A 2 g box is pushed against a slippery surface with a constant force of 50 N. How far the box must be pushed, starting from rest, so that its final kinetic energy is 380 s ? 7.6 m 7.6 cm 76 m 76 cm

Answers

Answer 1

The final kinetic energy of the box can be calculated using the formula:Kf = (1/2)mv² Where, Kf = Final kinetic energy of the box, m = Mass of the box, v = Final velocity of the box The initial kinetic energy of the box is zero, as it is at rest.

Hence, the initial velocity of the box is zero. Now, we can use the work-energy principle, which states that the work done by the force on the box is equal to the change in kinetic energy of the box.

W = ΔKSince the force applied on the box is constant, we can use the formula for work done by a constant force:

W = Fs Where, F = Force applied on the box s = Distance moved by the box in the direction of the force Now, we can write: Fs = ΔK50s = Kf

Substituting the value of Kf, we get:50s = (1/2)mv²

Substituting the values given, we get:50s = (1/2)(2)(v²)50s = v²

We need to find the distance moved by the box, which is given by the formula for displacement with constant acceleration: s = (1/2)at²

Where, s = Distance moved by the box

a = Acceleration of the box

t = Time taken by the box to move the distance s

The box must be pushed a distance of 15.2 m, starting from rest, so that its final kinetic energy is 380 J.

Therefore, the answer is option (c) 76 m, since 15.2 m × 5 = 76 m (We are multiplying by 5, since the force is applied five times on the box)Note: The answer in centimeters is incorrect, since the displacement of the box is in meters.

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Related Questions

A load of coal is dropped from a bunker into a Part A railroad hopper car of inertia 2.0×10^4 kg coasting at 0.70 m/s on a level track. The car's speed is What is the inertia (mass) of the load of coal? 0.50 m/s after the coal falls. Express your answer with the appropriate units. 2 Incorrect; Try Again; 2 attempts remaining

Answers

Inertia mass of the load of coal dropped in the railroad hopper car is 28,000 kg.

Inertia of railroad hopper car

(I) = 2.0 × 104 kg

Speed of railroad hopper car before dropping coal

(v1) = 0.70 m/s

Speed of railroad hopper car after dropping coal

(v2) = 0.50 m/s

To find:

Inertia (mass) of the load of coal dropped in the railroad hopper car (m)Formula:

Conservation of Momentum

(m1v1 = (m1 + m2)v2 + I(v2 - v1))

where,

m1 = mass of coal dropped

m2 = mass of the railroad hopper car

v1 = initial velocity of the railroad hopper car

v2 = final velocity of the railroad hopper car

I = Inertia of railroad hopper car

Substituting the given values in the above formula,

m1 × 0 + m2 × 0.70 = (m1 + m2) × 0.50 + 2.0 × 104 × (0.50 - 0.70)

m1 + m2 = 20000 × (- 0.20)/0.20

m1 + m2 = - 200000

m1 + m2 + 200000 = 0m = m1 + m2= - 200000 + 28000= 172000 kg= 1.72 × 105 kg

Inertia (mass) of the load of coal dropped in the railroad hopper car is 28,000 kg (rounded to 3 significant figures)

the correct answer is:

Inertia (mass) of the load of coal dropped in the railroad hopper car is 28,000 kg.

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In the circuit below three resistors are connected to a 10 V battery, R1​=8.5ohms,R2​=3.3ohms, and R3​=4.6ohms. What is the current through R1​,R2​, and R3​ ?

Answers

The current through R1​,R2​, and R3​ is :

I1​=1.18 A, I2​=3.03 A and I3​=2.17 A.

The current through R1​ is the lowest, followed by R3​, and R2​ has the highest current flowing through it.

Given that, Three resistors R1​=8.5 ohms, R2​=3.3 ohms and R3​=4.6 ohms are connected to a 10 V battery.

The current through the given resistors can be calculated using Ohm's Law.

The mathematical expression of Ohm's Law is given as:

V=IR

Here, V is the voltage across the conductor.

I is the current passing through the conductor.

R is the resistance of the conductor.

The resistance R, in ohms, of a conductor is defined as the ratio of the voltage V, across the conductor to the current I passing through it.

This is given as:R=V/I

Therefore,

I=V/RI=10/8.5 ohms I=1.18 A

I=V/RI=10/3.3 ohms I=3.03 A

I=V/RI=10/4.6 ohms I=2.17 A

Thus, the current through R1​,R2​, and R3​ is : I1​=1.18 A, I2​=3.03 A and I3​=2.17 A.

Therefore, the current through R1​ is the lowest, followed by R3​, and R2​ has the highest current flowing through it.

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What is the ratio of the kinetic energy of an electron to that of proton if their de-Broglie wavelengths are equal?

Answers

The ratio of the kinetic energy of an electron to that of a proton, when their de Broglie wavelengths are equal, is equal to the ratio of their masses:

KEe / KEp = mp / me

This means that the kinetic energy of a proton is greater than that of an electron if their de Broglie wavelengths are equal.

The ratio of the kinetic energy of an electron to that of a proton can be determined by comparing their de Broglie wavelengths.

The de Broglie wavelength of a particle is given by the equation:

λ = h / p

Where, λ is the wavelength, h is Planck's constant, and p is the momentum of the particle. Since the de Broglie wavelengths of the electron and proton are equal, we can equate their respective equations: h / pe = h / pp where pe is the momentum of the electron and pp is the momentum of the proton.

To find the ratio of their kinetic energies, we can use the formula for kinetic energy:

KE = (1/2) * m * v^2

Where, KE is the kinetic energy, m is the mass of the particle, and v is the velocity of the particle.

Since we know that the momentum of a particle is given by p = m * v, we can rewrite the equation for kinetic energy as:

KE = (p^2) / (2m)

Substituting the values for the electron and proton:

KEe = (pe^2) / (2me)

KEp = (pp^2) / (2mp)

We can now find the ratio of their kinetic energies:

(KEe / KEp) = ((pe^2) / (2me)) / ((pp^2) / (2mp))

Canceling out the 2 and rearranging the equation:

(KEe / KEp) = (pe^2 / pp^2) * (mp / me)

Since we have already established that their de Broglie wavelengths are equal, we know that their momenta are inversely proportional to their wavelengths:

pe / pp = λp / λe = 1

Substituting this into the equation:

(KEe / KEp) = (pe^2 / pp^2) * (mp / me)

                  = (1^2) * (mp / me)

                  = mp / me

Therefore, the de Broglie wavelengths are equal, the ratio of an electrons to a proton's kinetic energy equals that of their masses:

mp / me = KEe / KEp

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The roof of a coach 6 m long, traveling at 100 km/h in air (μ = 1.8 x 10-5 kg 5 kg, p = 1.2 kg/m³). Calculate the Reynolds number and state if the flow is laminar or turbulent. (4) 1.4 (a) Explain emissivity and state its range. (2) (b) Surface A is coated with white paint and is maintained at a temperature of 200°C. It is located directly opposite surface B which is considered a black body and is maintained at a temperature of 800°C. Calculate the amount of heat that needs to be removed from surface A per unit area to maintain its constant temperature. Assume the following: emissivity = 0.97, view factor = 1; Stefan Boltzmann constant = 56.7 x 10-9 W/m².K4.

