A hollow copper wire with an inner diameter of 1.1 mm and an outer diameter of 1.8 mm carries a current of 15 A. What is the current density in the wire? Please show work. I got 3.9 *10^7 A/m^2, but I was wrong. Thanks in advance.

(a) The lowest temperature at the throat of the nozzle is 589.82 K.

(b) The lowest pressure at the throat of the nozzle is 516.65 kPa.


1. Identify given values: y = 1.4, P1 = 800 kPa, T1 = 700 K.
2. Apply isentropic relations for converging-diverging nozzle at the throat.
3. Calculate T2/T1 = (2/(y + 1)) = (2/(1.4 + 1)) = 0.2857.
4. Calculate the lowest temperature: T2 = T1 * T2/T1 = 700 K * 0.2857 = 589.82 K.
5. Calculate P2/P1 = (T2/T1)^(y/(y - 1)) = (0.2857)^(1.4/0.4) = 0.6458.
6. Calculate the lowest pressure: P2 = P1 * P2/P1 = 800 kPa * 0.6458 = 516.65 kPa.

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The average value of sin(2ωt) for a complete cycle is 0.

To find the average value of sin(2ωt) over a complete cycle, we need to integrate the function over a period and divide by the period length. The function is sin(2ωt), and its period is T = π/ω (since the period of sin(x) is 2π, and sin(2ωt) has twice the frequency).

Integrate sin(2ωt) over one period
∫(sin(2ωt)) dt from 0 to T (T = π/ω)

Evaluate the integral
[-(1/2ω)cos(2ωt)] from 0 to T

Substitute the limits and subtract
[-(1/2ω)cos(2ω(π/ω))] - [-(1/2ω)cos(2ω(0))]

[-(1/2ω)cos(2π)] - [-(1/2ω)cos(0)]

[-(1/2ω)(1)] - [-(1/2ω)(1)]

(1/2ω) - (1/2ω) = 0

Divide by the period length (T)
Average value = (0) / (π/ω) = 0

So, 0 is the average value of sin(2ωt) for a complete cycle.

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Maximum shear stress, τ_max, can be calculated using the formula [tex]τ_max = VQ/It,[/tex]  where V is the shear force, Q is the first moment of area of the cross-section, I is the moment of inertia, and t is the thickness of the beam.

Given [tex]v=36 kN[/tex]  and[tex]w=300 mm[/tex] , we need additional information such as the dimensions and material properties of the beam to calculate Q and I. Therefore, the maximum shear stress cannot be determined with the given information. In order to determine the maximum shear stress, we need additional information about the dimensions and material properties of the beam. However, we can use the formula [tex]τ_max = VQ/It,[/tex] where V is the shear force, Q is the first moment of area of the cross-section, I is the moment of inertia, and t is the thickness of the beam. With the given shear force of [tex]v=36 kN[/tex] and width of [tex]w=300 mm[/tex] , we can calculate τ_max once we have information about the beam's dimensions and material properties. It's important to note that the maximum shear stress occurs at the location where the shear force is maximum.

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During a vibration with frequency of 50 hz, the complex amplitude is 0.5j at time t=0.

The displacement at time t=0 can be determined by the equation:

x(t)=Acos(ωt+φ).

Substituting the values:

As displacement at t=0 is given,

x(0)=Acos(2π(50)t+φ)=Acos(φ)

As cos(φ) can take values from -1 to 1, the value of A can be determined from the given displacement at

t=0 (x(0)), A=x(0)/cos(φ).

Thus, the complex amplitude is A.j, where A is determined from the given displacement. For this problem, A=0.5, therefore, the complex amplitude is 0.5j at t=0.

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The main difference between using an ammeter and a voltmeter in a circuit is that the ammeter measures the current directly, while the voltmeter measures the potential difference across the circuit.

While attaching either meter will cause some alteration to the circuit, the effect on the ammeter reading is minimal because it measures the current directly.

When you attach a voltmeter to a circuit, you are essentially adding an additional load to the circuit. This means that the current flowing through the circuit will decrease slightly, causing a slight change in the overall circuit resistance. However, since an ammeter measures the current flowing through a circuit directly, this change in resistance will not significantly affect the ammeter reading.

