estimate of the energy (in joule) contained in a quart of soda.

The wavelength changes by a factor of 0.86, or 86%.

What is Wavelength?

Wavelength refers to the distance between two consecutive points on a wave that are in phase, or in other words, the distance between two similar points on a wave that are at the same point in their cycle. It is commonly denoted by the symbol "λ" (lambda) and is typically measured in meters (m) or other units of length.

If the wave speed decreases from c to 0.86c, we can use the formula for the wavelength of a wave to calculate the change in wavelength. The formula is:

λ' = λ * (v' / v)

where λ' is the new wavelength, λ is the original wavelength, v' is the new wave speed, and v is the original wave speed.

Plugging in the given values:

λ' = λ * (0.86c / c)

Simplifying:

λ' = λ * 0.86

The wavelength of a wave is inversely proportional to its wave speed, so if the wave speed decreases, the wavelength will also decrease.

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The driver produces a torque of 26.5 N-m while changing the flat tire using a tire iron 50.0 cm long and exerting a force of 53.0 N.

To calculate the torque produced by the driver when changing a flat tire using a tire iron 50.0 cm long and exerting a force of 53.0 N, you can follow these steps:

Step 1: Convert the length of the tire iron from centimeters to meters.
1 meter = 100 centimeters
50.0 cm = 50.0 / 100 = 0.5 meters

Step 2: Determine the angle between the force applied and the tire iron. Since the driver is applying the force perpendicularly to the tire iron, the angle is 90 degrees.

Step 3: Calculate the torque.
Torque (τ) = Force (F) × Distance (d) × sin(θ)
where θ is the angle between the force and the tire iron.

Step 4: Plug in the values.
τ = 53.0 N × 0.5 meters × sin(90°)

Step 5: Calculate sin(90°).
sin(90°) = 1

Step 6: Multiply the values.
τ = 53.0 N × 0.5 meters × 1
τ = 26.5 N-m

The driver produces a torque of 26.5 N-m while changing the flat tire using a tire iron 50.0 cm long and exerting a force of 53.0 N.

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The value of efficiency (η) in a DC motor can be calculated using the formula η = Pout / Pin, where τs is stall torque and ωn is no load speed.

To calculate the efficiency in a DC motor, follow these steps:

1. Determine the mechanical power output (Pout) by multiplying the stall torque (τs) by the no load speed (ωn) and dividing by 2: Pout = (τs × ωn) / 2

2. Measure the electrical power input (Pin) to the motor.

3. Calculate the efficiency (η) by dividing the mechanical power output (Pout) by the electrical power input (Pin): η = Pout / Pin

Efficiency indicates the ratio of useful mechanical power output to the electrical power input, and it is typically expressed as a percentage. A higher efficiency means the motor converts more electrical energy into mechanical energy, reducing energy waste.

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The rate of thermal energy dissipation in the battery can be found using the formula P = I² * r, where P is the power, I is the current (60 A), and r is the internal resistance (0.050 Ω). So, P = (60)² * 0.050 = 3600 * 0.050 = 180 W.  The potential difference will be V = emf + I * r = 12 + (60 * 0.050) = 12 + 3 = 15 V.    (a) The rate of thermal energy dissipation remains the same as in (b), which is 180 W

(a) The potential difference across the terminals can be found using Ohm's Law: V = emf - IR, where V is the potential difference, emf is the electromotive force of the battery, I is the current flowing through the battery, and R is the internal resistance of the battery. Plugging in the given values, we get V = 12 V - (60 A)(0.050 Ω) = 9 V.

(b) The rate at which thermal energy is being dissipated in the battery can be found using the formula: P = I^2R, where P is the power dissipated as thermal energy. Plugging in the given values, we get P = (60 A)^2(0.050 Ω) = 180 W.

(c) The rate at which electric energy is being converted to chemical energy can be found using the formula: P = VI, where P is the power used to charge the battery. Plugging in the given values, we get P = (12 V)(60 A) = 720 W.

