The voltage difference of which element is in phase with AC?
1. diode
2. resistor
3. inductor
4. capacitor

i. The kinetic energy of the object when it is launched from the ground is 1600 J.

ii. The maximum height attained by the object is 44.2 m.

iii. The speed of the object when it is 12 m above the ground is 34.9 m/s.

The potential energy of an object with mass m is given by the formula mgh where g is acceleration due to gravity and h is the height above the reference level. When an object is launched, it has kinetic energy. The kinetic energy of an object with mass m moving at a velocity v is given by the formula KE= 1/2mv².

i. Initially, the object has no potential energy as it is launched from the ground. Therefore, the kinetic energy of the object when it is launched from the ground is 1600 J (KE=1/2mv²).

ii. The maximum height attained by the object can be determined using the formula h= (v²sin²θ)/2g.

iii. When the object is at a height of 12 m, the potential energy is mgh. Therefore, the total energy at that point is KE + PE = mgh + 1/2mv².

By using energy conservation, the speed of the object can be calculated when it is 12 m above the ground using the formula v= √(vo²+2gh).

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Answer:

i. The kinetic energy of the object when it is launched from the ground is 1600 J.

ii. The maximum height attained by the object is 44.2 m.

iii. The speed of the object when it is 12 m above the ground is 34.9 m/s.

Explanation:

The potential energy of an object with mass m is given by the formula mgh where g is acceleration due to gravity and h is the height above the reference level. When an object is launched, it has kinetic energy. The kinetic energy of an object with mass m moving at a velocity v is given by the formula KE= 1/2mv².

i. Initially, the object has no potential energy as it is launched from the ground. Therefore, the kinetic energy of the object when it is launched from the ground is 1600 J (KE=1/2mv²).

ii. The maximum height attained by the object can be determined using the formula h= (v²sin²θ)/2g.

iii. When the object is at a height of 12 m, the potential energy is mgh. Therefore, the total energy at that point is KE + PE = mgh + 1/2mv².

By using energy conservation, the speed of the object can be calculated when it is 12 m above the ground using the formula v= √(vo²+2gh).

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The power delivered to resistor R of resistance 2.3 ohms and across which a potential difference of 20 V is applied is 173.91 W.

The given circuit diagram is shown below: We know that the power delivered to a resistor R of resistance R and across which a potential difference of V is applied is given by the formula:

P=V²/R  {Power formula}Given data:

Resistance of the resistor, R= 2.3

Voltage, V=20 V

We can apply the above formula to the given data and calculate the power as follows:

P = V²/R⇒ P = (20)²/(2.3) ⇒ P = 173.91 W

Therefore, the power delivered to the resistor is 173.91 W.

From the given circuit diagram, we are supposed to calculate the power delivered to the resistor R of resistance 2.3 ohms and across which a potential difference of 20 V is applied. In order to calculate the power delivered to the resistor, we need to use the formula:

P=V²/R, where, P is the power in watts, V is the potential difference across the resistor in volts, and R is the resistance of the resistor in ohms. By substituting the given values of resistance R and voltage V in the above formula, we get:P = (20)²/(2.3)⇒ P = 400/2.3⇒ P = 173.91 W. Therefore, the power delivered to the resistor is 173.91 W.

Therefore, we can conclude that the power delivered to resistor R of resistance 2.3 ohms and across which a potential difference of 20 V is applied is 173.91 W.

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The period of the pendulum on the surface of the Earth would be approximately 2.71 seconds.

To determine the period of the pendulum on the surface of the Earth, we need to consider the relationship between the period (T), the length of the pendulum (L), and the gravitational acceleration (g).

The formula for the period of a simple pendulum is given by:

T = 2π * √(L/g)

Where T is the period, L is the length of the pendulum, and g is the gravitational acceleration.

In this scenario, we are given the period on the unknown planet (4.0 s) and the gravitational acceleration on that planet (4.5 m/s²).

We can rearrange the formula to solve for L:

L = (T^2 * g) / (4π^2)

Plugging in the given values, we have:

L = (4.0^2 * 4.5) / (4π^2) ≈ 8.038 meters

Now, using the length of the pendulum, we can calculate the period on the surface of the Earth. Given the gravitational acceleration on Earth (9.80 m/s²), we use the same formula:

T = 2π * √(L/g)

T = 2π * √(8.038/9.80) ≈ 2.71 seconds

Therefore, the period of the pendulum on the surface of the Earth would be approximately 2.71 seconds.

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A projectile is launched from the origin with an initial velocity 3 = 207 + 20. m/s. Therefore :

(a) The initial projection angle is 53.13°.

(b) The velocity vector of the projectile after 3 seconds of launching is (20cos(53.13), 20sin(53.13)) = (14.24, 14.14) m/s.

(c) The position vector of the projectile after 3 seconds of launching is (14.243, 14.143) = (42.72, 42.42) m.

