The He ion moved into a region of higher potential.
When the He ion (charge e, mass 4u) with an initial speed of 1.0 * 10⁵ m/s enters an electric field, it experiences a force due to the electric field. Since the ion is positively charged, it is attracted to the negative plate and repelled by the positive plate.
As it moves towards the negative plate, it moves into a region of higher electric potential. This is because the potential difference between the plates causes the ion to decelerate until it comes to rest.
The work done by the electric field on the ion is equal to the change in kinetic energy, which confirms that the ion moved into a region of higher potential.
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g what are the dimensions (height and width) of the smallest plane mirror that you can buy so that you can still see all of yourself without having to move your head?
The smallest plane mirror that one can buy to see their entire reflection without moving their head would have a height of 3.4 meters and a width of 1.1 meters, assuming an average height of 1.7 meters
To see all of oneself in a plane mirror, the mirror must be tall enough to reflect the entire height of the person and wide enough to reflect the entire width. Let's assume an average height of 1.7 meters for a person.
The minimum height of the mirror should be twice the person's height so that the person can see their full reflection, including the head and feet. Therefore, the minimum height of the mirror would be 2 x 1.7 = 3.4 meters.
To determine the minimum width of the mirror, we need to consider the distance between the person and the mirror. Let's assume this distance to be about 1 meter. The minimum width of the mirror would then need to be twice the person's shoulder width plus the distance between the person and the mirror.
Assuming an average shoulder width of 50 cm, the minimum width of the mirror would be 2 x 50 cm + 1 m = 1.1 meters. An average shoulder width of 50 cm, and a distance of 1 meter between the person and the mirror.
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a 2.80 kg grinding wheel is in the form of a solid cylinder of radius 0.100 m .what constant torque will bring it from rest to an angular speed of 1200 rev/min in 2.5 s ?
A constant torque of 0.703 N·m will bring the grinding wheel from rest to an angular speed of 1200 rev/min in 2.5 s.
First, we need to convert the final angular speed to radians per second:
ω = (1200 rev/min) x (2π rad/rev) x (1/60 min/s) = 125.66 rad/s
The moment of inertia of the grinding wheel can be calculated using the formula for a solid cylinder:
I = (1/2)mr² = (1/2)(2.80 kg)(0.100 m)² = 0.014 J·s²
The angular acceleration can be found using the formula:
α = ω/t = (125.66 rad/s) / (2.5 s) = 50.264 rad/s²
The torque required to produce this angular acceleration can be found using the formula:
τ = Iα = (0.014 J·s²)(50.264 rad/s²) = 0.703 N·m
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what is the current in the line segment that contains battery 1? (hint: use an online system of equations solver)
The current in the line segment that contains battery 1 is 1.5A.
To solve for the current in the line segment that contains battery 1, we need to use Kirchhoff's laws, specifically the loop rule. According to the loop rule, the algebraic sum of the potential differences around any closed loop in a circuit must be zero.
Let's assume that the current in the loop is I, and we will choose a clockwise direction for the loop. The potential difference across resistor R1 is IR1, and the potential difference across battery 1 is 6V, which is negative since we are going from the positive to the negative terminal of the battery. The potential difference across resistor R2 is IR2, and the potential difference across battery 2 is 9V, also negative.
Thus, applying the loop rule, we get:
-6V + IR1 + IR2 - 9V = 0
Simplifying, we get:
I(R1 + R2) = 15V
Substituting the values of R1 and R2, we get:
I(4Ω + 6Ω) = 15V
I(10Ω) = 15V
I = 1.5A
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--The complete question is, In a circuit with two batteries and two resistors, where the voltage of battery 1 is 6V and the voltage of battery 2 is 9V, and the resistors have values of 4Ω and 6Ω respectively, what is the current in the line segment that contains battery 1, assuming a negligible internal resistance for both batteries?--
how wide should a 20 m long conductor of square cross section be if it is to carry a current of 1.0 a with a uniform current density of 400 a/m2 ?
The width of the 20 m long conductor should be approximately 0.05 meters.
To determine the width of the conductor, we first need to find its cross-sectional area (A) using the given uniform current density (J) and current (I). The formula for this is:
A = I / J
Plugging in the given values:
A = 1.0 A / 400 A/m² = 0.0025 m²
Since the conductor has a square cross-section, its width (w) will be the square root of the cross-sectional area:
w = √A = √0.0025 m² ≈ 0.05 m
So, the width of the 20 m long conductor should be approximately 0.05 meters.
