Which of the following statements concerning the nuclear force is false? O The nuclear force is attractive and not repulsive. O The nuclear is one of only four known types of forces in nature. O The nuclear force is very short-ranged. O The nuclear force acts on both protons and neutrons. O The nuclear force is very weak and much smaller in relative magnitude than the electrostatic and gravitational forces. Submit Request

Answer:

18.4 L

Explanation:

A chocolate sundae contains 500 Cal. Considering that 1 Cal = 1 kcal and 1 kcal = 4.184 kJ,  a chocolate sundae contains:

500 Cal × (4.184 kJ / 1 Cal) = 2.09 × 10³ kJ

Let's suppose we drink water at 10°C that increases its temperature to 37°C by absorbing this heat (Q). We can find the mass of water using the following expression.

Q = c × m × ΔT

where,

c: specific heat capacity of the water

m: mass

ΔT: change in the temperature

Q = c × m × ΔT

2.09 × 10³ kJ = (4.19 kJ/kg.°C) × m × (37°C - 10°C)

m = 18.4 kg

Considering the density of water to be of 1 kg/L, the volume of water is 18.4L.

Final answer:

To counteract the 500 kcal from a chocolate sundae, you would need to drink approximately 14.3 liters of ice-cold water. However, this is neither practical nor safe, and weight management should involve a balance of diet and exercise instead.

Explanation:

Drinking cold water does indeed require energy from the body to warm it up to body temperature, thus expending calories in the process.

To estimate the volume of cold water needed to negate the caloric intake of one chocolate sundae, we can use the given information that 250 mL of ice-cold water takes approximately 8,750 calories (or 8.75 kcal) to be heated up to body temperature.

If a chocolate sundae contains about 500 Cal (500 kcal), we would need to drink a significantly larger volume of cold water to burn those calories. Specifically, we can calculate this using a simple ratio:
500 kcal (chocolate sundae) / 8.75 kcal (250 mL water) = x / 250 mL

This gives us:

x = 250 mL × (500/8.75)

x = 14,285.71 mL

So, you would need to drink approximately 14.3 liters of ice-cold water to counteract the caloric intake from one chocolate sundae, which is not practical or safe.

Answer:

(B) Resistor only

Explanation:

Alternating Current: These are currents that changes periodically with time.

An LRC  Ac circuit is an AC circuit that contains a Resistor, a capacitor and an inductor, connected in series.

In a purely resistive circuit, current and voltage are in phase.

In a purely capacitive circuit, the current leads  the voltage by π/2

In a purely inductive circuit, the current lags the voltage by π/2.

Therefore when a alternating current is set up in LRC circuit, in the resistor, the current and the voltage are in phase.

The right option is (B) Resistor only.

The circuit elements are the current and voltage in phase in:

B) Resistor only

These are flows that changes occasionally with time. A LRC AC circuit is an AC circuit that contains a Resistor, a capacitor and an inductor, associated in series. In an absolutely resistive circuit, current and voltage are in stage. In an absolutely capacitive circuit, the current leads  the voltage by π/2. In an absolutely inductive circuit, the current slacks the voltage by π/2.

Thus, when an alternating current is set up in LRC circuit, in the resistor, the current and the voltage are in phase.

So, correct option is (B).

Find more information about Alternating current here:

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Answer:

461 N

Explanation:

Impulse = change in momentum

F Δt = m Δv

F (0.033 s) = (0.539 kg) (14.4 m/s − (-13.8 m/s))

F = 461 N

Answer:

Impulse, |J| = 0.6716 kg-m/s

Force, F = 63.35 N

Explanation:

It is given that,

Mass of the baseball, m = 0.146 kg

Initial speed of the ball, u = 15.3 m/s

Final speed of the ball, v = 10.7 m/s

To find,

(a) The magnitude of this impulse.

(b) The magnitude of the average force of the glass on the ball.

Solution,

(a) Impulse of an object is equal to the change in its momentum. It is given by :

[tex]J=m(v-u)[/tex]

[tex]J=0.146\ kg(10.7-15.3)\ m/s[/tex]

J = -0.6716 kg-m/s

or

|J| = 0.6716 kg-m/s

(b) Another definition of impulse is given by the product of force and time of contact.

t = 0.0106 s

[tex]J=F\times \Delta t[/tex]

[tex]F=\dfrac{J}{\Delta t}[/tex]

[tex]F=\dfrac{0.6716\ kg-m/s}{0.0106\ s}[/tex]

F = 63.35 N

Hence, this is the required solution.

The impulse direction is opposite to the baseball's initial direction, and its magnitude is 0.6716 kg·m/s. The average force magnitude exerted by the window on the baseball is 63.36 N.

The direction of the impulse imparted by the window to the baseball is opposite to the baseball's initial direction of motion. This is because impulse is equal to the change in momentum, and since the window slows the ball down, it is applying a force in the opposite direction of the ball's initial velocity.

To calculate the magnitude of the impulse (I), use the formula

I = change in momentum = m(vf - vi)
where m is the mass of the baseball, vf is the final velocity, and vi is the initial velocity. The mass m = 0.146 kg, vi = 15.3 m/s, and vf = 10.7 m/s.

I = (0.146 kg)(10.7 m/s - 15.3 m/s)
I = (0.146 kg)(-4.6 m/s)
I = -0.6716 kg·m/s.

