Wednesday, 21 April 2021
Monday, 19 April 2021
Saturday, 17 April 2021
Sunday, 14 February 2021
M42 - The Great Orion Nebula
I've been meaning to try out Astro Pixel Processor (APP) for a while now with a view to buying it as my main astro processing software, but I've not had any image data which I regarded as being worthy of extensive processing until now.
Following my successful Team Viewer based remote setup using a long weatherproof network cable from my house into to my garden, I can now control my laptop for finding targets, controlling my mount and capturing image data from the warmth and comfort of being indoors. I use Carte du Ciel to locate the target and Astro Photography Tool (APT) to plate-solve the image and centralise it in the field of view.
The first target I chose was M42, the Orion Nebula, my thoughts being that if I can't get decent images of this then I might as well give up. I setup an exposure plan in APT to capture a range of exposures from 10 seconds to 120 seconds, in order to have correctly exposed shots of both the core and the outer nebulosity. I also took some dark frames with the same exposure and corresponding bias frames, but no flats. Then I loaded them all into APP.
I'm not going to go into the processing details here as I'm still on the steep learning curve of this sophisticated software, but APP calibrates the main images (lights) with darks and bias frames, before analysing the stars it finds, aligning or registering the images, normalising them and finally stacking or integrating them into a single image file. All this is done automatically with no intervention if the default values are used.
Following integration, the image can be stretched to widen the dynamic range and reveal details unseen in the initial images and various other adjustments made before being saved. Although the image APP produces is pretty good, it is normal to process it further in a graphics package such as PhotoShop or GIMP to tease out even more subtle detail. And this is what I have done here.So these images all stem from the same set of data captured in APT and calibrated and stacked in APP. You can play around with the colours and fine detail for ever and it's difficult to know when to stop. Different techniques produce different colours and effects, it's up to the viewer to decide which they like best. To some extent it's impossible to know what the true colours are as we can't actually see them with the naked eye.
Sunday, 7 February 2021
The Main Sequence

After condensation and ignition of a star, it generates thermal energy in its dense core region through nuclear fusion of hydrogen into helium. During this stage of the star's lifetime, it is located on the main sequence at a position determined primarily by its mass, but also based upon its chemical composition and age. The cores of main-sequence stars are in hydrostatic equilibrium, where outward thermal pressure from the hot core is balanced by the inward pressure of gravitational collapse from the overlying layers. The strong dependence of the rate of energy generation on temperature and pressure helps to sustain this balance. Energy generated at the core makes its way to the surface and is radiated away at the photosphere. The energy is carried by either radiation or convection, with the latter occurring in regions with steeper temperature gradients, higher opacity or both.
The main sequence is sometimes divided into upper and lower parts, based on the dominant process that a star uses to generate energy. Stars below about 1.5 times the mass of the Sun (1.5 M☉) primarily fuse hydrogen atoms together in a series of stages to form helium, a sequence called the proton–proton chain. Above this mass, in the upper main sequence, the nuclear fusion process mainly uses atoms of carbon, nitrogen and oxygen as intermediaries in the CNO cycle that produces helium from hydrogen atoms. Main-sequence stars with more than two solar masses undergo convection in their core regions, which acts to stir up the newly created helium and maintain the proportion of fuel needed for fusion to occur. Below this mass, stars have cores that are entirely radiative with convective zones near the surface. With decreasing stellar mass, the proportion of the star forming a convective envelope steadily increases. Main-sequence stars below 0.4 M☉ undergo convection throughout their mass. When core convection does not occur, a helium-rich core develops surrounded by an outer layer of hydrogen.
In general, the more massive a star is, the shorter its lifespan on the main sequence. After the hydrogen fuel at the core has been consumed, the star evolves away from the main sequence on the HR diagram, into a supergiant, red giant, or directly to a white dwarf.
Thursday, 17 December 2020
Rosette Nebula Revisited
Equipment used:
- SkyWatcher EvoStar 80D with Skywatcher 0.85x focal reducer
- Canon 800D modded for Ha sensitivity
- Optolong L-eNhance narrowband filter
- MGEN-II standalone autoguider on 9x50mm SkyWatcher finder scope
- SkyWatcher HEQ5 Pro mount with belt mod
Saturday, 5 December 2020
Set the Controls for the Heart of the Sun
Today I have been mainly photographing an International Space Station's Solar Transit. This is when the ISS passes across the face of the sun creating a silhouette of its shape. Whether you can view a solar transit like this depends on where you are on earth at the time of its passing. Luckily, today it was viewable from some parts of the UK.
Planning
- Go to transitfinder.com
- Enter your location by using 'Auto-detect' or by entering your latitude and longitude co-ordinates
- Enter the dates in which you are interested - you can only go up to 30 days in advance
- Enter how far you would be willing to travel in km (100 is good number to choose)
- Click the 'Calculate' button.
From the above image it can be seen that when I was planning this, the next solar transit was 2020-12-05 (US date format) which is today. However, the quality of view was only going to be 2 star from where I live in Tyldesley with only 1.21 seconds of viewing time and the ISS is only just skirting the bottom of the sun. Clicking on the 'MORE INFORMATION' button revealed more detail:
Clicking on 'SHOW ON MAP' produces a map of the transit path showing my location as a red pin and an ideal location on the line of maximum viewing time with a green pin.
Anywhere along the central line would give a viewing of 2.37 seconds. So I closed the pop up box and zoomed into the map to find a good spot. It was at this point that my friend Paul Richardson suggested Dunham Massey, as it's an area not far from our homes and almost exactly on the central line. He suggested a free car park on Henshaw Lane, but when I actually got there it wasn't in the best position. However, I soon found another spot just 100 metres up the road and Paul joined me there.
Preparation
The preparation to get an image of the solar transit mainly requires a lot of thought. There are two main methods I considered:
- Fire a rapid burst at exactly the right time
- Take some video of the passing










