The circular velocity of an object in orbit is given on page 84 of the text:
Vc = Ö{GM/r} = Ö{[((6.67x10-10 m3/kg s2)( 4x1017 kg ))/(3x104 m)]} = 29.8 m/s
A major league pitcher can throw a fastball at:
[ 90 miles/hour]([ 90 miles/1 hour]) ([ 1 hour/60 minute])([ 1 minute/60 seconds])([ 1.6 km/1 mile])([ 1000 m/1 km]) = 40 m/s
So a major league pitcher could throw a baseball into orbit around the asteroid.
In case you're curious, a planet's escape velocity is given by:
Vesc = Ö{2GM/r} = Ö2 Vc = 42.1 m/s
So the pitcher could throw the ball slightly faster than 90 mph, he could throw the ball so hard that it would never come back to the asteroid.
The law of universal gravitation states that the gravitational force between two objects, with masses M1 and M2, separated by a distance d (p138) is
Fg = { G M1 M2 \over d2.
a) If the distance between two objects is quadrupled, the force between them would be weakened by a factor of 16. b) Jupiter is 5.2 times further away from the Sun and has a mass 318 times that of the Earth. According to the above formula, the force between Jupiter and the Sun is 12 times stronger than that between the Earth and the Sun. c) Gravity between THAT STAR and the Earth would increase by a factor of 2 from gravity between the Sun and the Earth. (Gravity between the Sun and the Earth will be the same).
According to Newton's law of universal gravitation (p140), the orbital period of a planet with a mass M2 around a star with a mass M1 and a separation $a$ is P2 = 4 \pi2 a3 / G (M1 + M2) where G is the universal gravitational constant. Since the mass of the Earth (M2) is much smaller than that of the Sun (M1), we generally neglect the contribution of M2 in the above formula. Even if another planet has twice the mass as the Earth, it would not modify significantly its period around its own host star (with a similar mass as the Sun). Thus, the orbital period of this planet at 1AU has the same period as that of the Earth, namely one year. b) If the central stars mass is 4 times more massive, we would find from the above formula that P2 would be 4 times smaller. Thus, the period of the planet at 1AU would be half that of the earth, ie 6 Earth month.
a) The amount of energy released in a 1-megaton hydrogen bomb is 5 x 1015 joules. The energy released by a major (magnitude 8) earth quake is 2.5 x 1016 joules which is 5 times that of the hydrogen bomb. b) The amount of US energy consumption per year is 1020 joules. The energy released by burning 1 liter of oil is 1.2 x 107 joules. A total of 8.3 x 1012 liter (or 2 trillion gallons) of oil is needed. That amount is also comparable to the energy release of 20,000 hydrogen bombs. c) The annual energy generation by the Sun is 1034 joules whereas the energy released by supernova is 1044-1046 joules. Thus the energy released at the end of a sun-like star's life is comparable to all that during it lifespan.
There are many possible answers. A few are: Black holes, the apparent position of stars near the sun during a total solar eclipse, and the precession of the perihelion of Mercury's orbit.
See page 105 of the book. A telescope's light gathering power depends on the area that's collecting light. The largest telescope in the world is the Keck telescope in Hawaii, which is 10 meters in diameter.
AKeck/Aeye = [(pRKeck2)/(pReye2)] = ([(RKeck)/(Reye)])2 = ([ 1000 cm/0.8 cm])2 = 1.5 million.
So the Keck telescope gathers 1.5 million times as much light as the human eye.
There several steps to this problem. First you need to estimate how good your telescope's resolution has to be to be able to count people in a crowd. Let's say that a person is about 1 meter across. Use the small angle formula on page 42 of the text to find out how big a 1 meter object looks when you're 400 km away:
angular size = [ (206,265 arcsec)(linear size)/distance] = [ (206,265 arcsec)(1 m)/(4x108 m)] = 0.5 arcsec
Now we need to know how big a telescope is needed to resolve details 0.5 arcseconds across. Page 106 of the text has a formula for the resolving power of a telescope:
D = [ 11.6 cm arcsec/(a)] = [ 11.6 cm arcsec/0.5 arcsec] = 23.2 cm.
So your telescope needs to be 23.2 cm in diameter to be able to see object 1 meter across from 400 km away.