The negative sign indicates the impulse is in the opposite direction of the ball's initial motion, but since the question asks for the magnitude, we take the absolute value: 0.6716 kg·m/s.

The magnitude of the average force (Favg) exerted on the ball can be found using the formula

Favg = I/t
where t is the contact time. For a contact time of 0.0106 s, we have:
Favg = 0.6716 kg·m/s / 0.0106 s
Favg = 63.36 N.

Answer:

In this equation the scale used must be Kelvin

Explanation:

The absolute temperature is the value of the measured temperature relative to a scale starting at Absolute Zero (0 K or -273.15 °C). It is one of the main parameters used in thermodynamics and statistical mechanics. In the international system of units it is expressed in kelvin, whose symbol is K

The absolute temperature should always be used in the ideal gas state equation as this can only be in kelvin grade scale.

Answer:

[tex]t=2.044\ hr[/tex]

Explanation:

From the schematic we can visualize the situation and the position of the rays falling on the floor.

Considering the given data from the lowest edge of the mirror.

Now applying the trigonometric ratio to known sides in the first instance:

[tex]tan\ \theta_1=\frac{1.86}{3.8}[/tex]

[tex]\theta_1=26.08^{\circ}[/tex]

Applying the trigonometric ratio to known sides in the second instance:

[tex]tan\ \theta_2=\frac{1.86}{1.22}[/tex]

[tex]\theta_2=56.74^{\circ}[/tex]

Now by the law of reflection we know that the angle of incidence is equal to the angle of reflection. So the sun would have been at the same angle on the opposite side of the normal.

Hence the change in angle of the sun with respect to the mirror (also the earth)

[tex]\Delta \theta=\theta_2-\theta_1[/tex]

[tex]\Delta \theta=56.74-26.08[/tex]

[tex]\Delta \theta=30.66^{\circ}[/tex]

Now the time past for this change:

[tex]t=\frac{\Delta \theta}{\omega}[/tex]

[tex]t=\frac{30.66}{15}[/tex]

[tex]t=2.044\ hr[/tex]

Answer:Time constant gets doubled

Explanation:

Given

L-R circuit is given and suppose R and L is the resistance and inductance of the circuit then current is given by

[tex]i=i_0\left [ 1-e^{-\frac{t}{\tau }}\right ][/tex]

where [tex]i_0[/tex] is maximum current

i=current at any time

[tex]\tau =\frac{L}{R}=time\ constant[/tex]

[tex]\tau '=\frac{2L}{R}=2\tau [/tex]

thus if inductance is doubled then time constant also gets doubled or twice to its original value.                                      

Answer:

The moment (torque) is given by the following equation:

[tex]\vec{\tau} = \vec{r} \times \vec{F}\\\vec{r} \times \vec{F} = \left[\begin{array}{ccc}\^{i}&\^j&\^k\\r_x&r_y&r_z\\F_x&F_y&F_z\end{array}\right] = \left[\begin{array}{ccc}\^{i}&\^j&\3k\\0.23&0.04&0\\150&260&0\end{array}\right] = \^k((0.23*260) - (0.04*150)) = \^k (53.8~Nm)[/tex]

Explanation:

The cross-product between the distance and the force can be calculated using the method of determinant. Since the z-components are zero, it is easy to calculate.

The ideal concept for solving this question is based on the Doppler effect, for which it is indicated that the source's listening frequency changes as the distance and the relative speed between the receiver and the transmitter are also changed. However, if the relative velocity between the two objects is zero as in the particular case presented (since both travel at 75km / h) we have that there will be no change in frequency.

Therefore the frequency that I hear and that my sister would listen would be the same.

Answer:

0.003034 s

1.035 m

4.5 m

Explanation:

[tex]f[/tex] = frequency of the tone = 329.6 Hz

[tex]T[/tex] = Time period of the sound wave

we know that, Time period and frequency are related as

[tex]T =\frac{1}{f}\\T =\frac{1}{329.6}\\T = 0.003034 s[/tex]

[tex]v[/tex] = speed of the sound in the air = 341 ms⁻¹

wavelength of the sound is given as

[tex]\lambda =\frac{v}{f} \\\lambda =\frac{341}{329.6}\\\lambda = 1.035 m[/tex]

[tex]v[/tex] = speed of the sound in the water = 1480 ms⁻¹

wavelength of the sound in water is given as

[tex]\lambda =\frac{v}{f} \\\lambda =\frac{1480}{329.6}\\\lambda = 4.5 m[/tex]

The work done by the child pulling the sled and dog, with a pulling force of 55 N, over a distance of 7.0 m, considering both pulling work and the work done against friction, is 59.42 J.

The question concerns the work done by a child pulling a sled with a dog. 'Work done' in physics is calculated using the equation, work done = force x distance x cosine of the angle. The force exerted is 55 N, the distance is 7.0 m, and the angle is 20 degrees. Thus, the work done by the child's pulling force as the system moves a distance of 7.0 m, ignoring friction and because cos(20) is approximately 0.94, is calculated as: Work done = 55 N x 7.0 m x cos(20) = 55 N x 7.0 m x 0.94 = 361.3 J.

