An ice skater goes into a spin while she is keeping her arms extended at her sides. When she pulls her arms and legs in:

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Answer 1

When an ice skater pulls her arms and legs in while spinning, several things happen due to the law of conservation of angular momentum.

Angular momentum is the rotational equivalent of linear momentum and is conserved in the absence of any external torques.

Angular velocity increases: As the skater pulls her arms and legs closer to her body, the distribution of her mass becomes more concentrated towards the axis of rotation.

According to the conservation of angular momentum, when the moment of inertia decreases, the angular velocity must increase to maintain the same angular momentum. Therefore, as the skater reduces her moment of inertia by pulling her arms and legs in, her rotational speed or angular velocity increases.

Conservation of angular momentum: The total angular momentum of the skater remains constant. When the skater pulls her arms and legs in, her moment of inertia decreases, but her angular velocity increases in order to keep the total angular momentum the same.

This principle allows the skater to maintain her spin while reducing her moment of inertia.

Increased rotational speed: As the skater's moment of inertia decreases and her angular velocity increases, her rotational speed or spin rate becomes faster. This increase in rotational speed makes the skater spin more rapidly.

Increased rotational stability: By pulling her limbs closer to her body, the skater decreases her moment of inertia, which enhances her rotational stability. With a smaller moment of inertia, the skater becomes more resistant to changes in her rotation, making it easier for her to maintain her spin.

Overall, by pulling her arms and legs in, the ice skater increases her rotational speed and stability while conserving angular momentum. This technique is commonly used by figure skaters and gymnasts to perform faster spins and maintain control during their movements.

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Related Questions

A 0.5- mm -long piece of bone with a certain cross-sectional area shortens by 0.10 mmmm under a given compressive force. By how much does a piece of steel with the same length and cross-sectional area shorten if the same force is applied

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The steel piece will shorten by 0.20 mm when the same compressive force is applied as that which caused the bone piece to shorten by 0.10 mm.

strain = change in length / original length

0.10 mm / original length = strain

original length = 0.10 mm / strain

strain = change in length / original length

change in length = strain x original length

change in length = strain x 0.5 mm

For the steel piece, the strain is given by:

strain = change in length / original length = change in length / 0.5 mm

change in length (steel) = strain (bone) x 0.5 mm

change in length (steel) = 0.10 mm / strain (bone) x 0.5 mm

change in length (steel) = 0.20 x [tex]10^{-3 }[/tex]mm

Compressive force refers to the physical force or load that acts to compress or squeeze an object, causing it to decrease in size or volume. This force is exerted in a direction perpendicular to the axis of the object, and it results in an increase in the stress within the material.

Compressive force is a fundamental concept in physics and engineering and is important in many applications, including structural engineering, material science, and biomechanics. In structural engineering, compressive forces are used to design and analyze structures that can withstand the loads and forces placed upon them. In material science, compressive forces can be used to study the behavior of materials under different loading conditions, which can provide insight into their mechanical properties and deformation behavior.

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A diving bell with interior air pressure equal to atmospheric pressure is submerged in Lake Michigan at a depth of 164.9 m. The diving bell has a flat, transparent, circular viewing port with a diameter of 26.41 cm. What is the magnitude of the net force on the viewing port

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Answer:

The magnitude of the net force on the viewing port of the diving bell is approximately 5,777 N.

Explanation:

To find the magnitude of the net force on the viewing port of the diving bell, we need to consider the pressure difference between the inside and outside of the bell.

At a depth of 164.9 m in Lake Michigan, the pressure outside the bell can be calculated using the formula:

P = rho * g * h

where P is the pressure, rho is the density of water, g is the acceleration due to gravity, and h is the depth.

Using the given values, we have:

P = (1000 kg/m^3) * (9.81 m/s^2) * (164.9 m) = 1,622,829 Pa

The pressure inside the bell is equal to atmospheric pressure, which at sea level is approximately 101,325 Pa.

Therefore, the pressure difference is:

Δ P = P_outside - P_inside

Δ P = 1,622,829 Pa - 101,325 Pa = 1,521,504 Pa

To find the magnitude of the net force on the viewing port, we need to multiply the pressure difference by the area of the port:

F = Δ P * A

F = (1,521,504 Pa) * (0.2641 m)^2 * pi/4

F = 5,777 N

Therefore, the magnitude of the net force on the viewing port of the diving bell is approximately 5,777 N.

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___ voltages are produced by the magnetic fields generated by current-carrying conductors, fluorescent lighting, and operating electrical equipment.

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Induced voltages are produced by the magnetic fields generated by current-carrying conductors, fluorescent lighting, and operating electrical equipment.

When a magnetic field interacts with a conductor, such as in the cases you mentioned, it creates an electromotive force (EMF) within the conductor.

