Chapter #5 Chaisson and McMillan
Problem #1, 3, 4, 9
1. A CCD chip 1024x1024 pixels used with a certain telescope has a 10'x10'arc field of view. What angle of the sky corresponds to 1 pixel ? What would be the diameter of a typical seeing disk (2" arc radius) in pixels?
The CCD chip sees an area of the sky 10'x10' in angular size.
Each pixel then
sees 10'/1024 = 0.0098'= 0.59" (since 1' = 60" arc)
A seeing disk of 4" diameter will be 4"/0.6" = 6.8 pixels
3. A 2 metre telescope can collect a given amount of light in 1 hour. Under the same conditions, how much time would be required for a 6 metre to perform the same task? A 12 metre telescope?
A telescope collects light in a rate proportional to the area of its primary mirror
which is proportional to the diameter squared.
Hence a 6 m telescope collects light (6/2)2 = 9 times faster
than a 2 m telescope.
Time required to collect the same light is 60min/9 = 6.7 minutes
A 12 m telescope collects light (12/2)2 = 36 times fasters.
Time required for the 12m telescope = 60min/36 = 1.7 minutes = 100 seconds
4. A certain space-based telescope can achieve angular resolution of 0.05' for red light (wavelength 700 nm). What would be its resolution
The angular resolution is proportional to the wavelength of the electromagnetic
radiation. (Same telescope)
angular resolution in radians = 1.2 x(wavelength)/(diameter)
(a) 700 nm = 0.70 micrometers so 3.5 micrometers is 5 times larger
hence resolution of 3.5 micrometers is 5 x 0.05' = 0.25'
(b) 140 nm is 1/5 of 700 nm so the resolution is 0.05' x 0.2 = 0.01'
9. Estimate the angular resolution of
Angular Resolution("arc) = 0.25 x (wavelength in micrometers)/(diameter in meters)
(a)5 GHz = 5x109 Hz
wavelength = (3x108 m/s)/ 5x109 Hz = 0.06 m
=
60000 micrometers
5000 km = 5x106 m
So
resolution = 0.25 (60000/5x106m) = 0.003" arc
(b)Infrared Interferometer: wavelength = 1 micrometer, base = 50 m
angular resolution = 0.25 (1/50) = 0.005" arc
1 - Determine the capabilities of the following two telescopes
The telescopes use eyepieces with focal lengths of 7mm, 12mm, and 25mm.
Make a table of the following properties
(use magnitude scale and brightness conversion - as an example: a 70mm diameter lens will collect 10x10 =100 times more light than the 7 mm diameter eye and since a brightness ratio of 100 corresponds to 5 magnitudes, that means the dimmest star visible in a telescope with 70 mm lens is 5.5+5 = 10.5.)
(a) The magnification = (focal length of the objective)/(focal length of the eyepiece)
7 mm | 12 mm | 25 mm | |
---|---|---|---|
A: dia = 125 mm fl = 600 mm | 86 | 50 | 24 |
B: dia = 333 mm fl = 1500 mm | 214 | 125 | 60 |
(b) Field of view (degrees) = 57.3(object size)/(focal length of the objective)
A: 125 mm telescope: FOV = 57.3 (20/600) = 1.9 degrees B: 333 mm telescope: FOV = 57.3 (20/1500) = 0.76 degrees
(c) The light gathering power (LGP) compared with the eye of each telescope is given by the ratio of the of the area of the telescope objective to that of the pupil of the eye. That LGP is a brightness ratio and has an equivalence in magnitude difference. The eye can see the limit of 5.5 magnitude in the telescope but the telescope's LGP increases limit by the magnitude difference.
LGP = [(diameter of objective)/(7 mm)]2
Equivalent magnitude difference = 2.5 log10(B1/B2) = 2.5 log10(LGP)
A: 125 mm telescope: LGP = (125/7)2 = 319 mag difference = 2.5 log10(319) = 6.3 Limiting visible magnitude = 5.5 + 6.3 = 11.8 B: 333 mm telescope: LGP = (333/7)2 = 2263 mag difference = 2.5 log10(2263) = 8.4 Limiting visible magnitude = 5.5 + 8.4 = 13.9
(d) The ideal angular resolution (in " arc) (AR) is given by 138/(diameter of objective in mm)
A: 125 mm telescope: AR = 138/125 = 1.1" arc B: 333 mm telescope: AR = 138/333 = 0.4" arc
(e) The brightness of an extended celestial object is proportional to the inverse of the focal ratio of the objective squared. Focal ratio (f#) = focal length/diameter
Brightness, B ~ (D/fo)2
A: 125 mm telescope: f# = 600/125 = 4.8 B ~ (1/4.8)2 = 0.043 B: 333 mm telescope: f# = 1500/333 = 4.5 B ~ (1/4.5)2 = 0.049 The two telescopes have almost the same focal ratios and hence yield almost the same brightness of image of the Moon. However, the image given by the larger telescope is brighter by 0.049/0.043 = 1.14
2. - Find the shape of the orbit of a space probe sent to an asteroid with a circular orbit of radius 2.5 AU The probe will start at a perihelion near Earth orbit (1 AU from the Sun) and be at apihelion at 2.5 AU. Determine
(a) The orbit of the probe: rp = Perihelion = 1.0 AU ra = Aphelion = 2.5 AU Semi-major axis = (ra+rp)/2 = 3.5/2 = 1.75 AU (b) The period of the orbit: P2 = a3 (Kepler's 3rd Law for the solar system) P = (1.75)3/2= 2.32 years Time of flight to the asteroid = 2.32/2 = 1.16 years (c) The velocity of probe in its orbit at perihelion: vp = vc[(1+e)/(1-e)]1/2 The circular velocity, vc= 2(pi)a/P can be calculated But we would like the units in km/s a = 1.75 AU = 1.75 x 1.5x108km/AU = 2.63x108km P = 2.32 years = 2.32 x (3.16x107 s/yr)=7.33x107s So vc = 6.28 (2.63x108km)/(7.33x107s) = 22.4 km/s The eccentricity, e, may be calculated from e = ra/a - 1 e = (2.5/1.75) - 1 = 0.428 vp = 22.4[(1+0.428)/(1-0.428)]1/2=22.4[(1.428)/(0.572)]1/2 = 35.4 km/s Compare this with the velocity of Earth in its orbit = 29.8 km/s Change in velocity of the probe to put it into its orbit to the asteroid = 35.4 - 29.8 = 5.6 km/s = 20,160 km/hr