(d) The time to reach the maximum height is 1.5 seconds.

(e) The time of flight is 3 seconds.

(f) The maximum horizontal range reached is 76.6 meters.

Here are the steps involved in solving for each of these values:

(a) The initial projection angle can be found using the following equation:

tan(Ф) = [tex]v_y/v_x[/tex]

where [tex]v_y[/tex] is the initial vertical velocity and [tex]v_x[/tex] is the initial horizontal velocity.

In this case, [tex]v_y[/tex] = 20 m/s and [tex]v_x[/tex] = 20 m/s. Therefore, Ф = [tex]\tan^{-1}\left(\frac{20}{20}\right)[/tex] = 53.13°.

(b) The velocity vector of the projectile after 3 seconds of launching can be found using the following equation:

v(t) = v₀ + at

where v(t) is the velocity vector at time t, v₀ is the initial velocity vector, and a is the acceleration vector.

In this case, v₀ = (20cos(53.13), 20sin(53.13)) and a = (0, -9.8) m/s². Therefore, v(3) = (14.24, 14.14) m/s.

(c) The position vector of the projectile after 3 seconds of launching can be found using the following equation:

r(t) = r₀ + v₀t + 0.5at²

where r(t) is the position vector at time t, r₀ is the initial position vector, v0 is the initial velocity vector, and a is the acceleration vector.

In this case, r₀ = (0, 0) and v₀ = (14.24, 14.14) m/s. Therefore, r(3) = (42.72, 42.42) m.

(d) The time to reach the maximum height can be found using the following equation:

v(t) = 0

where v(t) is the velocity vector at time t.

In this case, v(t) = (0, -9.8) m/s. Therefore, t = 1.5 seconds.

(e) The time of flight can be found using the following equation:

t = 2v₀ / g

where v₀ is the initial velocity and g is the acceleration due to gravity.

In this case, v₀ = 20 m/s and g = 9.8 m/s². Therefore, t = 3 seconds.

(f) The maximum horizontal range reached can be found using the following equation:

R = v² / g

where R is the maximum horizontal range, v is the initial velocity, and g is the acceleration due to gravity.

In this case, v = 20 m/s and g = 9.8 m/s². Therefore, R = 76.6 meters.

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Given that a lightbulb is 52 cm from a convex lens and its image appears on a screen located 30 cm on the other side of the lens.

We know that image distance (v) = -30 cm (negative because the image is formed on the other side of the lens)

Object distance (u) = -52 cm (negative because the object is placed before the lens)

Focal length (f) is the distance between the center of the lens and the focal point.

It can be calculated using the lens formula;

1/f = 1/u + 1/v

Substituting the given values;

1/f = 1/-52 + 1/-30

= (-30 - 52) / (-52 x -30)

= -82 / 1560 = -0.0526f

= -1 / -0.0526f = 19.012 ≈ 19 cm.

The focal length of the convex lens is approximately 19 cm.

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Main Answer:

The maximum and minimum values of the tank level after the flow rate disturbance has occurred for a long time are approximately 4.047 m and 3.953 m, respectively.

Explanation:

The transfer function of the liquid storage tank system is given as H'(s) = 10 / (50s + 1), where h represents the tank level (in meters) and q represents the flow rate (in cubic meters per second). The system is initially at steady state with q = 0.4 m³/s and h = 4 m.

When a sinusoidal perturbation in the inlet flow rate occurs with an amplitude of 0.1 m³/s and a cyclic frequency of 0.002 cycles/s, we need to determine the maximum and minimum values of the tank level after the disturbance has settled.

To solve this problem, we can use the concept of steady-state response to a sinusoidal input. In steady state, the system response to a sinusoidal input is also a sinusoidal waveform, but with the same frequency and a different amplitude and phase.

Since the input frequency is much lower than the system's natural frequency (given by the time constant), we can assume that the system reaches steady state relatively quickly. Therefore, we can neglect the transient response and focus on the steady-state behavior.

The steady-state gain of the system is given by the magnitude of the transfer function at the input frequency. In this case, the input frequency is 0.002 cycles/s, so we can substitute s = j0.002 into the transfer function:

H'(j0.002) = 10 / (50j0.002 + 1)

To find the steady-state response, we multiply the transfer function by the input sinusoidal waveform:

H'(j0.002) * 0.1 * exp(j0.002t)

The magnitude of this expression represents the amplitude of the tank level response. By calculating the maximum and minimum values of the amplitude, we can determine the maximum and minimum values of the tank level.

After performing the calculations, we find that the maximum amplitude is approximately 0.047 m and the minimum amplitude is approximately -0.047 m. Adding these values to the initial tank level of 4 m gives us the maximum and minimum values of the tank level as approximately 4.047 m and 3.953 m, respectively.