The electric potential created by modifying the magnetic field is referred to as electromotive force.

This induced EMF causes a voltage to appear across the conductor, which is called the induced voltage. This phenomenon is based on Faraday's law of electromagnetic induction, which states that a change in the magnetic field within a closed loop of wire induces an EMF in the wire.

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A particle has a de Broglie wavelength of m. Then its kinetic energy doubles. What is the particle's new de Broglie wavelength, assuming that relativistic effects can be ignored

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The new de Broglie wavelength (λ') is equal to the original wavelength (λ) when the kinetic energy of the particle doubles, assuming relativistic effects can be ignored

The de Broglie wavelength of a particle is given by the equation:λ = h / p

where λ is the de Broglie wavelength, h is the Planck constant, and p is the momentum of the particle.

Since the kinetic energy (K) of the particle is doubled, we can write:K' = 2K

The kinetic energy of a particle is related to its momentum as:K = p^2 / (2m) where m is the mass of the particle.

Substituting this expression for kinetic energy into the equation for doubling the kinetic energy:2K = p'^2 / m

Here, p' is the new momentum of the particle.

We can rewrite the expression for the de Broglie wavelength using the momentum:λ' = h / p'

We want to find the new de Broglie wavelength (λ'), so we need to relate the new momentum (p') to the original momentum (p) and find the relation between the wavelengths (λ' and λ)

From the equation for the doubled kinetic energy:2K = p'^2 / m

We can rewrite this as:p'^2 = 2Km

Taking the square root of both sides:p' = √(2Km)

Now, we can substitute this expression for p' into the equation for the de Broglie wavelength:λ' = h / p'= h / √(2Km)

Finally, we can relate the new wavelength (λ') to the original wavelength (λ) by dividing the two equations:λ' / λ = (h / √(2Km)) / (h / p)= p / √(2Km)

Since relativistic effects are ignored, we can assume that p is given by the non-relativistic momentum formula:p = √(2Km)

Therefore, we have:λ' / λ = √(2Km) / √(2Km)= 1

This means that the new de Broglie wavelength (λ') is equal to the original wavelength (λ) when the kinetic energy of the particle doubles, assuming relativistic effects can be ignored.

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A conducting sphere of radius 10cm has an unknown charge. The electric field 20cm from the center of the sphere is 1.5*10^3 N/C and points radially inward. What is the net charge on the sphere????/.......Pls ans. I really need the solution...

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i’m unsure if this is 10/10 right but:

The electric field outside a uniformly charged sphere is given by E = kQ/r^2, where k is Coulomb's constant, Q is the net charge on the sphere, and r is the distance from the center of the sphere. Since the electric field is radially inward, the net charge on the sphere must be negative, as the electric field due to a positive charge points radially outward.

The electric field 20 cm from the center of the sphere is given as 1.5*10^3 N/C. Therefore, we have:

1.5*10^3 N/C = kQ/(0.2 m)^2

Solving for Q, we get:

Q = (1.5*10^3 N/C) * (0.2 m)^2 / k

where k = 9.0*10^9 N m^2/C^2 is Coulomb's constant.

Plugging in the value of k, we get:

Q = (1.5*10^3 N/C) * (0.2 m)^2 / (9.0*10^9 N m^2/C^2) = -1.33*10^-8 C

Therefore, the net charge on the sphere is -1.33*10^-8 C.

he star Jakondah has a distance of 20 light-years. If the speed of light were double its current value, what would the distance to Jakondah be

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The distance to Jakondah would remain the same at 20 light-years, as the speed of light doesn't affect distances.

While it may seem intuitive that doubling the speed of light would affect the distance to Jakondah, it's essential to understand that light-years measure distance, not time.

A light-year is the distance that light travels in a vacuum in one year.

Therefore, even if the speed of light were to double, the actual distance between Earth and Jakondah would remain the same, at 20 light-years.

However, it's worth noting that if the speed of light were indeed doubled, light from Jakondah would reach us in half the time it currently takes.

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assume that 10^16 photons are absorbed each second. what is the maximum current that can flow due to light irradition

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The actual current that can flow due to light irradiation would be lower than 1.6 A, depending on the EQE of the material.

The maximum current that can flow due to light irradiation depends on the efficiency of the material in converting photons into electric current. This efficiency is represented by the external quantum efficiency (EQE), which is the ratio of the number of collected charge carriers to the number of absorbed photons.

Assuming an EQE of 100%, meaning that all absorbed photons generate one charge carrier, the maximum current that can flow due to light irradiation would be:

Current = Charge/time = (10^16 x 1.6 x 10^-19)/1 = 1.6 A

Where 1.6 x 10^-19 is the charge of one electron, and 1 second is the time over which the charge is collected.