On the other hand, a voltmeter measures the potential difference, or voltage, across a circuit. This means that it needs to be connected in parallel with the circuit, which creates an additional path for the current to flow through. Since the voltmeter has a very high resistance, it draws very little current from the circuit, and the change in resistance caused by adding the voltmeter is relatively small. However, the presence of the voltmeter will still cause a slight decrease in current, which is why it is important to connect the voltmeter in parallel to the circuit rather than in series.
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An Earth satellite travels in an elliptical orbit with a semimajor axis of a, a period T, and an eccentricity of the maximum radial velocity of the satellite is 2πaɛ/(T√(1 - ɛ^2)).

At the point of greatest distance from the Earth (apogee), the distance between the Earth and the satellite is (1+ɛ)a.

Using conservation of energy, we can write:

E = [tex]1/2 mv^2 - GmM/(r)[/tex]

where v is the velocity of the satellite, and r is the distance between the Earth and the satellite.

At perigee, the velocity of the satellite is maximum and the distance is (1-ɛ)a. At apogee, the velocity of the satellite is minimum and the distance is (1+ɛ)a.

Setting the energy at perigee and apogee equal to each other, we get:

1/2 mv_perigee^2 - GmM/((1-ɛ)a)) = [tex]1/2 mv_{apogee}^2 - GmM/((1+\epsilon)a))[/tex]

Simplifying this equation, we get:

[tex]v_{perigee}^2 - v_{apogee}^2[/tex] = 2GM(ɛ/a)

At perigee, the velocity of the satellite is equal to the sum of the radial and tangential components of the velocity. The tangential component is given by:

v_tangential = 2πa/T

The radial velocity at perigee can be found by subtracting the tangential velocity from the total velocity:

v_radial = [tex]\sqrt{(v_{perigee}^2 - v_{tangential}^2)[/tex]

Substituting v_perigee^2 - v_apogee^2 = 2GM(ɛ/a), we get:

v_radial = [tex]\sqrt{(2GM(\epsilon/a) - (2\pi a/\tau)^2)[/tex]

Simplifying this expression, we get:

v_radial = [tex]2\pi a\epsilon/(\tau\sqrt{(1 - \epsilon^2))[/tex]

Radial velocity refers to the speed at which an object moves towards or away from an observer along the line of sight. This can be determined by measuring the Doppler shift of spectral lines in the light emitted by the object. When an object is moving towards an observer, the wavelength of the emitted light is shortened, resulting in a shift towards the blue end of the spectrum. Conversely, when an object is moving away from an observer, the wavelength is lengthened, causing a shift towards the red end of the spectrum. By measuring this shift, astronomers can determine the radial velocity of the object.

Radial velocity measurements have a wide range of applications in astronomy, including the detection of exoplanets through the radial velocity method, the determination of the rotation rate of stars, the measurement of the mass and motion of galaxies, and the study of the expansion of the universe.

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The maximum kinetic energy that a photoelectron ejected in this process can have is 0.806 eV.

The maximum kinetic energy that a photoelectron can have is given by the difference between the energy of the incident photon and the work function of the metal.

The energy of a photon is given by Planck's equation:

E = hf

where E is the energy of the photon, h is Planck's constant, and f is the frequency of the light.

In this case, the frequency of the light is given as 8.70 × 10^14 Hz. So, the energy of the photon is:

E = hf = (6.626 × 10-³⁴ J s) × (8.70 × 10¹⁴ Hz) = 5.77 × 10-¹⁹ J

The work function of the metal is given as 2.8 eV. We need to convert this to joules to be able to subtract it from the energy of the photon:

1 eV = 1.602 × 10-¹⁹ J

So, the work function in joules is:

2.8 eV × (1.602 × 10-¹⁹ J/eV) = 4.48 × 10-¹⁹ J

The maximum kinetic energy of the photoelectron is:

KEmax = E - work function = 5.77 × 10-¹⁹ J - 4.48 × 10-¹⁹ J = 1.29 × 10-¹⁹ J

We can convert this to electronvolts (eV) by dividing by the charge of an electron:

1.29 × 10-¹⁹ J / 1.602 × 10-¹⁹ C = 0.806 eV

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For7-Ω and 20-Ω resistors in a parallel circuit connected across a 240-v dc line.

a) The resistance is approximately 11.49 Ω.

b) The total current through the parallel combination is approximately 20.88 A.

c) The current through the 27 Ω resistor is approximately 20.88 A.

d) The current through the 20 Ω resistor is also approximately 20.88 A.

a) To find the equivalent resistance of the parallel circuit resistors, we use the formula:

1/R_parallel = 1/R1 + 1/R2

where R1 = 27 Ω and R2 = 20 Ω.

Substituting the values:

1/R_parallel = 1/27 + 1/20

1/R_parallel = (20 + 27)/(20*27)

1/R_parallel = 47/540

R_parallel = 540/47 ≈ 11.49 Ω

Therefore, the resistance of the parallel combination is approximately 11.49 Ω.

b) The total current through the parallel combination is equal to the current through each resistor. To find the current, we use Ohm's Law:

I = V/R

where V = 240 V and R is the resistance of the parallel combination.

Substituting the value of R_parallel we calculated in part (a):

I = 240/11.49

I ≈ 20.88 A

Therefore, the total current through the parallel combination is approximately 20.88 A.

c) The current through the 27 Ω resistor is also equal to the current through the parallel combination, since they are in parallel. Therefore, the current through the 27 Ω resistor is approximately 20.88 A.

d) Similarly, the current through the 20 Ω resistor is also equal to the current through the parallel combination, since they are in parallel. Therefore, the current through the 20 Ω resistor is also approximately 20.88 A.

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(a) To find the matrix inverse, we start by writing the system of equations in matrix form as Ax = b:

To do this, we can perform the following row operations:

R2 = R2 + (3/15)R1

R3 = R3 + (4/15)R1

R1 = (1/15)R1

R3 = R3 + (1/18)R2

R2 = (1/18)R2

R1 = R1 + (1/12)R3

R2 = R2 - (1/4)R3

After performing these row operations, we get:

|  1   0   0  |  311.11 |

|  0   1   0  |  50     |

|  0   0   1  |  235.42 |

Therefore, the matrix inverse is:

|  311.11   50      235.42 |

|  52.78   33.33   29.17  |

|  45.83    8.33   42.36  |

(b) To determine the solution, we multiply the matrix inverse by the right-hand side of the augmented matrix:

| c1 |   |  311.11   50      235.42 |   | 4000 |

| c2 | = |  52.78   33.33   29.17  | * | 1200 |

| c3 |   |  45.83    8.33   42.36  |   | 2350 |

Multiplying the matrices and solving for c1, c2, and c3, we get:

c1 = 200

c2 = 100

c3 = 150

Therefore, the concentrations in the reactors are:

c1 = 200 g/m3

c2 = 100 g/m3

c3 = 150 g/m3

(c) To determine how much the rate of mass input to reactor 3 must be increased to induce a 10 g/m3 rise in the concentration of reactor 1, we can use the formula:

where Δc1 is the change in concentration of reactor 1, Δd3 is the change in mass

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Answer: False

The numbers after "W" indicate the beam's nominal depth and weight per foot. In this case, W18x55 has a weight of 55 pounds per foot, while W14x68 has a weight of 68 pounds per foot. Therefore, the W14x68 beam is heavier than the W18x55 beam. A W14x68 beam weighs 68 pounds per linear foot, while a W18x55 beam weighs 55 pounds per linear foot. Therefore, the W18x55 beam is lighter than the W14x68 beam. A W18x55 beam is indeed heavier than a W14x68 beam. Sometimes called a W-beam, a wide flange beam is a type of steel beam shaped like a sideways H. The web can be of equal width or wider than the flange. The size of a W-beam is identified by the first number in the product description followed by the weight per foot. For example, a W21x44 beam measures about 21 inches in width and 44 pounds per foot. The web bears shear forces while the flange resists bending forces.

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The resistance of the silver wire at 34 degrees Fahrenheit is approximately 5.23 ohms.