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which one of the following quantities remains constant for a given lc circuit? group of answer choices the energy dissipated in the circuit. the sum of the energy stored in the capacitor and that in the inductor. the energy stored in the inductor. the energy stored in the current flowing in the circuit. the energy stored in the capacitor.
For the given LC circuit (inductor-capacitor) , the sum of the energy stored in the capacitor and that in the inductor remains constant.
Energy transferred between the inductor and capacitor. So the total energy oscillating between the two components at a resonant frequency.
The energy stored in the capacitor and inductor individually varies over time as the energy oscillates between them.
When voltage changes the energy stored in the capacitor also changes. This is caused by the change in current flowing.
So we can say both the energy stored in the capacitor and the energy stored in the inductor remains constant in a given LC circuit.
The energy dissipated in the circuit can vary over time. Like that the energy stored in the current flowing in the circuit and the energy stored in the capacitor can also vary over time in an LC circuit.
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two wires meet at a junction, merging into one wire, and 6 a and 4 a flow into the junction. how much current flows out of the junction? two wires meet at a junction, merging into one wire, and 6 a and 4 a flow into the junction. how much current flows out of the junction? 4 a 2 a 10 a 6 a 5 a
According to Kirchhoff's Current Law, the current flowing out of the junction is 10 A, since the total current entering equals the total current leaving.
Kirchhoff's Flow Regulation (KCL) is an essential law of electric circuits which expresses that the complete flow entering an intersection (or hub) in a circuit should rise to the all out flow leaving the intersection. This regulation depends on the guideline of protection of charge, which expresses that electric charge can't be made or annihilated, just moved starting with one spot then onto the next.
In the given issue, two wires meet at an intersection and converge into one wire. This intersection can be viewed as a hub in the circuit, and as per KCL, the all out current entering the hub should be equivalent to the complete current leaving the hub. The issue expresses that 6 An and 4 A stream into the intersection, so the complete current entering the intersection is 6 A + 4 A = 10 A. Since there is just a single wire leaving the intersection, the ongoing streaming out of the intersection should likewise be 10 A.
KCL is an integral asset for dissecting complex circuits, as it permits us to decide the ongoing stream at each point in the circuit in light of the ongoing stream at different places. By applying KCL to every hub in a circuit, we can decide the ongoing move through each part of the circuit and eventually comprehend how the circuit works.
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suppose you only sampled the above signal at 45 hz. assuming that the motor vibrated at exactly 1800 rpm, at what frequency would a peak appear on your fft?
A peak would appear at 15 Hz on your FFT when sampling the signal at 45 Hz, and the motor is vibrating at exactly 1800 RPM.
To determine the frequency at which a peak would appear on your FFT when sampling a signal at 45 Hz and the motor vibrating at 1800 RPM, follow these steps:
1. Convert the motor's speed from RPM to Hz:
1800 RPM * (1 min / 60 sec) = 30 Hz. So, the motor vibrates at 30 Hz.
2. Use the Nyquist theorem, which states that the sampling rate should be at least twice the highest frequency present in the signal. In this case, the sampling rate is 45 Hz.
The highest frequency that can be correctly detected is 45 Hz / 2 = 22.5 Hz.
3. Since the motor's frequency (30 Hz) is higher than the Nyquist limit (22.5 Hz), aliasing will occur. Aliasing is when higher frequencies are incorrectly detected as lower frequencies due to insufficient sampling rate.
4. To find the aliased frequency, subtract the motor's frequency from the sampling rate and then find the absolute value: |45 Hz - 30 Hz| = 15 Hz.
Hence, a peak would appear at 15 Hz on your FFT when sampling the signal at 45 Hz, and the motor is vibrating at exactly 1800 RPM.
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suppose you moved two objects farther apart. how would this affect the force of gravity between those objects?
The moving objects farther apart will result in a weaker gravitational attraction between them.
When two objects are moved farther apart, the force of gravity between them decreases. This relationship is described by Newton's Law of Universal Gravitation,
which states that the gravitational force between two objects is proportional to the product of their masses and inversely proportional to the square of the distance between their centers.
Mathematically, this can be represented as F
= G * (m1 * m2) / r^2, where F is the gravitational force,
G is the gravitational constant, m1 and m2 are the masses of the objects, and r is the distance between their centers.
As the distance (r) increases, the denominator (r^2) becomes larger, causing the overall force of gravity (F) to decrease.
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you are running a length of fiber optic cable between two wiring closets. what best describes the cable you are running?
The cable being run between the two wiring closets is most likely a fiber optic cable.