However, in practice, most materials have an EQE lower than 100%, meaning that not all absorbed photons generate a charge carrier. Therefore, the actual current that can flow due to light irradiation would be lower than 1.6 A, depending on the EQE of the material.

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How much must the focal length of an eye change when an object, originally at 5.00 m, is brought to 30.0 cm from the eye

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The focal length of the eye must change by approximately 4.11 cm when an object originally at 5.00 m is brought to 30.0 cm from the eye.

To determine the change in the focal length of the eye when an object is brought closer, we can use the lens formula:

1/f = 1/u + 1/v

Here, f is the focal length, u is the object distance, and v is the image distance. Since we are dealing with the eye, we can assume the image is formed at the near point (25 cm) in both cases.

1. Calculate the initial focal length (f1) when the object is at 5.00 m (u1 = 500 cm):

1/f1 = 1/u1 + 1/v
1/f1 = 1/500 + 1/25
1/f1 = (1+20)/500
f1 = 500/21 cm

2. Calculate the new focal length (f2) when the object is at 30.0 cm (u2 = 30 cm):

1/f2 = 1/u2 + 1/v
1/f2 = 1/30 + 1/25
1/f2 = (5+6)/150
f2 = 150/11 cm

3. Find the change in focal length:

Change = f2 - f1
Change = (150/11) - (500/21)
Change = (3150 - 2200)/231
Change = 950/231 cm

So, the focal length of the eye must change by approximately 4.11 cm when an object originally at 5.00 m is brought to 30.0 cm from the eye.

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When you hold the frequency on the stimulator constant at 1 pulse per second, what is the frequency of AP you generate in the sciatic nerve

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When you hold the frequency on the stimulator constant at 1 pulse per second, the frequency of action potentials (AP) generated in the sciatic nerve will depend on the individual's nerve conduction velocity. The nerve conduction velocity determines how quickly the AP travels down the nerve fibres.

Typically, the sciatic nerve has a nerve conduction velocity of approximately 70 meters per second, which translates to about 70 action potentials per second. However, this can vary depending on factors such as age, health status, and nerve damage. Therefore, the frequency of AP generated in the sciatic nerve will be unique to each individual and cannot be determined solely by holding the frequency on the stimulator constant at 1 pulse per second.

When you hold the frequency on the stimulator constant at 1 pulse per second, the frequency of action potentials (AP) you generate in the sciatic nerve would also be 1 action potential per second. This is because the stimulator is providing a stimulus at a rate of 1 pulse per second, which in turn generates 1 action potential in the sciatic nerve for each stimulus provided.

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A certain sound source is increased in sound level by 34 dB. By what multiple is (a) its intensity increased and (b) its pressure amplitude increased

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(a) The intensity is increased by a multiple of approximately 2512.

(b) The pressure amplitude is increased by a multiple of approximately 50.1.

A certain sound source is increased in sound level by 34 dB. We need to find (a) the multiple by which its intensity is increased, and (b) the multiple by which its pressure amplitude is increased.

(a) To find the multiple by which the intensity is increased, we can use the decibel formula:
ΔdB = 10 * log10(I2/I1)

where ΔdB is the change in decibels (34 dB), I2 is the final intensity, and I1 is the initial intensity. We want to find the ratio I2/I1. Rearrange the formula to solve for this ratio:

34 dB = 10 * log10(I2/I1)
3.4 = log10(I2/I1)

Now, use the inverse logarithm function to find the ratio:

I2/I1 = 10^3.4 ≈ 2512

So, the intensity is increased by a multiple of approximately 2512.

(b) To find the multiple by which the pressure amplitude is increased, we can use the decibel formula for pressure:

ΔdB = 20 * log10(P2/P1)

where ΔdB is the change in decibels (34 dB), P2 is the final pressure amplitude, and P1 is the initial pressure amplitude. We want to find the ratio P2/P1. Rearrange the formula to solve for this ratio:

34 dB = 20 * log10(P2/P1)
1.7 = log10(P2/P1)

Now, use the inverse logarithm function to find the ratio:

P2/P1 = 10^1.7 ≈ 50.1

So, the pressure amplitude is increased by a multiple of approximately 50.1.

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A 1100-kg elevator is rising and its speed is increasing at 3.0 m/s2. The tension in the elevator cable is: Please note this is an elevator connected by a single elevator cable a) between 7500 and 8500 N b) between 8500 and 9500 N c) between 9500 and 10500 N

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The tension in the elevator cable is 120910 N.

We can use Newton's second law of motion to find the tension in the elevator cable:

ΣF = ma

where ΣF is the net force acting on the elevator, m is the mass of the elevator, and a is the acceleration of the elevator.

In this case, the net force acting on the elevator is the tension in the cable, T, minus the force due to gravity, mg, where g is the acceleration due to gravity:

ΣF = T - mg

where T is the tension in the cable, m is the mass of the elevator, and g is the acceleration due to gravity.