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Momentum and Energy Multiple Choice Section. Make no marks. Bubble in best answer on Scantron sheet. 1) A student uses a spring to calculate the potential energy stored in the spring for various extensions.

If the force constant of the spring is 500 N/m and it is extended from its natural length of 0.20 m to a length of 0.40 m, (a) 5.0 J

(b) 20 J

(c) 50 J

(d) 100 J

(e) 200 J

Answer:Option (a) 5.0 J Explanation: Given:

F = 500 N/mΔx = 0.4 - 0.2 = 0.2 m

The potential energy stored in the spring is given by the formula:

U = 1/2kΔx²

where k is the force constant of the spring.

Substituting the given values, we get:

U = 1/2 × 500 N/m × (0.2 m)²= 1/2 × 500 N/m × 0.04 m²= 1/2 × 500 N/m × 0.0016 m= 0.4 J

Therefore, the potential energy stored in the spring for the given extension is 0.4 J, which is closest to option (a) 5.0 J.

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The maximum height reached by a projectile launched vertically from the surface of the earth at a speed of VagR is R. In the special case a = 2, the projectile will escape the gravitational field of the earth and never return.

(a)The projectile's motion can be modeled by the following equation of motion:

      m*dv/dt = -mg

where, m is the mass of the projectile, v is its velocity, and g is the gravitational acceleration.

We can integrate this equation once to get:

      m*v = -mgh + C

where C is a constant of integration.

At the highest point of the projectile's trajectory, its velocity is zero. So we can set v = 0 in the equation above to get:

     0 = -mgh + C

This gives us the value of the constant of integration:

     C = mgh

The maximum height reached by the projectile is the height it reaches when its velocity is zero. So we can set v = 0 in the equation above to get:

     mgh = -mgh + mgh

This gives us the maximum height:

h = R

(b) In the special case a = 2, the projectile's initial velocity is equal to the escape velocity. This means that the projectile will escape the gravitational field of the earth and never return.

The escape velocity is given by:

∨e = √2gR

So in the case a = 2, the maximum height reached by the projectile is infinite.

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The bowling ball would have to spin at approximately 9.63 rpm to have an angular momentum of 0.16 kgm²/s. To find the angular velocity of the bowling ball in rpm (revolutions per minute), we can use the formula:

Angular momentum (L) = moment of inertia (I) * angular velocity (ω)

The moment of inertia (I) of a solid sphere is given by:

I = (2/5) * m * r^2

m = mass of the bowling ball = 4.6 kg

r = radius of the bowling ball = (19 cm) / 2 = 0.095 m (converting diameter to radius)

0.16 kgm²/s = (2/5) * 4.6 kg * (0.095 m)^2 * ω

ω = (0.16 kgm²/s) / [(2/5) * 4.6 kg * (0.095 m)^2]

ω ≈ 1.009 rad/s

To convert this angular velocity from radians per second to revolutions per minute, we can use the conversion factor:

1 revolution = 2π radians

1 minute = 60 seconds

So, the angular velocity in rpm is:

ω_rpm = (1.009 rad/s) * (1 revolution / 2π rad) * (60 s / 1 minute)

ω_rpm ≈ 9.63 rpm

Therefore, the bowling ball would have to spin at approximately 9.63 rpm to have an angular momentum of 0.16 kgm²/s.

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The phase angle in a series R L C circuit at resonance is 0 (option c).

At resonance, the inductive reactance (XL) of the inductor and the capacitive reactance (XC) of the capacitor cancel each other out. As a result, the net reactance of the circuit becomes zero, which means that the circuit behaves purely resistive.

In a purely resistive circuit, the phase angle between the current and the voltage is 0 degrees. This means that the current and the voltage are in phase with each other. They reach their maximum and minimum values at the same time.

To further illustrate this, let's consider a series R L C circuit at resonance. When the current through the circuit is at its peak value, the voltage across the resistor, inductor, and capacitor is also at its peak value. Similarly, when the current through the circuit is at its minimum value, the voltage across the resistor, inductor, and capacitor is also at its minimum value.

Therefore, the phase angle in a series R L C circuit at resonance is 0 degrees.

Please note that option e ("None of those answers is necessarily correct") is not applicable in this case, as the correct answer is option c, 0 degrees.

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The energy conservation approach used for the block does not directly apply to the rolling cylinder

To find the expression for the time it takes for the block to slide down the inclined plane without friction, we can use the concept of conservation of energy.

The block's initial potential energy at the top of the inclined plane will be converted into kinetic energy as it slides down.

Without friction:

The potential energy (PE) at the top of the inclined plane is given by:

[tex]PE = mgh[/tex]

where m is the mass of the block, g is the acceleration due to gravity, and h is the height difference between the lowest and highest point on the inclined plane.

The kinetic energy (KE) at the bottom of the inclined plane is given by:

[tex]KE = (1/2)mv^2[/tex]

where v is the final velocity of the block at the bottom.

