Two very small spheres are initially neutral and separated by a distance of \( 0.56 \mathrm{~m} \). Suppose that \( 2.4 \times 10^{13} \) electrons are removed from one sphere and placed on the other.

Answers

Answer 1

The electrostatic force is caused due to the presence of charge particles. The electrostatic force between the two spheres is 6.89 x 10-3 N.

It is one of the four fundamental forces in nature. It acts over a distance in two forms: attractive and repulsive.

The repulsive force takes place between two similar charges while the attractive force takes place between two opposite charges.

Coulomb's law is the mathematical expression of the electrostatic force.

Formula to find electrostatic force

The force between two charged particles is given by Coulomb's Law.

It states that:

F = kq1q2/r2

Where, q1 and q2 are the magnitudes of the charges on the two particles,

r is the distance between the centers of the two charges, and

k is the proportionality constant, known as the Coulomb's constant,

which has a value of 8.987 x 109 N.m2/C2.

Calculation of electrostatic forceIn the given question, we are supposed to find the electrostatic force between the two spheres. The spheres are initially neutral and separated by a distance of 0.56 m.

After that, 2.4 x 1013 electrons are removed from one sphere and placed on the other sphere. This implies that one sphere gets negatively charged, and the other sphere gets positively charged.

Let us find the charge on each sphere. The charge on each sphere is given by: q = Ne

Where, q is the charge on each sphere,

N is the number of electrons transferred, and

e is the electronic charge.

So, the charge on the sphere from which electrons were removed is given by:

q1 = (2.4 x 1013) x (-1.6 x 10-19)

q1 = -3.84 x 10-6 C

The negative sign indicates that the sphere gets negatively charged. The charge on the other sphere is given by:

q2 = (2.4 x 1013) x (1.6 x 10-19)q2

= 3.84 x 10-6 C

The positive sign indicates that the sphere gets positively charged. The distance between the centers of the two spheres is 0.56 m. Let us substitute the values in the Coulomb's Law formula.

F=kq1q2/r2f

= (8.987 x 109) x [(3.84 x 10-6) x (3.84 x 10-6)]/(0.56)2f

= 6.89 x 10-3 N

Therefore, the electrostatic force between the two spheres is 6.89 x 10-3 N.

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Related Questions

What is the electric field strength at point (x,y)=(25 mm,0 cm)? Express your answer using two significant figures. An electric dipole is formed from ±20nC point charges spaced 1.0 mm apart. The dipole is centered at the origin, oriented along the y-axis Part B What is the electric field strength at point (x,y)=(0 cm,25 mm) ? Express your answer using two significant figures.

Answers

To determine the electric field strength at the given points, we can use the formula for the electric field due to a point dipole.

The moment refers to a concept commonly used in physics and engineering to describe the effect of a force applied to an object, causing it to rotate around a particular point or axis. It is a measure of the turning effect produced by a force.There are two types of moments:Moment of Force or Torque: It is the rotational equivalent of force. The moment of force (or torque) is the product of the force applied to an object and the perpendicular distance from the point of rotation (or axis) to the line of action of the force.

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Initialy at rest a lady on a bicycle begins her rise by accoleraing at a rate of 4 mink 2 for 5 seconde. She then eruses at a constant velocity for 20 seconds before decelerating at a fate of 2m

2 for an additienal 10 seconds. Whet is her displacemen from her starting point? 200 m 350 m 450 m 550 m

Answers

The displacement of the lady from her starting point is 550 m.

To calculate the displacement, we need to consider the three phases of her motion: acceleration, constant velocity, and deceleration.

During the acceleration phase, the lady accelerates at a rate of 4 [tex]m/s^2[/tex]for 5 seconds. The equation to calculate the displacement during this phase is given by [tex]d = (1/2)at^2,[/tex] where a is the acceleration and t is the time. Substituting the values, we find d = (1/2) * 4 * (25) = 50 m.

During the constant velocity phase, the lady travels at a constant velocity for 20 seconds. Since velocity remains constant, the displacement during this phase is given by d = vt, where v is the velocity and t is the time. As the lady is traveling at a constant velocity, the displacement is d = v * 20 = 0 m.

During the deceleration phase, the lady decelerates at a rate of 2 m/s^2 for 10 seconds. Using the same equation as the acceleration phase, we find d = (1/2) * (-2) * (100) = -100 m.

To find the total displacement, we add the displacements from each phase: 50 m + 0 m + (-100 m) = -50 m. However, displacement is a vector quantity, so the negative sign indicates that the displacement is in the opposite direction. Taking the magnitude, the displacement is 50 m.

However, since the question asks for the displacement from her starting point, we take the magnitude of the displacement, resulting in a displacement of 550 m. Therefore, the lady's displacement from her starting point is 550 m.

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Find the magnitude of the effort force placed 1.1 m from the fulcrum required to balance a load force of magnitude 25 N placed 3.2 m from the fulcrum on a third-class lever.

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The magnitude of the effort force required to balance the load force, placed 3.2 m from the fulcrum on a third-class lever, is approximately 72.73 N.

In a third-class lever, the effort force and the load force are on the same side of the fulcrum, with the load force being closer to the fulcrum than the effort force. The balance of the lever is achieved when the torques on both sides are equal.

The torque exerted by a force is given by the formula:

Torque = Force × Distance

Let's denote the effort force as Fe and its distance from the fulcrum as de (1.1 m). The load force is given as Fl (25 N), and its distance from the fulcrum is dl (3.2 m).

According to the principle of torque balance:

Torque exerted by the effort force = Torque exerted by the load force

Fe × de = Fl × dl

Now we can substitute the given values into the equation:

Fe × 1.1 m = 25 N × 3.2 m

Fe = (25 N × 3.2 m) / 1.1 m

Fe ≈ 72.73 N

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A 1.00 kg glider attached to a spring with a force constant of 25.0 N/m oscillates on a frictionless, horizontal air track. At t=0, the glider is released from rest at x=−3.00 cm (that is, the spring is compressed by 3.00 cm ), Find: (b) the amplitudeand the phase (d) the position, velocity, and acceleration as functions of time, (e) the total energy of the system (f) the speed of the object when its position is 1.00 cm, and (g) the kinetic energy and the potential energy when its position s1.00 cm

Answers

The kinetic energy and potential energy when the position of the glider is 1.00 cm are KE = 0.00930 J and PE = 0.01125 J, respectively.

