A Nichrome wire 86 cm long and 0.25 mm in diameter is connected to a 1.3 volt flashlight battery. What is the electric field inside the wire

Answers

Answer 1

The electric field inside the Nichrome wire of length 86 cm and diameter 0.25mm is 1.51 V/m.

What is electric field?

Electric fields are created by electric charges. A positive charge creates an electric field that radiates outward from the charge, while a negative charge creates an electric field that points toward the charge.

The electric field inside the wire is given by the formula,

E = V / L,

where,

E = electric field,

V = potential difference across the wire,  

L = length of the wire

Thus, substituting the given values, we get;

E = V / L = 1.3 V / 0.86 m = 1.51 V/m

Thus, the electric field inside the Nichrome wire is 1.51 V/m.

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Related Questions

An arbitrarily shaped piece of conductor is given a net negative charge and is alone in space. What can we say about the electric potential within the conductor

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An arbitrarily shaped piece of conductor is given a net negative charge and is alone in space. Positive and continuous electric potential will exist throughout the conductor.

Electric potential at a point in an electric field is the amount of work done to move the unit positive charge there from infinity, whereas electric potential energy is the energy required to move a charge against the electric field. This is the main distinction between the two terms.

The electric field inside a conductor must be zero for it to be in balance.

Equipotentiality applies to conductors. Moving a charge from one point in a conductor to another requires no work because a charge is free to move about in it. As a result, it is equipotential.

Electric field lines are prependicular to the surface of a conductor because, as we already know, they are perpendicular to equipotential surfaces.

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Complete question is:

An arbitrarily shaped piece of conductor is given a net negative charge and is alone in space. What can we say about the electric potential within the conductor?

A ball is tossed up vertically from ground level and returns to Earth 14 s later. What was the initial velocity of the ball and what maximum height does the ball reach

Answers

The maximum height reached by the ball is 240.1 meters above the ground.

To determine the initial velocity of the ball and the maximum height it reaches, we can use the equations of motion for vertical motion.

When a ball is tossed up vertically, its initial velocity (u) is positive, and the acceleration due to gravity (g) is negative (taking downward as the negative direction).

Finding the initial velocity:

The time taken for the ball to reach the maximum height is half the total time of flight. Therefore, the time taken to reach the maximum height is 14 s / 2 = 7 s.

Using the equation of motion: v = u + at, where v is the final velocity, u is the initial velocity, a is the acceleration, and t is the time.

At the maximum height, the final velocity is 0 m/s, and the acceleration is -9.8 m/s² (acceleration due to gravity). Plugging these values into the equation, we have:

0 = u - 9.8 * 7

Solving for u:

u = 9.8 * 7 = 68.6 m/s (upward)

Therefore, the initial velocity of the ball is 68.6 m/s upward.

Finding the maximum height:

The equation to find the maximum height (h) reached by the ball is given by:

h = u * t - (1/2) * g * t²

Substituting the values:

h = 68.6 * 7 - (1/2) * 9.8 * 7²

h = 480.2 - 240.1

h = 240.1 m

Thus, the maximum height reached by the ball is 240.1 meters above the ground.

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What are two density changes that each make it possible for a moon to get closer to its planet without breaking apart

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When a moon gets closer to its planet, the gravitational forces between the two bodies increase. In order for the moon to get closer without breaking apart, two possible density changes could occur:

1. Decrease in Density: If the moon's density decreases, it becomes less compact and more spread out. This allows the moon to withstand stronger gravitational forces without experiencing excessive internal stresses.

2. Increase in Strength: Another way for a moon to get closer to its planet without breaking apart is by increasing its strength or structural integrity. If the moon's materials become stronger, they can better resist the gravitational forces acting on them.

Both of these density changes, either by decreasing density or increasing strength, allow the moon to maintain its structural integrity and withstand the increased gravitational forces as it moves closer to its planet. These mechanisms ensure that the moon does not break apart during the process.

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The current in an RL circuit builds up to one-third of its steady state value in 5.40 s. Find the inductive time constant.

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The inductive time constant in RL circuit is approximately 13.31 seconds.

The inductive time constant can be found using the formula:

τ = t / ln(1 / (1 - 1/3))

where τ is the inductive time constant and t is the time it takes for the current to build up to one-third of its steady state value.

Substituting the given value t = 5.40 s into the equation, we can calculate the inductive time constant as follows:

τ = 5.40 s / ln(1 / (1 - 1/3))

τ ≈ 5.40 s / ln(1 / (2/3))

τ ≈ 5.40 s / ln(3/2)

Using the natural logarithm ln(3/2) ≈ 0.4055, we can evaluate the expression:

τ ≈ 5.40 s / 0.4055

τ ≈ 13.31 s

Therefore, the inductive time constant is approximately 13.31 seconds.

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Consider an ideal monatomic gas, but one for which the freedom. atom has two internal energy states, one an energy delta above the other. There are N atoms in volume V at temperature taw. find the chemical potential free energy pressure heat capacity at constant pressure.