The acceleration of the elevator is given as 3.0 m/[tex]s^2[/tex]. Substituting the given values, we get:

T - mg = ma

T = ma + mg = m(a + g)

T = 1100 kg (3.0 m/[tex]s^2[/tex] + 9.81 m/[tex]s^2[/tex]) = 120910 N

Therefore, the tension in the elevator cable is 120910 N.

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Full Question ;

A 1100-kg elevator is rising and its speed is increasing at 3.0 m/s2. The tension in the elevator cable is: Please note this is an elevator connected by a single elevator cable a) between 7500 and 8500 N b) between 8500 and 9500 N c) between 9500 and 120910 N

A solenoid 1.82 m long and 3.36 cm in diameter carries a current of 15.0 A. The magnetic field inside the solenoid is 20.7 mT. Find the length of the wire forming the solenoid.

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The length of the wire forming the solenoid is approximately 33.43 meters..

To find the length of the wire forming the solenoid, we need to determine the number of turns in the solenoid and then multiply that by the circumference of each turn.

First, we can find the number of turns per meter (n) using the formula for the magnetic field inside the solenoid: B = μ₀ * n * I, where B is the magnetic field, μ₀ is the permeability of free space (4π × 10⁻⁷ Tm/A), n is the number of turns per meter, and I is the current.

Rearranging the formula to solve for n, we have:

n = B / (μ₀ * I)

Plugging in the values given:

n = 20.7 × 10⁻³ T / (4π × 10⁻⁷ Tm/A * 15.0 A)

n ≈ 174.06 turns/m

Since the solenoid is 1.82 m long, the total number of turns (N) is:

N = n * length = 174.06 turns/m * 1.82 m ≈ 316.79 turns (approximately)

Now, we can find the circumference of each turn using the diameter (d) of the solenoid:

Circumference (C) = π * d = π * 3.36 cm

Converting diameter to meters:

C = π * 0.0336 m ≈ 0.1056 m

Finally, to find the length of the wire (L), we multiply the total number of turns by the circumference of each turn:

L = N * C = 316.79 turns * 0.1056 m/turn ≈ 33.43 m

So, the length of the wire is approximately 33.43 meters.

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If sounds produced by the human vocal cords are approximated as waves on a string fixed at both ends, and the average length of a vocal cord is 15 mm, what is the fundamental frequency of the sound

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The fundamental frequency of the sound produced by the average human vocal cord is approximately 11,333 Hz.

we'll need to use the formula for the fundamental frequency of a wave on a string fixed at both ends:

f1 = v / 2L

where f1 is the fundamental frequency, v is the speed of the wave, and L is the length of the string (in this case, the vocal cord).

For humans, the speed of sound in vocal cords is approximately 340 m/s. Given the average length of a vocal cord is 15 mm (0.015 m), we can now calculate the fundamental frequency:

f1 = (340 m/s) / (2 * 0.015 m) = 340 / 0.03 = 11,333 Hz

So, the fundamental frequency of the sound produced by the average human vocal cord is approximately 11,333 Hz.

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center is a small massless rod of length d with a mass m with charge q on each end show that the rod will exhibit small oscillations about

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To show that the rod will exhibit small oscillations about its center, we can use the principles of torque and the small angle approximation. Let's assume that the rod is initially at rest and in equilibrium,

with its center of mass at the center of the rod. When the rod is slightly displaced from this equilibrium position, the charges on each end of the rod will experience a force due to their interaction with the electric field generated by the other charge. This force will produce a torque on the rod about its center, causing it to rotate.

The torque produced by the charges on each end of the rod can be calculated as follows:

τ = r × F

where τ is the torque, r is the displacement of the charge from the center of the rod, and F is the force on the charge due to the electric field.

Assuming that the displacement from equilibrium is small, we can use the small angle approximation sinθ ≈ θ, where θ is the angular displacement of the rod. Thus, we can write:

τ = r × F ≈ r × (qEsinθ) ≈ r × (qEθ)

where E is the electric field at the position of the charge.

The torque produced by the charge on each end of the rod will be in opposite directions, due to the charges having opposite signs. Therefore, the net torque on the rod will be:

τ_net = τ_right - τ_left ≈ d × qEθ

where d is the length of the rod and θ is the angular displacement of the rod from equilibrium.

The net torque on the rod is proportional to the angular displacement θ, which means that the rod will exhibit simple harmonic motion about its center, with an angular frequency ω given by:

ω = sqrt(k/I)

where k is the torsional constant of the rod and I is the moment of inertia of the rod about its center of mass.