(d) When the battery is used to supply 60 A to the starter motor, the potential difference across the terminals will be the same as in part (a), which is 9 V. The rate at which thermal energy is being dissipated in the battery can be found using the same formula as in part (b), since the internal resistance of the battery is the same. Plugging in the given values, we get P = (60 A)^2(0.050 Ω) = 180 W.

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Answer:

Option (c) is the correct answer.

Explanation: When two substances does not exchange any energy with each other then they are said to be in thermal equilibrium with each other. This means the temperature of both the substances will be equal, that is why, there is no exchange of energy between them. Thus, we can conclude that when the objects have the same temperature then you can tell the two objects are in thermal equilibrium.

The energy associated with the change of orientation of a free electron in a 3.84 T magnetic field is [tex]2.92 × 10^-24 J.[/tex]

The energy associated with flipping the orientation of a free electron in a magnetic field is given by [tex]ΔE = gμBΔmB[/tex] , where g is the electron's g-factor, μB is the Bohr magneton, Δm is the change in the electron's magnetic quantum number, and B is the magnetic field strength. For an electron flipping its orientation from parallel to anti-parallel in a 3.84 T magnetic field, [tex]Δm = 1 and g = 2.0023.[/tex]  Plugging in these values, we get [tex]ΔE = 2.92 × 10^-24 J.[/tex]

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The speed with which the particles enter the cyclotron is given by:

v = sqrt(2qV / mr).

In a cyclotron, the magnetic field B and the electric field E are perpendicular to each other and to the direction of motion of the particles. The magnetic field causes the particles to move in a circular path, while the electric field accelerates the particles between the two Dees.

The frequency of the electric field is adjusted so that it matches the frequency of the circular motion, causing the particles to gain energy with each pass through the Dees. This leads to an increase in the speed of the particles, which can be calculated using the following equation:

mv^2 / r = qvB

where m is the mass of the particle, v is its speed, r is the radius of the circular path, q is the charge of the particle, and B is the magnetic field.

The radius of the circular path can be expressed as:

r = mv / (qB)

Substituting this expression for r into the first equation, we get:

mv^2 / (mv / (qB)) = qvB

Simplifying and solving for v, we get:

v = sqrt(2qV / mr)

where V is the potential difference applied to accelerate the particles.

Therefore, the speed with which the particles enter the cyclotron is given by:

v = sqrt(2qV / mr)

Note that the speed of the particles will continue to increase as they pass through the Dees, until relativistic effects become significant. At that point, the frequency of the electric field must be adjusted in order to maintain resonance and continue accelerating the particles.

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The value of lo is -8.48 A, which is approximately equal to -8.5 A. Option c is correct.

To find the value of current,

I = V/Z

Where V is the voltage amplitude, Z is the impedance of the circuit, and I is the current amplitude.

Impedance (Z) of a series LCR circuit is given by,

Z = sqrt((R^2)+((wL)-(1/(wC)))^2)

Where R is the resistance, L is the inductance, C is the capacitance, w is the angular frequency (2pif), and f is the frequency of the sinusoidal voltage.

Substituting the given values,

w = 200 rad/s

R = 40 ohms

L = 160 mH = 0.16 H

C = 100 F = 0.0001 F

V = 40 V

Z = sqrt((40^2)+((2000.16)-(1/(2000.0001)))^2) = 50 ohms

Now, we can find the current amplitude as,

I = V/Z = 40/50 = 0.8 A

So, the current amplitude is 0.8 A.

Next, we need to find the phase angle (phi) between the voltage and current.

tan(phi) = ((wL)-(1/(wC)))/R

Substituting the given values,

tan(phi) = ((2000.16)-(1/(2000.0001)))/40 = 1.6

phi = tan^-1(1.6) = 57.99 degrees

So, the phase angle is 57.99 degrees.

Now, we can use the given equation for the current to find the value of lo,

1(t) = 10 sin(wt-phi)

At t=0, sin(wt-phi) = sin(-phi) = -sin(phi) = -0.848

So, 1(0) = 10*(-0.848) = -8.48 A

Therefore, the value of lo is -8.48 A, which is approximately equal to -8.5 A. Option c is correct.