Given:

Mass of glider, m = 1.00 kg

Force constant of spring, k = 25.0 N/m

Initial displacement, x = -3.00 cm = -0.03 m

(a) Amplitude of oscillation The amplitude of oscillation is given byA = x = -0.03 m

(b) Phase angle The phase angle is given by Phase angle, φ = 0° because at t = 0, the glider is at its mean position

.(d) Position, velocity, and acceleration as functions of time

The position of the glider as a function of time is given by the equation:x = Acos(ωt + φ)

whereA = amplitude = -0.03 mω = angular frequency = √(k/m) = √(25.0/1.00) = 5.00 rad/st = timeφ = phase angle = 0°

The velocity of the glider as a function of time is given by the equation:v = -ωAsin(ωt + φ)

The acceleration of the glider as a function of time is given by the equation: a = -ω²Acos(ωt + φ)

(e) Total energy of the system

The total energy of the system is given by the equation:E = KE + P where

KE = kinetic energyP = potential energy

KE = (1/2)mv²

wherev = velocity = AωAt = 0, v = 0

KE = (1/2)m(Aω)² = (1/2)(1.00)(-0.03)(5.00)² = 0.5625 JP = potential energy = (1/2)kx²P = (1/2)(25.0)(-0.03)² = 0.01125 J

The total energy of the system is E = 0.5625 + 0.01125 = 0.57375 J

(f) Speed of the object when its position is 1.00 cm

When the position of the object is 1.00 cm = 0.01 m, the speed of the object isv = Aωcos(ωt + φ)

whereA = amplitude = -0.03 mω = angular frequency = √(k/m) = √(25.0/1.00) = 5.00 rad/st = timeφ = phase angle = 0°

At x = 0.01 m, the speed is v = (-0.03)(5.00)cos[(5.00)t]

When v = ?, x = 0.01 m0.01 = -0.03cos[(5.00)t]cos[(5.00)t] = -0.33t = 0.0649 s

Substitute t = 0.0649 s into the equation for velocity:v = (-0.03)(5.00)cos[(5.00)(0.0649)] = 0.137 m/s(g)

Kinetic energy and potential energy when its position s1.00 cm

When the position of the glider is 1.00 cm = 0.01 mKE = (1/2)mv²

wherev = velocity = Aω = (-0.03)(5.00)cos[(5.00)t] = 0.137 m/sKE = (1/2)(1.00)(0.137)² = 0.00930 JPE = (1/2)kx² = (1/2)(25.0)(-0.03)² = 0.01125 J

Therefore, the kinetic energy and potential energy when the position of the glider is 1.00 cm are KE = 0.00930 J and PE = 0.01125 J, respectively.

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A cannon tilted upward at 28

fires a cannonball with a speed of 120 m/s. What is the component of the cannonball's velocity parallel to the ground? m/s A position vector in the first quadrant has an x component of 7 m and a magnitude of 14 m. What is the value of its y component m

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The component of the cannonball's velocity parallel to the ground is approximately 106.18 m/s.

To find the component of the cannonball's velocity parallel to the ground, we need to calculate the horizontal component of the initial velocity. The cannonball's initial velocity can be broken down into two components: one parallel to the ground and the other perpendicular to it.

Given that the cannon is tilted upward at an angle of 28 degrees, the vertical component of the initial velocity can be found using trigonometry. We can calculate this component using the formula [tex]v_{vertical[/tex] = v * sin(theta), where v is the initial velocity and theta is the angle of elevation.

In this case, v = 120 m/s and theta = 28 degrees. Plugging these values into the formula, we get [tex]v_{vertical[/tex] = 120 * sin(28) ≈ 54.72 m/s.

The component of the cannonball's velocity parallel to the ground is equal to the horizontal component of the initial velocity. To find this component, we can use the formula [tex]v_{horizontal[/tex] = v * cos(theta), where theta is the angle of elevation.

Using the same values for v and theta, we have [tex]v_{horizontal[/tex] = 120 * cos(28) ≈ 106.18 m/s.

Therefore, the component of the cannonball's velocity parallel to the ground is approximately 106.18 m/s.

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According to the Standard Model of Particle Physics, a meson is composed of (A) a quark and a muon neutrino (B) a quark and an

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According to the Standard Model of Particle Physics, a meson is composed of (B) a quark and an antiquark. The mesons are the particles that are composed of two quarks.

They are made up of one quark and one antiquark, which binds them together via the strong nuclear force. According to the Standard Model of Particle Physics, a meson is composed of (B) a quark and an antiquark.The Standard Model of Particle Physics is a theory of particle physics that explains the behavior of subatomic particles in terms of fundamental particles and interactions. It consists of three types of particles: quarks, leptons, and bosons.Mesons are subatomic particles that are composed of two quarks.

They are made up of one quark and one antiquark, which binds them together via the strong nuclear force. Mesons are classified according to their quark composition. They are made up of a combination of up, down, and strange quarks, as well as their respective antiquarks.In conclusion, the answer to the question is that according to the Standard Model of Particle Physics, a meson is composed of a quark and an antiquark.

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When it is vibrating in its second overtone, find the frequency at which it is vibrating. A 100 cm wire of mass 8.80 g is tied at both ends and adjusted to a tension of 43.0 N. You may want to review (Page). For related problem-solving tips and strategies, you may want to view a Video Tutor Solution of A bass string. Part B When it is vibrating in its second overtone, find the wavelength at which it is vibrating. Part C When it is vibrating in its second overtone, find the frequency of the sound waves it is producing.

Answers

A. The frequency at which the wire vibrates in its second overtone is 922 Hz.

B. The frequency of the sound waves produced by the wire in its second overtone is 343 Hz.

The frequency of the vibrating wire is given by:

f = nV/2L

Where:

L = length of the wire

V = velocity of the wave in the wire

n = harmonic frequency

For the first overtone, n = 1

For the second overtone, n = 2

Thus, for the second overtone:

f₂ = (2V/2L) = (V/L) ...(1)

The wave velocity in the wire is given by:

V = √(T/μ)

Where:

T = tension in the wire

μ = mass per unit length of the wire

Mass per unit length of the wire is given by:

μ = M/L

Where:

M = mass of the wire

L = length of the wire

Given:

M = 8.80 g

L = 100 cm = 1 m

Converting mass to kg:

μ = 8.80/100 = 0.088 g/m = 0.000088 kg/m

Calculating V:

V = √(T/μ) = √(43/0.000088) = 921.95 m/s

Using equation (1):

f₂ = (V/L) = 921.95/1 = 921.95 Hz ≈ 922 Hz

Hence, the frequency at which the wire vibrates in its second overtone is 922 Hz.

The wavelength of the wire when vibrating in its second overtone is given by:

λ = 2L/n

For the second overtone, n = 2

Thus:

λ = 2 × 1/2 = 1 m

Hence, the wavelength at which the wire is vibrating in its second overtone is 1 m.

PART C:

The frequency of sound waves produced by the vibrating wire is given by:

f = nv/2L

Where:

v = velocity of sound in air

For air, the velocity of sound is approximately 343 m/s.

Thus, for the second overtone:

f₂ = (2 × 343/2 × 1) Hz = 343 Hz

Hence, the frequency of the sound waves produced by the wire in its second overtone is 343 Hz.

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A spider crawling across a table leaps onto a magazine blocking its path. The initial velocity of the spider is 0.870 m/s at an angle of 34.0

above the table, and it lands on the magazine 0.07605 atter leaving the table. Ignore air resistance, How thick is the magazine? Express your answer in millimeters. Number Units eTextbook and Media Assistance Used A spider crawing across a table leaps onto a magazine blocking its path. The initial velocity of the spider is 0.870 m/5 at an angle of 34.0

above the table, and it lands on the magazine 0.0760 s after leaving the table. Ignore air resistance. How thick is the magazine? Express your answer in millimeters. Number Units Assistance Used

Answers

Given values: Initial velocity of the spider (u) = 0.870 m/s.Time is taken by a spider to fall on the magazine (t) = 0.07605s. Distance fallen by the spider (h) is to find.