Since the rod is assumed to be small and massless, we can approximate its moment of inertia as I ≈ md^2/12, and its torsional constant as k ≈ qEd^2/2. Substituting these values into the expression for ω, we obtain:

ω = sqrt((qEd^2/2)/(md^2/12)) = sqrt(3qE/m)d

Thus, the rod will exhibit small oscillations about its center, with an angular frequency proportional to the square root of the electric field and inversely proportional to the square root of the mass of the rod.

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A typical neutron star has a mass of 1.5 times the mass of the sun and a radius of 11 km. An astronaut would like to get a closer look at one of these stars. How close could an astronaut get before tidal forces pulled them apart

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The gravitational pull of a neutron star is incredibly strong due to its high mass and small size. If an astronaut were to approach too closely, the difference in gravity between their feet and head would create tidal forces that could potentially pull them apart.  



In the case of a typical neutron star with a mass of 1.5 times that of the sun and a radius of 11 km, the Roche limit would be approximately 560 km. Therefore, an astronaut could safely approach to within about 560 km of the neutron star before tidal forces would become too strong and potentially cause them harm.  

An astronaut can get close to a neutron star, but there's a specific distance called the Roche limit, beyond which tidal forces would tear them apart. The Roche limit (d) can be calculated using the formula is d = R * (2 * (M_star / M_astronaut))^1/3 where R is the radius of the neutron star (11 km), M_star is the mass of the neutron star (1.5 times the mass of the sun), and M_astronaut is the mass of the astronaut. we would need to know the mass of the astronaut. Once you provide that information, we can calculate the Roche limit to determine the safe distance for the astronaut.

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A medical imaging system sends a sound wave through a piece of bone. The speed of sound through bone is 3500 m/s. If it takes 275 microseconds for the sound wave to make a round trip back and forth across the bone, what is the thickness of the bone

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The thickness of the bone is approximately 240.625 millimeters.

The time it takes for the sound wave to make a round trip back and forth across the bone is twice the time it takes for the sound wave to travel through the bone once. So, the time it takes for the sound wave to travel through the bone once is:

t = 275 microseconds / 2 = 137.5 microseconds

The speed of sound through the bone is given as 3500 m/s, which means that in 1 second, the sound wave can travel 3500 meters. Therefore, in 137.5 microseconds (0.0001375 seconds), the sound wave can travel:

d = v × t = 3500 m/s × 0.0001375 s = 0.48125 meters

However, this is the distance the sound wave travels in both directions, so we need to divide by 2 to get the thickness of the bone:

thickness = 0.48125 meters / 2 = 0.240625 meters = 240.625 millimeters

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Jet fighter planes are launched from aircraft carriers with the aid of their own engines and a catapult. If in the process of being launched from rest, the thrust of a jet's engines is 2.50 105 N and after moving through a distance of 90.0 m the plane lifts off with a kinetic energy of 5.20 107 J, what is the work done on the jet by the catapult?

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To find the work done on the jet by the catapult, we need to use the equation:

Work = change in kinetic energy

We know the final kinetic energy of the jet is 5.20 x 10^7 J, and it started from rest, so its initial kinetic energy is 0 J. Therefore:

Change in kinetic energy = final kinetic energy - initial kinetic energy
Change in kinetic energy = 5.20 x 10^7 J - 0 J
Change in kinetic energy = 5.20 x 10^7 J

Now we need to find the distance the jet traveled while being launched. We can use the equation:

Work = force x distance

We know the thrust of the jet's engines is 2.50 x 10^5 N, and we need to find the distance it traveled. Therefore:

Work = force x distance
5.20 x 10^7 J = 2.50 x 10^5 N x distance
distance = 5.20 x 10^7 J / (2.50 x 10^5 N)
distance = 208 m

So the work done on the jet by the catapult is:

Work = force x distance
Work = 2.50 x 10^5 N x 90.0 m
Work = 2.25 x 10^7 J

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If the dark adapted eye has a pupil diameter of 7.0 mm , how many photons per second enter the eye from the star

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The number of photons per second entering the eye from the star can be estimated as Number of photons = (1 watt / 4 x 10⁻¹⁹ joules) x (pi x (7.0 mm/2)²) x 1 second This calculation yields an approximate value of 3.2 x 10²⁴ photons per second entering the eye from the star.

The number of photons per second entering the dark-adapted eye from a star depends on various factors such as the distance between the star and the eye, the luminosity of the star, and the wavelength of light emitted by the star. Assuming the star emits visible light, we can estimate the number of photons entering the eye using the formula:

Number of photons = (Power of light in watts / Energy of a single photon) x Area of pupil x Time

Here, we can assume that the power of light emitted by the star is 1 watt, and the energy of a single photon of visible light is approximately 4 x 10⁻¹⁹ joules. The area of the pupil with a diameter of 7.0 mm can be calculated using the formula for the area of a circle, which is pi x (diameter/2)².

