Caldwell 22, C22, NGC7662

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C22 is a fairly popular planetary nebula for casual observers.

A small refractor will reveal a star-like object with slight nebulosity. A 6 in. telescope with a magnification around 100x will reveal a slightly bluish disk. Telescopes of diameter 16" or greater may reveal slight colour and brightness variations in the interior.

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c22_aw01

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Imaged by: Andy Wilson
Method: LX200, MX916 CCD

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Caldwell 21, C21, NGC4449

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Irregular galaxy, about 3 degrees from M106

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C21_NGC4449_DH01

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Imaged by: Debra Holton using the Faulkes 2m Telescope

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Caldwell 20, C20, The North America Nebula

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The North America Nebula covers an area of more than four times the size of the full moon, but its surface brightness is low so normally it cannot be seen with the unaided eye.

Binoculars and telescopes with large fields of view (approximately 3°) will show it as a foggy patch of light under sufficiently dark skies.

However, using a UHC filter which filters out some unwanted wavelengths of light, it can be seen by the naked eye under dark skies. Its prominent shape and especially its reddish colour (from the hydrogen Hα emission line) only show up in photographs of the area.

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DoubleClusterWideFieldSD

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Image of the Double Cluster and North American Nebula taken from Kelling Heath by Simon Dawes, with a Canon 600D, Modified with the Full Spectrum Mod and a Clip-in CLSCCD filter

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c20_aw01

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Imaged by: Andy Wilson
Method:LX200 8" MX916CCD

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C20_jt01

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Imaged by: Julian Tworek
Method: Canon 100 - 400 Lens @ 200mm, ISO 800, 22 x 120s exposures on Modified Canon 20D and AstroTrac
Taken from Kelling Heath Star Party

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20201014_205650-C20-LS

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Image by Leigh Slomer NGC 7000, Sharpless 117, Caldwell 20 The North America Nebula. An emission nebula located close to Deneb in the constellation of Cygnus. My 1st serious attempt at an astro image. Taken from images captured over 3 nights in late September and early October, it was my 1st image to go more than a few minutes over 1 hour in total exposure time and the 1st to incorporate proper calibration frames.

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Caldwell 15, C15, The Blinking Planetary

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C15 is a planetary nebula located in the constellation Cygnus. It is commonly referred to as the "blinking planetary", although many other nebulae can exhibit such "blinking".

When viewed through a small telescope, the brightness of the central star overwhelms the eye when viewed directly, obscuring the surrounding nebula. However, it can be viewed well in the peripheral vision (averted vision), which causes it to "blink" in and out of view as the observer's eye wanders.

A distinctive feature of this nebula are the two bright patches on either side, which are known as FLIERs.

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c15_aw01

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Imaged by: Andy Wilson
Method: LX200 8" MX916 CCD

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Beginners guide to using your telescope

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This guide is intended for those using a telescope for the first time, the tips are based on common problems that get encountered by those new to astronomy. We are more than happy to meet you and your telescope and help solve your problems so feel free to contact us. You don't even have to join but we would love it if you did.

I can't find anything!

Aligning the finder

Telescopes usually come with a finder of some sort, this will either be a small telescope mounted to the main instrument, a 'red dot' finder or some method of sighting along the telescope tube. The purpose of the finder is to help you point the telescope in the direction of the object you are interested in, and thus it is important that the centre of the field of the finder and the main telescope are pointing to the same area of sky.

The easiest way to align the finder is to focus the main instrument on to a distant object such as a street lamp or roof top aerial, this is best done in daylight so you can see what you are doing, make sure you have the drives off, if you have them, and 25mm or larger eyepiece. DONT POINT THE TELESCOPE NEAR THE SUN

Once you have a reference in the centre of the field of the main telescope lock the mount so that it doesn't move and adjust the finder until this is pointing at the same object, once you have done this move to a different object and confirm both are still pointing to the same thing. You can refine this by using smaller and smaller eyepieces in the main telescope which will magnify the view. Practice moving the telescope to new stationary objects and seeing how good you can get at getting the object in the centre of the eyepiece -  this will all help when it is dark.