However, the total work done is reduced due to friction between the sled and the ground. The sled's total weight (15 kg sled + 5.0 kg dog = 20 kg) multiplied by gravity (9.8 m/s²) gives  the normal force (20 kg * 9.8 m/s² = 196 N). Multiplying the normal force by the friction coefficient (0.22), gives the frictional force (196 N * 0.22 = 43.12 N). Hence, the work done against friction is: Work done against friction = frictional force x distance = 43.12 N x 7.0 m = 301.88 J. Therefore, the actual work done by the child equals the pull work minus the work against friction, which is 361.3 J - 301.88 J = 59.42 J.

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A. [tex]\( \iint_{S_2} F \cdot dS = 128 \)[/tex]

B. [tex]\( \iint_{S_2} F \cdot dS = 128 \)[/tex]

(A) If the magnitude of (F) is inversely proportional to the square of the distance from the origin:

We know that the flux integral over [tex]\( S_1 \)[/tex] is [tex]\( \iint_{S_1} F \cdot dS = 8 \)[/tex].

Since ( F ) is a radial force field, (F) and (dS) are parallel, and the dot product simplifies to [tex]\( |F| \cdot |dS| \)[/tex].

The surface area of a sphere is [tex]\( 4\pi r^2 \)[/tex], so the magnitude of [tex]\( dS \)[/tex] on [tex]\( S_1 \)[/tex] is [tex]\( |dS| = 16\pi \)[/tex].

Therefore, [tex]\( |F| \cdot |dS| = 8 \implies |F| \cdot 16\pi = 8 \)[/tex], which gives [tex]\( |F| = \frac{1}{2\pi} \)[/tex].

For [tex]\( S_2 \)[/tex], with radius 16, [tex]\( |dS| = 256\pi \)[/tex].

So, [tex]\( \iint_{S_2} F \cdot dS = |F| \cdot 256\pi = \frac{1}{2\pi} \cdot 256\pi = 128 \)[/tex].

(B) If the magnitude of (F) is inversely proportional to the cube of the distance from the origin:

For [tex]\( S_1 \)[/tex], [tex]\( |dS| = 16\pi \)[/tex] as before. So, [tex]\( |F| \cdot |dS| = 8 \implies |F| = \frac{1}{2} \)[/tex].

For [tex]\( S_2 \)[/tex], [tex]\( |dS| = 256\pi \)[/tex] as before.

So, [tex]\( \iint_{S_2} F \cdot dS = |F| \cdot 256\pi = \frac{1}{2} \cdot 256\pi = 128 \)[/tex].

Answer:

D) True. This is what creates the body weight

Explanation:

Let's write Newton's second law for this case. For inclined planes the reference system takes one axis parallel to the plane (x axis) and the other perpendicular to the plane (y axis)

X axis

          Wx -fr = ma

Y Axis

          N - Wy = 0

With trigonometry we can find the components of weight

          sin θ = Wₓ / W

         cos θ = [tex]W_{y}[/tex] / W

         Wₓ = W sin θ

          [tex]W_{y}[/tex] = W cos θ

        W  sin θ - fr = ma

From this expression as it indicates that the body is descending the force greater is the gravity that create the weight of the body

Let's examine the answers

A False This force does not apply because it is not a spring

B) False. It is balanced at all times with the component (Wy) of the weight

C) False. For there to be a rope, if it exists you should be less than the weight component for the block to lower

D) True. This is what creates the body weight

E) False. The cutting force occurs for force applied at a single point and gravity is applied at all points

For a block to move down an inclined plane, the force of gravity must be greater than the other forces. This includes the normal force and any friction that may be present. Other forces such as compression, tension, and shear are not directly involved in this process.

For a block to move down an inclined plane, the greatest force must be gravity. The force of gravity acts downward and causes the block to slide down the slope. This force must be stronger than the others such as the normal force (the force exerted by the plane on the block) and any friction forces that may be present.

The other forces listed (compression, tension, and shear) are not directly related to the movement of the block down the inclined plane. Compression and tension are forces that act in opposite directions either pushing (compression) or pulling (tension) an object. Shear is a force that causes materials to slide past each other and is not directly applicable to this scenario

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Answer:

w = 4,786 rad / s ,  f = 0.76176 Hz

Explanation:

For this problem let's use the concept of angular momentum

       L = I w

The system is formed by the two discs, during the impact the system remains isolated, we have the forces are internal, this implies that the external torque is zero and the angular momentum is conserved

Initial Before sticking

      L₀ = 0 + I₂ w₂

Final after coupling

      [tex]L_{f}[/tex] = (I₁ + I₂) w

The moments of inertia of a disk with an axis of rotation in its center are

      I = ½ M R²

How the moment is preserved

      L₀ = [tex]L_{f}[/tex]

      I₂ w₂ = (I₁ + I₂) w

      w = w₂ I₂ / (I₁ + I₂)

Let's reduce the units to the SI System

      d₁ = 60 cm = 0.60 m

      d₂ = 40 cm = 0.40 m

      f₂ = 200 min-1 (1 min / 60 s) = 3.33 Hz

Angular velocity and frequency are related.

      w₂ = 2 π f₂

      w₂ = 2π 3.33

      w₂ = 20.94 rad / s

Let's replace

       w = w₂ (½ M₂ R₂²) / (½ M₁ R₁² + ½ M₂ R₂²)

       w = w₂ M₂ R₂² / (M₁ R₁² + M₂ R₂²)

Let's calculate

      w = 20.94 8 0.40² / (12 0.60² + 8 0.40²)

      w = 20.94 1.28 / 5.6

      w = 4,786 rad / s

Angular velocity and frequency are related.

      w = 2π f

      f = w / 2π

      f = 4.786 / 2π

      f = 0.76176 Hz

To solve this problem it is necessary to apply the concepts related to the magnetic flow of a coil and take into account the angles for each case.