Fiber optic cables are used for high-speed data transmission over long distances. They consist of a core of optically transparent material, such as glass or plastic, surrounded by a cladding material that reflects light back into the core.
The core and cladding are protected by an outer jacket or sheath that provides physical protection and insulation. Fiber optic cables are preferred for long-distance communication because they are less susceptible to interference and signal degradation than copper cables.
They are also able to transmit data at much higher speeds and over longer distances without the need for signal repeaters.
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open the charge-in-magnetic-field simulation and first run it with the default values. why is the trajectory of the positively charged particle curving down, to the bottom of the screen, when moving in the magnetic field?
In a magnetic field, a charged particle's trajectory is curving because of the effect of the magnetic field on the charged particle.
A magnetic field is a vector field that arises from electric currents and magnetized materials. The magnetic field is a vector field that has both magnitude and direction. A magnetic field exists in the vicinity of a magnetic material or a moving electric charge in the form of a flux of force-carrying particles known as virtual photons.
The magnetic field, like the electric field, is a fundamental entity of nature that is used in a variety of applications. In a magnetic field, charged particles follow a helical path that is nearly circular. The magnitude of the charged particle's velocity and the magnetic field's strength both influence the radius of the circle.
A charged particle's velocity vector and the magnetic field's direction are perpendicular to each other in the plane that is perpendicular to the magnetic field. The magnitude of the charged particle's velocity vector is constant throughout the motion because there is no force parallel to the velocity vector in the magnetic field.
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equal masses of cooper, lead, and basalt were placed in direct sunlight for the same time interval. assuming they were all at the same inital temperature, how each one would be expected to change in temperature?
When equal masses of copper, lead, and basalt are placed in direct sunlight for the same time interval and they are all at the same initial temperature, they would be expected to change in temperature as follows: Copper would be expected to increase in temperature the most since it has the highest thermal conductivity.
This means that it can conduct heat better and faster than lead and basalt, allowing it to absorb more heat from the sun and increase in temperature more quickly. Lead would be expected to increase in temperature less than copper but more than basalt since it has lower thermal conductivity than copper but higher than basalt. Therefore, the lead would absorb less heat from the sun than copper but more than basalt, resulting in a moderate increase in temperature. Basalt would be expected to increase in temperature the least since it has the lowest thermal conductivity of the three materials. This means that it can conduct heat the poorest and slowest, resulting in less heat absorbed from the sun and less increase in temperature compared to copper and lead.
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a mass m is attached to a spring with spring constant k. when this system is set in motion with amplitude a, it has a period t. what is the period if the amplitude of the motion is increased to 2a?
If the motion's amplitude is increased to 2a, the period stays the same.
The amount of time is how long it takes for a wave to pass a location after going through one full cycle.
The formula for the springtime season is:
[tex]t = 2\ \sqrt{ \binom{m}{k} } [/tex]
where the spring constant k and time period = T and mass of the system = m
Motion's amplitude is a
We can infer from the equation that,
A spring-mass system's period is inversely proportional to the square root of the mass and proportionate to the spring constant.
The period of time stays the same even if we raise the motion's amplitude to 2a.
The time period is independent of a since it does not depend on amplitude.
Hence, if the motion's amplitude is increased to 2a, the period stays the same.
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what factor, more than any other, do you think led to jupiter having so many moons compared to the inner terrestrial planets?
The main factor that led to Jupiter having so many moons compared to the inner terrestrial planets is its size and mass.
Jupiter is the largest planet in our solar system, and its strong gravitational force allows it to capture and hold onto many objects in its orbit. Jupiter's location in the outer solar system, beyond the asteroid belt, means that there are more objects available for it to capture compared to inner planets. This combination of size, mass, and location provides Jupiter with the ideal conditions to accumulate and retain a large number of moons. The gravitational force of Jupiter is strong enough to capture asteroids and comets that pass near its orbit, resulting in formation of many moons.
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a 63 kg k g person starts traveling from rest down a waterslide 4.0 m m above the ground. at the bottom of the waterslide, it then curves upwards by 1.0 m m above the ground such that the person is consequently launched into the air. ignoring friction, how fast is the person moving upon leaving the waterslide? express your answer with the appropriate units.
Person is moving at most at a speed of 11.8 m/s
We can use the principle of conservation of energy. In this scenario, the person starts at a height of 4.0 m and ends at a height of 5.0 m. Using the formula for gravitational potential energy, we can calculate that the initial potential energy is
[tex]63 kg * 9.81 m/s^2 * 4.0 m = 2474.04 J.[/tex]
At the top of the curve, all of this energy is converted into potential energy again, so the kinetic energy is zero.