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The rotation period of the asteroid

Period (in days) = Time between successive minima × 2 of light curve

To find the rotation period of the asteroid using the given information, you need to follow these steps:

1. Identify the time between successive minima in the light curve.
2. Multiply the time between successive minima by two.

The rotation period of the asteroid will then be calculated as follows:

Period (in days) = Time between successive minima × 2

Make sure to use the specific data from your light curve to plug into the formula, and you will get the rotation period of the asteroid in days.

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The largest resistance is [tex]759.0 ω (670+55+34)[/tex] , and the smallest resistance is[tex]19.7 ω (1/((1/34)+(1/55)+(1/670))).[/tex]

To obtain the largest resistance, you simply add all three resistors together. To obtain the smallest resistance, you need to use the formula for calculating resistors in parallel: [tex]1/R(total) = 1/R(1) + 1/R(2) + 1/R(3).[/tex] In this case,[tex]R(1) is 34.0 ω, R(2) is 55.0 ω, and R(3) is 670 ω.[/tex]  Plugging these values into the formula gives you[tex]1/R(total) = 0.0294[/tex] , which simplifies to [tex]R(total) = 34.0 Ω, 55.0 Ω, and 670 Ω.[/tex]

Note that the answer to this question assumes that the resistors are connected in parallel, as that is the only way to calculate the smallest resistance. If the resistors were connected in series, the smallest resistance would be 759.0 Ω and the largest resistance would be 759.0 Ω as well.

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In summary, the work needed to turn the generator is related to Lenz's Law because it involves overcoming the opposing force created by the induced EMF and current in the coil, as described by Lenz's Law.

The work needed to turn the generator is related to Lenz's Law through the following process:

1. A generator converts mechanical energy into electrical energy by rotating its coils within a magnetic field.
2. As the coil rotates, the magnetic field induces an electromotive force (EMF) and a current in the coil, according to Faraday's Law of electromagnetic induction.
3. Lenz's Law states that the induced EMF and current will generate a magnetic field that opposes the change in magnetic flux that produced it.
4. This opposition creates a force that resists the rotation of the generator's coils, which is called the "back EMF" or "counter EMF."
5. The work needed to turn the generator is directly related to overcoming this back EMF, as it is the force that opposes the rotation of the coils.

In summary, the work needed to turn the generator is related to Lenz's Law because it involves overcoming the opposing force created by the induced EMF and current in the coil, as described by Lenz's Law.

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The x-component of the 1 kg object's velocity just after the collision is 4.5 m/s.

To find the x-component of the 1 kg object's velocity just after the collision, we will use the conservation of momentum principle. Here's a step-by-step explanation:

1. Calculate the initial momentum of the 2 kg object:

p1_initial = m1 * v1_initial = 2 kg * 3 m/s = 6 kg*m/s.

2. Calculate the final momentum of the 2 kg object:

p1_final = m1 * v1_final = 2 kg * 1.5 m/s = 3 kg*m/s.

3. Find the x-component of the final momentum of the 2 kg object using the angle given:

p1_final_x = p1_final * cos(60°) = 3 kg*m/s * 0.5 = 1.5 kg*m/s.

4. Apply the conservation of momentum principle in the x-direction:

p1_initial_x = p1_final_x + p2_final_x.

Since the 1 kg object is initially at rest, its initial x-component of momentum is zero.

5. Calculate the x-component of the final momentum of the 1 kg object:

p2_final_x = p1_initial_x - p1_final_x = 6 kg*m/s - 1.5 kg*m/s = 4.5 kg*m/s.

6. Finally, find the x-component of the 1 kg object's velocity just after the collision:

v2_final_x = p2_final_x / m2 = 4.5 kg*m/s / 1 kg = 4.5 m/s.

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By following these , you can compute the maximum stress due to bending in the bar.

Apply the bending stress formula to find the maximum stress: σ = (M * c) / I.