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In the case, the chemical potential free energy pressure is P = NkT/V and heat capacity at constant pressure is  Cp = 3Nk/2

Consider an ideal monatomic gas with two internal energy states, one energy delta above the other. There are N atoms in volume V at temperature taw. To find the chemical potential free energy pressure heat capacity at constant pressure, we will make use of the following relationships:

Relation between internal energy and temperature: E = 3NkT / 2

Relation between entropy and temperature: S = Nk [ln(V/N) + 3 / 2 ln(T) + const.]

Relation between pressure and temperature: PV = NkT

Chemical potential of an ideal gas:

μ = E/N - TS

N = number of atoms in the system

μ = chemical potential of the system

T = temperature of the system

P = pressure of the system

V = volume of the system

E = internal energy of the system

We can find the internal energy of the system:

E = N[1/2(0) + 1/2(δ)] = Nδ/2

Chemical potential of an ideal gas:

μ = E/N - TS

From the relations above, we get:

S = Nk[ln(V/N) + 3/2 ln(T) + const.]

Therefore

μ = δ/2 - T[Nkln(V/N) + 3/2 Nk ln(T) + const.]

Since, PV = NkT we can rewrite the above equation as:

μ = δ/2 - PV[N/V + 3/2]

We can also calculate the free energy of the system:

F = E - TS = Nδ/2 - 3/2 NkTln(V/N) - 3/2 NkT ln(T) - NkT const.

By differentiating the above expression with respect to V, we get the pressure:

P = -∂F/∂V = NkT/V

By differentiating the above expression with respect to T, we get the heat capacity at constant pressure:

Cp = (∂E/∂T)p = 3Nk/2

Therefore,

μ = δ/2 - PV[N/V + 3/2]F = Nδ/2 - 3/2 NkTln(V/N) - 3/2 NkT ln(T) - NkT const.

P = NkT/V at constant temperature

Cp = 3Nk/2 at constant pressure.

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A baseball approaches home plate at a speed of 48.0 m/s, moving horizontally just before being hit by a bat. The batter hits a pop-up such that after hitting the bat, the baseball is moving at 59.0 m/s straight up. The ball has a mass of 145 g and is in contact with the bat for 2.10 ms. What is the average vector force the ball exerts on the bat during their interaction

Answers

The ball interacts with the bat with an average vector force of 759.52 N.

The average vector force the ball exerts on the bat during their interaction is found as follows:

Initial velocity of the ball ,

u = 48.0 m/s

Final velocity of the ball after hitting the bat,

v = 59.0 m/s

Duration of the collision,

t = 2.10 ms = 2.10 × 10⁻³ s

Mass of the ball,

m = 145 g = 0.145 kg

Initial momentum of the ball,

p₁ = mu = 0.145 × 48

   = 6.96 kg m/s

Final momentum of the ball,

p₂ = mv = 0.145 × 59

    = 8.555 kg m/s

Change in momentum of the ball,

Δp = p₂ - p₁

     = 8.555 - 6.96

     = 1.595 kg m/s

Average vector force on the ball during their interaction is given by:

F = Δp / t

F = 1.595 / 2.10 × 10⁻³

F = 759.52 N

The ball interacts with the bat with an average vector force of 759.52 N.

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A 7.80 - g bullet moving at 575 m/s penetrates a tree trunk to a depth of 5.50 cm. (a) Use work and energy considerations to find the average frictional force that stops the bullet. (b) Assuming the frictional force is constant, determine how much time elapses between the moment the bullet enters the tree and the moment it stops moving.

Answers

The average frictional force that stops the bullet is approximately -2.26 × 10⁴ N, and the time elapsed between the moment the bullet enters the tree and the moment it stops moving is approximately 1.99 × 10⁻⁴ s. These calculations were made using work and energy considerations and the kinetic equation of motion, assuming constant frictional force.

(a) Work and Energy considerations to find average frictional force;

First, we should find the Kinetic Energy of the bullet before it strikes the tree.

Kinetic energy of bullet = (1/2)mv²

Where;

m = mass of the bullet, and

v = velocity of the bullet.

Kinetic energy of bullet = (1/2)(7.8 g) × (575 m/s)²= 1244.1 J

Now, work done by the average frictional force acting on the bullet,

W = ΔK

Where,

ΔK = change in kinetic energy = final kinetic energy - initial kinetic energy = 0 - 1244.1 J= - 1244.1 J

The negative sign indicates that work is done against the motion of the bullet by the frictional force.

W = Ff × d

Where,

Ff = average frictional force, an

dd = distance covered by the bullet before stopping.

In this case, the distance covered by the bullet before stopping = 5.50 cm = 0.0550 m

So, Ff = W / d= (- 1244.1 J) / (0.0550 m)= - 22584.5 N ≈ - 2.26 × 10⁴ N

Therefore, the average frictional force that stops the bullet is approximately equal to - 2.26 × 10⁴ N.

(b) Time elapsed between the moment the bullet enters the tree and the moment it stops moving

Assuming that the frictional force acting on the bullet is constant, we can use the Kinetic equation of motion to find the time taken for the bullet to stop moving.

The Kinetic equation of motion:

v = u + at

Where,

v = final velocity of the bullet, which is 0 in this case.

u = initial velocity of the bullet, which is 575 m/s in this case.

a = acceleration of the bullet, which is equal to the deceleration caused by the frictional force, and

t = time taken for the bullet to stop moving.