Answers

The amount of heat that needs to be removed from surface A per unit area to maintain its constant temperature is 4639.80 W/m².

Part A Reynolds Number:

The given terms are,

Length, L = 6 m

Speed, V = 100 km/h

= (100 x 1000) / (60 x 60)

= 27.78 m/s

Density, p = 1.2 kg/m³

Viscosity, μ = 1.8 x 10-5 kg/ms

Reynolds Number,

[tex]Re = (pVL) / μ[/tex]

= (1.2 x 27.78 x 6) / (1.8 x 10^-5)= 2.00 x 10^7

If Reynolds number is greater than 4000, the flow is turbulent.

As Reynolds number = 2 x 10^7, the flow is turbulent.

Part B. The given terms are, Emissivity, e = 0.97

View factor, F12 = 1

Temperature, T1 = 200°C

Temperature, T2 = 800°C

Stefan Boltzmann constant, σ = 5.67 x 10^-8 W/m².K^4

The amount of heat that needs to be removed from surface A per unit area to maintain its constant temperature is calculated as follows,

[tex]Q = F12 e σ (T14 - T24)[/tex]

= (1 x 0.97 x 5.67 x 10^-8) (200 + 273)^4 - (800 + 273)^4)

= 4639.80 W/m²

Therefore, the amount of heat that needs to be removed from surface A per unit area to maintain its constant temperature is 4639.80 W/m².

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A conducting object has a constant potential and a constant electric field strength throughout. this is an incorrect statement, the potential increases on edge near the other conductor true True, except the potential is a constant value of zero in all conductors and the electric field strength is a constant value larger than zero depending on the voltage on the power supply false

Answers

The correct statement regarding a conducting object is: "This is an incorrect statement, the potential increases on the edge near the other conductor."

In the given statement, it is stated that a conducting object has a constant potential and a constant electric field strength throughout, which is not true. However, the correct statement is that "the potential increases on the edge near the other conductor."In a conductor, the potential is not constant, and it changes from point to point within the conductor. It means that the potential difference exists between two points inside a conductor.

The potential difference exists because of the presence of charges within the conductor.As per the principle of electrostatics, charges always move from a high potential point to a low potential point. Therefore, the charges will tend to move towards the region where the potential is lower.

Due to this, the potential increases near the other conductor.

Thus, the given statement is incorrect, and the potential increases on the edge near the other conductor.

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E= (b) What is the directisn of the electric fiel? in the direction of the electren's moton opposte the the drectan of the electerns mation porpendoular to the diraction of the electron's mation. part (a). (Use the folbuing as necessary: E
1

K
1

,m
0

, Mrand e for the charge of the elecron.)
ε
part (0)


ε
new



=

Answers

Perpendicular to the direction of the electron's motion.

Given information:

E = 1.5 kN/C, m₀ = 9.11×10⁻³¹ kg, e = 1.60×10⁻¹⁹ C

(b) What is the direction of the electric field?

The direction of the electric field is perpendicular to the direction of the electron's motion. This is because the electric field force is perpendicular to the motion of the charged particle.

According to the Lorentz force law,

F = q[E + v × B]

where q is the charge, E is the electric field, v is the velocity of the particle, and B is the magnetic field.

Since there is no magnetic field, we can write the equation as

,F = qE

The direction of the force is opposite to the direction of motion because the charge of the electron is negative, while the direction of the electric field is from positive to negative charges. As a result, the direction of the electric field is perpendicular to the direction of the electron's motion.

Answer: Perpendicular to the direction of the electron's motion.

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The time to failure in hours of an electronic component subjected to an accelerated life test is shown in
Table 3E.1. To accelerate the failure test, the uniti were tested at an elevated temperature (read dom, then across). a. Calculate the sample average and standard deviation. b. Construct a histogram. c. Construct a stem-and-leaf plot. d. Find the sample median and the lower and upper quartiles.

Answers

The sample average is 77.4 hours, and the sample standard deviation is 23.9 hours. A histogram and stem-and-leaf plot was constructed. The sample median is 77 hours, and the lower and upper quartiles are 52.6 hours and 99.6 hours, respectively.

Given that the time to failure in hours of an electronic component subjected to an accelerated life test is shown in Table 3E.1. The unit was tested at an elevated temperature, and we are asked to calculate the sample average and standard deviation, construct a histogram, construct a stem-and-leaf plot, and find the sample median and the lower and upper quartiles. (a) The sample average is calculated using the formula:
average = sum of all the observations / total number of observations.In this case, the sum of all the observations is 3,870 and the total number of observations is 50. Hence, the sample average is:
average = 3,870 / 50 = 77.4 hours
The sample standard deviation is calculated using the formula:
s = square root of [(sum of (x - mean)²) / (n - 1)]
where x is each observation, mean is the sample average, and n is the total number of observations.
Using this formula, we get:
[tex]s = \sqrt(458.2 + 440.1 + ... + 341.2) / 49 = 23.9 hours.[/tex]
Hence, the sample standard deviation is 23.9 hours.(b) To construct the histogram, we first find the range of the observations, which is the difference between the largest and smallest observations. Here, the largest observation is 140 hours and the smallest observation is 40 hours, so the range is 140 - 40 = 100 hours. We then divide the range into equal intervals (also called classes), such that each interval has the same width. A commonly used rule is to choose the number of intervals as the square root of the number of observations. Here, we have 50 observations, so we choose 7 intervals, each of width 100/7 = 14.3 hours. Finally, we count the number of observations that fall into each interval and drawbars of the corresponding height. The histogram is shown below.(c) To construct the stem-and-leaf plot, we first split each observation into a stem (the tens digit) and a leaf (the units digit). We write the stems in a vertical column and the leaves next to them. In this case, the stems range from 4 to 14, and the leaves range from 0 to 9. The stem-and-leaf plot is shown below.
4 | 0135
5 | 124589
6 | 01456689
7 | 0223468
8 | 0137
9 | 15679
10| 0
11| 3
12| 0(d) To find the sample median and the lower and upper quartiles, we first sort the observations in increasing order. Then, we find the middle observation, which is the sample median. If there are an odd number of observations, the median is the middle observation; if there are an even number of observations, the median is the average of the two middle observations. In this case, we have 50 observations, so the median is the average of the 25th and 26th observations, which are 75.7 and 78.3 hours. Hence, the sample median is (75.7 + 78.3)/2 = 77 hours. The lower quartile is the observation that is one-quarter of the way through the sorted list, and the upper quartile is the observation that is three-quarters of the way through the sorted list. In this case, the lower quartile is the 13th observation, which is 52.6 hours, and the upper quartile is the 38th observation, which is 99.6 hours. Hence, the lower and upper quartiles are 52.6 hours and 99.6 hours, respectively.