According to the principle of conservation of energy, the potential energy at the top is equal to the kinetic energy at the bottom:

[tex]mgh = (1/2)mv^2[/tex]

We can cancel out the mass (m) from both sides of the equation, and rearrange to solve for the final velocity (v):

[tex]v = sqrt(2gh)[/tex]

The time (t) it takes for the block to slide down the entire inclined plane can be calculated using the equation of motion:

[tex]s = ut + (1/2)at^2[/tex]

where s is the height difference, u is the initial velocity (which is zero in this case), a is the acceleration (which is equal to g), and t is the time.

Since the block starts from rest, the initial velocity (u) is zero, and the equation simplifies to:

[tex]s = (1/2)at^2[/tex]

Substituting the values of s and a, we have:

[tex]h = (1/2)gt^2[/tex]

Solving for t, we get the expression for the time it takes for the block to slide down the entire inclined plane without friction:

[tex]t = sqrt(2h/g)[/tex]

With friction:

To determine the frictional force acting on the block, we need additional information about the block's mass, coefficient of friction, and other relevant factors.

Without this information, it is not possible to provide a specific value for the friction coefficient.

Solid Cylinder Rolling Down:

If a homogeneous solid cylinder is released from the top of the inclined plane and rolls without sliding, the analysis becomes more complex.

The energy conservation approach used for the block does not directly apply to the rolling cylinder.

To find an expression for the time it takes for the cylinder to roll down the inclined plane, considering that the cylinder's axis is always horizontal, a more detailed analysis involving torque, moment of inertia, and rotational kinetic energy is required.

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a) Define the activity of a radioactive source.

The activity of a radioactive source can be defined as the rate at which the number of radioactive nuclei of that source undergoes decay or the amount of radiation produced by the source per unit of time.

b) The activity of a radioactive source is proportional to the number of radioactive nuclei present within it. The activity of a radioactive source is directly proportional to the number of radioactive nuclei present within it.

The higher the number of radioactive nuclei, the greater the activity of the radioactive source.

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The Power is the amount of work done per unit time. Power is denoted by P. The formula for power is given as;P= W/t where W is the amount of work done and t is the time taken. UnitsThe SI unit of power is Joule per second (J/s) or Watt (W).

Calculation of PowerThe power is calculated as shown below;Given that a man lifts a box 1.85 meters in 0.75 seconds, and the box has a weight of 375 NThe work done by the man is given asW = Fswhere F is the force applied and s is the distance moved by the boxF = m*gwhere m is the mass of the box and g is the acceleration due to gravitySubstituting valuesF = 375N (mass of the box = weight/g = 375/9.81) = 38.14ms^-2W = Fs = 375 x 1.85 = 693.75JThe time taken is given as t = 0.75sPower is given by the formula P = W/tSubstituting values;P = 693.75J/0.75s = 925W7. Formula for Potential Energy

The potential energy is defined as the energy an object possesses due to its position. It is denoted by PE.The formula for potential energy is given as;PE = mgh

where m is the mass of the object, g is the acceleration due to gravity and h is the height or distance from the ground.UnitsThe SI unit of potential energy is Joule (J).

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This means that the spring constant of the spring is 310 N/m.

(a) The change in gravitational potential energy of the marble-Earth system is ΔUg = mgh = 6.2 * 10^-3 kg * 9.8 m/s^2 * 21 m = 13.0 J.

(b) The change in elastic potential energy of the spring is ΔUs = 1/2kx^2 = 1/2 * k * (0.086 m)^2 = 2.1 J.

(c) The spring constant of the spring is k = 2 * ΔUs / x^2 = 2 * 2.1 J / (0.086 m)^2 = 310 N/m.

Here are the details:

(a) The gravitational potential energy of an object is given by the following formula:

PE = mgh

Where:

* PE is the gravitational potential energy in joules

* m is the mass of the object in kilograms

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

* h is the height of the object above a reference point in meters

In this case, the mass of the marble is 6.2 * 10^-3 kg, the acceleration due to gravity is 9.8 m/s^2, and the height of the marble is 21 m. Plugging in these values, we get:

PE = 6.2 * 10^-3 kg * 9.8 m/s^2 * 21 m = 13.0 J

This means that the gravitational potential energy of the marble-Earth system increases by 13.0 J as the marble moves from the spring to the target.

(b) The elastic potential energy of a spring is given by the following formula:

PE = 1/2kx^2

where:

* PE is the elastic potential energy in joules

* k is the spring constant in newtons per meter

* x is the displacement of the spring from its equilibrium position in meters

In this case, the spring constant is 310 N/m, and the displacement of the spring is 0.086 m. Plugging in these values, we get:

PE = 1/2 * 310 N/m * (0.086 m)^2 = 2.1 J

This means that the elastic potential energy of the spring increases by 2.1 J as the marble is compressed.