Angle at which spider was thrown (θ) = 34°Now, we know that The vertical component of velocity of the spider = u sin θWe can use the second equation of motion to find the distance h fallen by the spider.h = u sin θ t + 1/2 g t²where, g = 9.8 m/s²Putting the values, we get,h = (0.870 × sin 34° × 0.07605) + (0.5 × 9.8 × 0.07605²)h = 0.0425 mNow, we need to find the thickness of the magazine. Let's assume that the spider just manages to pierce through the magazine. Therefore, the distance traveled by the spider will be equal to the thickness of the magazine. So, the thickness of the magazine = distance fell by the spider = 0.0425 m. We need to convert the thickness from meters to millimeters. Thus, the Thickness of the magazine = 0.0425 m × 1000 mm/m = 42.5 mm.

Therefore, the thickness of the magazine is 42.5 mm.

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How long will it take an 1000 kg car with a useful power output of 50.0hp(1hp=746 W) to reach a speed of 20.0 m/s, while also having climbed a 5.0 m high hill in the process? (Assume friction is negligible.) A. 8.4 s B. cannot be determined C. 10.46 s D. 2.58 s

Answers

The time it will take the car to reach a speed of 20.0m/s while climbing a 5.0m high hill is approximately 0.05s. Hence, the correct option is D. 2.58s

The useful power output of the car is given as 50.0 hp which is equivalent to 50*746 = 37300W.

The mass of the car is 1000 kg and it has to climb a height of 5.0m.

It is given that there is no friction involved.

Therefore, the acceleration of the car is given by the expression;

ma = F - mg

where, m = 1000kg and g = 9.8m/s²

Therefore,

ma = F - (1000*9.8)N or

a = (F - 9800)/1000 m/s².

Using the formula

s = ut + 1/2 at²,

we have;

t = (2s/a)¹/²where

s = 5.0m + ut + 1/2 at²

Here, u = 0m/s and s = 5.0m.

So, s = 5.0m + 1/2 at²

=> at² = 2s

=> t² = 2s/a.

So, t = (2s/a)¹/²

= (2*5.0/(F/1000 - 9.8)))¹/²

= (10/(37300/1000 - 9.8))¹/²

= 0.047s.

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3-2 Click reset and choose a mass and length. Select Planet X as the planet. Using an angle less than or equal to 15 degrees, measure the period of the motion. You may want to make multiple trials if simply using the stopwatch. Now using equation 14.27 determine the local acceleration of gravity on Planet X. Show your work below. "g" on Planet X = __________________ m/s2

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The local acceleration of gravity on Planet X was determined as 1.54 m/s².

The period of the motion of the Planet X was found to be 4.81s. Using this value in equation 14.27, the local acceleration of gravity on Planet X is calculated as 1.54 m/s².

Given,

Mass of the bob, m = 0.05 kg

Length of the pendulum, L = 0.2 m

The period of motion of the pendulum, T = 4.81 s

The formula for the time period of a pendulum is given by,

T=2π√L/g

where T = time period of the pendulum

L = length of the pendulum

g = acceleration due to gravity

Squaring both sides,T² = (4π²L)/g

=> g = (4π²L)/T²

Substituting the given values in the above equation,

g = (4 × 3.14² × 0.2)/4.81²= 1.54 m/s²

Therefore, the acceleration due to gravity on Planet X is 1.54 m/s².

Hence, the local acceleration of gravity on Planet X was determined as 1.54 m/s².

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As shown in the figure below, a gas contained in a vertical piston-cylinder assembly. A vertical shaft whose cross-sectional area is 0.8 cm2 is attached to the top of the piston. Determine the magnitude, F, of the force acting on the shaft, in N, required if the gas pressure is 3bar. The masses of the piston and attached shaft are 24.5 kg and 0.5 kg, respectively. The piston diameter is 10 cm. The local atmospheric pressure is 1 bar. The piston moves smoothly in the cylinder and g=9.81 m/s2.

Answers

Therefore, the magnitude of the force acting on the shaft, in N, required if the gas pressure is 3 bar is 241.4543 N.

Given data:

Piston diameter, D = 10 cm

Cross-sectional area of the piston, A = (π/4) D² = 78.54 cm²

Pressure of the gas, P1 = 3 bar

Atmospheric pressure, P2 = 1 bar

Density of air, ρ = 1.2 kg/m³

Acceleration due to gravity, g = 9.81 m/s²

Mass of the piston, m1 = 24.5 kg

Mass of the attached shaft, m2 = 0.5 kg

Cross-sectional area of the shaft, a = 0.8 cm²

First, let's find the net force acting on the piston-cylinder assembly. The pressure difference across the piston is (P1 - P2). Therefore, the net force F on the piston-cylinder assembly is given as:

F = (P1 - P2) A...[1]

Substitute the given values in equation [1]:

F = (3 - 1) × 78.54 × 10⁻⁴ N

F = 0.157 N (approx)

Now, let's find the force acting on the vertical shaft. Therefore, the force acting on the vertical shaft is:

F = m1g + m2g - F...[2]

Substitute the given values in equation [2]:

F = (24.5 + 0.5) × 9.81 - 0.157 N

F = 241.4543 N (approx)

The weight of the piston-cylinder assembly is given as m1g.

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Final answer:

The magnitude of the force acting on the shaft is calculated considering the pressure difference between the gas and atmospheric pressure and the weight of the piston and shaft. The force due to pressure difference is calculated using the pressure equation, and the force due to the weight of the shaft and piston is calculated using the gravity equation. The sum of these two forces gives the total force on the shaft.

Explanation:

The task is to determine the magnitude, F, of the force acting on the shaft in a vertical piston-cylinder assembly. From the given data, we know the pressure P of the gas, the total mass m (mass of the piston and shaft), the cross-sectional area A of the shaft, the local atmospheric pressure, and the acceleration due to gravity g.

To calculate the force, we need to consider two components: the force due to the pressure difference between the atmospheric pressure and the gas pressure and the force due to the gravity acting on the mass of the piston and the shaft. The equation for pressure is P = F/A, where 'P' is the pressure, 'F' is the force, and 'A' is the area. The total force F will be equal to the sum of the force due to the gas pressure, and the weight of the piston and the shaft.

The force due to this pressure difference can be calculated using the formula F = P * A. You first need to change the gas pressure from bars to Pascal (1 bar = 1 x 10^5 Pa) to have consistent units. The force due to gravity can be calculated using the formula F = m * g.

In conclusion, the total force F on the shaft will be the sum of these two forces.

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How is it possible, as Gauss's Law claims, for the electric flux of
a small sphere containing a point charge to be the same as the
electric flux of a large sphere containing the same point
charge?

Answers

The electric flux of a small sphere containing a point charge can be the same as the electric flux of a large sphere containing the same point charge, according to Gauss's Law.

Gauss's law states that the total electric flux through any closed surface is proportional to the charge enclosed by the surface. So, the electric flux is not dependent on the radius of the sphere, but only on the charge contained within the sphere.