To solve this problem, we need to use the temperature coefficient of resistance (TCR) for silver, which is 0.0038 per degree Celsius.

First, we need to convert the temperature from degrees Celsius to degrees Fahrenheit, since the TCR is typically given in Fahrenheit units. To do this, we can use the formula:

°F = (°C x 1.8) + 32

So for 20 degrees Celsius, we have:

°F = (20 x 1.8) + 32 = 68°F

Now we can use the TCR to calculate the new resistance at 34 degrees Fahrenheit. We can use the formula:

R2 = R1 * [1 + TCR * (T2 - T1)]

Where:
R1 = initial resistance (6.00 ohms)
T1 = initial temperature (68°F)
TCR = temperature coefficient of resistance (0.0038 per degree Fahrenheit)
T2 = final temperature (34°F)
R2 = final resistance (what we're trying to find)

Plugging in the values, we get:

R2 = 6.00 * [1 + 0.0038 * (34 - 68)]
R2 = 6.00 * [1 - 0.1292]
R2 = 6.00 * 0.8708
R2 = 5.23 ohms (rounded to two decimal places)

Therefore, the resistance of the silver wire at 34 degrees Fahrenheit is approximately 5.23 ohms.

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Answer:

Landon threw his rifle higher than Natalie threw her baton.

Explanation:

The gravitational potential energy (GPE) of an object is given by:

GPE = mgh

where m is the mass of the object, g is the acceleration due to gravity, and h is the height of the object.

Assuming that the baton and rifle have the same mass, we can set their GPEs equal to each other:

mgh = mgh

260 J = mgh

Now we can solve for h:

h = 260 J / (mg)

The mass cancels out, so we can use the same height formula for both objects.

For Natalie's baton:

F = ma

a = F/m

Using the given values, we get:

a = 15.4 N / m (since the mass is not given)

Now we can use the height formula:

h = 260 J / (mg)

h = 260 J / (m * 9.81 m/s²) (acceleration due to gravity)

h = 26.53 / m

h = (1/2)at²

h = (1/2)(15.4 N / m)(t²)

Setting the two expressions for height equal to each other, we get:

26.53 / m = (1/2)(15.4 N / m)(t²)

Solving for t, we get:

t = sqrt((2 * 26.53) / (15.4 N / m))

t = 1.41 s

Now we can use the time and acceleration to find the height:

h = (1/2)at²

h = (1/2)(15.4 N / m)(1.41 s)²

h = 15.33 m

For Landon's rifle, we can use the same height formula:

h = 260 J / (mg)

h = 260 J / (m * 9.81 m/s²)

h = 26.53 / m

h = (1/2)at²

h = (1/2)(15.1 N / m)(4.2 s²)

h = 35.77 m

Therefore, Landon threw his rifle higher than Natalie threw her baton.

Hope this helps!

To find the total magnetic field, you would need to integrate dB over the entire length of the unshielded section of the wire.

Here's the step-by-step explanation:
1. The Biot-Savart law relates the differential magnetic field dB to the current I, the distance from the wire to the point P (r), and the angle between the current and the position vector (θ). The equation is:
dB = (μ₀ * I * dl * sinθ) / (4π * r²)

2. Calculate the distance r: Point P is x/2 above the wire, and the distance l from the midpoint of the unshielded section. Using the Pythagorean theorem, r = √((x/2)² + l²).

3. Calculate the angle θ: Since the angle is between the current and the position vector, we can use the right triangle formed by the distances x/2 and l. Using the inverse tangent function, θ = arctan((x/2) / l).

4. Plug the values of I, dl, r, and θ into the Biot-Savart law equation and calculate the differential magnetic field dB at point P due to the small length of wire dl.

Remember that this calculation is for the differential magnetic field dB at point P due to a small length of wire dl.

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The object moving in a uniform circular motion with a radius of 0.6 m and a period of 0.4 s has a tangential velocity of 3.77 m/s.

Uniform circular motion is characterized by a constant speed and a changing direction, which means that the object is constantly accelerating toward the center of the circle. The magnitude of the centripetal acceleration is given by:

a = v^2/r

where v is the tangential velocity of the object and r is the radius of the circle.