(c) The spring constant of a spring is a measure of how stiff the spring is. It is calculated by dividing the force required to compress or stretch the spring by the amount of compression or stretching.

In this case, the force required to compress the spring is 2.1 J, and the amount of compression is 0.086 m. Plugging in these values, we get:

k = F / x = 2.1 J / 0.086 m = 310 N

This means that the spring constant of the spring is 310 N/m.

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The final velocity of the two cars, after colliding at an icy intersection, is 6.51 m/s at an angle of 309 degrees from the south.

When two cars collide and stick together, their masses and velocities determine their final velocity.

In this case, using the law of conservation of momentum, we can calculate the final velocity of the two cars.

The initial momentum of the first car is (1200 kg)(7.74 m/s) = 9292.8 kgm/s south.

The initial momentum of the second car is (805 kg)(15.7 m/s) = 12648.5 kgm/s west.

After the collision, the total momentum of the two cars is conserved and is equal to (1200 + 805)*(final velocity).

Solving for the final velocity, we get a magnitude of 6.51 m/s.

The direction of the final velocity can be found using trigonometry, where the tangent of the angle between the final velocity and the south direction is equal to -15.7/7.74.

This gives us an angle of 309 degrees from the south.

Therefore, the final velocity of the two cars is 6.51 m/s at an angle of 309 degrees from the south.

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A. The acceleration of the shuttle is 15 m/s^2.

B. The acceleration of the shuttle will not change in space as long as the thrust force remains the same, but its velocity will continue to increase until it reaches a point where the thrust force is equal to the force of gravity acting on it.

The mass of the space shuttle, m = 2.0 x 10^6 kg

The upward force generated by engines, F = 3.0 x 10^7 N

We know that Newton’s Second Law of Motion is F = ma, where F is the net force applied on the object, m is the mass of the object, and a is the acceleration produced by that force.

Rearranging the above formula, we geta = F / m Substituting the given values,

we have a = (3.0 x 10^7 N) / (2.0 x 10^6 kg)= 15 m/s^2

Therefore, the acceleration of the shuttle is 15 m/s^2.

According to Newton’s third law of motion, every action has an equal and opposite reaction. The action is the force produced by the engines, and the reaction is the force experienced by the rocket. Therefore, in the absence of air resistance, the acceleration of the shuttle would depend on the magnitude of the force applied to the shuttle. Let’s assume that the shuttle is in outer space. The upward force produced by the engines is still the same, i.e., 3.0 x 10^7 N. However, since there is no air resistance in space, the shuttle will continue to accelerate. Newton’s first law states that an object will continue to move with a constant velocity unless acted upon by a net force. In space, the only net force acting on the shuttle is the thrust produced by the engines. Thus, the shuttle will continue to accelerate, and its velocity will increase. In other words, the acceleration of the shuttle will not change in space as long as the thrust force remains the same, but its velocity will continue to increase until it reaches a point where the thrust force is equal to the force of gravity acting on it.

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Given that the radiation push outside the Earth is I = 1400 W/m².

We know that the solar radiation pressure is given as F = IA/c, where F is the force per unit area of radiation, I is the intensity of the radiation, A is the area and c is the speed of light.

From the above, it can be calculated that the radiation pressure outside Earth is

F = I/c = 1400/3×10⁸ = 4.67×10⁻⁶ N/m².

For an area A, the radiation push can be expressed as

F = IA/c ⇒ A = Fc/I, where F = 3 N.

Therefore, the area required for the radiation sail to obtain a radiation push of 3N just outside of Earth (I=1400W/m²) can be calculated as follows:

A = Fc/I= 3 × 3 × 10⁸/1400 = 6.43×10⁴ m²

Therefore, the area required for the radiation sail to obtain a radiation push of 3N just outside of Earth (I=1400W/m²) is 6.43×10⁴ m².

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In this scenario, a child on a swing has a speed of 2.05 m/s at the lowest point of their path, and the centripetal acceleration at that point is 3.89 m/s².

The task is to determine the height (r) at which the swing is suspended above the child's center of mass.

The centripetal acceleration at the lowest point of the swing can be related to the speed and height by the equation a = v² / r, where a is the centripetal acceleration, v is the speed, and r is the radius or distance from the center of rotation.

In this case, we are given the values for v and a, and we need to find the value of r. Rearranging the equation, we have r = v² / a.

Substituting the given values, we find r = (2.05 m/s)² / (3.89 m/s²).

Evaluating the expression, we can calculate the value of r, which represents the height at which the swing is suspended above the child's center of mass.

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Thermal State is defined as the state of a substance in which the energy, pressure, and volume are constant. The answer to the first part of your question is as follows:

As a result, the feed is in the superheated vapor state, which means that it is at a temperature above the boiling point. A vapor is called superheated when it is heated beyond its saturation point and its temperature exceeds the boiling point at the given pressure. Since the enthalpy of the feed stream (1828 MJ/kg) is greater than the enthalpy of a saturated vapor (1935 MJ/kg), it implies that the temperature of the feed stream is higher than the boiling point at that pressure, indicating a superheated state.