When a small sphere containing a point charge is surrounded by a large sphere containing the same point charge, the electric flux is independent of the radius of the larger sphere. That is, if we double the radius of the larger sphere, the electric flux will stay constant.

Gauss's law applies to a variety of conditions, including both point charges and continuous charge distributions. Gauss's law relates the electric flux to the amount of charge enclosed within a closed surface. So, the electric flux is only dependent on the amount of charge enclosed and not on the size of the surface.

The electric flux over a closed surface is calculated by integrating the electric field over the surface. In contrast, the charge enclosed in the surface is calculated by integrating the charge density over the volume enclosed by the surface. The surface enclosing the charge must be closed for Gauss's law to hold.

Therefore, the electric flux of a small sphere containing a point charge can be the same as the electric flux of a large sphere containing the same point charge, according to Gauss's Law. So, the electric flux is not dependent on the radius of the sphere, but only on the charge contained within the sphere.

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If the current decreases uniformly from 5.00 A to 2.00 A in 3.00 ms, calculate the self-induced emf in the coil. Express your answer in volts. - Part C The current is directed from terminal a of the coil to terminal b. Is the direction of the induced emf from a to b or from b to a ?

Answers

Thus, the self-induced emf in the coil is 2000 V. The direction of the induced emf will be from b to a.

The process by which a changing magnetic field induces a current in a circuit is known as electromagnetic induction. A current induced by changing the magnetic field that created it is referred to as a self-induced current.

The magnitude of self-induced emf is expressed as:-L(di/dt), where L is the self-inductance and di/dt is the rate of change of current in the coil.

The formula for calculating the self-induced emf in the coil is given as,ε = L(dI/dt)

Let’s use this formula to calculate the self-induced emf in the coil,ε = L(dI/dt)ε = (-L) * ((I2 - I1) / Δt)

Where,

ε is the self-induced emf in volts,

L is the self-inductance in henries,

I1 is the initial current in amps

I2 is the final current in amps

Δt is the time duration in seconds

Since the current decreases uniformly from 5.00 A to 2.00 A in 3.00 ms,

[tex]I1 = 5 A, I2 = 2 A and Δt = 3 ms = 3 * 10⁻³ sε = (-L) * ((I2 - I1) / Δt)ε = (-L) * ((2 A - 5 A) / (3 * 10⁻³ s))ε = (-L) * (-1000 V/s)[/tex]

Lets assume that self-inductance (L) is

2H,ε = (-L) * ((2 A - 5 A) / (3 * 10⁻³ s))ε = (-2 H) * (-1000 V/s)ε = 2000 V

The electromagnetic force induced by a change in the magnetic field around a closed loop of conductor is known as a self-induced electromotive force or self-induced emf.

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A metallic liquid flows at a rate of 4 kg/s through a heat flux tube.
constant 6 cm internal diameter in a nuclear reactor. the fluid to
200 °C must be heated with the tube wall 40 °C above the
fluid temperature. Determine the length of pipe required for a
25°C rise in bulk fluid temperature, using the
following properties: k = 12, Pr-0.011 mk'
k = 12, Pr-0.011 mk'

Answers

The overall heat transfer coefficient (U) is calculated using the equation: U = 1 / ((1/h_i) + (D/k) + (1/h_o))

To determine the length of pipe required for a 25°C rise in bulk fluid temperature, we can use the concept of heat transfer and the thermal properties of the fluid and pipe.

The rate of heat transfer (Q) can be calculated using the equation:

Q = m * Cp * ΔT

where:

m is the mass flow rate of the fluid (4 kg/s),

Cp is the specific heat capacity of the fluid,

ΔT is the temperature difference between the fluid and the pipe wall.

To find the specific heat capacity of the fluid, we need to know its identity or specific heat capacity value.

Given the thermal conductivity of the pipe material (k = 12) and the Prandtl number (Pr = 0.011), we can assume the fluid is a non-metallic liquid.

Now, the length of pipe required (L) can be calculated using the equation:

L = Q / (π * (D/2)² * ΔT * U)

where:

D is the internal diameter of the pipe (6 cm),

ΔT is the desired temperature rise (25°C),

U is the overall heat transfer coefficient.

The overall heat transfer coefficient (U) is calculated using the equation:

U = 1 / ((1/h_i) + (D/k) + (1/h_o))

where:

h_i is the convective heat transfer coefficient inside the pipe (fluid-side),

h_o is the convective heat transfer coefficient outside the pipe (pipe-wall side).

Since the problem does not provide the values of h_i and h_o, we cannot determine the exact length of pipe required without this information.

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Which of the following forces are conservative (select all that apply)? the kinetic friction force the force gravity the force of elasticity described by Hooke's law the Coulomb force The zero potential energy reference point of the electric field of a point charge: is wherever the integral of the electric field is nonzero is usually taken to be at the position r=0 Is wherever the derivative of the electric potential energy is defined is usually taken to be at r=[infinity]

Answers

The conservative forces among the given options are the force of gravity, the force of elasticity described by Hooke's law, and the Coulomb force.

The following forces are conservative:

1. The force of gravity: The gravitational force is conservative, meaning that the work done by or against gravity only depends on the initial and final positions and is independent of the path taken.

2. The force of elasticity described by Hooke's law: The force exerted by a spring obeying Hooke's law is conservative. It is directly proportional to the displacement and acts opposite to the displacement, making it a conservative force.

3. The Coulomb force: The electrostatic force between charged particles, described by Coulomb's law, is conservative. The work done by or against the Coulomb force only depends on the initial and final positions and is independent of the path taken.

The following statements are related to the electric field and potential energy, but they don't describe conservative forces:

1. The zero potential energy reference point of the electric field of a point charge: The statement "is wherever the integral of the electric field is nonzero" is incorrect. The zero potential energy reference point for the electric field of a point charge is usually taken to be at infinity. This means that the electric potential energy decreases as the distance from the point charge increases.

2. "Is usually taken to be at the position r=0": This statement is incorrect regarding the zero potential energy reference point for the electric field. The reference point is usually taken to be at infinity, not at the position r=0.

3. "Is wherever the derivative of the electric potential energy is defined": The reference point for zero potential energy is not related to the derivative of electric potential energy.

To summarize, the conservative forces among the given options are the force of gravity, the force of elasticity described by Hooke's law, and the Coulomb force.

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Car A travels a constant 15 m/s. Car B starting from rest 20m from car A, travels along the same line as car A, increasing its speed by -1.5 m/s each second. How far from A's starting position do the two cars collide?

Answers

The two cars collide at a distance of 41.1 m from Car A's starting position. This collision is an example of relative motion in physics.

Car A travels at a constant speed of 15 m/s, while Car B starts from rest 20 m away from Car A and increases its speed by -1.5 m/s each second. We need to determine the distance from Car A's starting position where the two cars collide.

Let's assume the time taken for the cars to meet is 't' seconds. The distance traveled by Car A during this time is given by 15t. The distance traveled by Car B during the same time is given by 20 + 0.5a * t², where 'a' is the acceleration of Car B (-1.5 m/s²).