It is also necessary to delve into part C, the concept of electromotive force (emf) which is defined as the variation of the magnetic flux as a function of time.

By definition the magnetic flux is determined as:

[tex]\phi = NBA cos\theta[/tex]

Where

N = Number of loops [tex]\rightarrow[/tex] We will calculate the value for each of the spins

B = Magnetic Field

A = Cross-sectional Area

[tex]\theta =[/tex] Angle between the perpendicular cross-sectional area and the magnetic field.

PART A) The magnetic flux through the coil after it is rotated is as follows:

[tex]\phi_i = NBA cos\theta[/tex]

[tex]\phi_i = (1turns)(6*10^{-5}T)(12*10^{-4}m^2)cos(0)[/tex]

[tex]\phi_i = 7.2*10^{-8}T\cdot m^2[/tex]

PART B) For the second case the angle formed is perpendicular therefore:

[tex]\phi_f = NBA cos\theta[/tex]

[tex]\phi_f = (1turns)(6*10^{-5}T)(12*10^{-4}m^2)cos(90)[/tex]

[tex]\phi_f = 0[/tex]

PART C) The average induced emf of the coil is as follows:

[tex]\epsilon = - (\frac{\phi_f-\phi_i}{dt})[/tex]

[tex]\epsilon = -(\frac{0-7.2*10^{-8}}{0.04})[/tex]

[tex]\epsilon = 1.8*10^{-6}V[/tex]

Answer:

Explanation:

Given

Displacement is [tex]\frac{1}{3}[/tex] of Amplitude

i.e. [tex]x=\frac{A}{3}[/tex] , where A is maximum amplitude

Potential Energy is given by

[tex]U=\frac{1}{2}kx^2[/tex]

[tex]U=\frac{1}{2}k(\frac{A}{3})^2[/tex]

[tex]U=\frac{1}{18}kA^2[/tex]

Total Energy of SHM is given by

[tex]T.E.=\frac{1}{2}kA^2[/tex]

Total Energy=kinetic Energy+Potential Energy

[tex]K.E.=\frac{1}{2}kA^2 -\frac{1}{18}kA^2[/tex]

[tex]K.E.=\frac{8}{18}kA^2[/tex]

Potential Energy is [tex]\frac{1}{8}[/tex] th of Total Energy

Kinetic Energy is [tex]\frac{8}{9}[/tex] of Total Energy

(c)Kinetic Energy is [tex]0.5\times \frac{1}{2}kA^2[/tex]

[tex]P.E.=\frac{1}{4}kA^2[/tex]

[tex]\frac{1}{2}kx^2=\frac{1}{4}kA^2[/tex]

[tex]x=\frac{A}{\sqrt{2}}[/tex]                  

Answer:

Explanation:

Let the amplitude is A.

Displacement, x = one third of the amplitude = A/3

The total energy of the body executing Simple Harmonic Motion is given by

[tex]T=\frac{1}{2}KA^{2}[/tex]

(a) Kinetic energy of the particle executing SHM is given by

[tex]K=\frac{1}{2}K\left (A^{2} -x^{2} \right )[/tex]

[tex]K=\frac{1}{2}K\left (A^{2} -\frac{A}{9}^{2} \right )[/tex]

[tex]K=\frac{1}{2}\times \frac{8A^{2}}{9}[/tex]

So, the ratio of kinetic energy to the total energy is given by

K / T = 8 / 9

(b) Potential energy of a particle executing SHM is given by

[tex]U=\frac{1}{2}Kx^{2}[/tex]

[tex]T=\frac{1}{2}\times \frac{A^{2}}{9}[/tex]

So, the ratio of potential energy to the total energy is given by

U / T = 1 / 9

(c) Let at a displacement y the kinetic energy is equal to the potential energy

[tex]\frac{1}{2}\times K\times \left ( A^{2}-y^{2} \right )=\frac{1}{2}\times K\times y^{2}[/tex]

[tex]y=\frac{A}{\sqrt{2}}[/tex]

Answer:

    d = 142.5 m

Explanation:

This is a vector exercise. Let's calculate how much the boat travels in the 40s

     d₀ = [tex]v_{b}[/tex] t

    d₀ = 0.75 40

    d₀ = 30 m

Let's write the kinematic equations

Boat

     x = d₀  +  [tex]v_{b}[/tex] t

     x = 0 +  [tex]v_{h}[/tex] t

At the meeting point the coordinate is the same for both

    d₀  +  [tex]v_{b}[/tex] t =  [tex]v_{h}[/tex] t

    t ( [tex]v_{h}[/tex] -  [tex]v_{b}[/tex]) = d₀  

    t = d₀  / ( [tex]v_{b}[/tex]-  [tex]v_{h}[/tex])

The two go in the same direction therefore the speeds have the same sign

     t = 30 / (0.95-0.775)

     t = 150 s

The distance traveled by man is

     d =  [tex]v_{h}[/tex] t

     d = 0.95 150

     d = 142.5 m

The distance of the boat downstream when you catch it is 60 meters.

To find the distance of the boat downstream when you catch it, we can use the equation d = vt, where d is the distance, v is the velocity, and t is the time.