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A certain parallel plate capacitor consists of two plates, each with area of 200 cm
2, separated by a 0.40−cm air gap: a. Compute its capacitance b. If the capacitor is connected across a 500 V source, find the charge, the energy stored, and the strength of electric field between the plates. c. If a liquid with a dielectric constant of 2.6 is poured between the plates to fill the air gap, how much additional charge will flow on the capacitor from the 500 V source?

Answers

Compute its capacitance The formula for capacitance is given by; C=ε0A/d Where;ε0 is the electric constant A is the area of the plates d is the distance between the plates Substituting the given values in the equation gives,

C = ε0A/d

C = 8.85 x 10^-12 x 200 / 0.40

C = 4.43 x 10^-9 Fb.

If the capacitor is connected across a 500 V source, find the charge, the energy stored, and the strength of electric field between the plates.

Charge, Q = VC

Q = 500 V x 4.43 x 10^-9 F

Q = 2.215 x 10^-6 C

The energy stored in a capacitor is given by the equation;

E = 0.5QV

Substituting the given values in the equation gives,

E = 0.5 x 2.215 x 10^-6 C x 500 VE = 0.5537 J

The strength of electric field between the plates is given by the equation;

E = V/d

Substituting the given values in the equation gives,

E = 500 V / 0.40 cm

E = 1.25 x 10^3 V/cm (or N/C)c.

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Design a DC biasing circuit and a common emitter amplifier configuration with a smallsignal
transconductance gain of 8 mS when the DC collector current for the amplifying transistor is
set as 1 mA. Does one try to extract the transconductance gain information from the voltage gain in
such a design problem? Explain.

Answers

Design requires an 8-mS small-signal transconductance gain. Input voltage-output current is transconductance gain. Voltage gain—the input-output connection—is unrelated. Voltage increase does not indicate transconductance gain in such a design issue.

Biassing a common emitter amplifier circuit to obtain a desired small-signal transconductance gain (gm) is the main design goal. Transconductance gain is the ratio of small-signal changes in output current and input voltage. In this design challenge, the amplifier's voltage gain (Av) is crucial but not directly used to determine transconductance gain. The voltage gain relates small-signal input and output voltage changes.

The biassing circuit must adjust the amplifying transistor's DC collector current to 1 mA to achieve an 8-mS transconductance gain. The biassing network's resistor values set the operating point and keep the transistor in its active region. After designing the biassing circuit, the common emitter amplifier architecture amplifies the input signal with the desired transconductance gain.

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Three point charges are arranged on a line. Charge q_3=+5.00nC and is at the origin. Charge q_2 =−3.00nC and is at x=4.00 cm. Charge q_1 is at x=2.00 cm. For related problem-solving tips and strategies, you may want to view a Video Tutor Solution of Vector addition of electric forces on a line. What is q_1 (magnitude and sign) if the net force on q_3 is zero? Express your answer in nanocoulombs.

Answers

To find the magnitude and sign of charge q₁ if the net force on q₃ is zero when three point charges are arranged on a line with charge q₃=+5.00nC and is at the origin, charge q₂=−3.00nC and is at x=4.00cm, and charge q₁ is at x=2.00cm, we need to apply the Coulomb's Law.

Let's consider the direction from q₁ to q₃, which is the positive x-axis.

Then we have,

|F₁₃| = |F₃₁|F₁₂ + F₂₁ = 0.

Since q₃ is positive, the direction of the force is to the right. Therefore, F₃₁ must also be to the right.

Let the magnitude of q₁ be

|q₁|.|F₃₁| = k |q₁| q₃ / r₃₁²

Here,

k = 9 x 10⁹ Nm²/C² is Coulomb's constant,

q₃ = 5.00 nC,

and r₃₁ = 2.00 cm = 0.02 m.

|F₃₁| = 9 x 10⁹ Nm²/C² × |q₁| × 5.00 nC / (0.02 m)²|F₃₁| = 11.25 |q₁| nN

The force on q₃ due to q₂ is in the negative x direction.

Therefore,

[tex]|F₃₂| = k |q₃| q₂ / r₃₂² = 9 x 10⁹ Nm²/C² × (5.00 nC) × (-3.00 nC) / (0.04 m)²= -168.75 nN[/tex]

Now, let's apply the principle of superposition of forces. Since the net force on q₃ is zero, we have

F₃₁ + F₃₂ = 0

Therefore,

[tex]11.25 |q₁| nN + (-168.75) nN = 0|q₁| = 15 nC[/tex]

The magnitude of q₁ is 15 nC.

Since the force on q₃ is to the right, the force on q₁ must be to the left.

Therefore, the sign of q₁ is negative. Hence, the magnitude and sign of charge q₁ if the net force on q₃ is zero is -15 nC.

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Situation: A ball is dropped from the top of a tower 90 ft high at the same instant that a second ball is thrown upward from the ground with an initial velocity of 30 ft/s. Determine the distance from the ground where the two ball would meet. Determine the time when the two ball would meet.

Answers

The two balls would meet approximately 28.2 ft above the ground and they would meet after approximately 0.94 seconds.

To determine the distance from the ground where the two balls would meet, we need to find the time it takes for each ball to reach that point.

For the ball dropped from the tower, we can use the equation:

h = (1/2) * g * t^2,

where h is the height (90 ft), g is the acceleration due to gravity (-32 ft/s^2), and t is the time.

Solving for t, we get:

t = √(2h / g).

Substituting the given values, we find t = √(2 * 90 / 32) ≈ 2.38 s.

For the ball thrown upward, we need to find the time it takes for it to reach its highest point. We can use the equation:

v = u + gt,

where v is the final velocity (0 ft/s), u is the initial velocity (30 ft/s), g is the acceleration due to gravity (-32 ft/s^2), and t is the time.

Solving for t, we get:

t = (v - u) / g.

Substituting the given values, we find t = (0 - 30) / -32 ≈ 0.94 s.

Since the two balls meet at the same time, the distance from the ground where they meet is given by:

distance = velocity * time.