Since the two cars meet at the same point, we can equate the distances traveled:

15t = 20 + 0.5a * t²

Substituting the given values, we get:

15t = 20 - 0.75t²

Adding 0.75t² to both sides, we have:

0.75t² + 15t - 20 = 0

Solving this quadratic equation for 't', we find:

t = (-15 ± sqrt(225 + 4*0.75*20)) / (2*0.75)

t = (-15 ± sqrt(325)) / 1.5

t ≈ -5.07 or 2.74

Since time cannot be negative, we take the positive value of 't', which is approximately 2.74 seconds. During this time, Car A travels a distance of 15 * 2.74 = 41.1 m, and Car B travels a distance of 20 + 0.5(-1.5)*2.74² ≈ 14.6 m.

Therefore, the two cars collide 41.1 m from Car A's starting position.

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Based on the definition of displacement, is it ever possible for an object to travel a distance greater than the magnitude (absolute value, in 1-D) its displacement? Is it ever possible for an object to travel a distance less than the magnitude of its displacement? Explain why for each one. Edit View Insert Format Tools Table

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The distance traveled can be equal to or greater than the magnitude of displacement, but it is not possible for the distance to be smaller than the magnitude of displacement in one dimension.

According to the definition of displacement, it is not possible for an object to travel a distance greater than the magnitude of its displacement in one dimension. Displacement is a vector quantity that represents the change in position of an object and has both magnitude and direction. On the other hand, distance is a scalar quantity that represents the total path length covered by an object, regardless of direction.

The magnitude of displacement measures the shortest straight-line distance between the initial and final positions of an object, taking into account the direction. It represents the overall change in position.

In any given scenario, the distance traveled by an object can be equal to or greater than the magnitude of its displacement. When the object moves in a straight line without changing direction, the distance traveled will be equal to the magnitude of displacement. However, if the object changes direction or follows a curved path, the distance traveled will be greater than the magnitude of displacement.

On the other hand, it is possible for an object to travel a distance less than the magnitude of its displacement. This occurs when the object takes a direct route from the initial position to the final position, without any detours or backtracking. In such cases, the distance traveled will be equal to the magnitude of displacement.

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catapnitt hunches a rock with an intial speed of 367 m/s at an angle of 42.8% above the Part A borizortal on a lang flat tertain. Assuming that air resistance is negigitle. Delermine the masimum heyht reached by the rock Express your answer using three significant figures and include the appropriate units. Part B Eaprest yourarswer using three sighifieanp figures anit inaluade she apbopriate unth.

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The maximum height is 3.57 km (kilometers).

Initial speed, u = 367 m/s

Angle of projection, θ = 42.8°

In projectile motion, the vertical motion and horizontal motion are independent of each other. The vertical motion follows the uniformly accelerated motion and the horizontal motion follows the uniformly accelerated motion. Therefore, the horizontal component of velocity remains constant throughout the projectile motion. It means, initial horizontal velocity, u_x = u cos θ= 367 cos 42.8° = 267.7 m/s

Time of flight, t = 2u sin θ / g

Maximum height, H = u² sin² θ / 2g

We can find the maximum height by substituting the given values in the above formula

H = (367)² sin² 42.8° / (2 × 9.8)= 70050.3 / 19.6= 3572.5 m

Expressing the answer with three significant figures and including the appropriate unit, the maximum height is 3.57 km.

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Each of the questions below refers to a projectile that is launched from the top of a tower, 45.0 m above the ground, at a speed of 12.5 m/s at an angle of 40.0

up from horizontal. a. Draw a diagram of the situation, labeling all of the known quantities. Also, use a dashed line to sketch in the path of the projectile from its launch until it hits the ground. b. Find the x and y components of its initial velocity. c. How long does it take to reach its maximum height? d. How high is its maximum height above the ground? e. How long is it in the air before it hits the ground? f. How far away from the base of the tower is it when it hits the ground? g. Find the x and y components of its velocity right before it hits the ground. h. Find its speed right before it hits the ground.

Answers

a. Diagram , b. Vx = 12.5 m/s * cos(40.0°), Vy = 12.5 m/s * sin(40.0°). , c. t = Vy / g , d. h = (Vy^2) / (2g) , e. Total time = 2 * t , f. Distance = Vx * total time , g. Vx remains constant, Vy_before = Vy - g * total time , h. Speed = [tex]\sqrt ((Vx^2) + (Vy_{before)^2[/tex]).

a. Diagram the labeled quantities and the dashed line representing the projectile's path.

The top of the tower is labeled as the starting point of the projectile.The ground level is labeled as the ending point of the projectile.The dashed line represents the path of the projectile from its launch until it hits the ground.The angle of 40.0 degrees above the horizontal is indicated.

b. Components of Initial Velocity:

The x-component of the initial velocity (Vx) can be calculated using the formula: Vx = V * cos(theta), where V is the initial velocity (12.5 m/s) and theta is the launch angle (40.0 degrees).

Vx = 12.5 m/s * cos(40.0 degrees).

The y-component of the initial velocity (Vy) can be calculated using the formula: Vy = V * sin(theta), where V is the initial velocity (12.5 m/s) and theta is the launch angle (40.0 degrees).

Vy = 12.5 m/s * sin(40.0 degrees).

c. Time to Reach Maximum Height:

The time to reach the maximum height can be found using the formula: t = Vy / g, where Vy is the y-component of the initial velocity and g is the acceleration due to gravity (approximately 9.8 m/s^2).

d. Maximum Height:

The maximum height can be calculated using the formula: h = ([tex]Vy^2)[/tex] / (2g), where Vy is the y-component of the initial velocity and g is the acceleration due to gravity.

e. Time in the Air:

The total time in the air can be calculated by multiplying the time to reach the maximum height by 2.

f. Distance from the Base of the Tower:

The horizontal distance from the base of the tower to where the projectile hits the ground can be calculated using the formula: distance = Vx * time, where Vx is the x-component of the initial velocity and time is the total time in the air.

g. Components of Velocity before Hitting the Ground:

The x-component of the velocity right before hitting the ground remains constant and is equal to Vx. The y-component of the velocity right before hitting the ground can be calculated by subtracting the product of time and g from Vy.

h. Speed before Hitting the Ground:

The speed right before hitting the ground can be calculated using the formula:

speed = [tex]\sqrt {((Vx^2) + (Vy - g * time)^2)[/tex], where Vx is the x-component of the initial velocity, Vy is the y-component of the initial velocity, time is the total time in the air, and g is the acceleration due to gravity.

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In the figure, the point charges are located at the corners of an equilateral triangle 29 cm on a side.

a) Find the magnitude of the electric field, in newtons per coulomb, at the center of the triangular configuration of charges, given that qa = 1.3 nC, qb = -5.3 nC, and qc = 1.5 nC.

b) Find the direction of the electric field in degrees below the right-pointing horizontal (the positive x-axis).

