Sunday, 11 September 2011

Distances, Magnitudes and Spectral Classes Equations

m = -2.5 log I + constant

d = R / tan θp   (d = Distance (m))

θp = (t / 3600)°

θ = 2θp = W / d   (d = Distance (m))

mb - ma = 2.5 log (La / Lb)

m - M = 5 log (d / 10)      (d = Distance (parsecs))


R (Radius of Earth Orbit and 1 Astronomical Unit (AU)) = 1.5x1011 m

W (Width of Earth Orbit) = 3x1011 m

1 pc = 3.09x1016 m

1 Mpc = 3.09x1022m


m, ma, mb (Apparent Magnitude)

I (Intensity) = W m-2

θp (Angle of Parallax) = degrees

t (Time of Parallax) = s

La, Lb (Luminosity) = W

M (Absolute Magnitude)

©2011 Grant Dwyer

Monday, 5 September 2011

Lenses and Telescopes Equations

P = 1 / f 

1 / f = 1 / u + 1 / v   (Convex Lens)

1 / f = 1 / v - 1 / u   (Concave Lens)

M = θi / θo = fo / fe = β / α 

α = h / fo

β = h / fe

θ ≈ λ / D

f = fo + fe

s = r θ


P (Power) = D (Dioptres)

f (Focal Length) = cm

u (Object Distance) = cm

v (Image Distance) = cm

M (Magnification)

θi (Image Angle) = Degrees

θo (Object Angle) = Degrees

fo (Objective Lens Focal Length) = cm

fe (Eyepiece Lens Focal Length) = cm

β (Angle Subtended at Eye Using Instrument) = Radians

α (Angle Subtended at Unaided Eye) = Radians

h (Height of Object) = cm

θ (Angular Resolution) = Radians

λ (Wavelength) = m

D (Aperture) = m

r (Radius) = m

s (Distance) = m

©2011 Grant Dwyer

Sunday, 28 August 2011

Ray Diagrams and Telescopes


The rays parallel to the principal axis are converged onto the principal focus

The focal length is the distance between the lens axis and the principal focus

Thicker lenses bend light more, and are therefore described as more powerful. 

Powerful lenses have short focal lengths.

Rules for Ray Diagrams

1) Any incident ray travelling parallel to the principal axis of a converging lens will refract through the lens and travel through the focal point on the opposite side of the lens.

2) Any incident ray travelling through the focal point on the way to the lens will refract through the lens and travel parallel to the principal axis.

3) Any incident ray which passes through the centre of the lens will in effect continue in the same direction that it had when it entered the lens.

Positive Image Distance
Negative Image Distance
Real
Virtual
Inverted
Upright
Erect (More Positive than Focal Length)
Diminished (Less Positive than Focal Length)
Erect (More Negative than Focal Length)
Diminished (Less Negative than Focal Length)


Refracting Telescope

A simple telescope is made of 2 converging lenses.

One is the objective lens of long focal length

One is the eyepiece of short focal length


Concave Reflecting Telescope

In a reflecting telescope, a large concave mirror is used as the objective, instead of a lens.

               
Parabolic Reflecting Telescope

Parabolic reflectors are used to collect energy from a distant source and bring it to a common focal point, thus correcting spherical aberration found in simpler reflectors.


Cassegrain Reflecting Telescope

The Cassegrain reflector is a combination of a primary concave mirror and a secondary convex mirror, often used in optical telescopes and radio antennas.

In a symmetrical Cassegrain, both mirrors are aligned about the optical axis, and the primary mirror usually contains a hole in the centre thus permitting the light to reach an eyepiece. 

©2011 Grant Dwyer

Sunday, 21 August 2011

The Plough (Ursa Major)


Compilation of the stars in 'The Plough' that were 
taken and put back in their original position.

©2011 Grant Dwyer

Saturday, 20 August 2011

Phad (Ursa Major)



Meade Telescope with SPC900NC 
Camera on 14/8/11

©2011 Grant Dwyer

Friday, 19 August 2011

Merak (Ursa Major)



Meade Telescope with SPC900NC 
Camera on 14/8/11

©2011 Grant Dwyer

Thursday, 18 August 2011

Megrez (Ursa Major)



Meade Telescope with SPC900NC 
Camera on 14/8/11

©2011 Grant Dwyer

Wednesday, 17 August 2011

Tuesday, 16 August 2011

Alioth (Ursa Major)



Meade Telescope with SPC900NC 
Camera on 14/8/11

©2011 Grant Dwyer

Monday, 15 August 2011

Arcturus (Bootes)


Meade Telescope with SPC900NC 
Camera on 14/8/11

©2011 Grant Dwyer


Sunday, 14 August 2011

Stellar Evolution


Stars are in a cloud of dust and gas, most of which was left when previous stars blew themselves apart in supernovae. The denser clumps of the cloud contract (very slowly) under the force of gravity.