Now let's move to the second part of the question. The answer is as follows:

The thermal state of the feed that condenses 1 mole of vapor for every 3.0 moles of feed that enter the feed stage is saturated vapor. This is because the feed is made up of a combination of subcooled liquid and saturated vapor. When one mole of vapor condenses, it transforms from a saturated vapor to a two-phase liquid-vapor state. As a result, the feed is now a combination of subcooled liquid, two-phase liquid-vapor, and saturated vapor. Since the feed contains more than 90% vapor, it can be classified as a saturated vapor.

The thermal state of an object is considered with reference to its ability to transfer heat to other objects. The body that loses heat is defined as having a higher temperature, the body that receives it has a lower temperature.

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As 180-ohm resistor can dissipate a maximum power of .250W The maximum current that can pass through the resistor while meeting the power limit is 0.027 A which can be obtained by the formula P = I²R

The resistance of the resistor, R = 180 Ω. The maximum power dissipated by the resistor, P = 0.250 W. We need to find the maximum current that can be passed through the resistor while maintaining the power limit. The maximum power that can be dissipated by the resistor is given by the formula;

P = I²R …………… (1)

Where; P = Power in watts, I = Current in amperes, and R = Resistance in ohms.

Rewriting the above equation, we get,

I = √(P / R) ………… (2)

Substitute the given values into the equation 2 and solve for the current,

I = √(0.250 / 180)

⇒I = 0.027 A

The maximum current that can pass through the resistor while meeting the power limit is 0.027 A.

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The maximum speed, vmax, that the car can take on the banked curve is approximately 31.6 m/s.

To determine the maximum speed, we need to consider the forces acting on the car during the banked turn. The gravitational force acting on the car can be resolved into two components: one perpendicular to the road (Fn) and one parallel to the road (Fg).

The maximum speed can be achieved when the static friction force (Fs) between the tires and the road provides the centripetal force required for circular motion. The maximum static friction force can be calculated using the formula:

Fs(max) = μs * Fn

The normal force (Fn) can be determined using the vertical equilibrium equation:

Fn = mg * cos(θ)

where m is the mass of the car, g is the acceleration due to gravity, and θ is the angle of the banked turn.

The centripetal force (Fc) required for circular motion is given by:

Fc = m * v^2 / r

where v is the velocity of the car and r is the radius of curvature.

Setting Fs(max) equal to Fc, we can solve for the maximum velocity:

μs * Fn = m * v^2 / r

Substituting the expressions for Fn and μs * Fn, we get:

μs * mg * cos(θ) = m * v^2 / r

Simplifying the equation and solving for v, we find:

v = √(μs * g * r * tan(θ))

Substituting the given values, we have:

v = √(0.63 * 9.8 m/s^2 * 104 m * tan(24°))

Calculating the value, we find:

v ≈ 31.6 m/s

Therefore, the maximum speed, vmax, that the car can take on this banked curve is approximately 31.6 m/s.

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The average velocity of the car after half a lap if it completes a lap in 13 seconds is approximately 14.1 m/s.

To find the average velocity of the car after half a lap, we need to determine the distance traveled and the time taken.

Radius of the circular track (r) = 136 meters

Time taken to complete a lap (t) = 13 seconds

The distance traveled in half a lap is equal to half the circumference of the circle:

Distance = (1/2) × 2π × r

Distance = π × r

Plugging in the value of the radius:

Distance = π × 136 meters

The average velocity is calculated by dividing the distance traveled by the time taken:

Average velocity = Distance / Time

Average velocity = (π × 136 meters) / 13 seconds

Average velocity = 14.1 m/s

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Temperatures are often measured with electrical resistance thermometers. Suppose that the resistance of such a resistance thermometer is 1080 when its temperature is 18.0 °C. Therefore, the temperature of the liquid is approximately 33.99 °C.

To find the temperature of the liquid,

ΔR = R₀ ×a ×ΔT

Where:

ΔR is the change in resistance

R₀ is the initial resistance

a is the temperature coefficient of resistivity

ΔT is the change in temperature

The following values:

R₀ = 1080 Ω (at 18.0 °C)

ΔR = 85.89 Ω (change in resistance)

a = 5.46 x 1[tex]0^(^-^3^)[/tex] (°[tex]C^(^-^1^)[/tex]

To calculate ΔT, the change in temperature, and then add it to the initial temperature to find the temperature of the liquid.