To compute the maximum stress due to bending in the bar, we can follow these steps:

Identify the bending moment (M) at the point where maximum stress occurs. In this case, we have two forces acting on the bar: 840 N and 600 N. Since both forces are at equal distances from the ends (400 mm), the bending moment will be maximum at the center of the bar.

Calculate the bending moment (M) at the center of the bar. M = (840 N * 400 mm) - (600 N * 400 mm) = 96,000 Nmm.

Calculate the moment of inertia (I) for the bar's cross-sectional area. Since we're given a typical T-shaped cross-section, we can calculate I using the parallel axis theorem: I = I_center + A * d^2, where I_center is the moment of inertia of the individual rectangles about their own centroidal axes, A is the area of each rectangle, and d is the distance between the centroids of each rectangle and the centroid of the entire cross-section.

Compute the distance (c) from the neutral axis to the farthest point of the cross-section. In this case, c is half the height of the T-shape, which is 45 mm / 2 = 22.5 mm.

Apply the bending stress formula to find the maximum stress: σ = (M * c) / I.

By following these steps, you can compute the maximum stress due to bending in the bar.

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This statement is known as Pascal's Law, which states that any change in pressure applied to a confined fluid will be transmitted equally and uniformly in all directions throughout the fluid.

This means that if pressure is increased at one point in the fluid, it will be transmitted to all other points in the fluid. This is because fluids are considered incompressible, meaning that they cannot be easily compressed or squished together. Therefore, any change in pressure must be transmitted equally throughout the fluid.

This law has many practical applications in engineering, such as in hydraulic systems where pressure is used to move liquids or gases.

For example, in a car's braking system, applying pressure to the brake pedal increases pressure in the brake fluid, which is then transmitted uniformly throughout the brake lines to apply pressure to the brake pads, slowing the car down.

Understanding Pascal's Law is important for ensuring the proper function and safety of many mechanical systems.

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The value of t0.05t0.05 for a tt-distribution with 1616 degrees of freedom is  -1.645.

To find the value of t0.05t0.05 for a t-distribution with 1616 degrees of freedom, we need to look up the critical value in a t-distribution table or use a calculator.

Using a calculator, we can input the degrees of freedom (df) as 1616 and the confidence level (α) as 0.05. The formula to calculate the t-score is:

t = invT(α, df)

where invT is the inverse t-distribution function.

Plugging in the values, we get:

t = invT(0.05, 1616)

≈ -1.645

Therefore, the value of t0.05t0.05 for a t-distribution with 1616 degrees of freedom is -1.645 (rounded to three decimal places).

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The equation that expresses the tangent of the angle to the first dark fringe (θdark) in terms of the width of the central maximum (D) and the distance from the slit to the screen (L) is tan θdark = tan((D/2) / L).

To express tan θdark in terms of D and L, we can use the formula for the angular width of the central maximum in a single-slit diffraction pattern:

θdark = (D/2) / L

where θdark is the angle to the first dark fringe from the central maximum, D is the width of the central maximum, and L is the distance from the slit to the screen. We want to express tan θdark in terms of D and L, so we can rewrite the formula as:

tan θdark = tan((D/2) / L)

This equation expresses the tangent of the angle to the first dark fringe (θdark) in terms of the width of the central maximum (D) and the distance from the slit to the screen (L).

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The final temperature of air is approximately 198.6°C when it is expanded isentropically from 1000 kPa and 477°C to 100 kPa in a piston-cylinder device.

The final temperature when air is expanded isentropically from 1000 kPa and 477°C to 100 kPa in a piston-cylinder device can be determined using the ideal gas law and the isentropic process equation. The final temperature is approximately 198.6°C.

Initial pressure, P1 = 1000 kPa

Initial temperature, T1 = 477°C

Final pressure, P2 = 100 kPa

Assuming isentropic process, we have:

P1^(γ) / T1 = P2^(γ) / T2

where γ = Cp / Cv is the ratio of specific heats.

For air, Cp = 1.005 kJ/kgK and Cv = 0.718 kJ/kgK at room temperature.