Since the motion is uniform, the period T of the motion is related to the tangential velocity by:

[tex]v = 2πr/Ta = (2πr/T)^2 / r = 4π^2r/T^2[/tex]

The magnitude of the centripetal acceleration is also related to the net force acting on the object by:

a = F_net/m

where F_net is the net force and m is the mass of the object.

Since the object is moving in a uniform circular motion, the net force is given by the centripetal force:

F_net = F_c = mv^2/r

where F_c is the centripetal force.

Substituting this into the expression for the centripetal acceleration and equating it to the expression for the net force, we get:

[tex]mv^2/r = 4π^2r/T^2v = sqrt(4π^2r^2/T^2) = 2πr/T = 3.77 m/s (approx)[/tex]

Therefore, the tangential velocity of the object is 3.77 m/s (approx).

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Jupiter has the strongest magnetic field in our solar system, about 1.4 mT at its poles and consult Appendix E, its magnetic dipole moment is approximately 1.4 x 10^4 Am².

To find Jupiter's magnetic dipole moment, we will use the formula for the magnetic field at the poles of a dipole:
B = μ₀ * (m * R³) / (4π * R³)
where:
- B is the magnetic field strength at the poles
- μ₀ is the permeability of free space (4π x 10^(-7) Tm/A)
- m is the magnetic dipole moment
- R is the distance from the dipole (in this case, the radius of Jupiter)

We are given B = 1.4 mT (1.4 x 10^(-3) T) and the radius of Jupiter (R) = 69,911 km (6.9911 x 10^7 m). We want to find m, the magnetic dipole moment.

First, let's rearrange the formula to solve for m:
m = (B * 4π * R³) / (μ₀ * R³)

Now, plug in the values for B, R, and μ₀:
m = (1.4 x 10^(-3) T * 4π * (6.9911 x 10^7 m)³) / (4π * 10^(-7) Tm/A * (6.9911 x 10^7 m)³)

Notice that (6.9911 x 10^7 m)³ cancels out in the numerator and the denominator, as well as the 4π:
m = (1.4 x 10^(-3) T) / (10^(-7) Tm/A)

Now, simply divide the numbers:
m = 1.4 x 10^(4) Am².

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For a real cell in a circuit, the terminal potential difference is at its closest to the emf when (a) the internal resistance is much smaller than the load resistance.

When a current flows through a cell, the internal resistance of the cell causes a drop in voltage, which reduces the terminal potential difference. The larger the load resistance, the greater the voltage drop across the internal resistance, resulting in a lower terminal potential difference. However, if the internal resistance is much smaller than the load resistance, the voltage drop across the internal resistance becomes negligible, and the terminal potential difference is closest to the emf. Therefore, option A is the correct answer.

Furthermore, options B, C, and D are incorrect because they do not affect the terminal potential difference. A large current flowing in the circuit does not necessarily mean that the terminal potential difference is closest to the emf. The cell being not completely discharged or being recharged does not affect the internal resistance, which is the determining factor in the terminal potential difference.

In conclusion, the terminal potential difference of a real cell in a circuit is closest to the emf when the internal resistance is much smaller than the load resistance.

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To fully describe the ejection of electrons from a metal's surface, scientists need to consider both light and matter as the energy of photons and energy levels of electrons in the metal are quantized.

What factors need to be considered to fully describe the ejection of electrons from a metal's surface?

C. Both light and matter.

To fully describe the ejection of electrons from a metal's surface, scientists need to consider the photoelectric effect, which involves the interaction of both matter (electrons) and light (photons). The energy of the photon must be equal to or greater than the work function of the metal in order for electrons to be emitted.

The energy of the photon is quantized, meaning it can only take on certain discrete values, and this energy is transferred to the electron, which can also only have certain quantized energy levels in the metal. Therefore, both the energy of the photons and the energy levels of the electrons in the metal are quantized and must be considered to fully describe the photoelectric effect.

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True. If the position pf an object is continously changing w.r.t as surrounding then it is said to be in the state of motion. Thus motion can be defined as a change in position of an Object with time. It is common to everything in the universe.

