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tester [92]
4 years ago
15

A stone is tied to s string and whirled around in a circle at constant speed. Is the string more likely to break when the circle

is horizontal or when it is vertical? Account for your answer, assuming the constant speed is the same.
Physics
1 answer:
Bad White [126]4 years ago
3 0

Answer:

Vertical

Explanation:

When the circle is horizontal, the tension in the string is equal to the centripetal force. When the circle is vertical, the tension is greater since it is equal to the centripetal force plus the weight of the stone. Therefore, the string is more likely to break when the circle is vertical

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What is the overall effect of Earth's global atmospheric circulation?
yulyashka [42]
Atmospheric Circulation is the large-scale movement of air by which heat is distributed on the surface of Earth.
The wind belts and the jet streams girdling the planet are steered by three convection cells: the Hadley cell, the Ferrel cell, and the Polar cell.
While the Hadley, Ferrel, Polar cells are major players in global heat transport, they do not act alone.
Disparities in temperature also drive a set of longitudinal circulation cells, and the overall atmospheric motion is known as the zonal overturning circulation.
6 0
4 years ago
Consider two identical objects released from rest high above the surface of the earth (neglect air resistance for this question)
topjm [15]

Answer:

the relationship between the two scientific energies is   K2 / K1 = 8/9

Explanation:

They ask us to compare the kinetic energies, so we must use the energy conservation theorem, let's start calculating the gravitational potential energy, to use the universal gravitation equation

      F = G m1 m2 / R²

With the mass m1 the Earth mass  and m2 the mass of the object, R the distance from the center of the Terra to the object

Let's calculate the potential energy from the equation

      F = - dU / dr

     dU = - F dr

      ∫ dU = - ∫ F dr

     Uf - Uo = - (Gme m2) I dr / r²

     Uf - Uo = - (Gme m2) (1 /rf - 1 /ro)

Let's see the distances in each case

Case 1. tell us that it is launched from 1 terrestrial radio

      R = Re + Re = 2 Re

Case 2. It is released from 2 terrestrial radios

      R = Re + 2 Re = 3 Re

Let's calculate the potential energy for each case

Case 1

     ΔU = (Gme m2) [1 / (Re + Re) - 1 / Re)] = (Gme m2) 1 / Re [1/2 +1)

     ΔU = (G m2 / Re) 3/2 m2

Case 2

    ΔU (Gme m2) [1 / (Re + 2Re) + 1 / Re] = (Gme m2) 1 / Re [1/3 + 1]

    Δu = (Gme) 1 / Re 4/3 m2

Having the potential energies We can use the energy conservation theorem applied to the initial and final points of the movement.

 

     Em1 = ​​Uo

     Em2 = Uf + K

how do they tell us that there is no friction force

    Em1 = ​​Em2

    Uo = Uf + K

    K = Uf -Uo = ΔU

    K = ΔU

Let's calculate the kinetic energy for each case

Case 1  r = Re

     K1 = (G m2 / Re) 3/2 m2

Case 2 r = 2Re

     K2 = (Gme) 1 / Re 4/3 m2

To compare the two energies let's divide one another

 

      K2 / K1 = [(Gme) 1 / Re 4/3 m2] / [= (G m2 / Re) 3/2 m2]

      K2 / K1 = (4/3) / (3/2)

      K2 / K1 = 8/9

6 0
4 years ago
A square coil (length of side = 24 cm) of wire consisting of two turns is placed in a uniform magnetic field that makes an angle
kupik [55]

Answer:

The magnitude of the emf induced in the coil is 60 mV.

Explanation:

We have,

Side of the square coil, a = 24 cm = 0.24 m

Number of turns in the coil, N = 2

It is placed in a uniform magnetic field that makes an angle of 60 degrees with the plane of the coil. If the magnitude of this field increases by 6.0 mT every 10 ms, we need to find the magnitude of the emf induced in the coil.

We know that the induced emf is given by the rate of change of magnetic flux throughout the coil. So,

\epsilon=N\dfrac{d\phi}{dt}\\\\\epsilon=N\dfrac{d(BA\cos \theta)}{dt}

\theta is the angle between magnetic field and the normal to area vector.

But in this case, a uniform magnetic field that makes an angle of 60 degrees with the plane of the coil. So, the angle between magnetic field and the normal to area vector is 90-60=30 degrees.

Now, induced emf becomes :

\epsilon=N\dfrac{d(BA\cos \theta)}{dt}\\\\\epsilon=NA\dfrac{dB}{dt}\cos \theta\\\\\epsilon=2\times (0.24)^2\times \dfrac{6\times 10^{-3}}{10\times 10^{-3}}\times \cos (30)\\\\\epsilon=0.0598\ V\\\\\epsilon=59.8\ V

or

\epsilon=60\ mV

So, the magnitude of the emf induced in the coil is 60 mV. Hence, this is the required solution.

5 0
4 years ago
Three loops of wire, one circular, one rectangular, and one square, are made from identical lengths of wire. If the loops are pl
Kisachek [45]

Answer:

A) The circular one

Explanation:

When there is a loop of wire in a magnetic field, and the magnetic flux through the coil changes, an electromotive force is induced in the coil, according to Faraday-Newmann-Lenz law:

\epsilon = - \frac{ N\Delta \Phi}{\Delta t}

where

N is the number of turns in the coil

\Delta \Phi is the change in magnetic flux through the coil

\Delta t is the time interval

The variation of flux through a coil can be written as

\Delta \Phi =A \Delta B

where

A is the area of the coil

\Delta B is the change in magnetic field

Here we have three loops of wire: one circular, one rectangular, one square.

The length of the wire used for the 3 loops is the same, therefore their perimeter is also the same.

The change in magnetic flux is directly proportional to the area enclosed by the loop: therefore, the loop that will experience the greatest induced emf is the one having the greatest area.

Since the circle is the 2D figure that maximizes the area for a given perimeter, this means that the circular loop has the greatest area, and so also the greatest induced emf.

4 0
3 years ago
Explained why the thread behaves in this manner​
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