Solving for T2, we get:

T2 = T1 * (P2 / P1)^(γ-1)

Substituting the given values, we get:

T2 = 477 + 273.15 * (100 / 1000)^(1.4-1)

T2 = 471.75 K or 198.6°C (approximately)

Therefore, the final temperature of air is approximately 198.6°C when it is expanded isentropically from 1000 kPa and 477°C to 100 kPa in a piston-cylinder device.

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The index of refraction for this material is 3.

What is Refractions?

Refraction is the bending of light as it passes through a medium such as air, water, or glass. This bending occurs because light travels at different speeds in different media, and when it enters a new medium at an angle, the change in speed causes the light to change direction

The index of refraction (n) of a material is defined as the ratio of the speed of light in a vacuum (c) to the speed of light in the material (v):

n = c/v

If light travels one-third as fast in the material as it does in a vacuum, then the speed of light in the material (v) is:

v = (1/3)c

Substituting this into the equation for the index of refraction:

n = c/v = c/((1/3)c) = 3

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a) The maximum magnitude of the electric field in the electromagnetic wave is 1.66 × 10^3 V/m.

b) The peak intensity of the wave is 1.86 × 10^-5 W/m^2 and the average intensity of the wave cannot be determined without additional information.

a) The relationship between the maximum magnitude of the magnetic field (B) and the maximum magnitude of the electric field (E) in an electromagnetic wave is given by E/B = c, where c is the speed of light in a vacuum. Solving for E, we get E = B × c = 499 μT × 3 × 10^8 m/s = 1.66 × 10^3 V/m.

b) The peak intensity of an electromagnetic wave is given by I = (cε0/2) × E^2, where ε0 is the permittivity of free space. Plugging in the given values, we get I = (3 × 10^8 m/s × 8.85 × 10^-12 F/m) / 2 × (374 × 10^-6 T)^2 = 1.86 × 10^-5 W/m^2. The average intensity of the wave cannot be determined without additional information.

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Rounding to two significant figures and including the appropriate units, we get: v = 32 m/s

(a) The top of the slope, Sam has only potential energy, which is given by: Ep = mgh

m is his mass, g is the acceleration due to gravity, and h is the height of the slope. Substituting the given values, we get:

Ep = [tex](70 kg)(9.81 m/s^2)(52 m)[/tex]= 35,938.4 J

At the bottom of the slope, all of Sam's potential energy is converted into kinetic energy, which is given by:

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

where v is his speed. Equating Ep and Ek, we get:

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

Simplifying and solving for v, we get:

v = √(2gh)

Substituting the given values, we get:

v = [tex]\sqrt{(2(9.81 m/s^2)(52 m)) } = 32.2 m/s}[/tex]

The headwind does not affect Sam's potential energy or the work done by gravity, so we can ignore it in this calculation.

(b) Rounding to two significant figures and including the appropriate units, we get: v = 32 m/s

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The most severe flight hazard caused by wingtip vortices of the greatest strength in a large jet airplane typically occurs during low-speed, high-angle of attack conditions, such as during takeoff and landing.

In these situations, the airplane generates a large amount of lift, which in turn produces strong wingtip vortices, potentially posing a risk to nearby aircraft.
One of the key factors that determines the strength of wingtip vortices is the weight of the aircraft. Heavier planes tend to create stronger vortices, which can be particularly hazardous during takeoff and landing when other aircraft may be in close proximity.
Another important factor is the speed of the aircraft. When planes are flying at low speeds, such as during takeoff or landing, the vortices tend to be more intense and longer-lasting than at higher speeds.
Finally, weather conditions can also play a role in the severity of wingtip vortices.