We already know that Ff = m × a

Where,

m = mass of the bullet = 7.8 g = 0.0078 kgs

Therefore, a = Ff / m= (- 2.26 × 10⁴ N) / (0.0078 kg)= - 2.89 × 10⁶ m/s²

Now, using the Kinetic equation of motion;

v = u + at0 = (575 m/s) + (- 2.89 × 10⁶ m/s²)t

So,t = - (575 m/s) / (- 2.89 × 10⁶ m/s²)= 1.99 × 10⁻⁴ s

Therefore, the time elapsed between the moment the bullet enters the tree and the moment it stops moving is approximately equal to 1.99 × 10⁻⁴ s.

The estimated frictional force that brings the bullet to a stop is around -2.26 × 10⁴ N, and the time it takes for the bullet to stop moving from the moment it enters the tree is approximately 1.99 × 10⁻⁴ s.

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a.  The average frictional force that stops a 7.80 g bullet moving at 575 m/s penetrates a tree trunk to a depth of 5.50 cm.  is 0.11 N

b. The time elapsed between the moment the bullet enters the tree and the moment it stops moving is 40.6 microseconds.

To calculate the average frictional force that stops the bullet, we are given data are:

Mass of bullet, m = 7.80 g = 0.00780 kgSpeed of bullet, v = 575 m/sDepth of penetration, d = 5.50 cm = 0.0550 mDensity of wood, ρ = 550 kg/m³

We are supposed to find the average frictional force that stops the bullet and how much time elapses between the moment the bullet enters the tree and the moment it stops moving. Thus, let's solve the problem:

a. To find the average frictional force that stops the bullet, we can use the work-energy principle.

W = ΔKE + ΔPE

Here,

ΔKE = change in kinetic energy = (1/2) mv² - 0, since the bullet comes to rest.

ΔPE = change in potential energy = mgd = ρVgd where V = volume of bullet

= (4/3)πr³

= (4/3)π(0.007/2)³

= 1.02 × 10⁻⁵ m³and g = 9.8 m/s².

Thus, ρVgd = 0.0060 J = W and, W = Fs, where s = distance travelled before coming to rest. Here, s = d.

Thus, F = W/s = 0.0060/0.055

= 0.11 N

B. To find the time elapsed, we need to use kinematic equations. We know that,

F = ma = m(v/t)

Hence, t = mv/F

= (0.00780 kg)(575 m/s)/0.11 N

= 40.6 × 10⁻⁶ s = 40.6 μs

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A straight 1.0-m long wire is carrying a current. The wire is placed perpendicular to a magnetic field of magnitude 0.20 T. If the wire experiences a force of 0.60 N, what is the current flowing through the wire

Answers

The current flowing through the wire is 3.0 Amperes.

Given information,

F = 0.60 N

L = 1.0 m

B = 0.20 T

θ = 90° (since the wire is perpendicular to the magnetic field)

To determine the current flowing through the wire, the magnetic force experienced by a current-carrying wire in a magnetic field:

F = I × L × B × sin(θ)

Substituting the values into the formula:

0.60 N = I × 1.0 m × 0.20 T × sin(90°)

sin(90°) = 1, so the equation simplifies to:

0.60 N = I × 1.0 m × 0.20 T

I = 0.60 N / (1.0 m × 0.20 T)

I = 0.60 N / 0.20 N/A

I = 3.0 A

Therefore, the current flowing through the wire is 3.0 Amperes.

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Bats use sound echoes to navigate and hunt. They emit pulses of high frequency sound waves which reflect off obstacles in the surroundings. By detecting the time delay between the emission and return of a pulse, a bat can determine the location of the object. What is the time delay between the sending and return of a pulse from an object located 12.5 m away

Answers

The time delay of a pulse from an object located 12.5 m away is 0.0724637 s

Given:

Distance, d = 12.5 m

Let the speed of sound be 345 m/s

From a distance, time, and speed relation

v = d/t

t= d/v

t= 12.5×2/345

t=0.0724637 s.

The time delay between the sending and return of a pulse from an object located 12.5 m away is 0.0724637 s.

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An object accelerates uniformly from rest for t seconds. The average speed for this time interval is

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When an object accelerates uniformly from rest for t seconds, the average speed for this time interval is at.

The average speed for this time interval can be calculated as follows:

The formula for uniform acceleration is,`

v = u + at`

Where:

v is the final velocity,

u is the initial velocity,

a is the acceleration,

t is the time interval

Substituting `u = 0` in the above formula,`v = at`

Thus, the final velocity of an object that accelerates uniformly from rest is directly proportional to the time interval. Therefore, the average speed of an object is the total distance covered divided by the time interval.

t = time interval

Average speed = total distance covered / time interval

We know that the distance covered by an object is given by,

`d = (1/2)at²`

Substituting the value of d in the equation for average speed,

`Average speed = (2t * (1/2)at²) / t`

Average speed = at

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A 0.01kg Styrofoam ball is released from rest 2 m above the floor. It reaches a speed of 3m/s the moment before it hits the floor. How much heat due to air resistance is generated during this process

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The heat generated due to air resistance during the process of the Styrofoam ball falling from a height of 2 m and reaching a speed of 3 m/s just before hitting the floor can be calculated as follows:

To calculate the heat generated due to air resistance, we need to consider the work done by the air resistance force. The work-energy principle states that the work done on an object is equal to the change in its kinetic energy.