Given that the current of the river is 0.75 m/s and you hold onto the piling for 40 seconds, the distance drift with the current is:

After you start swimming with a speed of 0.95 m/s and catch up to the boat, the distance you swim against the current is equal to the distance the boat drifts:

Therefore, the total distance downstream when you catch the boat is:

Hence, the total distance downstream when you catch the boat is 60 m.

Answer

The answer and procedures of the exercise are attached in the following archives.

Explanation  

You will find the procedures, formulas or necessary explanations in the archive attached below. If you have any question ask and I will aclare your doubts kindly.  

The probability of finding a particle in its first excited state within the center 20% of an infinite square well of length L is approximately 11.8%. This involves integrating the square of the wavefunction over the specific interval. The key steps are defining the potential energy and solving the Schrödinger equation.

To find the probability of locating a particle in its first excited state within the center 20% of a one-dimensional box of length L, we follow these steps:

Define the Potential Energy, V: Inside the box (0 ≤ x ≤ L), V(x) = 0. Outside the box, V(x) = ∞.

Solve the Schrödinger Equation: The normalized wavefunction for the first excited state (n=2) is ψ2(x) = √(2/L) * sin(2πx/L).

The center 20% of the box is the interval from 0.4L to 0.6L. We calculate the probability of finding the particle in this region by integrating the square of the wavefunction:

Prob(center20%) = ∫0.4L0.6L |ψ2(x)|² dx = ∫0.4L0.6L ">2/L * sin²(2πx/L) dx.

Using integration techniques, the result is:

Prob(center20%) = 2 * [0.1 - (sin(0.4π))/(π)]. This computes to approximately 0.118 or 11.8%.

Answer:

225 m

Explanation:

[tex]f[/tex] = Frequency of the T wave = 6.8 Hz

[tex]v[/tex] = Speed of sound in seawater = 1530 ms⁻¹

[tex]\lambda[/tex] = Wavelength of the T wave

we know that, frequency, speed and wavelength are related as

[tex]wavelength = \frac{speed}{frequency}[/tex]

[tex]\lambda = \frac{v}{f}[/tex]

Inserting the values, we get

[tex]\lambda = \frac{1530}{6.8}\\\lambda = 225 m[/tex]

Final answer:

The wavelength of a T wave with a frequency of 6.8 Hz in seawater, where the speed of sound is 1,530 m/s, is calculated to be approximately 225 meters using the formula for wave speed.

Explanation:

To calculate the wavelength of a T wave with a frequency of 6.8 Hz in the Pacific Ocean, where the speed of sound in seawater is 1,530 m/s, we can use the formula for wave speed: v = f × λ, where v is the speed of sound, f is the frequency, and λ is the wavelength.

By rearranging the formula to solve for the wavelength (λ = v / f), and substituting in the known values, we get λ = 1,530 m/s / 6.8 Hz, which calculates to approximately 225 meters. Therefore, the wavelength of a T wave with a 6.8 Hz frequency in seawater is about 225 meters.

Answer:

Explanation:

C is center of mass of the bar ie middle point. Spring is attached with one end ie A of the bar . When this end is displaced by distance x ( small) a restoring force kx is produced which creates a torque

Torque created = kx . l /2  , which creates angular acceleration α

moment of inertia I = ml²/12

torque = I. x α

kx . L /2 = I. x α

α = L kx / 2I

a = linear acceleration

= α x L/2

=  L² kx / 4I

= L²x 12 kx / 4 mL²

a  = 3kx/m

This shows that motion is SHM as acceleration is proportional to displacement x .

angular frequency ω² = 3k / m

frequency f = 1/2π √ 3k/m

= (1/6.28) x √ 3x 500/8

= 2.18 Hz

Final answer:

The frequency of small oscillations is approximately 3.98 Hz, and the smallest value of the spring constant for which oscillations will occur is 0 N/m.

Explanation:

(a)  To determine the frequency of small oscillations, we can use the formula: f = (1/2π) × (√(k/m)), where f is the frequency, k is the spring constant, and m is the mass of the bar. Plugging in the values, we get:
f = (1/2π) × (√(500/8)) ≈ 3.98 Hz

(b)  To find the smallest value of the spring constant k for which oscillations will occur, we need to consider critical damping. Critical damping occurs when the damping force is equal to the force exerted by the spring. The formula for critical damping is c = 2√(mk), where c is the damping coefficient, m is the mass, and k is the spring constant. Since we know that the damping coefficient is 0, we can solve for k to get:
k = (c^2)/(4m). Substituting in the values, we get:
k = (0^2)/(4 x 8) = 0 N/m

To find the maximum values that four bricks of length L can be on the verge of falling while stacked on top of each other in equilibrium, we need to consider the moments of each brick and the conditions for equilibrium. The moments of each brick can be calculated by multiplying the mass of the brick by the distance from the axis of rotation, which is half the length of the brick. By setting the sum of the moments equal to zero, we can find the maximum values for the mass of each brick in terms of L.

When four identical and uniform bricks are stacked on top of each other such that part of each brick extends beyond the one beneath, the stack is in equilibrium and on the verge of falling. To find the maximum values in terms of L, we need to consider the moment of each brick and the conditions for equilibrium. The moment is the product of the mass of the brick and the distance from the axis of rotation, which is half the length of the brick.