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The speed of the 300 g block is 5.57 m/s, and the tension in the 56.0 cm-long string is 16.6 N

To find the speed of the 300 g block and the tension in the 56.0 cm-long string, we can follow these steps:
Step 1: Convert the given values to SI units
Mass (m) = 300 g = 0.3 kg
Length of the string (L) = 56.0 cm = 0.56 m
Angular velocity (ω) = 95.0 rpm = 95 × (2π/60) rad/s = 9.95 rad/s
Step 2: Calculate the linear speed (v) of the block
Use the formula v = ω × r, where r is the radius of the circle (equal to the length of the string)
v = 9.95 rad/s ×0.56 m = 5.57 m/s
Step 3: Calculate the tension (T) in the string
Use the formula T = m ×r × ω²
T = 0.3 kg ×0.56 m × (9.95 rad/s)² = 16.6 N
The speed of the 300 g block is 5.57 m/s, and the tension in the 56.0 cm-long string is 16.6 N.

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The amount of axial compression load may be placed on a short timber post is 445,086.4 N.

To calculate the axial compression load that can be placed on a short timber post, you can use the formula:

Axial compression load = Cross-sectional area x Allowable unit compressive stress

First, determine the cross-sectional area of the post:

Cross-sectional area = width x height = 242 mm x 242 mm = 58,564 mm²

Next, multiply the cross-sectional area by the allowable unit compressive stress:

Axial compression load = 58,564 mm² x 7.6 N/mm² = 445,086.4 N

Therefore, the axial compression load that may be placed on the short timber post is 445,086.4 N.

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The angular speed at the time t/2 is half of the angular speed at time t.

Calculation of the angular speed:

1: If the angular speed of the object is ω after the time t, its angular displacement can be calculated as θ = ωt. Therefore, at the time t/2, the angular displacement would be θ/2 = (ωt)/2 = (1/2)ωt.

Step 2: The formula for angular velocity, which is given by ω = Δθ/Δt, where Δθ is the change in angular displacement and Δt is the change in time
ω = Δθ/Δt
ω = [(1/2)ωt - 0]/[t/2 - 0]
ω = (1/2)ωt / (t/2)
ω = (1/2)ω
Hence, the angular speed at the time t/2 is half of the angular speed at time t.

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If you lift a 5.0 kg box straight up while maintaining a steady speed, you will move it 2.0 displacements. The box has undergone a total of 49.05 Joules of labour.

The force applied to the box is equal to its weight, which is given by:

F = mg

W = Fd cosθ = (mg)(d)(cos 0°)

Since the box is lifted straight up, the angle between the force and the displacement is 0°, so cos 0° = 1.

Substituting the values, we get:

[tex]W = (5 kg)(9.81 m/s^2)(1 m)(1)[/tex]= 49.05 J

Displacement refers to the movement of an object or person from one position to another. This can be a change in location, direction, or orientation. Displacements can occur in many different contexts, such as in physics, geography, or social situations. In physics, displacement is often used to describe the distance and direction of an object's movement from its starting point.

In geography, displacement is often used to describe the forced movement of people from their homes or communities due to conflict, natural disasters, or other factors. This can have significant impacts on the lives and well-being of those affected. In social situations, displacement can refer to the transfer of emotions or behaviors from one situation to another.

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Complete Question:-

If you lift a box f mass 5kg straight up at constant speed through a displacement of 1 m, the total work done on the box is?

The temperature range over which a nichrome wire resistor can be used without changing its resistance by more than 1.00Ω from its value at 20°C depends on its TCR. The specific TCR of the wire needs to be known to determine the range.

The resistance of a conductor, such as a nichrome wire resistor, changes with temperature. The temperature coefficient of resistance (TCR) is a measure of this change, typically expressed in parts per million per degree Celsius (ppm/°C). A resistor made of nichrome wire is used in an application where its resistance must not change by more than 1.00Ω from its value at 20°C. The temperature range over which it can be used without exceeding this limit depends on the TCR of the wire. The specific TCR of the wire needs to be known to calculate the temperature range. For example, if the TCR of the wire is 500 ppm/°C, the temperature range over which it can be used without exceeding the 1.00Ω limit would be approximately 40°C.

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Energy : 3.99keV and Number of photons : 6.47 * 10^9.