The initial kinetic energy of the Styrofoam ball is zero since it is released from rest. The final kinetic energy just before hitting the floor is given by:

KE_final = (1/2) * mass * velocity^2

Substituting the given values:

KE_final = (1/2) * 0.01 kg * (3 m/s)^2

= 0.045 J

Since the initial kinetic energy is zero, the work done by the air resistance force is equal to the change in kinetic energy:

Work = KE_final - KE_initial

= 0.045 J - 0 J

= 0.045 J

The work done by the air resistance force is equal to the heat generated during the process. Therefore, the heat generated due to air resistance is 0.045 J.

The heat generated due to air resistance during the process of the Styrofoam ball falling from a height of 2 m and reaching a speed of 3 m/s just before hitting the floor is 0.045 Joules.

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why the field of a toroid can be confined entirely to its interior, while a straight solenoid must have some field outside

Answers

The field of a toroid can be confined entirely to its interior because the magnetic field lines produced by the current-carrying wire in a toroid loop are circular and continuously loop inside the toroid. On the other hand, a straight solenoid has field lines that extend beyond its ends, resulting in some field outside the solenoid.

To understand why the field of a toroid is confined to its interior, let's consider the magnetic field produced by a single loop of wire. According to Ampere's law, the magnetic field at a distance r from a long, straight wire carrying current I is given by:

B = μ₀ * I / (2πr),

where μ₀ is the permeability of free space. The magnetic field decreases with distance from the wire, following an inverse relationship with r.

Now, let's examine the magnetic field produced by a toroid. A toroid consists of a loop of wire wound tightly in the shape of a donut. The current passing through the wire generates a magnetic field. However, the geometry of the toroid causes the field lines to loop continuously inside the toroid, without extending outside. This is because the field lines of each loop combine constructively inside the toroid, resulting in a magnetic field confined to the interior.

The magnetic field inside a toroid is given by:

B = (μ₀ * N * I) / (2π * r),

where N is the number of turns in the toroid and r is the distance from the center of the toroid. Notice that the magnetic field does not depend on the distance from the toroid's axis, only on the distance from its center.

In contrast, a straight solenoid is a long, cylindrical coil of wire with multiple turns. The magnetic field inside a solenoid is similar to that of a toroid, with field lines looping inside. However, at the ends of the solenoid, the field lines curve outward and extend beyond the coil. This is because the field lines of the outermost loops of the solenoid do not have an adjacent loop to combine with constructively. As a result, some field lines escape outside the solenoid.

In summary, the field of a toroid can be confined entirely to its interior because the geometry of the toroid allows the field lines to loop continuously inside. In contrast, a straight solenoid has some field lines that extend beyond its ends, as the outermost loops do not combine constructively with adjacent loops. This difference in field confinement is due to the distinct geometries of the toroid and the straight solenoid.

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why is the moment of inertia of a hoop taht has a mass m and a radius r greater than the moment of interia

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A hoop with a mass of m and a radius of r has a stronger moment of inertia than a hoop with the same mass distribution because this larger resistance to rotational motion changes results from the hoop's mass distribution being concentrated further away from the axis of rotation.

A measurement of an object's resistance to changes in its rotating motion is the moment of inertia (I).  It depends on the mass distribution and the shape of the object.

For a hoop or a circular ring with mass m and radius r, the moment of inertia is given by the formula:

I_hoop = m * r^2

On the other hand, for a solid disk with the same mass m and radius r, the moment of inertia is given by the formula:

I_disk = (1/2) * m * r^2

Comparing the two formulas, we can see that the moment of inertia of the hoop is greater than the moment of inertia of the disk:

I_hoop = m * r^2

I_disk = (1/2) * m * r^2

Since the hoop has a larger moment of inertia, it means that it has a greater resistance to changes in its rotational motion compared to the solid disk with the same mass and radius.

To understand why this is the case, we need to consider the mass distribution of the objects. The hoop has its mass concentrated at the outer edge, farthest from the axis of rotation, while the solid disk has a more distributed mass throughout its volume.

The mass distribution of the hoop being concentrated at a greater distance from the axis of rotation results in a larger moment of inertia. It requires more torque or rotational force to accelerate or decelerate the hoop compared to the solid disk with the same mass.

The moment of inertia of a hoop with mass m and radius r is greater than the moment of inertia of a solid disk with the same mass and radius. This is because the mass distribution of the hoop is concentrated at a greater distance from the axis of rotation, resulting in a larger resistance to changes in its rotational motion.

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Two charges, 3.3 nC and 1.6 nC are separated by 31 cm. An electron is placed at their midpoint initially at rest. How fast is the electron moving in m/s when it is 10 cm from the 3.3 nC charge

Answers

The electron is moving at approximately 24.9 m/s when it is 10 cm from the 3.3 nC charge.

To determine the speed of the electron when it is 10 cm from the 3.3 nC charge, we can use the principles of electrostatic force and conservation of energy.

