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skelet666 [1.2K]
4 years ago
5

A satellite circles the moon at a distance above its surface equal to 2 times the radius of the moon. The acceleration due to gr

avity of the satellite, as compared to the acceleration due to gravity on the surface of the moon is
Physics
2 answers:
KiRa [710]4 years ago
4 0
From Newton's Law of Universal Gravitation:

<span>F  =  GMm / r^2.    ( When at the surface).
</span>
<span>G = Universal gravitational constant, G = 6.67 * 10 ^ -11  Nm^2 / kg^2.
M = Mass of Moon
m = Mass of Satellite
r = distance apart, between centers = in this case it is the distance from Moon to the  Satellite.</span>

Recall:  F = mg.

mg =  <span>GMm / r^2
g  =  GM / r^2.........................(i).  When at surface.

Note when the satellite is at a distance 2 times the radius of the moon.
Therefore, the distance between centers =  2r + r = 3r.
Note, when need to add radius of the moon, because we are measuring from center of the satellite to center of the moon.

From (i)</span>
<span><span>g  =  GM / (3r)^2</span>.    The distance r is replaced with 3r

g  =  GM / 9r^2  =    (1/9) * GM / r^2

Therefore gravity on the satellite is (1/9) times that on the Moon.
</span>
SIZIF [17.4K]4 years ago
3 0
The orbit is a circle whose radius is 3 times the radius of the surface
(both measured from the center of the moon). So the acceleration due
to gravity at the orbital altitude is

                          1/3² = 1/9 = <em>11.1% of its value</em> on the surface.
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A garden hose with a small puncture is stretched horizontally along the ground. The hose is attached to an open water faucet at
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Answer:

The pressure inside the hose 7000 Pa to the nearest 1000 Pa.

<em>h₁ = \frac{\frac{128μLQ}{πD^{4} } + ρgh₂}{ρg}</em>

<em>V_{1} =V_{2}</em>

The pressure at the site of the puncture is <em>P₂ =7161.3 Pa</em>

Explanation:

<em>According to Poiseuille's law, P_{1} - P_{2}  = \frac{128μLQ}{πD^{4} } </em>

<em>Where P_{1} is the pressure at a point 1 before the leak, P_{2} is the pressure at the point of  the leak 2, μ = dynamic viscosity, L = the distance between points 1 and 2, Q = flow rate, D = the diameter of the garden hose. </em>

<em>Also,  from the equation P =ρgh, the equations h₁ = \frac{P₁} {ρg} and h₂ = \frac{P₂} {ρg} can be derived.</em>

Combining Poseuille's law with the above, we get h₁ - ρgh₂ =  \frac{128μLQ}{πD^{4} }

<em>h₁ = \frac{\frac{128μLQ}{πD^{4} } + ρgh₂}{ρg}</em>

<em>V =\frac{Q}{A}</em>

Since the hose has a uniform diameter, the nozzle at the end is closed and neither point <em>1 nor 2 lie after the puncture,</em>

<em>V_{1} =V_{2}</em>

The pressure at the site of the puncture <em>P₂ =ρgh₂</em>

<em>P₂ =1kgm⁻³ ×9.81ms⁻¹×0.73m</em>

<em>P₂ =7161.3 Pa</em>

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The intensity of the waves from a point source at a distance d from the source is I. At what distance from the sources is the in
Oliga [24]

Answer:d'=\frac{d}{\sqrt{2}}

Explanation:

Intensity of the waves from a point source can be given by Power divided by surface area.

For P Power source and at a distance d from source Intensity is given by

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when intensity is 2I then it is at a distance of let say d'

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