Let's assume the bricks have a length L and that they are stacked vertically with their centers of mass aligned. The distance from the axis of rotation to the center of mass is L/2 for each brick. The moment of the top brick is then (mass of the brick) * (L/2). The moment of the second brick is (mass of the brick) * (3L/2), considering the length of the first brick as the distance from the axis of rotation. Similarly, the moment of the third brick is (mass of the brick) * (5L/2), and the moment of the fourth brick is (mass of the brick) * (7L/2).

For the stack to be in equilibrium, the sum of the moments must be zero. Therefore, we have the equation:

(mass of the first brick) * (L/2) + (mass of the second brick) * (3L/2) + (mass of the third brick) * (5L/2) + (mass of the fourth brick) * (7L/2)

By simplifying this equation and substituting the mass of each brick with a constant value (let's say M), we can find the maximum values for the mass of each brick such that the stack is in equilibrium on the verge of falling, given a certain length L.

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To solve this problem it is necessary to apply the concepts related to the magnetic field

the flux density and the magnitude of the magnetization.

Each of these will be tackled as the exercise is carried out, for example for the first part we have to:

Part A) Magnitude of the magnetic field

[tex]H = \frac{NI}{L}[/tex]

Where,

N = Number of loops

I = Current

L = Length

If we replace the given values the value of the magnitude of the magnetic field would be:

[tex]H= \frac{340*13}{0.12}[/tex]

[tex]H = 36833 A\cdot turns/m[/tex]

For the second and third part we will apply the concepts of density both in vacuum and positioned at a point, like this:

PARTE B) Flux density in a vacuum

[tex]B = \mu_0 H[/tex]

Where,

[tex]\mu_0 =[/tex] Permeability constant

[tex]B = (4\pi*10^{-7})(36833)[/tex]

[tex]B = 0.04628T[/tex]

PART C) To find the Flux density inside a bar of metal but the magnetic susceptibility is given

[tex]X_m = 1.9*10^{-4}[/tex]

[tex]\mu_R = 1+X_m[/tex]

[tex]\mu_R = 1.00019[/tex]

Then the flux density would be

[tex]B = \mu_0 \mu_R H[/tex]

[tex]B = (4\pi*10^{-7})(1.00019)(36833)[/tex]

[tex]B = 0.04629T[/tex]

PART D) Finally, the magnetization describes the amount of current per meter, and is given by the magnetic susceptibility, that is:

[tex]M = X_m H[/tex]

[tex]M = 1.9*10^{-4}*36833[/tex]

[tex]M = 6.996A/m[/tex]

This solution calculates the magnetic field strength, flux density and magnetization in a wire coil, as well as the flux density inside a metal bar within the coil, using Ampere's law and the formulas for magnetic field and flux densities.

The calculations are derived from Ampere's law and the formulas for magnetic field strength and flux density. For part (a), to find the magnitude of the magnetic field strength H (in A/m), we consider the given length of the coil and the number of turns. H= nI, where n is the number of turns per unit length and I is the current. In the given case, n= 340/0.12 = 2833.33, so H = 2833.33 turns/m * 13 A = 36833 A/m.

For part (b), we need to calculate the flux density B (in T) inside the coil which is in a vacuum. Using the formula B = μH, where μ = 4π x 10-7 T. m/A is the permeability of vacuum, we find B= 4π x 10^-7 T.m/A * 36833 A/m = 4.6 x 10^-2 T.

For part (c), we need to calculate the flux density B inside a bar of metal with susceptibility χ_m = 1.90 x 10-4. In this case, B = μ(H + M), where M = χ_m H is the magnetization. We find M= 1.90 x 10^-4 * 36833 A/m = 7 A/m, so B in metal = 4π x 10^-7 T.m/A * (36833 A/m + 7 A/m) = 4.6 x 10^-2 T.

For part (d), we've already calculated the magnitude of the magnetization M to be 7 A/m.

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Answer:

d. meteoroid

Explanation:

Answer:

Explanation:

Given

initial velocity of particle u=274 m/s

one Particle moves up with velocity of v=235 m/s

and other moves u=484 m/s towards east

let [tex]v_y[/tex] and [tex]v_x[/tex] be the velocity of third Particle is Y and x direction

conserving momentum in y direction  

[tex]m(274)=\frac{m}{3}\times v_y+\frac{m}{3}\times 0+\frac{m}{3}\times 235[/tex]

[tex]v=587 m/s[/tex]

Now conserving momentum in  x direction

[tex]m\times 0=\frac{m}{3}\times v_x+\frac{m}{3}\times 0+\frac{m}{3}\times 484[/tex]

[tex]v_x=-484 m/s[/tex]

Net Velocity of third Particle

[tex]v^2=v_x^2+v_y^2[/tex]

[tex]v=\sqrt{v_x^2+v_y^2}[/tex]

[tex]v=\sqrt{484^2+587^2}[/tex]

[tex]v=760.80 m/s[/tex]  

To find the magnitude of the velocity of the third fragment, we need to consider the conservation of momentum. The magnitude of the velocity of the third fragment is 445 m/s.

To find the magnitude of the velocity of the third fragment, we need to consider the conservation of momentum. According to the law of conservation of momentum, the total momentum before the explosion is equal to the total momentum after the explosion. The momentum of an object is the product of its mass and velocity.