Charge of the first charge (q1) = 3.3 nC = 3.3 x 10⁻⁹ C

Charge of the second charge (q2) = 1.6 nC = 1.6 x 10⁻⁹ C

Distance between the charges (r) = 31 cm = 0.31 m

Distance from the 3.3 nC charge to the electron (d) = 10 cm = 0.1 m

The net electrostatic force acting on the electron is the sum of the forces exerted by the two charges:

F_net = (k * |q1 * q_electron| / r²) - (k * |q2 * q_electron| / (r - d)²)

k is the Coulomb's constant (k = 8.99 x 10⁹ N m²/C²)

q_electron is the charge of the electron (q_electron = -1.6 x 10⁻¹⁹ C)

Using the principle of conservation of energy, we can equate the change in potential energy to the change in kinetic energy of the electron:

ΔPE = -ΔKE

The change in potential energy is given by:

ΔPE = -∫(F_net * dr)

Integrating from r = ∞ to r = r_electron (distance from the 3.3 nC charge to the electron), we have:

PE_initial - PE_final = -∫(F_net * dr)

Simplifying and rearranging the equation, we can solve for the velocity (v) of the electron:

v = √(2 * |ΔPE| / m_electron)

m_electron is the mass of the electron (m_electron = 9.11 x 10⁻³¹ kg)

Substituting the values into the equations and performing the calculations, we find that the electron is moving at approximately 24.9 m/s when it is 10 cm from the 3.3 nC charge.

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A child rides a bicycle in a circular path with a radius of 2.00 m. The linear speed of the bike is 3.00 m/s. The combined mass of the bicycle and the child is 43.0 kg. What is the magnitude of the centripetal force on the bike

Answers

The magnitude of the centripetal force on the bike can be calculated using the formula F = m * v² / r, where F is the centripetal force, m is the combined mass of the bicycle and the child, v is the linear speed of the bike, and r is the radius of the circular path.

Combined mass of the bicycle and the child (m) = 43.0 kg

Linear speed of the bike (v) = 3.00 m/s

Radius of the circular path (r) = 2.00 m

Using the formula, we can substitute the given values to find the magnitude of the centripetal force:

F = (43.0 kg) * (3.00 m/s)² / (2.00 m)

Calculating the expression:

F = 43.0 kg * 9.00 m²/s² / 2.00 m

F = 387.0 N

Therefore, the magnitude of the centripetal force on the bike is 387.0 N. This force is directed towards the center of the circular path and is responsible for keeping the bike and the child moving in a curved trajectory.

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Bullet 2 has twice the mass of bullet 1. Both are fired so that they have the same speed. If the kinetic energy of bullet 1 is K, what is the kinetic energy of bullet 2

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Bullet 2 has twice the mass of bullet 1. Both are fired so that they have the same speed. If the kinetic energy of bullet 1 is K. The kinetic energy of bullet 2 is 2K.

In this scenario, both bullets are fired with the same speed, indicating that they possess the same kinetic energy. However, bullet 2 has twice the mass of bullet 1.

The kinetic energy of an object is given by the equation KE = (1/2)mv², where KE represents the kinetic energy, m represents the mass of the object, and v represents its velocity or speed.

Since the speed is the same for both bullets, we can compare their kinetic energies by looking at their masses. If bullet 2 has twice the mass of bullet 1, then the ratio of their kinetic energies can be calculated as follows:

KE2/KE1 = (1/2)m2v² / (1/2)m1v²

= m2 / m1

Since bullet 2 has twice the mass of bullet 1, the ratio of their kinetic energies is:

KE2/KE1 = 2/1

= 2

This means that the kinetic energy of bullet 2 (KE2) is twice that of bullet 1 (KE1). Therefore, the correct answer is that the kinetic energy of bullet 2 is 2K.

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An airplane is traveling with an airspeed of 500 mph in the direction N 60° E. A wind blows directly south at 50 mph. What is the plane’s drift angle? 3. 84° 5. 21° 60. 00° 65. 21°.

Answers

To find the plane's drift angle, we can use trigonometry and vector addition.

First, let's break down the velocities into their northward (N) and eastward (E) components:

Airspeed:

Velocity in the N direction (Vn) = 500 mph * cos(60°) = 250 mph

Velocity in the E direction (Ve) = 500 mph * sin(60°) = 433.01 mph

Wind:

Velocity in the S direction (Vs) = -50 mph (southward)

Velocity in the E direction (Ve) = 0 mph (no eastward component)

Next, we'll add the velocities to find the resultant velocity (Vr) of the plane:

VrN = Vn + Vs = 250 mph - 50 mph = 200 mph (southward)

VrE = Ve + Ve = 433.01 mph + 0 mph = 433.01 mph (eastward)

Now, we can find the drift angle (θ) using the arctan function:

θ = arctan(VrE / VrN) = arctan(433.01 mph / 200 mph) ≈ 65.21°

Therefore, the plane's drift angle is approximately 65.21°.

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A horizontal uniform board of weight 125 N and length 4m is supported by vertical chains at each end. A person weighing 500 N is sitting on the board. The tension in the right chain is 250N.

(A) What is the tension in the left chain?

(B) How far from the left end of the board is the person sitting?

Answers

(A) The tension in the left chain is 375 N.