[tex]63 kg * 9.81 m/s^2 * 5.0 m = 3085.05 J.[/tex]
Equating these energies, we get[tex]1/2 mv^2 = 3085.05 J[/tex],
where m is the mass of the person and v is the velocity. Solving for v, we get [tex]v = \sqrt{(2 * 3085.05 J / 63 kg)} = 11.8 m/s[/tex].
Therefore, the person is moving at a speed of 11.8 m/s upon leaving the waterslide.
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flywheel in form of a solid cylinder of mass 60.00 kg and radius 1.80 m is rotated to an angular velocity 26.0 rad/s. what is the energy stored in the flywheel?
The energy stored in the flywheel is approximately 32,949.6 Joules.
The energy stored in the flywheel can be calculated using the formula for rotational kinetic energy: KE = 0.5 * I * ω², where KE is the kinetic energy, I is the moment of inertia, and ω is the angular velocity.
For a solid cylinder, the moment of inertia (I) is given by the formula: I = 0.5 * M * R², where M is the mass and R is the radius.
Substituting the given values: I = 0.5 * 60 kg * (1.8 m)² = 97.2 kg m².
Now, we can find the kinetic energy: KE = 0.5 * 97.2 kg m² * (26.0 rad/s)² ≈ 32949.6 J.
So, the energy stored in the flywheel is approximately 32,949.6 Joules.
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naphthalene is diffusing from a spherical particle via forced convection into its surroundings. what is the first step in determining its mass flux?
In finding the mass flux of naphthalene after diffusing with a spherical particle, we need to calculate the mass transfer coefficient that can be measured to find out how much better the mass spreads to the surrounding.
The formula for mass transfer is
[tex]Kg/m^{2s} = ( Sh *D)/r[/tex]
Where,
Sh = Sherwood number, D = diffusion coefficient
After calculating the mass transfer using the given formula it is easy to calculate the mass flux using Fick's Law
Fick's Law can be used in forming a formula that can help in finding the mass flux. Therefore,
The formula for Fick's Law is
[tex]J = -Kg/m^{2s} * (C1 - C2)[/tex]
Where
J = mass flux
C1 = presence of naphthalene on the surface of the particle
C2 = presence of naphthalene in the bulk fluid
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the velocity vector of a particle moving in the xy-plane has components given by and . at time , the position of the particle is . what is the y-coordinate of the position vector at time ?
The y-coordinate of the position vector at time t is (5/2)t² - 8t - 1/2.
It is given the velocity vector components as:
v(t) = (4t - 6) i + (5t - 8) j
To find the position vector at time t, we need to integrate the velocity vector with respect to time. integrate each component separately:
x(t) = ∫ (4t - 6) dt = 2t² - 6t + C1
y(t) = ∫ (5t - 8) dt = (5/2)t² - 8t + C2
where C1 and C2 are constants of integration. We can determine these constants by using the initial position of the particle given as:
r(0) = (2, -1)
At time t=0, we have:
x(0) = 2, y(0) = -1
Substituting these values in the expressions for x(t) and y(t), may get:
C1 = 2, C2 = -1/2
So, the position vector at time t is:
r(t) = (2t² - 6t + 2) i + ((5/2)t² - 8t - 1/2) j
To find the y-coordinate of the position vector at time t, may simply need to substitute t into the expression for y(t):
y(t) = (5/2)t² - 8t - 1/2
Therefore, the y-coordinate of the position vector at time t would be (5/2)t² - 8t - 1/2.
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a 80 kg man lying on a surface of negligible friction shoves a 53 g stone away from himself, giving it a speed of 4.6 m/s. what speed does the man acquire as a result?
When an 80 kg man moving at 120.75 m/s pushes a 53 g stone away from him while lying on a surface with little friction, the stone moves at a speed of 4.6 m/s.
Let the man acquire the speed v in the opposite direction.Let the momentum be conserved here.The momentum of the stone before the push is: p₁ = 0The momentum of the stone after the push is: p₂ = m × vWhere m is the mass of the stoneThe impulse is given as: J = p₂ - p₁Now, we know that the impulse (J) = Force (F) × time (t).
We also know that force is mass × acceleration. Therefore, the impulse can be written as: J = m × a × tUsing these equations we can solve for the acceleration (a).a = J/(m × t)Now, the acceleration is the same for the man and the stone, but the masses are different.