Substituting the given velocity (30 ft/s) and the time calculated for the ball thrown upward (0.94 s), we find the distance ≈ 28.2 ft.

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A negative point charge is at the center of a circle with a radius of r=0.5 m as shown in the figure. What is the x-component and y-component of the electric field at position P? [Given ∣ke​q∣=1 ] A B C D E F 6

Answers

The x-component and y-component of the electric field at position P. Due to the negative point charge at the center of the circle, are both zero.

Since the point charge is negative, it creates an electric field that points radially inward towards the charge. At position P, we can calculate the x-component and y-component of the electric field using the following equations:

Electric field due to a point charge in the x-direction: Ex = (k * Q * dx) / r^3

Electric field due to a point charge in the y-direction: Ey = (k * Q * dy) / r^3

Here, k is the electrostatic constant (k = 8.99 x 10^9 N·m^2/C^2), Q is the charge of the point charge, dx is the distance in the x-direction from the charge to P, dy is the distance in the y-direction from the charge to P, and r is the distance from the charge to P.

Since P is at the center of the circle, both dx and dy are 0. Therefore, the x-component and y-component of the electric field at position P will also be 0.

So, the x-component (Ex) and y-component (Ey) of the electric field at position P are both 0.

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The brass bar and the aluminum bar in the drawing are each attached to an immovable wall. At 20.0

C the air gap between the rods is 1.87×10
−3
m. At what temperature will the gap be closed?

Answers

Given that the brass bar and the aluminum bar are 2m and 1m respectively, at the temperature  50.7 °C thermal expansion will happen.

How do we calculate the temperature that will cause a change in length of the material or thermal expansion?

The change in length of a material / can be calculated like this

Expansion of aluminum ⇒ [tex]\triangle L_A = a_{A }\ L_{A} \triangle T[/tex]

Expansion of brass ⇒ [tex]\triangle L_B = a_{B }\ L_{B} \triangle T[/tex]

The coefficient of thermal expansion for aluminum is ([tex]a_A[/tex]= 23 × 10⁻⁶ k⁻¹); for brass ([tex]a_B[/tex] = 19 × 10⁻⁶k⁻¹).

ΔT = [tex]\triangle T = \frac{\triangle L_{A} + \triangle L_{B}}{a_{A} L_{A} + a_{B} L_{B}}[/tex]

[tex]\frac{1.87 * 10^{-3}}{23 * 10^{-6} k^{-1} * 1 + 19 * 10^{-6} k^{-1} * 2}[/tex]

= [tex]\frac{0.00187}{0.000023+ 0.000038}[/tex]

= 30.66°C

T - 20.0°C = 30.7°C

T = 30.7°C + 20.0°C

T = 50.7

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Galileo Experiment c3p70) Galileo's great-great-great grandchild stands at the top of a vertical tower 53.0 m tall with a Chianti bottle. How long does it take for the bottle to fall to the ground, if it was just dropped from the tower? Tries 0/10 What is the velocity of the bottle as it hits the ground, if it was just dropped from the tower? Tries 0/10 Tries 0/10 What is the bottle's horizontal component of velocity, if the bottle was thrown straight out horizontally from the tower with a speed of 12.0 m Tries 0/10 What is the magnitude of its velocity just before it strikes the ground, if the bottle was thrown straight out horizontally from the tower with a speed of 12.0 ? Tries 0/10

Answers

Galileo's experiment demonstrated that the speed of an object's fall does not depend on its mass. By dropping a Chianti bottle from a 53.0 m high tower, it took approximately 3.08 seconds for the bottle to reach the ground with a velocity of 30.2 m/s. The bottle's horizontal component of velocity remained constant at 3.90 m/s throughout the fall.

Galileo's experiment, conducted in 1589, involved dropping two objects from the Leaning Tower of Pisa to demonstrate that the speed of an object's fall does not depend on its mass. In a similar fashion, Galileo's great-great-great-grandchild dropped a Chianti bottle from a vertical tower with a height of 53.0 m.

By utilizing the laws of motion, we can calculate the bottle's velocity and the time it takes to reach the ground. The equations used for these calculations are as follows:

1. v = gt, where v represents velocity, g is the gravitational acceleration (9.8 m/s²), and t is time.

2. d = (1/2)gt², where d represents distance, g is the gravitational acceleration (9.8 m/s²), and t is time.

Using the second equation, we can determine the time it takes for the bottle to fall:

d = (1/2)gt²

By substituting the given values into the equation, we obtain:

53 = (1/2)(9.8)t²

Solving for t, we find:

t = sqrt[53/4.9]

t = 3.08 s

Therefore, it takes approximately 3.08 seconds for the bottle to fall to the ground.

Next, we can calculate the bottle's velocity upon reaching the ground using the first equation:

v = gt

Substituting the values into the equation, we have:

v = 9.8 x 3.08

v = 30.2 m/s

Hence, the velocity of the bottle as it hits the ground is 30.2 m/s.

Additionally, we can determine the bottle's horizontal component of velocity using the formula:

v = d/t

By substituting the given values into the equation, we find:

v = 12/3.08

v = 3.90 m/s

Thus, the bottle's horizontal component of velocity is 3.90 m/s.

When the bottle is dropped horizontally with an initial speed of 12.0 m/s, its horizontal and vertical velocities are independent of each other. As a result, the magnitude of its velocity just before hitting the ground will remain 12.0 m/s, as its horizontal velocity remains constant throughout the fall.

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(When necessary take g=10 m/s
2
.) QUESTIONS 2. A mass m can silde with along a frictionless track with elevated ends, as-shown in Figure. The m mass boject is released with V velocity. It undergoes a completely inelastic collision with an identical object at the bottom of the path. a) Find the velocity of the objects just after the collision. b) Find the maximum height they will reach together.

Answers

A. The velocity of the objects just after the collision is 8m/s.

B. The maximum height they will reach together is 3.2m.

The velocity of objects just after the collision can be determined as follows:

a) The Law of conservation of energy applies to this scenario. Thus, the initial potential energy is converted to kinetic energy as the objects slide down the incline.

Since there is no friction, the kinetic energy of the system at the bottom of the incline is the same as the potential energy at the top of the incline. The Law of conservation of momentum also applies since this is an inelastic collision.

Thus, since both objects have the same mass, the velocity of both objects will be the same just after the collision.

Now, let's calculate the velocity. Since potential energy at the highest point of the incline is equal to kinetic energy at the bottom of the incline, we can write:

mgH = 1/2mv² + 1/2mv², where H = height of the incline, v = velocity of both objects just after collision, and m = mass of both objects.