(B) The person is sitting 2 meters from the left end of the board.

To determine the tension in the left chain, we can consider the equilibrium of forces acting on the board. The total weight of the board is 125 N, and the person weighs 500 N, resulting in a total downward force of 625 N. Since the board is in equilibrium, the sum of the upward forces must also be 625 N.

Let's denote the tension in the left chain as Tl and the tension in the right chain as Tr. The sum of the upward forces is equal to Tl + Tr. We know that Tr is 250 N, so substituting the values, we get:

Tl + 250 N = 625 N

Solving for Tl, we find that the tension in the left chain is 375 N.

To determine the distance from the left end of the board where the person is sitting, we can consider the torques acting on the board. The torques exerted by the person and the board's weight must balance each other for rotational equilibrium.

Let's denote the distance from the left end of the board to the person as d. The torque exerted by the person is given by 500 N × d, and the torque exerted by the board's weight is 125 N × 4 m (since the weight acts at the center of the board). To achieve rotational equilibrium, these torques must be equal:

500 N × d = 125 N × 4 m

Solving for d, we find that the person is sitting 2 meters from the left end of the board.

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A steel ball of mass 0.500 kg is fastened to a cord that is 70.0 cm long and fixed at the far end. The ball is released when the cord is horizontal as shown below. At the bottom of its path, the ball strikes a 2.50 kg steel block at rest on a frictionless surface. The collision is elastic. Find

(a) the speed of the ball and

(b) the speed of the block just after the collision.

Answers

(a) The speed of the steel ball at the bottom of its path is approximately 3.70 m/s.

(b) The speed of the steel block just after the collision with the ball is approximately 0.74 m/s.

To find the speed of the ball and the speed of the block after the elastic collision, we can apply the principles of conservation of momentum and conservation of kinetic energy.

(a) Speed of the ball:

Before the collision, the ball is released from rest, so its initial velocity is 0 m/s.

Using the principle of conservation of energy, we can equate the potential energy of the ball at the top of its path to the kinetic energy of the ball at the bottom of its path, where m is the mass of the ball, g is the acceleration due to gravity, h is the height of the path (70.0 cm), and v is the speed of the ball at the path's bottom.

Simplifying the equation:

v^2 = 2 * g * h

v^2 = 2 * 9.8 m/s^2 * 0.70 m

v^2 = 13.72 m^2/s^2

Taking the square root of both sides:

v ≈ 3.70 m/s

Therefore, the speed of the ball at the bottom of its path is approximately 3.70 m/s.

(b) Speed of the block:

Since the collision between the ball and the block is elastic, both momentum and kinetic energy are conserved.

Let's denote the speed of the block after the collision as Vb.

Using the principle of conservation of momentum:

m_ball * v_ball = m_block * Vb

where m_ball is the mass of the ball (0.500 kg), m_block is the mass of the block (2.50 kg), v_ball is the speed of the ball before the collision (3.70 m/s), and Vb is the speed of the block after the collision.

Substituting the given values:

(0.500 kg) * (3.70 m/s) = (2.50 kg) * Vb

1.85 kg m/s = 2.50 kg * Vb

Vb = 1.85 kg m/s / 2.50 kg

Vb ≈ 0.74 m/s

Therefore, the speed of the block just after the collision is approximately 0.74 m/s.

(a) The speed of the steel ball at the bottom of its path is approximately 3.70 m/s.

(b) The speed of the steel block just after the collision with the ball is approximately 0.74 m/s.

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What is the speed of the ball relative to a stationary observer on the side of the road

Answers

Then the speed of the ball relative to the stationary observer on the side of the road will remain constant at 20 m/s to the left.

To find out what the speed of the ball is relative to a stationary observer on the side of the road, we need more information. Specifically, we need to know the initial velocity of the ball, as well as its acceleration.

Let's assume that the ball is thrown horizontally from a moving car. If the car has a velocity of 20 m/s to the right and the ball is thrown with a velocity of 10 m/s to the left (in the opposite direction), then the initial velocity of the ball relative to the stationary observer on the side of the road is 20 m/s to the left (since the ball is thrown in the opposite direction of the car's velocity).

If we also assume that the ball experiences no acceleration, then the speed of the ball relative to the stationary observer on the side of the road will remain constant at 20 m/s to the left.

This is because the ball is not experiencing any changes in speed or direction.

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If the speakers are in phase, what is the smallest distance between the speakers for which the interference of the sound waves to the right of the speakers is maximum destructive

Answers

The path difference between the waves must be λ/2 if the speakers are in phase. The minimum distance between the speakers for which the interference of the sound waves to the right of the speakers is maximally destructive is half a wavelength.

Therefore, the distance between the speakers is half of the wavelength of the sound waves when the sound waves from the two speakers are in phase. This is known as destructive interference.

When two waves superimpose, they produce interference. When two waves interfere with each other and cancel each other out, this is known as destructive interference.

A loudspeaker or stereo speaker system can produce destructive interference if the speakers are arranged properly. When the two waves are out of phase by one-half of a wavelength, this occurs.