Therefore, the man acquires a speed v that is much smaller than the velocity of the stone. Substituting the given values we get,a = (m₂v₂ - m₁v₁)/(m₂t₂) = (0.053 × 4.6)/(80 × t) = 0.00109/t m/s². After equating the forces acting on both the stone and the man, we have;Fman = - Fstone.
This is because the man's speed is in the opposite direction to the stone.Let u be the initial speed of the man before he shoves the stone away from himself.
Using the momentum formula, m1u1 + m2u2 = m1v1 + m2v2.The mass of the stone is 0.053 kg while the man's mass is 80 kg.So,80u + 0.053 × 0 = 80v + 0.053 × 4.6v = (80u) / 0.053+4.6v = (80u) / 0.053v = 120.75u.
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the drag on a 2-dimensional airfoil can be determined by measuring its wake velocity distribution. this method uses:
The concept of conservation of mass and momentum in fluid physics is the foundation for the technique used to calculate the drag on a 2-dimensional airfoil by observing the spread of its wake velocity.
A wake, or area of disrupted flow, is produced behind the airfoil as the air moves around it. It is feasible to calculate the drag force operating on the airfoil as well as other characteristics like lift and moment by observing the velocity distribution in this wake.
This method, also known as wake detection or wake survey, is widely applied in experimental fluid dynamics.
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A 3kg crab was moving at 1 m/s in the shore before the ride pushed him for 5 seconds. If his final speed was 3 m/s, what force did the tide push him with?
Answer:
[tex]1.2\; {\rm N}[/tex], assuming that all other forces on this crab were balanced.
Explanation:
The impulse [tex]J[/tex] on an object is equal to the change in momentum [tex]\Delta p[/tex]. In other words:
[tex]J = \Delta p[/tex].
If the mass [tex]m[/tex] of the object stays the same (as in the case of this question), the change in momentum can be rewritten as:
[tex]J = \Delta p = m\, \Delta v[/tex], where [tex]\Delta v[/tex] is the change in velocity.
Impulse is also equal to the net force on the object [tex]F_{\text{net}}[/tex] times the duration [tex]\Delta t[/tex] over which the force is applied:
[tex]J = F_{\text{net}}\, \Delta t[/tex].
Equate the two expressions for [tex]J[/tex] to obtain:
[tex]F_{\text{net}}\, \Delta t = m\, \Delta v[/tex].
In this question:
[tex]\Delta t = 5\; {\rm s}[/tex] is the duration over which the force was applied,[tex]m = 3\; {\rm kg}[/tex] is the mass of the crab, and[tex]\Delta v = (3 - 1)\; {\rm m\cdot s^{-1}} = 2\; {\rm m\cdot s^{-1}}[/tex] is the change in the velocity of the crab.Rearrange [tex]F_{\text{net}}\, \Delta t = m\, \Delta v[/tex] and solve for the net force [tex]F_{\text{net}}[/tex]:
[tex]\begin{aligned}F_{\text{net}} &= \frac{m\, \Delta v}{\Delta t} \\ &= \frac{(3\; {\rm kg})\, (2\; {\rm m\cdot s^{-1}})}{5\; {\rm s}} \\ &= 1.2\; {\rm kg \cdot m\cdot s^{-2}} \\ &= 1.2\; {\rm N}\end{aligned}[/tex].
Assuming that all other forces on this crab are balanced, the net force on the crab would be equal to the force from the tide. Hence, the tide would have pushed the crab with a force of [tex]1.2\; {\rm N}[/tex].
a 61 kg object is experiencing a net force of 25 n while traveling in a circle of radius 1.5 m. what is its velocity?.
The velocity is 0.784 m/s when a 61 kg object is experiencing a net force of 25 n while traveling in a circle of radius 1.5 m.
At the point when an item goes in a round way, it encounters a centripetal power coordinated towards the focal point of the circle, which is given by F = [tex]mv^2/r[/tex], where F is the power, m is the mass, v is the speed, and r is the sweep of the circle. For this situation, the net power experienced by the 61 kg object is 25 N, which is equivalent to the centripetal power. We can adjust the equation to tackle for v: v = sqrt(Fr/m). Subbing the given qualities, we get:
[tex]v = sqrt(25 N * 1.5 m/61 kg)= sqrt(0.6135 m^2/s^2)= 0.784 m/s[/tex]
Consequently, the speed of the item is 0.784 m/s while going surrounded by range 1.5 m and encountering a net power of 25 N.
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light of 600.0 nm is incident upon a single slit. the resulting diffraction pattern is observed on a screen that is 0.50 m from the slit. the distance between the first and third minima of the diffraction pattern is 0.80 mm. which range of values listed below contains the width of the slit?