Field of view

Telescopes can have a small field of view, so to find an object follow these simple rules.

  1. Find the object first in your finder (see above for aligning it), this should have the largest field of view. Centre the object in the finder.
  2. Using your largest eyepiece in the telescope*, this will be the eyepiece with the largest focal length, or if your eyepieces are marked with their magnification it will be the smallest magnification, center the object in the telescope.
    * this eyepiece will have the widest field of view so you will have the biggest chance of seeing it if your finder and telescope are aligned.
  3. To get a more magnified view (and usually also a smaller field of view) move through your range of eyepieces, starting with the largest focal length and working down, re-centre the object each time.
    Tracking Problems

Telescope not tracking?

If you are using your telescope visually (i.e. you don't have a camera attached) and it has a clock drive it should keep your chosen object in the eyepiece for some time. If not, then you have probably set the telescope mount up incorrectly. For this article we will assume you are using a simple German Equatorial Mount (GEM)

The GEM has two axis (see Choosing a telescope) that move the telescope in RA and DEC. The RA axis (consult your manual) needs to point North, for visual use this doesn't have to be that good an alignment, indeed during daylight observation of the Sun (solar safety) I simply guess where North is and this rough alignment is good enough for visual use and for use when 'web camming', the other consideration is the angle of this axis, this needs to be roughly set to your latitude and anywhere in the south east of England setting it to 52 degrees will be fine.

Lock the axis

Once polar aligned, to drive the scope you need to turn on your drive and lock the RA axis (there is usually a clutch to do this)

if this still doesn't work...

  • Check the power to your scope drive
  • Check the drive is set for northern latitudes (there is usually a button or setting for this)
  • If you have access to the gears touch the RA gear and feel if the motor is turning it, if not you have an electrical/electronics problem, if it is check the gears are not slipping.

GOTO doesn't work

Ok so your GOTO doesn't behave as it was advertised, let's look at what might be going wrong...

Most GOTO systems require some level of set-up, first check your manual, especially check the polar alignment (see tracking above).

  • Check the starting position of the scope, many goto systems require the scope to be set to a specific 'home' position when first turned on - often pointing North but not always
  • Check the clutch's are not slipping
  • Check you are pointing at the correct star (then check again!), make sure this star isn't just in the field but in the centre of the field, if you don't have a reticule eyepiece use your highest magnification, which will have the smallest field to ensure the star is as central as possible before clicking 'align'
  • Check your scope is level (most have a small bubble level for this purpose

If you are still having problems especially if your scope point in radically in the wrong part of the sky (or ground!) then check points 2 and point 4 again.

Often it is best if you bring your scope along to us on a Thursday night, and we can walk you through using it, if you do come along please contact us to let us know.

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Dictionary of Astronomy

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Dictionary of Astronomy

If you have a word you are unsure of and want it added to this dictionary please ask.

A

Aberration

Defect in an image formed by a lens or mirror, e.g. coma

Aberration of light

Shift in the apparent position of stars due to the finite speed of light

Absolute Magnitude

A measure of the true brightness of an object assuming a distance from the observer of 10 parsecs, also see Magnitude

Achromat

A refracting telescope with a lens (usually a doublet) that tries to correct for chromatic aberrations.

Apochromat

A refracting telescope with a lens (usually a triplet) that tries to correct for chromatic aberrations, corrects better than an Achromat, also known as an 'APO'.

Apparent Magnitude

A measure of the brightness of an object as seen from the Earth, also see Magnitude

ALT

Abbreviation for Altitude

Altitude

A coordinate used alongside azimuth in the ALT/AZ coordinate system, to mark the position of an object in the sky, the Altitude or ALT as it is also known, is an angular measure of how high an object is in the sky at your location. The ALT/Az system is a local coordinate system and the positions of objects in the sky change with time and location.

