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Drupady [299]
3 years ago
10

A "synchronous" satellite is put in orbit about a planet to always remain above the same point on the planet’s equator. The plan

et rotates once every 10.2 h, has a mass of 2.2 × 1027 kg and a radius of 6.99 × 107 m. Given: G = 6.67 × 10−11 N m2 /kg2 . Calculate how far above the planet’s surface the satellite must be
Physics
1 answer:
zepelin [54]3 years ago
7 0

Answer:

h = 1.014 x 10^{8} m

Explanation:

Given that,

The planet rotates once every 10.2 h

Therefore, in one hour it would take 1/10.2 rev/h

The rotational speed of the planet

                               = 0.098 rev/h

Converting into seconds

                                = 2.72 x 10^{-5} rev/s

Converting to radians, the rotational angular velocity is

                             ω  = 1.709 x 10^{-4} rad/s

The mass of the planet, M = 2.2  x 10^{27} Kg

Radius of the planet,      R  = 6.99 x 10^{7}  m

Gravitational constant,   G  = 6.67 x 10^{-11}  Nm²/Kg²

To find the height 'h' of the synchronous orbit above the planet surface,

The orbital velocity of the planet is given by the expression

                                      V  = \sqrt{\frac{GM}{R + h} }

Since

                                       V  = (R+h)ω

Substituting in the above equation

                                (R+h)ω = \sqrt{\frac{GM}{R + h} }

Squaring on both sides

                                {(R+h)ω}² = {\frac{GM}{R + h} }

                                (R+h)³ =  {\frac{GM}{w^{2}}}

Solving for h

                                    h  =  \sqrt[3]{{\frac{GM}{w^{2}}}}  - R

Substituting the values in the above equation

                 h =  \sqrt[3]{\frac{6.67X10^{-11}X2.2X10^{27} }{(1.709X10 ^{-4})^{2} }}  m

                                   h  = 1.014 x 10^{8} m

So, the height of the synchronous orbit above the surface is 1.014 x 10^{8} m

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oee [108]

Answer:

1.324 × 10⁷ m

Explanation:

The centripetal acceleration, a at that height above the earth equal the acceleration due to gravity, g' at that height, h.

Let R be the radius of the orbit where R = RE + h, RE = radius of earth = 6.4 × 10⁶ m.

We know a = Rω² and g' = GME/R² where ω = angular speed = 2π/T where T = period of rotation = 1 day = 8.64 × 10⁴s (since the shuttle's period is synchronized with that of the Earth's rotation), G = gravitational constant = 6.67 × 10⁻¹¹ Nm²/kg², ME = mass of earth = 6 × 10²⁴ kg. Since a = g', we have

Rω² = GME/R²

R(2π/T)² = GME/R²

R³ = GME(T/2π)²

R = ∛(GME)(T/2π)²

RE + h = ∛(GMET²/4π²)

h = ∛(GMET²/4π²) - RE

substituting the values of the variables, we have

h = ∛(6.67 × 10⁻¹¹ Nm²/kg² × 6 × 10²⁴ kg × (8.64 × 10⁴s)²/4π²) - 6.4 × 10⁶ m

h = ∛(2,987,477 × 10²⁰/4π² Nm²s²/kg) - 6.4 × 10⁶ m

h = ∛75.67 × 10²⁰ m³ - 6.4 × 10⁶ m

h = ∛(7567 × 10¹⁸ m³) - 6.4 × 10⁶ m

h = 19.64 × 10⁶ m - 6.4 × 10⁶ m

h = 13.24 × 10⁶ m

h = 1.324 × 10⁷ m

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Answer:

F= 4788 N

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vf: final speed in m/s  

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Newton's second law of the car in direction  horizontal (x):

∑Fx = m*ax Formula (2)

∑F : algebraic sum of the forces in direction x-axis (N)

m : mass (kg)

a : acceleration  (m/s²)

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m=1800 Fkg

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