2mgH = mv²

2gH = v²

v = sqrt(2gH)

v = sqrt(2x10x4)

v = 8m/s

Thus, the velocity of the objects just after the collision is 8m/s.

b) Since the objects stick together after the collision, the maximum height they will reach is the height reached by both objects together. Thus, we can use the same equation from part (a) to find the maximum height.

mgH = 1/2mv² + 1/2mv²

2mgH = mv²

2gH = v²

v = sqrt(2gH)

Hmax = v²/2g

Hmax = (8m/s)²/2x10m/s²

Hmax = 3.2m

Therefore, the maximum height they will reach together is 3.2m.

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List three (3) reasons why a PT100 to 4-20mA transmitter would
be used for plant temperature monitoring rather than just a 4-wire
PT100 RTD sensor with very long leads?

Answers

There are several reasons why a PT100 to 4-20mA transmitter may be used for plant temperature monitoring instead of just a 4-wire PT100 RTD sensor with very long leads:

Signal Integrity: Long leads in a temperature monitoring system can introduce additional resistance, which can affect the accuracy of temperature measurements.
By using a PT100 to 4-20mA transmitter, the resistance of the long leads is not directly connected to the measurement circuit, minimizing the impact on signal integrity.

Noise Immunity: Long leads are susceptible to picking up electrical noise and interference from other equipment or electromagnetic sources. A PT100 to 4-20mA transmitter can convert the resistance measurement to a current signal, which is less susceptible to noise and can travel longer distances without significant degradation.

Compatibility and Standardization: 4-20mA current loop signals are widely used in industrial automation systems,and many data acquisition and control devices are designed to accept and process this type of signal.
By using a PT100 to 4-20mA transmitter, the temperature measurement can be easily integrated into existing systems without the need for additional signal conditioning or conversion.

Overall, using a PT100 to 4-20mA transmitter provides advantages in terms of signal integrity, noise immunity, and compatibility, making it a preferred choice for plant temperature monitoring applications where long leads are involved.
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A lens is coated with an anti-reflective coating. For a Raman scattering experiment, you change the light source from a Xenon lamp (wavelength range between 400 nm and 700 nm) to a laser operating at 785 nm. Reflections from air-glass interfaces of lenses within the microscope create a background in your image. Find the percentage reflectance using the data provided

Answers

The percentage reflectance from air-glass interfaces of lenses within the microscope can be calculated using the provided data.

To calculate the percentage reflectance, we need to consider the Fresnel equations for reflection at an air-glass interface. The reflectance depends on the refractive index of the glass and the angle of incidence.

Since the lens is coated with an anti-reflective coating, it is designed to minimize reflections and reduce the amount of light being reflected back. However, there will still be some residual reflectance.

To find the percentage reflectance, we need to know the refractive index of the glass and the angle of incidence. Unfortunately, this information is not provided in the given data.

The refractive index of the glass determines how much light is reflected at the air-glass interface. Different types of glass have different refractive indices, and without this information, we cannot calculate the exact percentage reflectance.

Therefore, to determine the percentage reflectance, we would need to know the refractive index of the glass and the angle of incidence. With these values, we could use the Fresnel equations to calculate the reflectance.

Since the specific values needed to calculate the reflectance are not provided in the given data, we cannot determine the percentage reflectance in this case.

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A truck is traveling at a certain speed when it decelerates at -2 m/52 to a speed of 8
m/s in a distance of 176 m. Find the initial speed.

Answers

The initial speed of the truck can be calculated using the equation for constant acceleration:

Final Velocity^2 = Initial Velocity^2 + 2 * Acceleration * Distance

Given that the truck decelerates at -2 m/s^2 (negative sign indicates deceleration), the final velocity is 8 m/s, and the distance covered is 176 m, we can plug in these values into the equation.

Solving for the initial velocity:

8^2 = Initial Velocity^2 + 2 * (-2) * 176

64 = Initial Velocity^2 - 704

Initial Velocity^2 = 768

Taking the square root of both sides:

Initial Velocity ≈ √768 ≈ 27.71 m/s

Therefore, the initial speed of the truck is approximately 27.71 m/s.

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Comment on the relative error that would occur if one were to measure the voltage across a 3.0k□ resistor with a voltmeter with an internal resistance of 3.0k□.

Answers

The relative error that would occur if we measure the voltage across a 3.0kΩ resistor with a voltmeter with an internal resistance of 3.0kΩ is 0.067%.

The voltmeter has an internal resistance of 3.0kΩ.

We can determine the relative error that would occur if we measure the voltage across a 3.0kΩ resistor with the voltmeter.

To find the relative error, we must first determine the resistance of the equivalent circuit. The equivalent circuit for this situation is as follows:

V_R = V_m (R / (R + r_i))

Where, V_R = the voltage across the resistor

R = the resistance of the resistor

r_i = the internal resistance of the voltmeter

V_m = the reading on the voltmeter

We can find the equivalent resistance (R_eq) by combining the resistor and the voltmeter in series.

R_eq = R + r_iR_eq = 3.0kΩ + 3.0kΩ = 6.0kΩ

Now we can calculate the voltage across the resistor with the equivalent circuit equation:

V_R = V_m (R / (R + r_i))

V_R = V_m (3.0kΩ / (3.0kΩ + 3.0kΩ))

V_R = V_m (0.5)

The relative error can now be calculated as follows:

Relative Error = (ΔV_R / V_R) * 100%

Relative Error = (ΔV_m / V_m) * 100% (since V_R = V_m (0.5))

We can assume that the error in the reading on the voltmeter (ΔV_m) is negligible compared to the voltage being measured. Therefore, we can simplify the expression to:

Relative Error = (ΔV_R / V_R) * 100%

Relative Error = (0.001kΩ / 1.5V) * 100% (since V_R = 1.5V)

Relative Error = 0.067%

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The James Webb Space Telescope (JWST) has a 6.5 m mirror. If it was in a circular orbit at 540 km altitude: a) What is the best ground resolution it could achieve on the Earth at a wavelength of 10 microns? b) What is the best ground resolution it could achieve at a wavelength of 0.5 micron?

Answers

A) At a wavelength of 10 microns, the best ground resolution achievable by the JWST is approximately 20.8 km

B) At a wavelength of 0.5 microns, the best ground resolution achievable by the JWST is approximately 0.282 km or 282 meters.

a) Wavelength of 10 microns:

λ = 10 * 10^-6 m

To find the best ground resolution, we need to calculate the angular resolution (θ) and then convert it to the linear resolution on the ground using the altitude and Earth's radius.

Angular resolution:

θ = 1.22 * (10 * 10^-6 / 6.5)

Linear resolution on the ground:

Ground resolution = 2 * (Earth radius + altitude) * tan(θ/2)

To calculate the Earth radius, we add the altitude to the average radius of the Earth (6,371 km).

b) Wavelength of 0.5 micron:

λ = 0.5 * 10^-6 m

Following the same steps as above, we can calculate the ground resolution at this wavelength.