Aperture

The diameter of the primary optical element in a telescope

AZ

Abbreviation for Azimuth

Azimuth

A coordinate used alongside altitude in the ALT/AZ coordinate system, to mark the position of an object in the sky, the Azimuth or AZ as it is also known, is an angular measure from North (or sometimes south) eastwards to an object in the sky at your location. The ALT/Az system is a local coordinate system and the positions of objects in the sky change with time and location.

B

Baade's Window

A gap between "curtains" of dust clouds which lets us see close to the galactiic center of the Milkyway and see stars on the far side of galactic bulge.

Blazhko Effect

The periodic variation of RR Lyrae type stars isn't as stable as you might think, the period and amplitude varies over a cycle of about 40 ish days around the extablished period for the star in question, the cause of the effect is not known but there are two popular hypothesis one to do with the resonance of the stars interior and the other to do with the magnetic field of the star when the axis of the magnetic field is out of line with it's rotational axis. The effect is named after Sergey Blazhko who discovered it.

Blue Shift

Light from an object traveling towards you is 'compressed' this pushes the spectral lines towards the blue end of the spectrum.

C

Catadioptric

A telescope that uses mirrors and lenses to focus the light

Chromatic Aberration

This is an aberration in an optical system that results in light from different wavelengths being focused at slightly different points, so it is impossible for all the light to be in focus at the same time, typically this results in a blue or purple haze around bright objects and a loss of contrast.

Collimation

The lining up of the optical elements in a telescope along with the tube and focuser, essential to get the best out of any telescope, refractors are usually collimated in the factory and don’t need nightly adjustment

Coma

An optical aberration that makes stars have little tails directed away from the centre of the field of view

Conjunction

A line of sight phenomena when two or more solar system bodies are visible in the same area of sky.

D

DEC

Abbreviation for Declination

Declination

A coordinate used alongside Right Ascension in the equatorial coordinate system, to mark the position of an object in the sky, the declination or DEC as it is usually known is an angular measure similar to that of Latitude, however whereas latitude starts at the Earth' equator, DEC starts at the celestial Equator.

Diagonal

Secondary mirror used to divert the light from the primary out to the side of a Newtonian telescope

Dichotomy

The exact point when the Moon (or Mercury or Venus) are at quarter phase (50% illuminated as seen from the Earth)

Drake Equation

An equation that predicts the number of observable alien civilisations in the Milkyway.

Doublet Lens

A lens made from two separate lenses, usually to combat chromatic aberration.

E

Ecliptic

The orbital plane of the Earth around the Sun, or you can think of it as the apparent path of the Sun in the sky over a year.

Extrinsic Variables

Stars that vary due to external influences, for example binary stars eclipsing each other.

F

Faculae

The bright regions on the Sun's photosphere observed in white light

Fermi Paradox

The contradiction between the estimates of the probability of the existence of alien civilizations see Drake equation - and the lack of evidence for these.

Field of View

The area of sky can see, to see the full Moon you need a Field of View of half a degree

Filaments

Dark areas on the solar disk when viewed in hydrogen alpha, occurring in the upper chromosphere, if they extend beyond the solar limb they become bright areas called solar prominences.

Filter

A coloured glass used to block specific wavelengths from the sensor (or eye) of the telescope.
V (Visual) Filters are used to approximate the visual view when using a CCD and are a common filter for photometry ensuring different observers have comparable observations.

FLIERs

Fast Low-Ionization Emission Regions. Emission regions moving outwards at supersonic speeds. Their formation is not easily explained by any models of stellar evolution.

Focal Length

The distance the focus is away from the primary objective

Focal ratio

Simply the focal length divided by the aperture of a telescope, usual expressed as FN, where N is the number of times larger the focal length is compared to the aperture. When ‘N’ is small this is termed ‘Fast’ when N is large this is termed’ Slow’

G

GEM

German equatorial mount, a type of telescope mount.

H

I

Intrinsic Variables

Stars that vary due to the internal nature of the star, for example a star that is pulsating.

J

Jellyhelion

The point in an orbit where you become nervous about having possibly made the wrong decision. Well it made me laugh.