When these clumps get dense enough, the cloud fragments into regions called protostars, that continue to contract and heat up.

Eventually the temperature at the centre of the protostar reaches a few million degrees, and hydrogen nuclei start to fuse together to form helium.

This releases an enormous amount of energy and creates enough pressure to stop the gravitational collapse.

The star has now reached the main sequence and will stay there, relatively unchanged, while it fuses hydrogen into helium.

Stars spend most of their lives as main sequence stars. The pressure produced from hydrogen fusion in their core balances the gravitational force trying to compress them. This stage is called core hydrogen burning.

When hydrogen in the core runs out nuclear fusion stops, and with it the outward pressure stops. The core contracts and heats up under the weight of the star.

The material surrounding the core still has plenty of hydrogen. The heat from the contracting core raises the temperature of this material enough for the hydrogen to fuse. This is called shell hydrogen burning.

The core continues to contract until, eventually, it gets hot enough and dense enough for helium to fuse into carbon and oxygen. This is called core helium burning. This releases a huge amount of energy, which pushes the outer layers of the star outwards. These outer layers cool, and the star becomes a red giant.

When the helium runs out, the carbon-oxygen core contracts again and heats a shell around it so that helium can fuse in this region. This is called shell helium burning.

In low-mass stars, the carbon-oxygen core isn’t hot enough for any further fusion and so it continues to contract under its own weight. Once the core has shrunk to about earth-size, electrons exert enough pressure to stop it collapsing any more.

The helium shell becomes more and more unstable as the core contracts. The star pulsates and ejects its outer layers into space as a planetary nebula, leaving behind the dense core.

The star is now a very hot, dense solid called a white dwarf, which will simply cool down and fade away.  

Monday, 8 August 2011

Perseids Meteor Shower

Every year from mid-July to late August.

Peaks between 9-14 August.

Observed for more than 2000 years.

Their radiant in the constellation of Perseus.

Primarily visible in the northern hemisphere.

In 2011, the peak meteor shower will be coinciding with the full moon so fainter meteors will be washed out.

File:Perseid meteor and Milky Way in 2009.jpgFile:IMG 8505n3.JPG

Pictures Courtesy of Mila Zinkova

©2011 Grant Dwyer

Friday, 5 August 2011

Vega (Lyra)

Meade Telescope with SPC900NC 
Camera on 4/8/11

©2011 Grant Dwyer

Alkaid (Ursa Major)


Meade Telescope with SPC900NC 
Camera on 4/8/11

©2011 Grant Dwyer

Monday, 1 August 2011

Advantages and Disadvantages of Different Types of Telescopes

Telescopes
Advantages
Disadvantages
Refracting
Closed tube so very little maintenance and images are more steadier and sharper
Hard to disrupt alignment
Production is expensive of large lenses and they can sag as there is no support in telescope
Works only at night
Prone to spherical and chromatic aberration
Thick lenses absorb more light
Reflecting
Large mirrors are cheaper to make than large lens
Mirror only needs to be polished on one side
Only parabolic removes spherical aberration
Not prone to chromatic aberration
Primary mirror is supported so they can be big
Works only at night
Open tube so needs maintenance
Easy to disrupt alignment
Secondary mirror can produce diffraction effects on image
Radio
Use a wire mesh as the long wavelength radio waves do not notice the gaps, construction is easier and cheaper
It does not need to be as precise as a polished mirror
Radio telescopes can work in all weather conditions
Radio telescopes can work during the day and night
Instead of one big dish, a number of dishes can be linked together and when the distance between them is increased, the image becomes sharper
The radio telescope dish has to have a precision of λ/20 to avoid spherical aberration
Radio telescopes have to scan across a radio source to build up an image which is time consuming
IR
Detects anything that gives off heat
Detector needs to be cooled to low temperatures as it gives off heat as well
Can only view near IR so high, dry altitudes or orbit to view higher wavelengths
UV
Can detect objects not seen in other wavelengths
Can only view near UV so orbit to view lower wavelengths
X-ray
Can detect objects not seen in other wavelengths
Mirrors need to be at very low angles in order to work
Can only view x-ray in orbit to view it’s wavelengths

©2011 Grant Dwyer

Sunday, 24 July 2011

Multiverse

Multiverses can be distinguished in 4 different levels

Level I is where other such regions far away in space where the apparent laws of physics are the same, but where history would be different because things happened differently.

Level II is where regions of space where even the apparent laws of physics are different.

Level III is where parallel worlds elsewhere in Hilbert space where quantum reality plays out.