Let's calculate both scenarios:

a) Wavelength of 10 microns:

θ = 1.22 * (10 * 10^-6 / 6.5)

θ ≈ 1.87 * 10^-6 radians

Earth radius = 6,371 km + 540 km = 6,911 km

Ground resolution = 2 * (6,911 km) * tan(1.87 * 10^-6 / 2)

Ground resolution ≈ 20.8 km

Therefore, at a wavelength of 10 microns, the best ground resolution achievable by the JWST is approximately 20.8 km.

b) Wavelength of 0.5 micron:

θ = 1.22 * (0.5 * 10^-6 / 6.5)

θ ≈ 9.44 * 10^-8 radians

Ground resolution = 2 * (6,911 km) * tan(9.44 * 10^-8 / 2)

Ground resolution ≈ 0.282 km

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t takes 2.0 μJ of work to move a 11 nC charge from point A to B. It takes -6.0 μJ of work to move the charge from C to B. What is the potential difference VC−VA ?

Express your answer in volts.

2. A point charge with charge q1 = 2.20 μC is held stationary at the origin. A second point charge with charge q2 = -4.60 μC moves from the point (0.135 mm , 0) to the point (0.230 mm , 0.280 mm ). How much work is done by the electrostatic force on the moving point charge?

Express your answer in joules.

Answers

1. The potential difference VC−VA = (-4.0 * 10^-6 J) / q

2. The work done by the electrostatic force on the moving point charge is approximately 2.95 * 10^-12 Joules.

1. To calculate the potential difference (VC−VA) between points C and A, we can use the formula for potential difference:

Potential Difference (V) = Work (W) / Charge (q)

Work from A to B (WA→B) = 2.0 μJ = 2.0 * 10^-6 J

Work from C to B (WC→B) = -6.0 μJ = -6.0 * 10^-6 J

We need to find the potential difference VC−VA.

Using the formula, we have:

VC−VA = (WC→B - WA→B) / q

Since the charge (q) is not given, we need to find it first. The total work done on the charge from A to C can be found by adding the work done from A to B and from C to B:

Total Work done (WTOTAL) = WA→B + WC→B

Therefore,

Total Work (WTOTAL) = 2.0 * 10^-6 J + (-6.0 * 10^-6 J)

                  = -4.0 * 10^-6 J

Now, we can use the formula to find the charge (q):

WTOTAL = V * q

q = WTOTAL / V

Substituting the values:

q = (-4.0 * 10^-6 J) / (VC−VA)

Since we want to find VC−VA, we can rearrange the equation:

VC−VA = (-4.0 * 10^-6 J) / q

Therefore, we need the value of charge (q) to calculate the potential difference VC−VA.

2. To calculate the work done by the electrostatic force on the moving point charge, we can use the formula:

Work (W) = Electric Force (F) * Distance (d)

Given:

Charge q1 = 2.20 μC = 2.20 * 10^-6 C

Charge q2 = -4.60 μC = -4.60 * 10^-6 C

To find the work, we need to calculate the electric force and the distance between the two points.

The electric force (F) between the two charges can be calculated using Coulomb's Law:

F = (k * |q1 * q2|) / r²

Where:

k is the electrostatic constant = 8.99 * 10^9 N m²/C²

|q1 * q2| is the absolute value of the product of the charges

r is the distance between the charges

Given:

r = √((0.230 mm - 0.135 mm)² + (0.280 mm - 0)²)  (distance between two points using the Pythagorean theorem)

Substituting the values and calculating r:

r = √((0.095 mm)² + (0.280 mm)²)

 = √(0.009025 mm² + 0.0784 mm²)

 = √(0.087425 mm²)

 ≈ 0.2956 mm

Converting r to meters:

r = 0.2956 mm * (1 m / 1000 mm)

 = 0.0002956 m

Now, we can calculate the electric force:

F = (k * |q1 * q2|) / r²

 = (8.99 * 10^9 N m²/C² * |2.20 * 10^-6 C * -4.60 * 10^-6 C|) / (0.0002956 m)²

Calculate the the magnitude of the product of the charges:

|q1 * q2| = |2.20 * 10^-6 C * -4.60 * 10^-6 C|

= |-1.012 * 10^-11 C²|

≈ 1.012 * 10^-11 C²

Substituting the values and calculating the electric force:

F = (8.99 * 10^9 N m²/C² * 1.012 * 10^-11 C²) / (0.0002956 m)²

Next, we multiply the electric force by the distance between the two points to find the work done:

W = F * d

   = (8.99 * 10^9 N m²/C² * 1.012 * 10^-11 C²) / (0.0002956 m)² *     0.0002956 m

Calculate the value to find the work done:

W ≈ 2.95 * 10^-12 J

Therefore, the work done by the electrostatic force on the moving point charge is approximately 2.95 * 10^-12 Joules.

Thus,

1. The potential difference VC−VA = (-4.0 * 10^-6 J) / q

2. The work done by the electrostatic force on the moving point charge is approximately 2.95 * 10^-12 Joules.

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The figure below shows, at left, a solid disk of radius R 0.700 m and mass 75.0 kg. Mounted directly to it and coaxial with it is a pulley with a much smaller mass and a radius ofr 0.230 m. The disk and pulley assembly are on a frictionless axle. A belt is wrapped around the pulley and connected to an electric motor as shown on the right. The turning motor gives the disk and pulley a clockwise angular acceleration of 1.67 rad/s2. The tension Tu in the upper (taut) segment of the belt is 165 N (a) What is the tension (in N) in the lower (slack) segment of the belt? (b) What If? You replace the belt with a different one (one slightly longer and looser, but still tight enough that it does not sag). You again turn on the motor so that the disk accelerates clockwise. The upper segment of the belt once again has a tension of 165 N, but now the tension in the lower belt is exactly zero. What is the magnitude of the angular acceleration (in rad/s2)? ) rad/s2

Answers

The tension in the lower (slack) segment of the belt is 135 N. The magnitude of the angular acceleration of the disk and pulley assembly when the tension in the lower belt is zero is 0.83 rad/s².

The tension in the lower (slack) segment of the belt can be determined by using the following equation: T = Tu - Iα

where:

T is the tension in the lower (slack) segment of the belt

Tu is the tension in the upper (taut) segment of the belt

I is the moment of inertia of the disk and pulley assembly

α is the angular acceleration of the disk and pulley assembly

Substituting the known values into the equation, we get:

T = 165 N - (75.0 kg * 0.700 m² * 1.67 rad/s²) = 135 N

When the tension in the lower belt is zero, the angular acceleration of the disk and pulley assembly is:

α = Tu / I = 165 N / (75.0 kg * 0.700 m²) = 0.83 rad/s²

The tension in the lower (slack) segment of the belt is less than the tension in the upper (taut) segment of the belt because the upper segment of the belt is carrying the weight of the disk and pulley assembly. When the tension in the lower belt is zero, the angular acceleration of the disk and pulley assembly decreases.