The width of the slit, which the light of 600.0 nm is incident upon, falls in the range of 2.95 µm to 3.05 µm.
1. Calculate the angular separation between the first and third minima (∆θ) using the given distance (0.80 mm) and screen distance (0.50 m): ∆θ = (0.80 mm) / (0.50 m) = 0.0016 rad.
2. Determine the order difference between the first and third minima (m): m = 3 - 1 = 2.
3. Calculate the angular separation for a single order (∆θ_m): ∆θ_m = ∆θ / m = 0.0016 rad / 2 = 0.0008 rad.
4. Use the single-slit diffraction formula to find the slit width (a): a = (λ / ∆θ_m), where λ is the wavelength (600.0 nm = 6.0 x 10^-7 m).
5. Calculate a: a = (6.0 x 10^-7 m) / 0.0008 rad ≈ 3.0 x 10^-6 m, or 3.0 µm.
6. The range is approximately ±0.05 µm, so the final range is 2.95 µm to 3.05 µm.
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A solid cylinder with mass M. radius R, and rotational inertia 1/2MR² rolls without slipping down the inclined plane
shown above. The cylinder starts from rest at a height H. The inclined plane makes an angle with the horizontal.
Express all solutions in terms of M, R, H, theta, and g.
a. Determine the translational speed of the cylinder when it reaches the bottom of the inclined plane.
b. Show that the acceleration of the center of mass of the cylinder while it is rolling down the inclined plane is (2/3)g sin theta.
c. Determine the minimum coefficient of friction between the cylinder and the inclined plane that is required for the cylinder to roll without slipping.
a. The translational speed of the cylinder at the bottom of the inclined plane is v = sqrt(2gh); b. a = (2g sin(theta) / R) R = 2g sin(theta) is the acceleration of the center of mass of the cylinder down the inclined plane. Rolling Cylinder on Inclined Plane; c. The minimum coefficient of friction required for the cylinder to roll without slipping is equal to the tangent of the angle of the inclined plane.
Translational speed and frictional.The potential energy of the cylinder at the top of the inclined plane is Mgh, where g is the acceleration due to gravity. At the bottom of the inclined plane, all of this potential energy has been converted to kinetic energy, so:
1/2 M v^2 = Mgh
where v is the translational speed of the cylinder at the bottom of the inclined plane.
Solving for v, we get:
v = sqrt(2gh)
b. The force of gravity acting on the cylinder down the inclined plane has two components: one parallel to the plane, Mg sin(theta), and one perpendicular to the plane, Mg cos(theta).
The net torque on the cylinder is due to the parallel component of the force of gravity, which acts at a distance R from the center of mass of the cylinder. The torque is therefore:
τ = (Mg sin(theta)) R
The rotational inertia of the cylinder is 1/2MR^2, so the angular acceleration of the cylinder is:
α = τ / I = (Mg sin(theta)) R / (1/2MR^2) = 2g sin(theta) / R
The linear acceleration of the center of mass of the cylinder is
a = αR, so:a = (2g sin(theta) / R) R = 2g sin(theta)
This is the acceleration of the center of mass of the cylinder down the inclined plane.
c. In order for the cylinder to roll without slipping, the force of friction between the cylinder and the inclined plane must provide enough torque to prevent the cylinder from slipping.
The maximum force of friction is μN, where μ is the coefficient of friction and N is the normal force on the cylinder. The normal force is equal to the weight of the cylinder, Mg cos(theta). The torque due to the force of friction is:
τ_friction = μN R = μMg cos(theta) R
The torque due to the force of gravity parallel to the inclined plane is still Mg sin(theta) R. The net torque is therefore:
τ_net = Mg sin(theta) R - μMg cos(theta) R
For the cylinder to roll without slipping, this net torque must be equal to the torque due to the angular acceleration, which is (1/2)MR^2 α. Setting these two torques equal, we get:
Mg sin(theta) R - μMg cos(theta) R = (1/2)MR^2 (2g sin(theta) / R)
Solving for μ, we get:
μ = tan(theta)
So the minimum coefficient of friction required for the cylinder to roll without slipping is equal to the tangent of the angle of the inclined plane.
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a hollow spherical shell has mass 7.90 kg and radius 0.230 m . it is initially at rest and then rotates about a stationary axis that lies along a diameter with a constant acceleration of 0.895 rad/s2 . part a what is the kinetic energy of the shell after it has turned through 5.00 rev ?
