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AnnyKZ [126]
4 years ago
11

In the water cycle, water vapor evaporates into the atmosphere and forms clouds through condensation. What happens in the atmosp

here to the water in order for the clouds to form? A) Water drops mix with air pollution to form clouds. B) The evaporated water warms up and moves closer together. C) The evaporated water cools and drops get closer together. D) The sun heats the evaporated water and the water drops move faster.
Physics
2 answers:
Alenkasestr [34]4 years ago
6 0

Answer: C

Explanation: The evaporated water cools and drops get closer together as it rises and cools.

Damm [24]4 years ago
4 0

Answer:

C

Explanation:

As water vapor rises, it cools. Then drops get closer and over time will form clouds.

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What are the periodic variations in Earth's rotation and orbit around the sun that alter the way solar radiation is distributed
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Answer:

1. The precession of the equinoxes.

2. Changes in the tilt angle of Earth’s rotational axis relative to the plane of Earth’s orbit around the Sun.

3. Variations in the eccentricity

Explanation:

These variations listed above;  the precession of the equinoxes (refers, changes in the timing of the seasons of summer and winter), this occurs on  a roughly about 26,000-year interval; changes in the tilt angle of Earth’s rotational axis relative to the plane of Earth’s orbit around the Sun, this occurs roughly in a 41,000-year interval; and changes in the eccentricity (that is a departure from a perfect circle) of Earth’s orbit around the Sun, occurring on a roughly 100,000-year timescale. which influences the mean annual solar radiation at the top of Earth’s atmosphere.

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3 years ago
The vertical deflecting plates of a typical classroom oscilloscope are a pair of parallel square metal plates carrying equal but
Usimov [2.4K]

Answer:

a) 4.33 pC  b) 5.44*10² N/C

Explanation:

a) The vertical deflecting plates of an oscilloscope form a parallel-plate capacitor.

The value of the capacitance, for a parallel-plate capacitor with air dielectric, can be found to be as follows, applying Gauss' law to the surface of one of the plates, and assuming a uniform surface charge density:

C = ε₀*A / d

where ε₀ = 8.85*10⁻¹² F/m, A = (0.03m)², and d = 0.046 m (we assume that the informed value of 4.6 m is a typo, as no oscilloscope exists with this separation between plates).

Replacing by these values, we find the equivalent capacitance of the plates, as follows:

C = \frac{8.85e-12F/m*(0.03m)^{2} }{0.046m} =1.73e-13 F = 0.173 pF

By definition, the capacitance of any capacitor can be expressed as follows:

C =\frac{Q}{V}

where Q= charge on any of the plates, and V= potential difference between them.

As we know C and V, we can find Q as follows:

Q = C*V = 0.173*10⁻¹² F * 25.0 V = 4.33*10⁻¹² C = 4.33 pC

b) We can find the electric field in several ways, but one very easy is applying Gauss' Law to a pillbox with a face outside one of the plates (paralllel to it) and the other inside the surface.

The total electric flux through the surface must be equal to the enclosed charge, divided by ε₀.

If we look to the flux crossin any face, we find that the only one that has a non-zero flux, is the one outside the surface.

As the electric crossing the boundary must be normal to the surface (in electrostatic conditions,  no tangential field can exist on the surface) , and we assume that the surface charge density that creates it is constant across the surface, we can write the Gauss ' Law as follows:

E*A = Q / ε₀

where A = area of the plate = (.03m)² = 9*10⁻⁴ m², Q= charge on one of the plates = 4.33*10⁻¹² C (as we found in a)) and ε₀ = 8.85*10⁻¹² N/C.

Replacing by these values, and solving for E, we have:

E = \frac{4.33e-12C}{(0.03m)^{2} 8.85e-12F/m} =5.44e2 N/C

⇒ E = 5.44*10² N/C

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