To find ΔT, the formula:

ΔT = ΔR / (R₀ × a)

Substituting the given values:

ΔT = 85.89 Ω / (1080 Ω ×5.46 x 1[tex]0^(^-^3^)[/tex] (°[tex]C^(^-^1^)[/tex])

Calculating ΔT:

ΔT = 85.89 / (1080 × 5.46 x 1[tex]0^(^-^3^)[/tex])

≈ 15.99 °C

Now, one can find the temperature of the liquid by adding ΔT to the initial temperature:

Temperature of the liquid = 18.0 °C + 15.99 °C

≈ 33.99 °C

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The force constant of the spring is approximately 471,386.5 N/m. The maximum velocity of the mass is around 7.73 m/s.

1. To find the force constant (k) of the spring, we can use Hooke's Law, which states that the force exerted by a spring is proportional to the displacement from its equilibrium position:

F = -k * x,

where F is the force applied, k is the force constant, and x is the displacement. Given information:

- Mass of the subway train (m): 3.00 x 10^5 kg

- Initial speed (v): 1.57 miles per hour = 0.701 meters per second (m/s)

- Stopping distance (x): 0.386 m

To bring the train to a stop, the spring bumper applies a force opposite to the motion of the train until it comes to rest. This force is given by:

F = m * a,

where m is the mass and a is the acceleration.

Using the equation of motion:

v^2 = u^2 + 2 * a * x,

where u is the initial velocity and v is the final velocity,

we can solve for the acceleration (a):

a = (v^2 - u^2) / (2 * x).

Substituting the given values:

a = (0 - (0.701 m/s)^2) / (2 * 0.386 m)

 ≈ -0.607 m/s^2.

Since the force applied by the spring is opposite to the motion, we can rewrite the force as:

F = -m * a

 = -(3.00 x 10^5 kg) * (-0.607 m/s^2).

Using Hooke's Law:

F = -k * x,

we can equate the two expressions for force:

-(3.00 x 10^5 kg) * (-0.607 m/s^2) = -k * 0.386 m.

Simplifying the equation:

k = (3.00 x 10^5 kg * 0.607 m/s^2) / 0.386 m.

Calculating the value:

k ≈ 471,386.5 N/m.

Therefore, the force constant (k) of the spring is approximately 471,386.5 N/m.

2. To find the maximum velocity of the mass in the horizontal configuration, we can use the principle of conservation of mechanical energy. At the maximum compression, all the potential energy stored in the spring is converted into kinetic energy.

The potential energy of the compressed spring is given by:

PE = (1/2) * k * x^2,

where k is the force constant and x is the compression of the spring.

Given information:

- Compression of the spring (x): 0.785 m

- Mass of the object (m): 0.111 kg

The potential energy is converted into kinetic energy at maximum velocity:

PE = (1/2) * m * v_max^2,

where v_max is the maximum velocity.

Setting the potential energy equal to the kinetic energy:

(1/2) * k * x^2 = (1/2) * m * v_max^2.

Simplifying the equation:

k * x^2 = m * v_max^2.

Solving for v_max:

v_max = sqrt((k * x^2) / m).

Substituting the given values:

v_max = sqrt((471,386.5 N/m * (0.785 m)^2) / 0.111 kg).

Calculating the value:

v_max ≈ 7.73 m/s.

Therefore, the maximum velocity of the mass in the horizontal configuration is approximately 7.73 m/s.

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Since the spheres are identical, their charges can be assumed to be the same, so we can denote the charge on each sphere as q. By rearranging Coulomb's law to solve for the charge (q), we get q = sqrt((F *[tex]r^2[/tex]) / k).

The magnitude of the charge on each sphere can be determined using Coulomb's law, which relates the electrostatic force between two charged objects to the magnitude of their charges and the distance between them.

By rearranging the equation and substituting the given values, the charge on each sphere can be calculated.

Coulomb's law states that the electrostatic force between two charged objects is directly proportional to the product of their charges and inversely proportional to the square of the distance between them.

Mathematically, it can be expressed as F = k * (|q1| * |q2|) / [tex]r^2[/tex], where F is the force, k is the electrostatic constant, q1 and q2 are the charges, and r is the distance between the charges.

In this case, we have two identical positively charged spheres experiencing an attractive force. Since the spheres are identical, their charges can be assumed to be the same, so we can denote the charge on each sphere as q.

We are given the distance between the spheres (r = 23.0 cm) and the force of attraction (F = 4.25x[tex]10^-9[/tex] N). By rearranging Coulomb's law to solve for the charge (q), we get q = sqrt((F *[tex]r^2[/tex]) / k).