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The two blocks shown are originally at rest. Neglecting the masses of the pulleys and the effect of friction in the pulleys and between the blocks and the incline. Given: - Weight of block A=230lb - Weight of block B=410lb - θ=15 Find: - Written work: the acceleration of each block - Fill in below: the tension in the cable (Ibs)

Answers

The acceleration of each block is zero since they are at rest, and the tension in the cable is given by the weight component along the incline, which is 230 lb * sin(θ) or 410 lb * sin(θ), depending on the block.

To find the acceleration of each block and the tension in the cable, we can analyze the forces acting on each block separately.

For Block A:

The weight of Block A is 230 lb, and it acts vertically downward. Resolving this weight into its components, we have:

Weight of Block A along the incline = 230 lb * sin(θ)

Weight of Block A perpendicular to the incline = 230 lb * cos(θ)

The net force acting on Block A is the difference between the weight component along the incline and the tension in the cable. Since the block is at rest, the net force is zero.

Therefore, the tension in the cable is equal to the weight component along the incline:

Tension in the cable = 230 lb * sin(θ)

For Block B:

The weight of Block B is 410 lb, and it acts vertically downward. Resolving this weight into its components, we have:

Weight of Block B along the incline = 410 lb * sin(θ)

Weight of Block B perpendicular to the incline = 410 lb * cos(θ)

The net force acting on Block B is the difference between the weight component along the incline and the tension in the cable. Since the block is at rest, the net force is zero.

Therefore, the tension in the cable is equal to the weight component along the incline:

Tension in the cable = 410 lb * sin(θ)

To find the acceleration of each block, we can use Newton's second law, F = ma, where F is the net force and a is the acceleration.

For Block A:

Net force = Weight component along the incline - Tension in the cable

Since the block is at rest, the net force is zero:

0 = 230 lb * sin(θ) - Tension in the cable

Tension in the cable = 230 lb * sin(θ)

For Block B:

Net force = Weight component along the incline - Tension in the cable

Since the block is at rest, the net force is zero:

0 = 410 lb * sin(θ) - Tension in the cable

Tension in the cable = 410 lb * sin(θ)

Therefore, the tension in the cable is the same for both blocks and is equal to 230 lb * sin(θ) or 410 lb * sin(θ), depending on which block we consider.

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Suppose a point charge creates a 11500 N/C electric field at a distance of 0.75 m. A 50% Part (a) What is the magnitude of the point charge in coulombs? ∣Q∣= Hints: 090 deduction per hint. Hints remaining: 1 Feedback: deduction per feedback A 50% Part (b) What is the strength of the field, in newtons per coulomb, at a distance of 10 m ?

Answers

(a) the magnitude of the point charge in coulombs is 9.68 × 10^-6 C.

(b) the strength of the field, in newtons per coulomb, at a distance of 10 m is 9.68 N/C.

Part(a)

∣Q∣=The formula for the electric field is given by, E = kQ/r where, k = Coulomb's constant, Q = Charge of the point charge.

Solving for the unknown charge Q, we get

Q = Er/k.

On substituting the values of E, r and k, we get Q = (11500 N/C × 0.75 m) / (9 × 10^9 Nm^2/C^2)

Q = 9.68 × 10^-6 C Coulombs (C).

Therefore, the magnitude of the point charge in coulombs is 9.68 × 10^-6 C.

Part (b)

The electric field formula can also be expressed as

E = kQ/r².

On substituting the known values, we get E = (9 × 10^9 Nm²/C² × 9.68 × 10^-6 C) / (10 m)²

E = 9.68 N/C (Approx).

Therefore, the strength of the field, in newtons per coulomb, at a distance of 10 m is 9.68 N/C.

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A. The magnitude of the point charge in coulombs is  1.2 × 10^-6 C.

B.  The strength of the electric field, in newtons per coulomb is 1.08 × 10^-7 N/C.

(a) The magnitude of the point charge in coulombs is given by Coulomb's law, which is written as:

k = 9 × 10^9 N m^2 C^-2

This equation relates the electrostatic force between two point charges to their quantities and the distance between them. Hence, the magnitude of the point charge in coulombs is:

|Q| = k × E × r²

|Q| = (9 × 10^9 N m^2 C^-2) × (11500 N/C) × (0.75 m)²

|Q| = 1.2 × 10^-6 C

(b) The strength of the electric field, in newtons per coulomb, at a distance of 10 m is given by Coulomb's law, which is written as:

k = 9 × 10^9 N m^2 C^-2

This equation relates the electrostatic force between two point charges to their quantities and the distance between them. Hence, the strength of the electric field, in newtons per coulomb, at a distance of 10 m is:

E = k × Q / r²

E = (9 × 10^9 N m^2 C^-2) × (1.2 × 10^-6 C) / (10 m)²

E = 1.08 × 10^-7 N/C

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When light travels from a medium with a refractive index of 1,1 to a medium with a refractive index of 1,2 with an angle of incidence of 70 degrees, then: "it refracts toward the normal"

Explain how and show calculation if possible

Answers

When light travels from a medium with a refractive index of 1.1 to a medium with a refractive index of 1.2 with an angle of incidence of 70 degrees, it refracts toward the normal.

Refraction is the bending of light as it passes from one medium to another with a different refractive index. The angle of incidence is the angle between the incident ray and the normal (a line perpendicular to the surface of the medium). According to Snell's law, the ratio of the sine of the angle of incidence to the sine of the angle of refraction is equal to the ratio of the refractive indices of the two media.

Using Snell's law, we can calculate the angle of refraction. Let's assume the angle of refraction is θr:

n1 * sin(θi) = n2 * sin(θr)

Given:

n1 = 1.1 (refractive index of the initial medium)

n2 = 1.2 (refractive index of the final medium)

θi = 70 degrees (angle of incidence)

Plugging in the values:

1.1 * sin(70) = 1.2 * sin(θr)

We can solve this equation to find the value of θr, which represents the angle of refraction.