Level IV is where totally disconnected realities are governed by different mathematical equations.


Here are George Ellis' main anti-multiverse arguments:

Inflation might be wrong

String theory may be wrong

Quantum mechanics may be wrong

Multiverses may be unfalsifiable

Some claimed multiverse evidence is dubious

Fine-tuning arguments may assume too much

It's a slippery slope to even bigger multiverses


Inflation makes Level I multiverse

Level I multiverse with string theory makes Level II multiverse

Level II multiverse with quantum mechanics makes Level III multiverse


For more information go to: http://www.scientificamerican.com/article.cfm?id=multiverse-the-case-for-parallel-universe

Tuesday, 12 July 2011

Space Junk



Picture Courtesy of CosmOnline


Dangers of Junk


A 1mm metal chip can cause as much damage as a .22-caliber bullet

A pea-sized lump of debris moving at about 8 km per second is as dangerous as a 180 kg safe travelling at 100 km per hour.

A metal sphere the size of a tennis ball is as deadly as 25 sticks of dynamite.


Since the late 1950's, debris has increased to about 14000 for objects bigger than 10 cm in diameter.


Since the launch of Sputnik in the 1950's, there are 6500 satellites in orbit. Some 3000 satellites are operating in orbit at any one time.


In 2005, there were 13 collisions between objects.

It is predicted that by 2012, there will be 130 collisions between objects.

Some major collisions include a fragment of Ariane rocket that struck a French military satellite, cutting its 20 ft boom in half in 1996 and a 950 kg retired Russian satellite collided with a 560 kg operational satellite in 2009.

For more information go to http://www.cosmonline.co.uk/blog/2011/07/04/close-earth-space-bit-rubbish

Monday, 4 July 2011

Right Hand Column has my Pictures Published

Possible Mini Ice Age

Firstly, recent research in the UK, predicts an 8% chance that we will return to Maunder minimum conditions over the next 40 years, based on past behaviour of the Sun over the last 9000 years.
Secondly, there are still debates over the details of the Little Ice Age and the role played by the Maunder minimum. In Europe, there were considerably more cold winters in this interval, but they were not unrelentingly cold as they were in an ice age. Also, the Earth's climate is evidently a highly complicated system, involving interconnected feedback systems, so it is difficult to disentangle causes and effects. For instance, several recent studies have suggested that solar-induced changes to the jet stream in the northern hemisphere may cause colder winters in Europe but this would be offset by milder winters in Greenland.
Finally, even if the Sun were to head into a quiet period, others argue that the reduction in solar irradiance on Earth would still be small compared with the heating caused by man-made global warming. Mike Lockwood, a researcher at the University of Reading, estimates that the change in climate radiative forcing since the Maunder minimum is about one tenth of the change caused by man-made trace greenhouse gases.

(Info from physicsworld)

Early records of sunspots indicate that the Sun went through a period of inactivity in the late 17th century. (Courtesy: NASA)
Picture Courtesy of NASA

Sunday, 22 May 2011

Dubhe (Ursa Major)


Meade Telescope with SPC900NC 

Camera on 22/5/11

©2011 Grant Dwyer

Saturday, 21 May 2011

Saturn

Meade Telescope with SPC900NC 
Camera and #11 filter
on 20/5/11

©2011 Grant Dwyer

Monday, 16 May 2011

Supermoon


Taken with 2x barlow.

Both: Skywatcher Telescope with EE300
Camera on 18/3/11

©2011 Grant Dwyer

Venus

Skywatcher Telescope with EE300 
Camera on 19/1/11

©2011 Grant Dwyer

Stars

Betelgeuse (Orion) (26/12/10)

Sirius A (Canis Major) (25/12/10)

Both: Skywatcher Telescope with 
EE300 Camera

©2011 Grant Dwyer

Sunday, 1 May 2011

First Light of Cloud Observatory

Telescope looking at Capella.

Telescope looking at Spica.

Computer videoing Spica.

Capella

Spica

Both Stars: Skywatcher Telescope
with EE300 Camera on 1/5/11

©2011 Grant Dwyer

Friday, 29 April 2011

Roof Configuration Finished

Marking out lines for cutting.


Michael making first cut.


Cutting centre beam of roof.

Drilling ready to jigsaw sides.

Jigsawing second side...lots of dust.

Jigsaw from roof angle.

A man with a power tool.

Breakthrough from below !!!!

Breakthrough from above !!!

Lunchtime !!!!

Nailing felt to roof hatch.

Added support beams to roof hatch.





Little brother in way.



Flashing in place around hatch.



Extra waterproofing cover.

Inside view of tarpaulin in place.

Roof hatch closing.

Aerial view of completed roof

©2011 Grant Dwyer