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The value of the phase constant, φ is 0

Graph of x(t)Using the graph, we can see that the equation for the position function x(t) = A sin (ωt + φ)  is as follows;

x(t) = A sin (ωt + φ)  ....... (1)

where; A = amplitude

ω = angular frequency = 2π/T

T = time period of oscillation = 2π/ω

φ = phase constant

x(t) = displacement from the mean position at time t

From the graph, we can see that the amplitude, A is 4 m. Using the given information in the question, we can find the angular frequencyω = 2π/T, but T = time period of oscillation. We can get the time period of oscillation, T from the graph. From the graph, we can see that one complete cycle is completed in 2 seconds. Therefore,

T = 2 seconds

ω = 2π/T

   = 2π/2

   = π rad/s

Again, from the graph, we can see that at time t = 0 seconds, the displacement, x(t) is 0. This means that φ = 0.  Putting all this into equation (1), we have;

x(t) = 4 sin (πt + 0)

The phase constant, φ = 0.

The value of the phase constant, φ is 0 and this means that the equation for the position function is; x(t) = 4 sin (πt)

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The value of a is 100, as it represents the coefficient π in the equation. Therefore, if B = 5 Tesla, the magnitude of the torque on the loop is 500π N·m, or approximately 1570 N·m.

The torque on a current-carrying loop placed in a magnetic field is given by the equation τ = NIABsinθ, where τ is the torque, N is the number of turns in the loop, I is the current, A is the area of the loop, B is the magnitude of the magnetic field, and θ is the angle between the magnetic field and the normal to the loop.

In this case, the loop has a radius of 10 meters, so the area A is πr² = π(10 m)² = 100π m². The current I is 2 amps, and the magnitude of the magnetic field B is 5 Tesla. The angle θ between the magnetic field and the z-axis is 30°.

Plugging in the values into the torque equation, we have: τ = (2)(1)(100π)(5)(sin 30°)

Using the approximation sin 30° = 0.5, the equation simplifies to: τ = 500π N·m

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The correct answer is (C) 10 N/C, 37 degrees upward with the +x axis.

The electric field at the origin due to charge QI is directed upward and has a magnitude of:

E_1 = k * QI / r^2

where:

* k is Coulomb's constant

* QI is the charge of QI

* r is the distance between the origin and QI

Plugging in the known values, we get:

E_1 = (8.99 x 10^9 N m^2 C^-2) * (3.0 x 10^9 C) / ((4.5 m)^2) = 10 N/C

The electric field at the origin due to charge QII is directed downward and has a magnitude of:

E_2 = k * QII / r^2

Plugging in the known values, we get,

E_2 = (8.99 x 10^9 N m^2 C^-2) * (-9.0 x 10^9 C) / ((4.5 m)^2) = -20 N/C

The total electric field at the origin is the vector sum of E_1 and E_2. The vector sum is directed upward and has a magnitude of 10 N/C. The angle between the total electric field and the +x axis is 37 degrees.

Therefore, the correct answer is **C) 10 N/C, 37 degrees upward with the +x axis.

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The equation of the object's velocity as a function of time is v(t) = -71 + 424t - 24t^2 and the acceleration a(t) is 424 - 48t.

To find the velocity and acceleration as functions of time, we need to differentiate the position equation with respect to time.

a) Velocity (v) as a function of time:

To find the velocity, we differentiate the position equation with respect to time (t):

v(t) = d(x)/dt

Given:

x(t) = 414 - 71t + 212t^2 - 8t^3 + 11

Differentiating with respect to t, we get:

v(t) = d(414 - 71t + 212t^2 - 8t^3 + 11)/dt

v(t) = -71 + 2(212t) - 3(8t^2)

Simplifying the equation:

v(t) = -71 + 424t - 24t^2

Therefore, the equation of the object's velocity as a function of time is v(t) = -71 + 424t - 24t^2.

b) Acceleration (a) as a function of time:

To find the acceleration, we differentiate the velocity equation with respect to time (t):

a(t) = d(v)/dt

Given:

v(t) = -71 + 424t - 24t^2

Differentiating with respect to t, we get:

a(t) = d(-71 + 424t - 24t^2)/dt

a(t) = 424 - 48t

Therefore, the equation of the object's acceleration as a function of time is a(t) = 424 - 48t.

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When a light ray travels from air at an incident angle of 25 degrees with the normal, and the corresponding angle of refraction in glass was measured to be 16 degrees. To find the refractive index (n) of glass, we need to use the formula:

Equation 1:

Nair sin 01 = n glass sin O2The given values are:

01 = 25 degreesO2

= 16 degrees Nair

= 1  We have to find n glass Substitute the given values in the above equation 1 and solve for n glass. n glass = [tex]Nair sin 01 / sin O2[/tex]

[tex]= 1 sin 25 / sin 16[/tex]

= 1.538 Therefore the refractive index of glass is 1.538.To find the speed of light in glass, we need to use the formula:

Equation 2:

[tex]n = c/V[/tex] where, n is the refractive index of the glass, c is the speed of light in air, and V is the speed of light in glass Substitute the given values in the above equation 2 and solve for V.[tex]1.538 = (3 x 108) / VV = (3 x 108) / 1.538[/tex]

Therefore, the speed of light in glass is[tex]1.953 x 108 m/s.[/tex]

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