A satellite is moving very close to a planet of density $\mathrm{\rho }$. The time period of the satellite is:

1.  $\sqrt{\frac{3\mathrm{\pi }}{\mathrm{\rho G}}}$

2.  ${\left(\frac{3\mathrm{\pi }}{\mathrm{\rho G}}\right)}^{3/2}$

3.  $\sqrt{\frac{3\mathrm{\pi }}{2\mathrm{\rho G}}}$

4.  ${\left(\frac{3\mathrm{\pi }}{2\mathrm{\rho G}}\right)}^{3/2}$

Subtopic:  Satellite |
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A projectile is fired upwards from the surface of the earth with a velocity ${\mathrm{kv}}_{\mathrm{e}}$ where ${\mathrm{v}}_{\mathrm{e}}$ is the escape velocity and k < 1. If r is the maximum distance from the center of the earth to which it rises and R is the radius of the earth, then r equals:

1.  $\frac{\mathrm{R}}{{\mathrm{k}}^{2}}$

2.  $\frac{\mathrm{R}}{1}$ $-$ ${\mathrm{k}}^{2}$

3.  $\frac{2\mathrm{R}}{1}$ $-$ ${\mathrm{k}}^{2}$

4.  $\frac{2\mathrm{R}}{1}$ $+$ ${\mathrm{k}}^{2}$

Subtopic:  Escape velocity |
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The gravitational potential difference between the surface of a planet and 10 m above is 5 J/kg. If the gravitational field is supposed to be uniform, the work done in moving a 2 kg mass from the surface of the planet to a height of 8 m is

1.  2J

2.  4J

3.  6J

4.  8J

Subtopic:  Gravitational Potential |
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A planet is moving in an elliptical orbit. If T, V, E, and L stand, respectively, for its kinetic energy, gravitational potential energy, total energy and angular momentum about the center of the orbit, then:

 1 T is conserved 2 V is always positive 3 E is always negative 4 the magnitude of L is conserved but its direction changes continuously

Subtopic:  Satellite |
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In planetary motion, the areal velocity of the position vector of a planet depends on the angular velocity ($\omega$) and the distance of the planet from the sun (r). The correct relation for areal velocity is:

1. $\frac{dA}{dt}$ $\alpha$ $\omega r$

2. $\frac{dA}{dt}$ $\alpha$ ${\omega }^{2}r$

3. $\frac{dA}{dt}$ $\alpha$ $\omega {r}^{2}$

4. $\frac{dA}{dt}$ $\alpha$ $\sqrt{\omega r}$

Subtopic:  Kepler's Laws |
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If $$A$$ is the areal velocity of a planet of mass $$M,$$ then its angular momentum is:
1. $$\frac{M}{A}$$
2. $$2MA$$
3. $$A^2M$$
4. $$AM^2$$

Subtopic:  Kepler's Laws |
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Two bodies of masses m and 4m are placed at a distance r. The gravitational potential at a point on the line joining them where the gravitational field is zero is

1.  $-\frac{5\mathrm{Gm}}{\mathrm{r}}$

2.  $-\frac{6\mathrm{Gm}}{\mathrm{r}}$

3.  $-\frac{9\mathrm{Gm}}{\mathrm{r}}$

4.  0

Subtopic:  Gravitational Field |
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Magnitude of potential energy (U) and time period (T) of a satellite are related to each other as:

1. ${T}^{2}$ $\alpha$ $\frac{1}{{U}^{3}}$

2. $T$ $\alpha$ $\frac{1}{{U}^{3}}$

3. ${T}^{2}$ $\alpha$ ${U}^{3}$

4. ${T}^{2}$ $\alpha$ $\frac{1}{{U}^{2}}$

Subtopic:  Satellite |
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A projectile fired vertically upwards with a speed v escapes from the earth. If it is to be fired at 45$°$ to the horizontal, what should be its speed so that it escapes from the earth?

1.  v

2.  $\frac{\mathrm{v}}{\sqrt{2}}$

3.  $\sqrt{2}\mathrm{v}$

4.  2v

Subtopic:  Escape velocity |
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Kepler's second law regarding constancy of the areal velocity of a planet is a consequence of the law of conservation of:

(1) Energy

(2) Linear momentum

(3) Angular momentum

(4) Mass

Subtopic:  Kepler's Laws |
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