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Low-mass stars have much longer lifetimes than high-mass stars. Which stellar property is a direct cause of this difference

Answers

Low-mass stars have much longer lifetimes than high-mass stars. This is a result of the difference in their stellar property which is the rate of fusion in their core. The rate of fusion in the core of a low-mass star is much slower compared to that of a high-mass star.

A low-mass star is a star whose mass is less than 8 times the mass of the sun. For low-mass stars, they spend most of their lifetime as a main sequence star slowly burning hydrogen in their core. In their core, hydrogen atoms are fused into helium atoms, releasing energy in the process. This process is called nuclear fusion.

The amount of energy produced from nuclear fusion depends on the mass of the star.

A high-mass star is a star whose mass is more than 8 times the mass of the sun. For high-mass stars, they consume the hydrogen in their core at a much faster rate than low-mass stars. This causes them to evolve much faster, and they have a shorter lifespan as compared to low-mass stars.

The core temperature of a high-mass star is much higher than a low-mass star due to its high mass. This leads to the production of heavier elements in its core.The final stage of a low-mass star is the red giant phase. After this phase, they collapse into a white dwarf and eventually cool down. On the other hand, high-mass stars end their life in a supernova explosion followed by the creation of a neutron star or a black hole.

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Whether or not two sounds that are of similar amplitude and close together in frequency can be discriminated depends on what physical mechanism

Answers

Whether or not two sounds that are of similar amplitude and close together in frequency can be discriminated depends on the mechanism of auditory perception or the human auditory system.

The discrimination of two sounds that are similar in amplitude and frequency is determined by the capabilities of the human auditory system. The human ear is responsible for perceiving and distinguishing different sounds based on their physical properties.

The process of discriminating sounds with similar amplitudes and close frequencies involves several mechanisms within the auditory system. These mechanisms include the cochlea, which is the main sensory organ of the inner ear, and the auditory nerve, which transmits electrical signals from the cochlea to the brain.

The cochlea contains specialized hair cells that respond to different frequencies of sound vibrations. When two sounds with similar frequencies reach the cochlea, the hair cells in the cochlea may respond to both sounds, but their relative activation patterns can help differentiate the sounds.

Additionally, the brain plays a crucial role in processing and interpreting auditory information. It analyzes the patterns of neural signals received from the auditory nerve and makes distinctions between different sounds based on their frequencies, temporal patterns, and other acoustic properties.

The discrimination of sounds with similar amplitudes and frequencies can vary among individuals and is influenced by factors such as hearing sensitivity, attention, and experience with specific sounds.

The discrimination of sounds that are similar in amplitude and close in frequency depends on the mechanisms of auditory perception or the human auditory system. The capabilities of the cochlea, auditory nerve, and brain in processing and interpreting auditory information play a crucial role in distinguishing between such sounds.

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A disk, a hoop, and a solid sphere are released at the same time at the top of an inclined plane. They all roll without slipping. In what order do they reach the bottom

Answers

The order from first to last is: solid sphere, hoop, and disk. The order in which the objects reach the bottom of the inclined plane depends on their moments of inertia and how mass is distributed around their axes of rotation.

The solid sphere will reach the bottom first. Due to its mass distribution, it has the lowest moment of inertia and therefore rolls down the inclined plane more easily.

Next, the hoop will reach the bottom. Although it has a larger moment of inertia than the solid sphere, its mass distribution allows it to roll more easily than the disk.

Lastly, the disk will reach the bottom last. It has the largest moment of inertia among the three objects due to its mass being distributed farther from its axis of rotation.

Therefore, the order from first to last is: solid sphere, hoop, and disk.

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A 190-lb man carries a 15-lb can of paint up a helical staircase that encircles a silo with radius 20 ft. The silo is 120 ft high and the man makes exactly four complete revolutions. Suppose there is a hole in the can of paint and 8 lb of paint leaks steadily out of the can during the man's ascent. How much work is done by the man against gravity in climbing to the top

Answers

The man does approximately 732,290 ft-lb of work against gravity while climbing to the top of the helical staircase.

The work done against gravity is equal to the change in potential energy. The potential energy is given by the product of the weight (mass * acceleration due to gravity) and the height. The man's weight is 190 lb, and the height climbed is 120 ft.

However, the man carries a can of paint that loses 8 lb of weight during the ascent. So, the net weight carried is (190 lb - 15 lb - 8 lb) = 167 lb. The work done against gravity is (167 lb * 120 ft) = 20,040 ft-lb per revolution. Since the man makes four complete revolutions, the total work done is approximately 732,290 ft-lb.

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A body of mass 15.0 kg is traveling at 2.4 m/s along the positive x-axis with no external force acting. At a certain instant an internal explosion occurs, splitting the body into two chunks of 7.5 kg mass each. The explosion gives the chunks an additional 16 J of kinetic energy. Neither chunk leaves the line of original motion.


Required:

Determine the speed and direction of motion of each of the chunks after the explosion.

Answers

After the internal explosion, the two chunks of mass 7.5 kg each will move in opposite directions along the positive x-axis. One chunk will have a speed of 6.4 m/s, while the other chunk will have a speed of 0.4 m/s.

1. Initially, a body of mass 15.0 kg is traveling at 2.4 m/s along the positive x-axis. The total initial momentum of the system is given by the product of mass and velocity, which is (15.0 kg)(2.4 m/s) = 36 kg·m/s.