We can use the equation E = hc/λ

λ = 0.0305 nm = 0.0305 x 10^-9 m

E = hc/λ = (6.626 x 10^-34 J s)(2.998 x 10^8 m/s)/(0.0305 x 10^-9 m) = 6.41 x 10^-16 J

1 eV = 1.602 x 10^-19 J

E = 6.41 x 10^-16 J x (1 eV/1.602 x 10^-19 J) = 3.99 keV

Therefore, the energy of a single photon of these x-rays is 3.99 keV.

To determine the number of photons absorbed during the dental x-ray, we can use the formula:

number of photons = energy of x-ray / energy of a single photon

4.15 μJ = 4.15 x 10^-6 J

number of photons = 4.15 x 10^-6 J / 6.41 x 10^-16 J = 6.47 x 10^9 photons

Therefore, about 6.47 x 10^9 photons are absorbed during the dental x-ray.

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Since V1/V2 is greater than 1, it indicates that the initial volume (V1) is smaller than the final volume (V2). Therefore, the picture that best represents the balloon when the pressure is changed to 1270 mm Hg at constant temperature would show a larger balloon compared to its initial size.

Plugging in the values, we get V1/V2=1270/750, which means that the final volume of the balloon is smaller than the initial volume. Therefore, the best picture that represents the balloon if the pressure is changed to 1270 mm Hg at constant temperature is a picture of a smaller balloon, as the volume of the balloon has decreased.
In order to determine which picture best represents the balloon when the pressure is changed to 1270 mm Hg at constant temperature, we need to consider the relationship between pressure and volume. According to Boyle's Law, at constant temperature, the pressure of a gas is inversely proportional to its volume. Mathematically, this is represented as P1V1 = P2V2.

In this case, the initial pressure (P1) is 750 mm Hg, and the final pressure (P2) is 1270 mm Hg. To compare the volumes, we can use the ratio:
V1/V2 = P2/P1 = 1270/750
V1/V2 ≈ 1.69

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Let the mass of piece B be m, then the mass of piece A is 3m.

Let the initial kinetic energy of the system be zero, and the final kinetic energy of the two pieces be KE_A and KE_B respectively.

The total kinetic energy of the two pieces is given by:

[tex]KE = (1/2) * m * v_B^2 + (1/2) * 3m * v_A^2[/tex]

where v_A and v_B are the velocities of pieces A and B respectively.

From the conservation of momentum, we have:

[tex]m * v_B + 3m * v_A[/tex] = 0

or

[tex]v_A = -(1/3) * v_B[/tex]

Substituting this expression into the equation for KE, we get:

[tex]KE = (1/2) * m * v_B^2 + (1/2) * 3m * (-v_B/3)^2[/tex]

Simplifying, we get:

[tex]KE = (7/18) * m * v_B^2[/tex]

From the given information, 90% of the released energy goes into kinetic energy, so:

[tex](7/18) * m * v_B^2 = 0.9 * 5600 J[/tex]

Solving for v_B, we get:

[tex]v_B = sqrt[(0.9 * 5600 J * 18)/(7 * m)] = 11.88 m/s[/tex]

Substituting this value of v_B into the expression for v_A, we get:

[tex]v_A = -(1/3) * v_B = -3.96 m/s[/tex]

Therefore, the final kinetic energy of piece A is:

[tex]KE_A = (1/2) * 3m * v_A^2 = 23[/tex]

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The probe's Mach number of its initial speed is 15,000 km/h is 94.7.

To calculate the probe's Mach number when its initial speed is 15,000 km/h and the speed of sound on the planet is 44 m/s, we first need to convert the probe's speed to meters per second (m/s).

1 km/h = 1000 m / 3600 s

15,000 km/h = 15,000 * (1000/3600) m/s

= 4166.67 m/s

Now we can find the Mach number:

Mach number = Probe's speed / Speed of sound

Mach number = 4166.67 m/s / 44 m/s

= 94.7

So, the probe's Mach number is 94.7 when its initial speed is 15,000 km/h in the thin atmosphere of the planet where the speed of sound is 44 m/s.

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