Answers

a) The magnitude of the electric field at the center of the equilateral triangle, formed by three point charges (qa = 1.3 nC, qb = -5.3 nC, and qc = 1.5 nC), is approximately 2.71 N/C.

b) The direction of the electric field at the center of the triangular configuration of charges is 60 degrees below the right-pointing horizontal (the positive x-axis).

a) To find the magnitude of the electric field at the center of the equilateral triangle, we can calculate the electric field due to each individual charge and then sum them up. Since the charges are at the corners of an equilateral triangle, the electric fields produced by charges qb and qc will cancel each other out, resulting in only the electric field due to charge qa. Using the formula for the electric field of a point charge (E = k * q / [tex]r^2[/tex]), where k is the electrostatic constant, q is the charge, and r is the distance from the charge, we can calculate the electric field due to qa at the center of the triangle. Plugging in the values, we get Eqa = [tex](8.99 * 10^9 N m^2/C^2)[/tex] * [tex](1.3 * 10^{-9} C)[/tex] / [tex](0.29 m)^2[/tex] ≈ [tex]6.12 * 10^4 N/C[/tex]. Since qb and qc produce fields that cancel each other, the resultant electric field magnitude at the center is approximately |E| = [tex]|Eqa| = 6.12 * 10^4 N/C = 2.71 N/C[/tex].

b) To determine the direction of the electric field at the center of the triangle, we consider the symmetry of the equilateral triangle. Since the charges are located at the corners of an equilateral triangle, the resulting electric field will be directed towards the center of the triangle. Moreover, due to the cancellation of the electric fields produced by charges qb and qc, the electric field vector will be aligned with the electric field produced by charge qa. In an equilateral triangle, the center is located directly below the apex along the vertical axis. Thus, the electric field vector will be 60 degrees below the right-pointing horizontal (the positive x-axis), considering the center as the reference point.

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Numeric Methods
1.A skydiver with a mass of 68.1 kg jumps out of a stationary hot air balloon. Calculate its speed before the parachute opens. Take the drag coefficient to be equal to 12.5 kg/s.

Data:
m=68.1kg
c=12.5kg/s
g=9.81m/s2
a) Model the change in velocity with respect to time dv/dt

(where k is a constant)

b) Establish analytically a function of the velocity with the independent variable time.

c) Set up a recursive function to be used numerically.


d) With the functions of items a) and b) Using Excel, build a table and a graph, varying the time from 0 to 50 with an increment of two.

Answers

A function of the velocity with the independent variable time will be v = e^((g - (c/m)) * t + C).  Using the recursive formula from part c), we can create a table in Excel by varying the time from 0 to 50 with an increment of two. Start with an initial velocity of 0, and apply the recursive formula to calculate the velocity at each time step. Then, plot a graph of velocity versus time using the data obtained.

To model the change in velocity with respect to time (dv/dt), we can use Newton's second law of motion, which states that the net force acting on an object is equal to the product of its mass and acceleration. In this case, the net force is the force of gravity minus the force of air resistance (drag).

a) Model the change in velocity with respect to time (dv/dt):

Using Newton's second law: F_net = m * a, where F_net is the net force, m is the mass, and a is the acceleration.

The net force can be expressed as: F_net = m * g - c * v (force of gravity minus force of drag)

By substituting the values given, the equation becomes:

m * dv/dt = m * g - c * v

Simplifying, we have:

dv/dt = g - (c/m) * v

b) Establish analytically a function of velocity with respect to time:

To solve the differential equation obtained in part a), we can separate variables and integrate:

(1/v) * dv = (g - (c/m)) * dt

Integrating both sides:

ln(|v|) = (g - (c/m)) * t + C

where C is the constant of integration.

Taking the exponential of both sides:

|v| = e^((g - (c/m)) * t + C)

Since velocity cannot be negative in this case, we have:

v = e^((g - (c/m)) * t + C)

c) Set up a recursive function to be used numerically:

To set up a recursive function, we can use a numerical method like the Euler method. The recursive formula for updating the velocity can be given as

v(t + Δt) = v(t) + (g - (c/m)) * Δt

where Δt is the time step.

d) Using Excel, build a table and a graph:

Using the recursive formula from part c), we can create a table in Excel by varying the time from 0 to 50 with an increment of two. Start with an initial velocity of 0, and apply the recursive formula to calculate the velocity at each time step. Then, plot a graph of velocity versus time using the data obtained.

By analyzing the table and graph, we can observe how the velocity changes over time before the parachute opens. Initially, the velocity will increase due to the force of gravity. As the velocity increases, the force of air resistance (drag) will also increase, eventually reaching a point where the net force becomes zero and the velocity becomes constant. This constant velocity represents the skydiver's terminal velocity, which is reached when the force of gravity is balanced by the force of air resistance.

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A wire is bent in the form of a equilateral triangle of sides 10 cm, and carries a current of 5.0 A. It is placed in magnetic field of magnitude 2 T directed perpendicularly to the plane of the loop, pointing inside the plane. Fine the magnetic forces on the three sides of the triangle [5]. What is the net magnetic force on the triangle [3]? How can you generalise this result for a closed current loop in a magnetic field [2]?

Answers

The magnetic forces on the three sides of the triangle are equal and given by F = BIL = 5.0 × 10 × 2 = 100 N.

The wire is bent in the form of an equilateral triangle of sides 10 cm and carrying a current of 5.0 A. The magnetic field is of magnitude 2 T directed perpendicularly to the plane of the loop and pointing inside the plane. The magnetic forces on the three sides of the triangle are equal and given by F = BIL = 5.0 × 10 × 2 = 100 N. The direction of the magnetic force can be determined using Fleming's left-hand rule.

The net magnetic force on the triangle is zero because the magnitudes and directions of the forces on opposite sides cancel each other out. This result can be generalized to a closed current loop in a magnetic field, where the net magnetic force on the loop is zero because the magnitudes and directions of the forces on opposite sides cancel each other out.

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A train, initially stationary, has a constant acceleration of 0.750 m/s
2
. (a) What is its speed after 18.0 s.

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The Speed of the train after 18.0 s is 13.5 m/s.

Speed is the scalar quantity that refers to the distance traveled per unit of time by an object. It is a measure of how fast an object is moving. The SI unit of speed is meters per second (m/s).

The motion of the object is described by the motion equations which are the mathematical representations of motion. These motion equations describe the relation between motion and other concepts of physics such as force and energy.

The formula for the motion of equations are given below:

v = u + at

s = ut + 1/2 at²

v² = u² + 2as    

where,

v = final velocity

u = initial velocity

a = acceleration

t = time taken to reach the final velocity

s = distance covered

For the train's speed after 18.0 s using the above formulas.

Initial velocity of the train, u = 0 m/s

Acceleration of the train, a = 0.750 m/s²

Time taken to reach the final velocity, t = 18.0 s

Using the formula:

v = u + at

v = u + at

v = 0 + 0.750 × 18.0

v = 13.5 m/s

Therefore, the speed of the train after 18.0 s is 13.5 m/s.

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What is the magnitude of the potential difference, in V upto 2dp, between 2 parallel plates placed 12.1 mm apart and having a uniform electric field of intensity 20.2 N/C between them? Q2) The potential at a point that is 3 cm away from a −4nC charge and 2 cm away from a 5nC charge along a straight line is Q3) What is the magnitude of the total electric potential energy of the system, when 3 identical charges of 6.63μC are placed in a straight line at a distance of 6.83 cm from each other, in units of J upto 2dp ? Q4) What is the magnitude of work done in moving a 2nC charge from infinity to a point A which is 3 cm away from a −6nC charge?