Let's assume the mass of each fragment is m. Since the first fragment continues to move upward with a speed of 235 m/s and the second fragment has a speed of 484 m/s and is moving east, we can write the momentum equation as:

m(235) + m(484) + m(v3) = m(274)

Simplifying the equation, we get:

719m + m(v3) = 274m

445m = - m(v3)

- 445m = m(v3)

Dividing both sides by m, we get:

-445 = v3

Therefore, the magnitude of the velocity of the third fragment is 445 m/s.

To determine the convection heat transfer coefficient of air at the upper surface, we need to know the surface area of the plate which is not provided in the given question.

The convection heat transfer coefficient of air at the upper surface can be determined using Newton's law of cooling. According to Newton's law of cooling, the rate of heat transfer through convection is directly proportional to the temperature difference between the solid surface and the surrounding fluid and the surface area of the solid.

Therefore, the heat transfer rate can be calculated using the formula:

Q = h * A * (Ts - T∞)

Where:

In this case, we are given the following values:

To find the surface area, we need to know the dimensions of the plate. Once we have the surface area, we can solve for the convection heat transfer coefficient using the given formula. However, the surface area is not provided in the question, so we cannot determine the convection heat transfer coefficient without that information.

Answer:

122.22 W/m²

Explanation:

Let the intensity of unpolarized light is Io.

from first polariser

I' = Io/2

From second polariser

I'' = I' Cos²30 = 3 Io/8

From third polariser

I''' = I'' Cos²30 = 9Io/32

According to the question

9Io/32 = 275

Io = 977.78 watt/m²

Now, from first polariser

I' = Io/2 = 977.78 / 2 = 488.89 W/m²

I'' = 488.89 x cos²60 = 122.22 W/m²

thus, the intensity of light is 122.22 W/m².

Answer:

Explanation:

Given

Intensity of light emerging out is [tex]I=275 W/m^2[/tex]

Polarizer axis are inclined at [tex]30^{\circ}] , [tex]60^{\circ}[/tex] , [tex]90^{\circ}[/tex]

If [tex]I_0[/tex] is the Intensity of Incoming light then

[tex]275=\frac{I_0}{2}\times \cos ^2{30}\times \cos^2 {30}[/tex]

as they are inclined to [tex]30^{\circ}[/tex]to each other

[tex]I_0=\frac{275}{9}\times 32[/tex]

[tex]I_0=977.77 W/m^2[/tex]

If middle Filter is removed then

[tex]I=0.5\cdot I_0\cos ^2{60}[/tex]

[tex]I=0.5\cdot 977.77\cdot \frac{1}{4}[/tex]

[tex]I=122.22 W/m^2[/tex]                                    

To solve this problem we will apply the concepts given by the principles of superposition, specifically those described by Bragg's law in constructive interference.

Mathematically this relationship is given as

[tex]dsin\theta = n\lambda[/tex]

Where,

d = Distance between slits

[tex]\lambda[/tex] = Wavelength

n = Any integer which represent the number of repetition of the spectrum

[tex]\theta = sin^{-1} (\frac{n\lambda}{d})[/tex]

Calculating the value for n, we have

n = 1

[tex]\theta_1 = sin^{-1} (\frac{\lambda}{d})\\\theta_1 = sin^{-1} (\frac{632.8*10^{-9}}{1.6*10^{-6}})\\\theta_1 = 23.3\°[/tex]

n=2

[tex]\theta_2 = sin^{-1} (\frac{2\lambda}{d})\\\theta_2 = sin^{-1} (2\frac{632.8*10^{-9}}{1.6*10^{-6}})\\\theta_2 = 52.28\°[/tex]

n =3

[tex]\theta_2 = sin^{-1} (\frac{2\lambda}{d})\\\theta_2 = sin^{-1} (3\frac{632.8*10^{-9}}{1.6*10^{-6}})\\\theta_2 = \text{not possible}[/tex]

Therefore the intensity of light be maximum for angles 23.3° and 52.28°

Answer:

The minimum coefficient of static friction should be 0.62.

Explanation:

Given that,

Mass of block = m

Mass of cart = 6.5 kg

Time period = 0.66 s

Displacement = 67 mm

We need to calculate the mass of block

Using formula of time period

[tex]T=2\pi\times(\dfrac{m}{k})[/tex]

Put the value into the formula

[tex]0.66=2\pi\times(\dfrac{m+6}{600})[/tex]

[tex]m=\dfrac{0.66\times600}{4\pi^2}-6[/tex]

[tex]m=4.03\ kg[/tex]

We need to calculate the maximum acceleration of SHM

Using formula of acceleration

[tex]a_{max}=\omega^2 A[/tex]

Maximum force on mass 'm' is [tex]m\omega^2 A[/tex]

Which is being provided by the force of friction between the mass and the cart.

[tex]\mu_{s}mg \geq m\omega^2 A[/tex]

[tex]\mu_{s}\geq \dfrac{\omega^2 A}{g}[/tex]

[tex]\mu_{s} \geq (\dfrac{2\pi}{T})^2\times\dfrac{A}{g}[/tex]

Put the value into the formula

[tex]\mu_{s} \geq (\dfrac{2\pi}{0.66})^2\times\dfrac{0.067}{9.8}[/tex]

[tex]\mu_{s} \geq 0.62[/tex]

Hence, The minimum coefficient of static friction should be 0.62.