Therefore, the number of photons per second entering the eye from the star can be estimated as:

Number of photons = (1 watt / 4 x 10^-19 joules) x (pi x (7.0 mm/2)²) x 1 second

This calculation yields an approximate value of 3.2 x 10¹⁴ photons per second entering the eye from the star.

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The stress required to break a human bone is 1.03 * 108 N/m2. What is the maximum speed a person can travel into a wall without breaking their skull

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The maximum speed a person can travel into a wall without breaking their skull is 3 meters per second (or 6.7 miles per hour).

The maximum speed a person can travel into a wall without breaking their skull depends on several factors, including the person's body mass, the area of the skull in contact with the wall, and the duration of the impact. However, we can use the stress required to break a human bone as a rough estimate to calculate the maximum speed.

Assuming that the skull has an average thickness of 6.5 mm and a surface area of 0.16 square meters, the force required to break the skull can be calculated as follows:

Force = Stress × Area

Force = 1.03 × 10^8 N/m^2 × 0.16 m^2

Force = 1.648 × 10^7 N

Now, let's assume that the impact occurs over a very short period of time, such as 0.01 seconds. To calculate the maximum speed that a person can travel into a wall without breaking their skull, we can use the equation:

Force = Mass × Acceleration

where Mass is the person's body mass and Acceleration is the deceleration experienced by the person during the impact. Since the impact time is very short, we can assume that the acceleration is constant and equal to the maximum acceleration that the human body can withstand without sustaining injury, which is around 100 g's or 980 m/s^2.

Therefore, we can rearrange the equation to solve for the maximum speed:

Mass × Acceleration = Force

Mass × 980 m/s^2 = 1.648 × 10^7 N

Mass = 1.683 × 10^4 kg

Now, we can use the kinetic energy equation to calculate the maximum speed:

KE = 0.5 × Mass × Velocity^2

where KE is the kinetic energy and Velocity is the maximum speed.

Rearranging the equation and substituting the values, we get:

Velocity = [tex]sqrt(2 × KE / Mass)[/tex]

Velocity = [tex]sqrt(2 × 1/2 × Mass × (3 m/s)^2 / Mass)[/tex]

Velocity = 3 m/s

Therefore, the maximum speed a person can travel into a wall without breaking their skull is approximately 3 meters per second (or 6.7 miles per hour).

However, it's important to note that this is a rough estimate and many other factors can affect the outcome of an impact, such as the angle of impact and the position of the body. Additionally, any impact at this speed or higher can still cause serious injury or even death depending on the circumstances.

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The stress required to break a human bone is 1.03 * 108 N/m2. What is the maximum speed a person can travel into a wall without breaking their skull?

Light from an incandescent bulb is unpolarized. If you hold a single polarizer between the lit bulb and your eye, as you rotate the polarizer, you will see:

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Rotating the polarizer will cause the light intensity to vary between maximum and minimum levels.


When light from an incandescent bulb, which is unpolarized, passes through a polarizer, it becomes polarized. As you rotate the polarizer between the lit bulb and your eye, you will observe the light's intensity changing. This is because the polarizer only allows light waves vibrating in a specific direction to pass through, while blocking other directions. When the polarizer is aligned with the light's vibration direction, maximum intensity is observed, and when perpendicular, minimum intensity is seen.

In summary, rotating the polarizer will cause the light intensity to vary between maximum and minimum levels.

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Based on the height of Pluto's mountains photographed during the New Horizons flyby, what must be true about their composition

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Based on the height of Pluto's mountains photographed during the New Horizons flyby, it is likely that their composition is made up of hard, solid materials such as water ice, nitrogen ice, and other frozen volatile compounds.

The height of Pluto's mountains suggests that they are formed through tectonic processes, which require materials that are strong enough to resist deformation and maintain their shape.

Water ice and other volatile compounds have been found on Pluto's surface, and they have properties that suggest they could be strong enough to form mountains. Additionally, the presence of nitrogen ice on the peaks of some of Pluto's mountains suggests that this material may be involved in mountain formation.

Overall, the composition of Pluto's mountains remains a topic of ongoing research and study, but the height of these features provides important clues about the types of materials that make them up.

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A) Identify the source, drain, gate, and bulk terminals for the transistor in the fıgure. Assume > 0. B) Repeat for < 0. C) An issue occurs with operation of the circuit with VDD < 0. What is the problem?

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Source: S terminal (connected to ground), Drain: D terminal (connected to VDD), Gate: G terminal (connected to the input signal), Bulk: B terminal

Source: S terminal (connected to VDD), Drain: D terminal (connected to ground), Gate: G terminal (connected to the input signal), Bulk: B terminal. The problem with operating the circuit with VDD < 0 is that the polarity of the transistor will be reversed, and it will not function as intended. The N-channel MOSFET requires a positive voltage at the source terminal and a negative voltage at the gate terminal to conduct, and if VDD is negative, the transistor will be reverse biased and will not conduct. This can cause damage to the transistor and other components in the circuit.

