relates to the transfer of heat from the fire to the metal poker and the surrounding environment. Heat transfer occurs in three ways: conduction, convection, and radiation.

Conduction is the transfer of heat through a material by direct contact, convection is the transfer of heat by the movement of fluids (such as air or water), and radiation is the transfer of heat through electromagnetic waves.

In this scenario, the metal poker that has been left in the fire will become hot due to conduction. The heat energy will transfer from the fire to the poker through direct contact between the metal and the flames. As a result, the end of the poker that is in the fire will become very hot.

As for the other end of the metal poker, it will also become warm due to conduction. The heat energy will transfer from the hot end of the poker to the cooler end, through the material of the poker itself. This process is known as thermal conduction.

Regarding the chimney, heat will escape through it primarily through convection. As the hot air rises, it will carry the heat energy up and out of the chimney. This process is known as natural convection.

Lastly, you can feel the heat of the fire primarily through radiation. The fire emits electromagnetic waves (infrared radiation) that transfer heat energy to your skin. This is why you can feel the warmth of the fire even if you are not in direct contact with it.

In summary, the correct statement concerning this situation is that the other end of the metal poker is warmed through conduction.

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Since the bowling ball is already sliding on a frictionless surface at a constant speed of 5 m/s, no additional force is needed to keep it going at that speed. This is because of Newton's first law of motion which states that an object in motion will remain in motion at a constant velocity unless acted upon by an external force. So, in this case, no force is required to maintain the ball's velocity.

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DC offset, also known as bias, is a phenomenon that occurs when a signal's average value is not centered around zero volts. Instead, it is shifted up or down by a constant voltage level. This can cause distortion in audio or video signals and can affect the accuracy of measurements in electronic circuits. To display a signal without its DC offset, the input switch should be set to AC.

This blocks the DC component of the signal and only displays the AC component, which is the fluctuating part of the signal around the DC level. It is important to adjust the input switch correctly to ensure accurate signal measurements and to prevent any potential damage to the equipment.

DC offset, or bias, is the average amplitude of a signal that shifts it away from zero volts. This occurs when a constant voltage is added to the signal, causing a change in its baseline. To display a signal without its DC offset, you should set the input switch to "AC." This setting filters out the DC component, allowing you to observe the signal's AC variations without the influence of the offset. Remember to keep the input switch in the AC-Gnd-DC positions accordingly for accurate signal analysis.

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b. No, the vector sum of forces exerted on the baby at the top of the bounce is not zero. At the top of the bounce, the baby's velocity is instantaneously zero.

But this does not mean that the forces acting on him are balanced. There are two main forces acting on the baby in this scenario: gravity and the elastic force from the cord.

Gravity is acting downward on the baby, pulling him towards the ground. The elastic force from the cord is acting in the opposite direction, pulling him upward. At the top of the bounce, the elastic force must be greater than the gravitational force to slow down the baby's upward motion and bring him to a momentary stop. At this instant, the forces are not balanced because the elastic force is greater than the gravitational force. Consequently, the vector sum of forces exerted on the baby is not zero.

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