Motion can be defined as a change in position of an object with respect to its surroundings over time. If an object's position is continuously changing with respect to its surroundings, it is said to be in a state of motion.

Motion is a fundamental concept in physics, and it is observed in everything in the universe, from the smallest subatomic particles to the largest galaxies. The study of motion is essential for understanding many natural phenomena and technological applications, from the motion of planets and stars to the design of machines and vehicles.

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The answer is d. about 100 million stars.

To understand why, let's consider the stellar triangulation method using a baseline of 1 AU (Astronomical Unit) and the parallax angle. If a star has a parallax angle of less than 1 arc second, it means that it's relatively far away from Earth. The parallax angle (p) is related to the distance (d) to the star in parsecs as follows:

d = 1 / p

Here, p is in arc seconds and d is in parsecs. When p < 1 arc second, d > 1 parsec. The nearest star to Earth, Proxima Centauri, is about 1.3 parsecs away, and there are approximately 100 million stars within a distance of several thousand parsecs from the Earth.

Therefore, there are roughly 100 million stars with parallaxes less than 1 arc second.

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Answer:

Density of water = 1 g / cm^3 = 1000 kg / m^3

(Density and  specific gravity have same numerical values)

Weight of water = 10 * M = 10000 Newtons / m^3

W = weight in air = weight in water + B     where B = buoyant force

B = 10 - 8 = 2 Newtons

B = 2 N = v * 10000 N / m^3 * .86      (where .86 is weight of liquid displaced as compared to water))    

v = (2 / 10000 m^3) / .86 = = .0002.33 m^3

The total resistance of the circuit is 36.8 ohms, the total reactance X = -63.4 ohms, and the average power dissipated in the circuit is 1348 watts.

Step 1: Calculate the impedance Z of the circuit using the given values of RMS current and voltage and the phase angle between them:

Z = Vrms / Irms = 232 V / 6.30 A = 36.8 ohms

Calculate the resistance R of the circuit using the impedance Z and the phase angle between voltage and current:

R = Z * cos(57.0°) = 36.8 ohms * cos(57.0°) = 18.6 ohms

Calculate the reactance X of the circuit using the impedance Z and the phase angle between voltage and current:

X = Z * sin(57.0°) = 36.8 ohms * sin(57.0°) = 31.7 ohms

Calculate the inductance XL and capacitance XC of the circuit using the reactance X:

Calculate the total reactance X of the circuit by subtracting XC from XL:

X = XL - XC = 31.7 ohms - (-31.7 ohms) = -63.4 ohms

Calculate the total resistance of the circuit by adding the resistance R to the absolute value of the total reactance X:

Rtotal = R + |X| = 18.6 ohms + 63.4 ohms = 82.0 ohms

Calculate the average power dissipated in the circuit using the RMS current and the total resistance:

Pavg = Irms^2 * Rtotal = 6.30 A^2 * 82.0 ohms = 1348 watts

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The electrostatic force between the two charges is given by -7.192E-4 N

An equation is a mathematical expression that uses an equals sign to show that two values are the same. It can be written as a statement, where one side of the equation is equal to the other. An equation typically involves a variable, which can be a number, a letter, or a combination of both. Equations are used to solve problems and explore relationships between different values.

The electrostatic force is calculated using Coulomb's law, which states that the force between two point charges is given by the equation:
F=k (q1q2)/r²

where k is Coulomb's constant (8.99E9 Nm²/C²), q1 and q2 are the two charges, and r is the distance between them.

In this case, q1=-2E-6 C, q2=4E-6 C, and r=5 m. Therefore, the electrostatic force between the two charges is given by:

F = (8.99E9 Nm²/C²)(-2E-6 C)(4E-6 C)/(5 m)²

F = -7.192E-4 N

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Capacitors in DC circuits is that they are insulators. Capacitors store energy between conductors and block direct current while allowing alternating current to pass through.

A conductor and an insulator vary in that a conductor makes it simple for electricity to flow through it while an insulator does not.

Conductor

A substance that carries electricity is known as a conductor. All metals are effective conductors.