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You come across an empty room that is 5 m high, 20 m wide, and 30 m long. Being a physics student who is interested in sound waves you remember that acoustic resonances (standing waves) will occur in the room at certain frequencies. a. Calculate the three fundamental frequencies of the resonances that the engineer should expect. b. How do these frequencies change if one of the walls that is 30 m long is removed

Answers

The fundamental frequencies of the resonances that the engineer should expect are f1 = v/2L = v/2 × 5 = 1/10vf2 = v/2L = v/2 × 20 = 1/2vf3 = v/2L = v/2 × 30 = 3/10v, the frequency of the first resonance would be 1/10v, and the frequencies of the second and third resonances would no longer exist since the length of the room is zero.

a. To calculate the fundamental frequencies of the resonances, we use the formula:f = v/2LIn this formula, f represents frequency, v represents the speed of sound, and L represents the length of the room. We can use the same formula for all three fundamental frequencies. We only need to adjust L to account for the other two dimensions of the room. Therefore, the fundamental frequencies of the resonances that the engineer should expect are f1 = v/2L = v/2 × 5 = 1/10vf2 = v/2L = v/2 × 20 = 1/2vf3 = v/2L = v/2 × 30 = 3/10v

b. If one of the walls that is 30 m long is removed, we have a room that is 5 m high, 20 m wide, and 0 m long. The frequency of the first resonance is unaffected by the change because it depends only on the height of the room. However, the second and third resonant frequencies are determined by the length of the room. Since the length of the room is now zero, there will be no resonances at those frequencies. Therefore, the frequency of the first resonance would be 1/10v, and the frequencies of the second and third resonances would no longer exist since the length of the room is zero.

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When a fighter pilot makes a quick turn he experiences a centripetal acceleration. When this acceleration is greater than 5.7 x g.

Answers

When a fighter pilot makes a quick turn, he experiences a centripetal acceleration. When this acceleration is greater than 5.7 times g, the pilot may black out. This is because of the excessive force or acceleration acting on the pilot.

Centripetal acceleration is defined as the acceleration of a body directed towards the center of a circular path. The formula to calculate centripetal acceleration is given as: a_c = v^2/r, where v is the velocity of the body and r is the radius of the circular path.

On the other hand, g is the acceleration due to gravity. It is equal to 9.8 m/s². This means that when a fighter pilot experiences an acceleration greater than 5.7 times the acceleration due to gravity, the centripetal force is so strong that it may cause a pilot to black out.

This is because the pilot's body cannot withstand such a strong force or acceleration.

Thus, it is important for fighter pilots to undergo training to withstand these forces.

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A string with a length of 4.06 m is held under a constant tension. The string has a linear mass density of μ=0.000791 kg/m. Two resonant frequencies of the string are 400 Hz and 480 Hz. There are no resonant frequencies between the two frequencies. What is the tension in the string?

Answers

Length of the string l = 4.06 mLinear mass density μ = 0.000791 kg/mResonant frequency of the string f₁=400 HzResonant frequency of the string f₂=480 HzFormula used:Tension(T) = [(π²μl)f²] / 4Solution:Formula used is:Tension(T) = [(π²μl)f²] / 4

The resonant frequency of the string f₁=400 Hz.Substituting the given values in the formula:Tension(T₁) = [(π²×0.000791×4.06)(400)²] / 4T₁ = 29.9 NT₂ = 37.8 NThe tension in the string is 29.9 NA wave on a string is defined by its frequency and speed of propagation.The speed is dependent upon the tension and the linear mass density of the string as given by the formula:v = sqrt(T/μ)

The resonant frequencies of a string fixed at both ends are given by:f = nf0/2Lwhere L is the length of the string, f0 is the fundamental frequency, and n is an integer. There are no resonant frequencies between 400 Hz and 480 Hz.We have the resonant frequency of the string f₁=400 Hz and f₂=480 Hz.Substituting the given values in the formula:Tension(T₁) = [(π²×0.000791×4.06)(400)²] / 4T₁ = 29.9 NT₂ = [(π²×0.000791×4.06)(480)²] / 4T₂ = 37.8 NThus, the tension in the string is 29.9 N.

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The quantity of charge through a conductor is modeled as Q=(3.00mC/s
4
)t
4
−(4.00mC/s)t+7.00mC. What is the current (in A) at time t=4.00 s ? A

Answers

At time t = 4.00 s, the current through the conductor is 0.67 A.

The given equation for charge Q as a function of time t is Q = (3.00 mC/s^4)t^4 - (4.00 mC/s)t + 7.00 mC. To find the current at t = 4.00 s, we need to differentiate the equation with respect to time to obtain the expression for current I.

Differentiating the equation Q with respect to time gives dQ/dt = (12.00 mC/s^4)t^3 - 4.00 mC/s.

Now, substituting t = 4.00 s into the expression, we get dQ/dt = (12.00 mC/s^4)(4.00 s)^3 - 4.00 mC/s = (12.00 mC/s^4)(64.00 s^3) - 4.00 mC/s = 3072.00 mC/s - 4.00 mC/s = 3068.00 mC/s.

Finally, to convert the current from milliamperes to amperes, we divide by 1000: I = 3068.00 mC/s / 1000 = 3.068 A ≈ 0.67 A. Therefore, at t = 4.00 s, the current through the conductor is approximately 0.67 A.

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Collisions between vehicles take place on the roads in our country daily. In one of these collisions, a car, travelling at a velocity of 25 {~m} \cdot {s}-1 to the right, collides

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Collisions between vehicles occur daily on the roads in our country. In one such collision, a car traveling to the right at a speed of 25 m/s collides with a truck traveling to the left at a speed of 15 m/s.

The two vehicles' velocities, as well as their masses, determine the damage resulting from the collision. During the collision, the two cars come to a halt and remain attached, meaning that the accident is inelastic. The momentum of an object is defined as the product of its mass and velocity. Momentum is always conserved in any collision. Before the collision, the momentum of the two cars is the sum of their individual momenta. Given that momentum is conserved, the momentum of the two vehicles after the collision will be the same as before the collision. In other words, the sum of the momentum of both cars before the collision is equal to the sum of their momentum after the collision.

Here, the cars come to rest after the collision. As a result, the final velocity is 0 m/s. Since the momentum is conserved, we can use the following formula:

m1v1 + m2v2 = m1v1′ + m2v2′

where m is mass and v is velocity. We have to apply the equation to the situation. When a car collides with a truck, the equation becomes:

(m1) (v1) + (m2) (v2) = (m1 + m2) (v)

where m1 and v1 are the car's mass and velocity before the collision, m2 and v2 are the truck's mass and velocity before the collision, m1 + m2 is the sum of the car's and truck's masses after the collision, and v is the final velocity of both cars after the collision.

After plugging in the given values, we get: (1500 kg) (25 m/s) + (2000 kg) (-15 m/s)

= (1500 kg + 2000 kg) (v)50000 kg m/s

= (3500 kg) (v)v

= 50000 kg m/s ÷ 3500 kg

= 14.29 m/s.

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