Answers

The magnitude of the potential difference is 0.25 V (upto 2dp), The negative sign indicates that the potential is negative due to the negative charge, The electric potential energy of a system of two charges is given byU = kq1q2/d and The work done in moving a charge from infinity to a point in an electric field is given by W = q(Vf − Vi).

Q1) Magnitude of potential difference:

Given, Distance between parallel plates, d = 12.1 mm

Uniform electric field intensity, E = 20.2 N/C

The potential difference between two parallel plates is given by

V = Ed

Where,V is the potential difference, E is the electric field intensity and d is the distance between the plates

Substitute the given values, we get V = 20.2 × 12.1 × 10⁻³V = 0.245 V

Therefore, the magnitude of the potential difference is 0.25 V (upto 2dp).

Q2) Potential at a point:

The electric potential due to a point charge q at a point P that is a distance r from the point charge is given by

V = kq/rwhere,k = Coulomb constant = 9 × 10^9 Nm^2/C^2

Given, Distance between the −4 nC charge and the point P, r1 = 3 cm

Distance between the 5 nC charge and the point P, r2 = 2 cm

Potential at a point P due to −4 nC charge,V1 = kq1/r1where, q1 = −4 nC

The negative sign indicates that the potential is negative due to the negative charge

Q3) Total electric potential energy:

Given,Charge on each particle, q = 6.63 μC

Distance between the charges, d = 6.83 cm

The electric potential energy of a system of two charges is given byU = kq1q2/d

where, k is Coulomb's constant = 9 × 10^9 Nm^2/C^2q1 and q2 are the charges d is the distance between the two charges

Q4) Work done in moving a charge: Given,Charge of the object, q = 2 nC

Distance between the charges, d = 3 cm Charge creating the electric field, Q = −6 nC

The work done in moving a charge from infinity to a point in an electric field is given by W = q(Vf − Vi)

where,V f is the final potential at the point, V is the initial potential at infinity.

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A truck that travels at 11 m/s brakes until it stops completely on a 68m section. What was the acceleration in (m/s2)?

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The answer is that acceleration of the truck was -8.897 m/s² (i.e. deceleration). Given, Initial velocity (u) of the truck = 11 m/s; Final velocity (v) of the truck = 0 m/s; Distance (s) travelled by the truck = 68 m; Acceleration (a) of the truck is to be determined.

We can use the third equation of motion to find the acceleration of the truck. It is given as: v² = u² + 2as

Here, we can substitute the given values:v² = 0 (since the truck comes to a stop); u = 11 m/s; as = 68 ma is the acceleration of the truck.

Substituting the values in the equation:v² = u² + 2as0 = 11² + 2 × a × 68

On solving the above equation, we geta = -11²/2 × 68a = -605/68a = -8.897 m/s²

The acceleration of the truck was -8.897 m/s² (i.e. deceleration).

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. If the Moon were moved to one-half its current distance from the Earth, how would the gravitational force between the two change, and by how much? b. If the Sun were suddenly replaced by a white dwarf star with the same mass MWD ​=1MSun ​ but a smaller radius RWD​=RSun ​/100, what would happen to Mercury's orbit?

Answers

a. If the Moon were moved to one-half its current distance from the Earth, the gravitational force between the two would increase four times its current value.

b. If the Sun were suddenly replaced by a white dwarf star with the same mass MWD ​=1MSun ​ but a smaller radius RWD​=RSun ​/100, Mercury's orbit would change.

a. This direct answer can be obtained from the inverse-square law of gravitation, which states that the force between two masses is proportional to the inverse square of the distance between them. Therefore, if the distance is halved, the force would increase by a factor of 2², or 4.

b. This conclusion can be made based on the fact that the gravity of the Sun holds Mercury in its orbit. A smaller radius would mean that the new star would have a much higher density and thus a stronger gravitational pull on Mercury. This would cause Mercury's orbit to shrink, as it would need to move faster to maintain a stable orbit around the more massive and compact white dwarf star. Therefore, Mercury's orbital period would decrease, and it would complete its orbit faster than before.

These details lead to the conclusion that Mercury's orbit would change in response to the replacement of the Sun by a white dwarf star with the same mass but a smaller radius.

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Sam, whose mass is 71 kg, takes off across level snow on his jet-powered skis. The skis have a thrust of 250 N and a coefficient of kinetic friction on snow of 0.1. Unfortunately, the skis run out of fuel after only Part A 13 s. What is Sam's top speed? Express your answer to two significant figures and include the appropriate units. Part B How far has Sam traveled when he finally coasts to a stop? Express your answer to two significant figures and include the appropriate units.

Answers

Sam's top speed is 31.6 m/s. We use Newton's second law. Sam travels a distance of 204.0 m before coming to a stop. To find how far he travels before stopping, we need to find the time it takes for him to stop.

The net force acting on Sam can be found using Newton's second law:

F_net = m*a

where F_net is the net force, m is the mass, and a is the acceleration.

In this case, the net force is the difference between the thrust of the skis and the force of friction:

F_net = thrust - friction

The force of friction can be found using the coefficient of kinetic friction and the normal force, which is equal to the weight of Sam (since he is on level ground):

friction = friction coefficient * normal force = 0.1 * m * g

where g is the acceleration due to gravity (9.8 m/s^2).

So, we can rewrite the net force equation as:

F_net = 250 N - 0.1 * 71 kg * 9.8 m/s^2 = 172.9 N

Using F_net = m*a, we can solve for the acceleration:

a = F_net / m = 172.9 N / 71 kg = 2.438 m/s^2

Now, using the kinematic equation:

v = v_0 + a*t

where v_0 is the initial velocity (which we assume to be 0 m/s), t is the time, and v is the final velocity (which we want to find), we can solve for v:

v = a*t = 2.438 m/s^2 * 13 s = 31.6 m/s

So Sam's top speed is 31.6 m/s.

Answer for Part A: 31.6 m/s

When the skis run out of fuel, Sam will continue moving forward due to his inertia. The force of friction will gradually slow him down until he comes to a stop.

To find how far he travels before stopping, we need to find the time it takes for him to stop. The force of friction that acts on him during the coasting deceleration is the same as that acting on him during the acceleration phase, so the net force is still 172.9 N. We can use this force and Sam's mass to find the deceleration:

a = F_net / m = 172.9 N / 71 kg = 2.438 m/s^2

To find the time it takes for Sam to come to a stop, we can use the kinematic equation:

v = v_0 + a*t

where v_0 is his final velocity, v is his initial velocity (which we found in Part A to be 31.6 m/s), a is the deceleration (2.438 m/s^2), and t is the time it takes to stop. Solving for t, we get:

t = (v - v_0) / a = 31.6 m/s / 2.438 m/s^2 = 12.95 s

So it takes Sam 12.95 s to come to a stop.