Answer

Initial radius of the artery is (1.1 cm) / 2 = 0.55 cm

final radius of the artery is (0.90 cm) / 2 = 0.45 cm

initial velocity of the blood is 17 cm/s

Using  equation of continuity is

                                      A₁v₁=A₂v₂

                                 π r₁² x v₁ = π r₂² x v₂

                                  r₁² x v₁ = r₂² x v₂

                                  0.55² x 17 =0.45² x v₂

                                        v₂=25.39 cm/s

Bernoulli's equation is

[tex]P_1 - P_2 = \dfrac{1}{2}\rho (v_2^2-v_1^2)[/tex]

rho is the density of blood = 1060 kg/m^3

[tex]P_1 - P_2 = \dfrac{1}{2}\times 1060 \times (0.254^2-0.17^2)[/tex]

[tex]P_1 - P_2 =18.87\ Pa[/tex]

The student uses the continuity equation to correctly solve the first part, but for pressure drop, they need to apply Bernoulli's principle. Using the equation P1 + 1/2ρv1² = P2 + 1/2ρv2², with ρ being the blood's density and v1 and v2 the speeds, they can find the pressure drop. However, real-life complications due to blood viscosity and turbulence might affect the results.

The subject of this question is Physics (specifically, fluid dynamics). The concept being applied here is that of continuity and Bernoulli's principle. The continuity equation for fluid states that the mass flow rate must be constant throughout the length of the pipe. This translates to: Area 1 × Speed 1 = Area 2 × Speed 2. You correctly set up this equation to find Speed 2, which is the speed of the blood flow within the plaque region.

For the pressure drop, we need to use Bernoulli's principle, which describes that the sum of the pressure, kinetic energy per unit volume, and potential energy per unit volume is constant in a non-viscous, steady-flowing system. Applying Bernoulli's Equation: P1 + 1/2ρv1² = P2 + 1/2ρv2². Solving this equation gives us the pressure difference within the plaque region.

Keep in mind that you might have to use the change in blood speed, and also the density of blood within the equations to find the accurate pressure drop. Also, Bernoulli's principle applies to ideal situations and there could be changes in real-life situations due to the viscosity of blood and turbulence caused by plaque.

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Answer:

Explanation:

a)

[tex]l[/tex] = length of each blade = 3 m

[tex]m[/tex] = mass of each blade = 120 kg

[tex]L[/tex] = length of the rod

[tex]M[/tex] = mass of the rod

Length of the rod is given as

[tex]L = 2 l = 2 (3) = 6 m[/tex]

[tex]w_{0}[/tex] = Angular velocity at t = 0, = 0 rad/s

[tex]w_{30}[/tex] = Angular velocity at t = 30, = 1200 rpm = 125.66  rad/s

[tex]\Delta t[/tex] = time interval = 30 - 0 = 30 s

angular acceleration is given as

[tex]\alpha = \frac{w_{30} - w_{0}}{\Delta t} = \frac{125.66 - 0}{30} = 4.2 rad/s^{2}[/tex]

Angular velocity at t = 10 s is given as

[tex]w_{10} = w_{0} + \alpha t\\w_{10} = 0 + (4.2) (10)\\w_{10} = 42 rad/s[/tex]

Angular velocity at t = 20 s is given as

[tex]w_{20} = w_{0} + \alpha t\\w_{20} = 0 + (4.2) (20)\\w_{10} = 84 rad/s[/tex]

Mass of the rod is given as

[tex]M = 2m = 2(120) = 240 kg[/tex]

Moment of inertia of the propeller is given as

[tex]I = \frac{ML^{2} }{12} =  \frac{(240)(6)^{2} }{12} = 720 kgm^{2}[/tex]

Angular momentum at t = 10 s is given as

[tex]L_{10} = I w_{10} = (720) (42) = 30240 kgm^{2}/s[/tex]

Angular momentum at t = 20 s is given as

[tex]L_{20} = I w_{20} = (720) (84) = 60480 kgm^{2}/s[/tex]

b)

Torque on propeller is given as

[tex]\tau = I \alpha \\\tau = (720) (4.2)\\\tau = 3024 Nm[/tex]

Answer:

(a) 4800 kg m^2/s^2 , 9600 kg m^2/s^2

(b) 480 Nm

Explanation:

length of each blade = 3 m

total length, L = 2 x 3 = 6 m

mass of each blade = 120 kg

total mass, m = 2 x 120 = 240 kg

initial angular velocity, ωo = 0 rad/ s

final angular velocity, ω = 1200 rpm = 1200 / 60 = 20 rps = 125.6 rad/s

t = 30 s

Let the angular acceleration is α.

α = (ω - ωo)/t = 120 / 30 = 4 rad/s^2

(a) moment of inertia. I = mL^2 / 12

I = 240 x 6 / 12 = 120 kg m^2

Let ω' be the angular velocity at the end of 10 s

use first equation of motion

ω' = 0 + αt

ω' = 4 x 10 = 40 rad/s

Angular momentum at t = 10 s

L = I x ω = 120 x 40 = 4800 kg m^2/s^2

Let ω'' be the angular velocity at the end of 20 s

use first equation of motion

ω'' = 0 + αt

ω'' = 4 x 20 = 80 rad/s

Angular momentum at t = 20 s

L = I x ω = 120 x 80 = 9600 kg m^2/s^2

(b) Torque, τ = I x α

τ = 120 x 4 = 480 Nm