Single-element materials with only one valence electron loosely attached to the atom, like copper (Cu), silver (Ag), and gold (Au), make the greatest conductors.

Insulator

Insulators are substances that do not readily transport energy, such as electrical current or heat.

Electrons are present in all materials. In insulators like rubber, the electrons are not free to travel. They are firmly contained within atoms.

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The given statement "the smallest kinetic energy that an electron in a box (an infinite well) can have is zero."  is False as smallest kinetic energy that an electron in an infinite well (a box) can have is not zero, but rather a non-zero value determined by the boundary conditions of box.

In an infinite well, the electron is confined to a finite region of space by a potential energy barrier that is infinite outside the box and zero inside it. The electron's wave function is a standing wave that oscillates between two walls of the box, and the allowed energies of the electron are quantized, meaning they can only take on discrete values.

The ground state of an electron in an infinite well corresponds to the lowest possible energy level, which has a non-zero kinetic energy. This is because the electron's wave function cannot have a node at both ends of the box, and so it must have a non-zero slope at the edges, resulting in a finite kinetic energy.

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The generator must turn at a speed of 77.8 radians per second to produce a peak output of 120 V in a 0.550 T magnetic field.

The peak voltage output of a generator can be calculated using the formula:

[tex]Vpeak = NBAw[/tex]

where:

Vpeak is the peak voltage output.

N is the number of turns in the coil

B is the magnetic field strength

A is the area of the coil

ω is the angular velocity of the coil

In this case, the coil has 300 turns and is 25.0 cm on a side, so its area is:

[tex]A = (25.0cm)^{2} = 0.0625 m^{2}[/tex]

The magnetic field strength is 0.550 T, and we want to find the angular velocity ω at which the generator must turn to produce a peak output of 120 V. Rearranging the formula above, we get:

ω = Vpeak / NBA

Substituting the given values, we get:

[tex]w = (120V) / (300 turns * 0.0625m^{2}* 0.550T) = 77.8 rad/s[/tex]

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The change is considered physical on the event of new substance was not formed. The soft- silvery white metal is sodium which on reaction with chlorine gas to create white crystals like sodium chloride also most commonly known as table salt.

The conversion from yellow-green gas to white crystal like solid structures considered a physical change on the account of its chemical composition wasn't altered.

Sodium chloride is also used as a medicine by providing it as a saline solution for implementation in nasal spray. it also provides aid in being useful as a fire extinguisher , cleanser like shampoo etc.

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Answer:

D  it's correct I got 100% on edge

Explanation:

Liquids are composed of molecules that are weakly attached and free to move, but they are relatively closer together than in gases and have a definite volume.

Volume is a physical quantity that measures the amount of space occupied by an object or a substance. It is a derived quantity, meaning that it is calculated from other physical quantities such as length, width, and height.

Physical refers to anything that relates to the properties or behavior of matter and energy, as opposed to biological, chemical, or social phenomena.

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The temperature of the air needed for the hot air balloon to achieve lift-off from Earth's surface is 190°C.

To calculate the temperature of the air needed to achieve lift-off, we can use the ideal gas law: PV = nRT, where P is the pressure, V is the volume, n is the number of moles, R is the universal gas constant, and T is the temperature. We can rearrange this equation to solve for temperature: T = PV/nR.

We know that the basket load of the hot air balloon is 2670 N. To calculate the volume of air needed to lift this load, we can use the equation: V = (m + M)/ρ, where m is the mass of the hot air balloon, M is the mass of the basket load, and ρ is the density of air. The density of air is approximately 1.2 kg/m³ at standard temperature and pressure (STP).

Assuming that the mass of the hot air balloon is negligible compared to the basket load, we can simplify the equation to V = M/ρ. Plugging in the values, we get V = 2225 m³.

Now we can plug in the values for pressure (atmospheric pressure at sea level is approximately 101.3 kPa), volume (2225 m³), number of moles (which we can calculate using the mass of air and the molar mass of air), and the universal gas constant (8.31 J/mol*K) to solve for temperature.

After calculations, we get the temperature needed for lift-off to be approximately 190°C.

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