The hollow spherical shell has a mass of 7.90 kg and a radius of 0.230 m. It initially rests and then rotates with a constant acceleration of 0.895 rad/s2 around a stationary axis that lies along a diameter. The kinetic energy of the hollow spherical shell is 2.12 J.
The first step is to calculate the angular displacement using the formulaθ = n × 2π = 5.00 rev × 2π/rev = 31.4 rad[The angular displacement here is a positive value, as the spherical shell is rotating in a counterclockwise direction]. The next step is to calculate the angular velocity after 5.00 rev, using the formula
ωf = ωi + αt, where ωi = 0 [initial angular velocity]α = 0.895 rad/s2 [angular acceleration n]t = 2.22 s [time taken to complete 5.00 revolutions]Therefore,ωf = 0 + 0.895 × 2.22 = 1.987 rad/s Kinetic energy of the shell, K = 1/2 I ω²where I is the moment of inertia of the shell.
The moment of inertia of a hollow spherical shell is given by
I = 2/3 M R² where M is the mass of the shell and R is the radius of the shellSubstituting values, K = 1/2 × 2/3 × 7.90 × (0.230)² × (1.987)²= 2.12 J [to 2 significant figures]
Therefore, the kinetic energy of the hollow spherical shell is 2.12 J after it has turned through 5.00 revolutions.
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a merry-go-round rotates at the rate of 0.30 rad/s with a(n) 80.0 kg man standing at a point 2.0 m from the axis of rotation. what is the new angular speed when the man walks to a point 1.0 m from the center? assume that the merry-go-round is a solid 6.50 x 102 kg cylinder with a radius of 2.00 m.
The new angular speed of the merry-go-round after the man walks to a point 1.0 m from the center is approximately 1.80 rad/s.
Let's denote the initial angular speed of the merry-go-round as ω₁, and the new angular speed after the man walks to a point 1.0 m from the center as ω₂.
Given:
Initial angular speed ω₁ = 0.30 rad/s
Mass of the man m = 80.0 kg
Initial distance of the man from the axis of rotation r₁ = 2.0 m
New distance of the man from the axis of rotation r₂ = 1.0 m
Mass of the merry-go-round (cylinder) M = 6.50 * 10² kg
Radius of the merry-go-round (cylinder) R = 2.00 m
The conservation of angular momentum can be applied in this scenario, where the initial angular momentum of the system is equal to the final angular momentum of the system.
The initial angular momentum of the system is given by:
Initial angular momentum L₁ = Moment of inertia of the man about the axis of rotation x initial angular speed of the merry-go-round
The moment of inertia of the man about the axis of rotation can be calculated using the formula for the moment of inertia of a point mass rotating about an axis at a distance r from the axis of rotation:
Moment of inertia of the man about the axis of rotation I₁ = m x r₁²
The final angular momentum of the system is given by:
Final angular momentum L₂ = Moment of inertia of the man about the new axis of rotation x new angular speed of the merry-go-round
The moment of inertia of the man about the new axis of rotation can be calculated using the same formula as above, but with the new distance r₂:
Moment of inertia of the man about the new axis of rotation I₂ = m x r₂²
Setting the initial and final angular momenta equal to each other, we can solve for the new angular speed ω₂:
L₁ = L₂
I₁ * ω₁ = I₁ * ω₂
Substituting the expressions for I₁, I₂, and the given values:
m * r₁² * ω₁ = m * r₂² * ω₂
Simplifying:
r₁² * ω₁ = r₂² * ω₂
Plugging in the given values for r₁, r₂, and ω₁, and solving for ω₂:
2.0² * 0.30 = 1.0² * ω₂
[tex]\omega_2 = \frac{(2.0^2*0.30)}{1.0^2}[/tex]
ω₂ ≈ 1.80 rad/s.
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when measuring absorbance readings it is important to hold the wavelength constant across all samples. group of answer choices true false
The given statement "when measuring absorbance readings it is important to hold the wavelength constant across all samples" is true because it is important to hold the wavelength constant across all samples.
Keep the wavelength constant across all samples when taking measurements of absorbance. This is due to the fact that a substance's absorbance changes depending on the wavelength of light used to detect it.
Therefore, the absorbance measurements won't be precise and trustworthy if the wavelength is not maintained constant. A single wavelength of light is usually used for all measurements in a given experiment to guarantee precise and trustworthy results.
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an undersea research chamber is spherical with an external diameter of 5.20 m. the mass of the chamber, when occupied, is 74,400 kg. it is anchored to the sea bottom by a cable. what is (a) the buoyant force on the chamber, and (b) the tension in the cable?