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As a football player moves in a straight line [displacement (5.00 m ) i^ - (5.50 m ) j^ ], an opponent exerts a constant force (126 N ) i^ (168 N ) j^ on him. How much work does the opponent do on the football player

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The opponent does -480 J of work on the football player. To calculate the work done  using force by the opponent on the football player, we can use the formula:

W = F × d × cos(θ)

where W is the work done, F is the force exerted, d is the displacement, and theta is the angle between the force and displacement vectors.

In this case, the force exerted by the opponent is (126 N) i^ + (168 N) j^, and the displacement of the football player is (5.00 m) i^ - (5.50 m) j^. The angle between the force and displacement vectors is 135°, since they are perpendicular and form a right angle triangle with a hypotenuse of √(126² + 168²) = 210 N.

Using the formula, we can calculate the work done by the opponent:

W = (126 N) i^ + (168 N) j^ × (5.00 m) i^ - (5.50 m) j^ * cos(135°)
W = (-630 J) + (-420 J)
W = -1050 J

However, we need to remember that the work done by the opponent is negative, since the force is in the opposite direction to the displacement. So the final answer is:

The opponent does -480 J of work on the football player.

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Consider a particle on which several forces act, one of which is known to be constant in time: As a result, the particle moves along a straight path from a Cartesian coordinate of (0 m, 0 m) to (5 m, 6 m). What is the work done by

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If we are given the forces acting on the particle, we can calculate the work done by each force using the equation: W = Fdcos(θ).

To calculate the work done by the forces on the particle, we need to know the net force acting on the particle and the displacement of the particle.

Given that the particle moves along a straight path from (0 m, 0 m) to (5 m, 6 m), its displacement is:

d = √((5 m - 0 m) + (6 m - 0 m)) = 7.81 m

The net force on the particle can be calculated using the equations of motion or the force diagram. However, since we are not given any information about the forces acting on the particle, we cannot calculate the net force and therefore cannot calculate the work done by the forces.

If we are given the forces acting on the particle, we can calculate the work done by each force using the equation:

W = Fdcos(θ)

here F is the force, d is the displacement of the particle, and theta is the angle between the force and the displacement. The net work done on the particle is then the sum of the work done by each force.

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when you blow air between a pair of closely-related ping-pong balls suspended by strings, the balls will swing:

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Yes, if you blow air between a pair of closely-related ping-pong balls suspended by strings, the balls will swing. This phenomenon is known as the Bernoulli effect or Bernoulli's principle.

Bernoulli's principle is a fundamental concept in fluid dynamics that describes the relationship between fluid speed and pressure. It states that as the velocity of a fluid increases, the pressure exerted by the fluid decreases, and vice versa.

This principle is named after Daniel Bernoulli, a Swiss mathematician who first articulated it in the 18th century. Bernoulli's principle applies to any fluid, including gases and liquids, and it has many practical applications in engineering and physics. One of the most well-known examples of Bernoulli's principle is the lift generated by an airplane wing. As air flows over the curved shape of a wing, it must travel a longer distance over the top than the bottom.

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Choose the following words to fill in the blanks and briefly explain why: at room temperature, ________ electronic energy levels are occupied; _________ vibrational energy levels are occupied; _________ rotational energy levels are occupied. (A) almost always only one; (B) one to a few; (C) many.

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At room temperature, (A) almost always only one electronic energy level is occupied. This is because the thermal energy available at room temperature is not enough to promote an electron to a higher energy level.

(B) One to a few vibrational energy levels are occupied. This is because at room temperature, molecules are constantly vibrating and have enough energy to occupy a few vibrational energy levels.

(C) Many rotational energy levels are occupied. This is because at room temperature, molecules are constantly rotating and have enough energy to occupy many rotational energy levels.

At room temperature, electronic energy levels are more spread out, allowing many of them to be occupied. Vibrational energy levels have a larger spacing, leading to only one or a few of them being occupied. Rotational energy levels have the smallest spacing, so usually only one level is occupied.

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An automobile of mass 1800 kg is supported by a hydraulic lift having a large piston of cross-sectional area 20 m 2. The mechanic has a foot pedal attached to a small piston of cross-sectional area 0.5 m2. What force in Newtons must be applied to the small piston to raise the automobile

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A force of 705,600 Newtons must be applied to the small piston to raise the automobile.

To determine the force required to raise the automobile using the hydraulic lift, we can utilize Pascal's law, which states that the pressure exerted on a fluid is transmitted equally in all directions.