2. An internal explosion occurs, splitting the body into two chunks of equal mass, 7.5 kg each. Due to the conservation of momentum, the total final momentum of the system remains the same as the initial momentum.

3. Let the velocity of one chunk after the explosion be v₁ m/s and the velocity of the other chunk be v₂ m/s.

4. The final momentum of the system is given by (7.5 kg)(v₁ m/s) + (7.5 kg)(v₂ m/s).

5. Since the total final momentum must be equal to the initial momentum, we have (7.5 kg)(v₁ m/s) + (7.5 kg)(v₂ m/s) = 36 kg·m/s.

6. The explosion gives the chunks an additional 16 J of kinetic energy. Each chunk receives an equal amount of kinetic energy, so we have (1/2)(7.5 kg)(v₁²) + (1/2)(7.5 kg)(v₂²) = 16 J.

7. Solving the system of equations from steps 5 and 6, we find v₁ = 6.4 m/s and v₂ = 0.4 m/s.

Therefore, after the explosion, one chunk will move with a speed of 6.4 m/s in the positive x-direction, while the other chunk will move with a speed of 0.4 m/s in the positive x-direction.

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Stars emit radiation whose spectrum is very similar to that of a blackbody. Imagine two stars identical in size, each of which is at the same distance from us. One of the stars appears reddish in color, while the other one looks distinctly bluish. Based on this information, what can you say about the relative temperatures of the two stars

Answers

Based on the information provided, the star that looks distinctly bluish is hotter, while the star that appears reddish is cooler in comparison.

The color of a star is directly related to its temperature. The color of a star is determined by the peak wavelength of light it emits, which is governed by its temperature according to Wien's displacement law. Hotter objects emit shorter wavelength (bluish) light, while cooler objects emit longer wavelength (reddish) light.

In this case, the star that appears bluish in color indicates that it has a higher temperature compared to the star that appears reddish.

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Within a ferromagnetic material, there are small regions called magnetic domains. What is responsible for the creation of these magnetic domains

Answers

Magnetic domains in ferromagnetic materials are created due to the alignment of atomic magnetic moments within small regions.

Magnetic domains are created in ferromagnetic materials as a result of the alignment of atomic magnetic moments within small regions. In an unmagnetized state, the atomic magnetic moments point in random directions, resulting in a cancellation of their magnetic fields. When an external magnetic field is applied, the magnetic moments begin to align in the direction of the field. However, due to various factors such as crystal structure and thermal effects, complete alignment doesn't occur uniformly throughout the material. Instead, the material forms regions where the magnetic moments align parallel to each other, known as magnetic domains. The boundaries between these domains are called domain walls, and the overall magnetic behaviour of the material is determined by the interaction between these domains and the applied field.

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Calculate the force exerted on a rocket when the propelling gases are being expelled at a rate 1100 kg/s with a speed of 3.5 x 104 m/s.

Answers

The force is the rate of change of momentum, we can conclude that the force exerted on the rocket is 3.85 x 10^7 N.

To calculate the force exerted on the rocket, we can use Newton's second law of motion, which states that force (F) is equal to the rate of change of momentum (dp/dt). In this case, the momentum change is caused by the expulsion of the propelling gases.

The momentum change (dp) is given by the equation: dp = m * Δv, where m is the mass of the propelling gases expelled per second and Δv is the change in velocity of the gases.

The force exerted on the rocket is then obtained by dividing the momentum change by the time interval during which the gases are expelled: F = dp/dt.

Substituting the given values of m = 1100 kg/s and Δv = 3.5 x 10^4 m/s:

dp = (1100 kg/s) * (3.5 x 10^4 m/s),

dp = 3.85 x 10^7 kg·m/s.

Since the force is the rate of change of momentum, we can conclude that the force exerted on the rocket is 3.85 x 10^7 N.

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X-rays strike a stationary target and undergo Compton scattering. If the energies of the incident and scattered X-ray are 414 keV and 334 keV respectively, determine the scattering angle (in degrees).

Answers

X-rays strike a stationary target and undergo Compton scattering, so the scattering angle is 43.56°

The energy of the incident X-ray, E = 414 keV

The energy of the scattered X-ray, E' = 334 keV

To determine: The scattering angle (θ)

Compton scattering is defined as the process in which an X-ray photon scatters off an electron and loses some of its energy. The scattered photon is said to undergo Compton scattering. The amount of energy lost by the photon is equal to the energy transferred to the electron during the collision.

The formula to determine the scattering angle (θ) is given by:

hc / (E (1 - cos θ)) - hc / (E') = mecc²

Where h = Planck’s constant, c = the speed of light, me = mass of an electron, and c² = the square of the speed of light

Substituting the values, we get:

6.626 x 10⁻³⁴ x 3 x 10⁸ / (414 x 10³ x (1 - cos θ)) - 6.626 x 10⁻³⁴ x 3 x 10⁸ / (334 x 10³) = 9.11 x 10⁻³¹

Solving for cos θ, we get:

cos θ = 0.7212

Scattering angle (θ) = cos⁻¹(0.7212)≈ 43.56°

Therefore, the scattering angle is approximately 43.56°.

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