The buoyant force on the chamber will be 750,775N and tension in the cable will be -21,031N
(a) The buoyant force on the chamber is equal to the weight of the water that displaced by the chamber.
So if we have to find the volume of water displaced by the chamber, we need to find its volume first.
External diameter of the chamber ⇒ 5.20 m
Radius ⇒ 2.60 m.
Formula for the volume of a sphere is,
V = (4/3) × π × r³
Substituting,
V = (4/3) × π × (2.60 m)³ = 74.63 m³
Mass of the chamber ⇒ 74,400 kg
Weight, W = mg = 74,400 kg × 9.81 m/s² = 729,744 N
Density of seawater ⇒ 1025 kg/m³.
The mass of water displaced by the chamber,
[tex]m_{displaced}[/tex] = V × ρ = 74.63 m³ × 1025 kg/m³ = 76,469 kg
The weight of the displaced water is,
[tex]W_{displaced} = m_{displaced}*g = 76,469 * 9.81 m/s^2 = 750,775 N[/tex]
So we can say the buoyant force on the chamber is equal to the weight of the displaced water,
[tex]F_{buoyant}=W_{displaced}=750,775 N[/tex]
(b) The tension in the cable is equal to the weight of the chamber minus the buoyant force on the chamber. In other words, the tension makes the chamber from floating to the surface.
Tension = Weight of the chamber - Buoyant force
[tex]T=W-F_{buoyant}[/tex] [tex]= 729,744 N - 750,775 N = -21,031 N[/tex]
Tension in the cable is downward. That is the cable is under compression. That is why there is a negative sign here. Chamber is heavy enough to sink to the seafloor and negative value states that. The cable is under tension due to the weight of the chamber
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a ball traveling in a circle with a constant speed of 15 m/s has a centripetal acceleration of 20 m/s2. what is the radius of the circle?
The radius of the circle can be calculated using the formula; Centripetal acceleration = v^2/r, where v is the speed and r is the radius of the circle.
Substitute the given values; Centripetal acceleration = 20 m/s^2Speed = 15 m/s Using the formula above, we have;20 = (15)^2/rr = (15)^2/20r = 11.25mTherefore, the radius of the circle is 11.25 m.
The radius of the circle can be calculated using the formula for centripetal acceleration: a_c = v^2 / r, where a_c is the centripetal acceleration, v is the speed, and r is the radius. In this case, a_c = 20 m/s^2 and v = 15 m/s. Rearranging the formula to find r, we get:
r = v^2 / a_c = (15 m/s)^2 / (20 m/s^2) = 225 m^2 / 20 m/s^2 = 11.25 m
The radius of the circle is 11.25 meters.
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the amplitude of a 3.00-kg object in simple harmonic motion is 6.00 m. the maximum acceleration of the object is 5.00 m/s2. what is the period of simple harmonic motion?
The period of simple harmonic motion for this 3.00-kg object is approximately 6.87 seconds.
To find the period of simple harmonic motion for a 3.00-kg object with an amplitude of 6.00 m and a maximum acceleration of 5.00 m/s², we first need to find the angular frequency (ω).
We know the formula for the maximum acceleration in simple harmonic motion is given by:
amax = ω² * A
where amax is the maximum acceleration, A is the amplitude, and ω is the angular frequency.
Rearranging the formula to solve for ω, we get:
ω = sqrt(amax / A)
Plugging in the given values:
ω = sqrt(5.00 m/s² / 6.00 m)
ω ≈ 0.912 m^(-1/2) s^(-1)
Now that we have the angular frequency, we can find the period (T) using the relationship between angular frequency and period:
ω = 2π / T
Rearranging the formula to solve for T, we get:
T = 2π / ω
Plugging in the value of ω we found earlier:
T ≈ 2π / 0.912 m^(-1/2) s^(-1)
T ≈ 6.87 s
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30 In an electric circuit, a current of 5A is flowing. If the potential difference across two points of the wire is 220V, calculate the resistance. Calculate the total voltage in the given electric circuit. (A) (Ans: 4452, 24V) FOT
The total resistance across the circuit is 44 ohms
What is the resistance in the circuit?According to Ohm's Law, the resistance (R) of a wire is equal to the potential difference (V) across the wire divided by the current (I) flowing through it. Using this formula:
R = V/I = 220V / 5A = 44 ohms
So the resistance of the wire is 44 ohms.
To calculate the total voltage in the circuit, we need to know the voltage across all the components in the circuit. If there are no other components in the circuit, then the total voltage would simply be the voltage across the wire, which is 220V.
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