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vaieri [72.5K]
2 years ago
9

As a moon follows its orbit around a planet, the maximum grav- itational force exerted on the moon by the planet exceeds the min

imum gravitational force by 11%. find the ratio rmax/rmin, where rmax is the moon's maximum distance from the center of the planet and rmin is the minimum distance.
Physics
1 answer:
Mars2501 [29]2 years ago
8 0
The gravitational force exerted on the moon by the planet when the moon is at maximum distance r_{max} is
F_{min}=G \frac{Mm}{r_{max}^2}
where G is the gravitational constant, M and m are the planet and moon masses, respectively. This is the minimum force, because the planet and the moon are at maximum distance.

Similary, the gravitational force at minimum distance is
F_{max}=G \frac{Mm}{r_{min}^2}
And this is the maximum force, since the distance between planet and moon is minimum.

The problem says that F_{max} exceeds F_{min} by 11%. We can rewrite this as
F_{max}=(1+0.11)F_{min}=1.11 F_{min}

Substituing the formulas of Fmin and Fmax, this equation translates into
\frac{1}{r_{min}^2}=1.11  \frac{1}{r_{max}^2}
and so, the ratio between the maximum and the minimum distance is
\frac{r_{max}}{r_{min}}= \sqrt{ 1.11 }=1.05
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Answer:  53.31\° East of North

Explanation:

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Speed of the wind from East to West: 6.68 m/s

Speed of the bee relative to the air:  8.33 m/s

If we graph these speeds (which in fact are velocities because are vectors) in a vector diagram, we will have a right triangle in which the airspeed of the bee (its speed relative to te air) is the hypotense and the two sides of the triangle will be the <u>Speed of the wind from East to West</u> (in the horintal part) and the <u>speed due North relative to the ground</u> (in the vertical part).

Now, we need to find the direction the bee should fly directly to the flower (due North):

sin \theta=\frac{Windspeed-from-East-to-West}{Speed-bee-relative-to-air}

sin \theta=\frac{6.68 m/s}{8.33 m/s}

Clearing \theta:

\theta=sin^{-1} (\frac{6.68 m/s}{8.33 m/s})

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2 years ago
An end of a light wire rod is bent into a hoop of radius r. The straight part of the rod has length l; a ball of mass M is attac
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Answer:

arcsin(\frac{R\mu}{(R+l)\sqrt{\mu^2+1}})

Explanation:

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And the last equation again from Newton's Law,

\mu N = mgsin\phi

Then if we collect all equations together,

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\theta = arcsin(\frac{R\mu}{(R+l)\sqrt{\mu^2+1}})

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Answer:

Answer is attached

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Sunny_sXe [5.5K]

Answer:

volcanic eruptions

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