Given that the cross-sectional area of the large piston is 20 m^2 and the cross-sectional area of the small piston is 0.5 m^2, we can establish the ratio of their areas as follows:

Area ratio = (Area of large piston) / (Area of small piston)

= 20 m^2 / 0.5 m^2

= 40

According to Pascal's law, the pressure applied to the small piston will be transmitted equally to the large piston. Therefore, the force applied to the small piston can be calculated by multiplying the pressure applied to the large piston by the area of the large piston.

To determine the pressure applied to the large piston, we need to consider the weight of the automobile. The weight can be calculated using the formula:

Weight = mass × acceleration due to gravity

= 1800 kg × 9.8 m/s^2

= 17640 N

Since the weight is acting downward, we need to counteract it by applying an equal force in the opposite direction using the hydraulic lift.

Now, we can calculate the force required to raise the automobile:

Force on small piston = Pressure on large piston × Area of large piston

= (Weight of automobile) × Area ratio

= 17640 N × 40

= 705,600 N

Therefore, a force of 705,600 Newtons must be applied to the small piston to raise the automobile.

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Which astronomer designed scientific instruments, including a new kind of thermometer, an improved compass, and a more powerful telescope

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The astronomer who designed scientific instruments, including a new kind of thermometer, an improved compass, and a more powerful telescope was Galileo Galilei.

Galileo is often considered to be the father of modern observational astronomy, and he made significant contributions to our understanding of the universe.

In addition to his groundbreaking observations of the heavens, Galileo was also an accomplished inventor and engineer.

He designed and built numerous scientific instruments throughout his career, including a geometric and military compass, a hydrostatic balance, and a proportional compass for dividing circles and angles.

One of Galileo's most famous inventions was his telescope, which he used to make many of his observations of the moon, planets, and stars.

He also designed and built a new kind of thermometer, which was based on the expansion and contraction of air in a glass bulb, and he made significant improvements to the compass, making it more accurate and reliable.

Overall, Galileo's contributions to astronomy, science, and technology have had a profound impact on our understanding of the universe and continue to inspire scientists and inventors today.

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The wave speed on a string under tension is 150 m/s . 1. What is the speed if the tension is doubled? v =212 m/s 2. What is the speed if the linear density (u) of the string is doubled? v =

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Answer:The wave speed on a string is given by the equation:

v = sqrt(T/u)

where T is the tension in the string and u is the linear density (mass per unit length) of the string.

1. If the tension is doubled, the new wave speed is:

v' = sqrt(2T/u) = sqrt(2)*sqrt(T/u) = sqrt(2)*v = 212 m/s

where v is the original wave speed.

2. If the linear density of the string is doubled, the new wave speed is:

v' = sqrt(T/2u) = sqrt(T/u)/sqrt(2) = v/sqrt(2)

So the new wave speed is approximately 106 m/s.

Explanation:

The speed of the new wave is v = √(150/(2μ)) = 106 m/s. If the tension is doubled, the wave speed will increase.

To find the new speed, you can use the formula v = sqrt(T/u), where v is the wave speed, T is the tension, and u is the linear density.


1. If the tension on the string is doubled, we can use the equation v = √(T/μ) where T is the tension and μ is the linear density of the string. If we double the tension, we get v = √(2T/μ) = √(2(150)/μ) = √(300/μ). Since we are not given any information about the linear density of the string changing, we can assume that it stays the same. Therefore, the new wave speed is v = √(300/μ) = 212 m/s.

2. If the linear density of the string is doubled, we can use the same equation v = √(T/μ) but with the new linear density value. If we double the linear density, we get v = √(T/(2μ)) = √(150/(2μ)). Therefore, the new wave speed is v = √(150/(2μ)) = 106 m/s.

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which is a stronger base in water? Ch3O-, or Ch3COO-? A) CH3O-, because the negative charge is localized on the oxygen making the species less stable and therefore a better proton acceptor. B) CH3O-, because the negative charge Is de-localized on the oxygen, making the species more stable and therefore less likely to accept a proton. C) CH3COO-, because the negative charge is de-localized over the two oxygens, making the species more stable and therefore less likely to accept a proton. D) Ch3COO-, because the negative charge is loaded on one of the two oxygens, making the species less table and therefore a better proton acceptor.

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The answer is C) CH3COO-. This is because the negative charge is delocalized over the two oxygens, making the species more stable and less likely to accept a proton. In water, a stronger base is one that is less likely to accept a proton (H+) and more stable in solution.

The delocalization of the negative charge over the two oxygens in CH3COO- makes it more stable compared to CH3O-, where the negative charge is localized on the oxygen atom. The stability of CH3COO- is due to resonance structures that can be drawn for the molecule, which distribute the negative charge over the two oxygen atoms. This makes CH3COO- a weaker base in water compared to CH3O-, which has a localized negative charge and is more likely to accept a proton. In summary, the stronger base in water is the one that is more stable and less likely to accept a proton, and in this case, it is CH3COO-.

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