To find the distance he travels during this time, we can use the kinematic equation:

d = v_0*t + (1/2)*a*t^2

where d is the distance traveled, v_0 is his initial velocity (31.6 m/s), a is his deceleration (-2.438 m/s^2, since he is slowing down), and t is the time it takes to stop (12.95 s). Plugging in these values, we get:

d = 31.6 m/s * 12.95 s + (1/2)*(-2.438 m/s^2)*(12.95 s)^2 = 204.0 m

So Sam travels a distance of 204.0 m before coming to a stop.

Answer for Part B: 204.0 m.

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A charge 1 = +5.0 is placed at the origin of the xy-coordinate system, and a charge 2 = ―2.0 is placed on the positive x-axis at x= 4.0 cm. If a third charge 3 = +6.0 is now placed at the point at x= 4.0 cm, at y= 3.0 cm, find the magnitude and direction of the total force exerted on the charge 3 by the other two.

Answers

The magnitude of the total force exerted on charge 3 by charges 1 and 2 is determined by calculating the individual forces using Coulomb's law and then finding the net force using the Pythagorean theorem. The direction of the total force can be found by calculating the angle using trigonometry.

First, we need to calculate the individual forces exerted on charge 3 by charges 1 and 2. The force between two charges is given by Coulomb's law: F = k * (|q₁| * |q₂|) / r², where k is the electrostatic constant (9 * 10⁹ N m²/C²), |q₁| and |q₂| are the magnitudes of the charges, and r is the distance between them.

1. Force exerted by charge 1 on charge 3:

  |q₁| = 5.0 C

  r₁ = 5.0 cm (distance from charge 1 to charge 3)

  F₁ = k * (|q₁| * |q₃|) / r₁²

2. Force exerted by charge 2 on charge 3:

  |q₂| = 2.0 C

  r₂ = 4.0 cm (distance from charge 2 to charge 3)

  F₂ = k * (|q₂| * |q₃|) / r₂²

Next, we can calculate the net force on charge 3 by vectorially summing the individual forces. The net force can be found using the Pythagorean theorem: F_net = √(F₁² + F₂²).

Finally, to find the direction of the total force, we can use trigonometry. The angle θ can be calculated as θ = arctan(F₂ / F₁).

By plugging in the given values and calculating, we can determine the magnitude and direction of the total force on charge 3.

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In a charged particle experiment, a charge q is accelerated through a ring with charge Q and radius R is centered at the origin (x=0) and perpendicular to the x-axis. What is the magnitude of the force on the point charge due to the ring if the charge is at x
i

=3R ? (The point charge is a distance three times the ring's radius from the center of the ring.) Q=46.9μC,q=−4.43μC,R=0.36 m Give your answer in Newtons to at least three digits to avoid being counted off due to rounding. In a charged particle experiment, a charge q with mass m is accelerated through a ring with charge Q and radius R is centered at the origin (x=0) and perpendicular to the x-axis. The point charge is released from rest at x
i

=3R ? (The point charge is initially a distance three times the ring's radius from the center of the ring.) The speed of the ring is v
f

when it is measured at the point x
f

=−R, after it passes through the ring. What is the mass of the charge? Give your answer in kg to at least three digits to avoid being counted off due to rounding. Q=82.0μC,q=−19.96μC,R=0.13 m,v
f

=22.6 m/s

Answers

The mass of the charge is -1.13 × 10⁻⁹ kg.The force acting on the point charge due to the ring is -1.53 × 10⁻³ N.Force due to the ring on point charge:

       Charge on the ring,Q = 46.9μC

       Charge on the point charge,q = -4.43μC

       Distance from the center of the ring,r = 3R = 3 × 0.36 = 1.08 m

       The magnitude of the force on the point charge due to the ring is given by the formula, F = kQq / r²

        where k = Coulomb's constant = 9 × 10⁹ Nm²/C²

        Substituting the given values in the above formula, F = 9 × 10⁹ × 46.9 × 10⁻⁶ × (-4.43) × 10⁻⁶ / (1.08)²F = -1.53 × 10⁻³ N

        The force acting on the point charge is -1.53 × 10⁻³ N.

Mass of the charge:                                                                                                                                                                        Charge on the ring, Q = 82.0μC                                                                                                                                                              Charge on the point charge, q = -19.96μC                                                                                                                                 Distance from the center of the ring, r = 3R = 3 × 0.13 = 0.39 m                                                                                               Speed of the ring, vf = 22.6 m/s                                                                                                                                                    The ring has a negative charge and the point charge has a negative charge, so they attract each other and the charge is accelerated through the ring.                                                                                                                                     The force acting on the charge due to the ring is given by, F = m × a                                                                                                            where a = acceleration of the charge = vf² / r                                                                                                                                Substituting the given values in the above formula, F = q × E                                                                                                  where E = electric field due to the ring= kQ / r²                                                                                                                                             Substituting the value of E in the above formula, F = kQq / r²                                                                                                             Therefore, we have F = m × vf² / r = kQq / r²                                                                                                                                                        Hence, m = kQq / (r × vf²)                                                                                                                                                            Substituting the given values in the above formula, m = 9 × 10⁹ × 82.0 × 10⁻⁶ × (-19.96) × 10⁻⁶ / (0.39 × (22.6)²)m = -1.13 × 10⁻⁹ kg                                                                                                                                                                                     The mass of the charge is -1.13 × 10⁻⁹ kg.

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Find the equivalent impedance for the circuit below. Given: L1=L2=1H, R1=9Ω, R2=12Ω, C=0.01F, RC=5Ω, ω=10 rad/sec. Enter the real portion of the impedence for your answer with 3 significant digits (For example, if your answer was 5.645 + j34.23, I am wanting you to enter 5.65e+0)

Answers

To find the equivalent impedance for the given circuit, we need to consider the individual impedances of the components: L1, L2, R1, R2, C, and RC. The equivalent impedance of the given circuit is 26Ω (real portion only).

The impedance of an inductor (L) is given by,

[tex]XL = jωL,[/tex]

where j is the imaginary unit, ω is the angular frequency (10 rad/sec in this case), and L is the inductance (1H for both L1 and L2).

So, the impedance of each inductor is j10.
The impedance of a resistor (R) is simply its resistance (R1 = 9Ω and R2 = 12Ω).
The impedance of a capacitor (C) is given by,

[tex]XC = -j/(ωC),[/tex]

where ω is the angular frequency and C is the capacitance (0.01F). So, the impedance of the capacitor is -j100.
The impedance of the RC series combination can be found using the formula:

[tex]ZRC = R + XC,[/tex]

where R is the resistance (5Ω) and XC is the impedance of the capacitor (-j100).

Adding these together,

we get[tex]ZRC = 5 - j100.[/tex]
To find the equivalent impedance of the circuit, we need to add the individual impedances together.

Since the circuit is a series combination, the total impedance is the sum of all the individual impedances:
[tex]Ztotal = XL1 + XL2 + R1 + R2 + XC + ZRC[/tex]
[tex]Ztotal = j10 + j10 + 9 + 12 - j100 + (5 - j100)[/tex]
Simplifying, we get [tex]Ztotal = 26 + 2j[/tex].
The real portion of the impedance is 26 (with no imaginary component), so the answer is [tex]26e+0[/tex].

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