K

L

Leptogenesis

Leptogenesis is the term used to describe the (hypothetical) physical processes that resulted in the universe being made up of matter rather than an even mix of matter and anti matter, 'Lepto' referring to particles called leptons, most famous of which is the electron.

Light Year

The distance light can travel in one year, equal to about 10 trillion kilometres, the nearest star (after the Sun) is about 4.2 light years

M

Magnitude

The 'brightness' scale used in Astronomy, the lower the figure the brighter, it is a logarithmic scale, so a difference of 1 magnitude is about 2.5 times, 5 magnitudes difference is 100 times thus a difference of 8 magnitudes would be (5+1+1+1) (100*2.5*2.5*2.5= 1560 times brighter/fainter)

Meridian

An imaginary line in the sky passing north south

Meteor Train

A meteor train appears as a faint nebulous streak of light left behind, along the track of a meteor, but AFTER the meteor itself has extinguished, about a quarter of meteors leave a momentary train and trains lasting over a second are quite rare .

Meteor Trail

The moving streak of light a meteor

N

Newtonian

A type of reflecting telescope

O

Obliquity

Axial tilt of a body, for the planets and the Sun in relation to its orbital plane.

Objective

The main mirror or lens in an optical system

Observed - Calculated (O-C)

This is generally a plot of an observed measurement minus the calculated measurement, by doing this you plot the residuals and can quickly identify any changes, used commonly for the measurement of eclipsing binary stars.

Occultation

The passing of one object behind another, for example an occultation of Saturn by the Moon, the object behind is said to be occulted, see also transit.

OTA

Optical Tube Assembly, a telescope is made from a mounting system and an optical tube assembly.

P

Parsec

A measure of distance, based on the parallax of the object using the Earth as a base line, 1 parsec is equal to 3.2615 light years.

Photometry

The measurement of an objects intrinsic brightness

Plage

Bright area in solar chromosphere seen in Hydrogen alpha

Primary

Generally referring to the main ‘light gathering’ optical element in a telescope

Q

R

Radiant

The point in the sky where meteor showers appear to originate, this is not to say that a meteor will start at this position, but if you plotted the observed meteors from a specific shower and extended their trail backwards they would all converge onto the radiant

Red Shift

Light from distant galaxies is stretched as space between the galaxy and you expands this results in the spectral lines appearing to be shifted towards the red end of the spectrum

Reflector

A telescope with a mirror that focuses the light

Refractor

A telescope with a lens that focuses the light

Resolution

Measured in arc seconds, this is the finest detail you can see, or image, it is generally limited by aperture and atmospheric conditions.

Right Ascension

A coordinate used alongside declination in the equatorial coordinate system, to mark the position of an object in the sky, the right ascension or RA as it is usually known is an angular measure similar to that of longitude, however whereas longitude starts at Greenwich England, RA starts at the position of the vernal equinox. Rather than using degrees, as longitude does, it uses hours, minutes and seconds, where 1 hour = 15 degrees.

RA

Abbreviation for Right Ascension

Refractor

A telescope with a lens that focuses the light

S

Schröter's Effect

This is the effect where by the theoretical and observed times for Venus to be at dichotomy differ by a day or two.

Secondary

Generally referring to a mirror in a telescope used to change the direction and or point of focus in a telescope

SID

Stands for Sudden Ionospheric Disturbance, a change in the ionosphere due to energetic matter from the Sun interacting with it. see our SID page

T

Transit

The passing of one object in front of another, for example the transit of Venus in front of the Sun, the object in front is said to transit the other object, see also occultation

Triplet

A lens made of 3 components used to make Achromatic Refractors

U

UT

Abbreviation for Universal Time

Universal Time

Closely related to Greenwich Mean Time (GMT) UT is measure of time used for all civil time keeping, for us astronomers in Crayford we just need to remember to remove an hour if we are in British summer time

V

VLF

Very Low Frequency, name given to the 3-30kHz range of the electromagnetic spectrum, VLF radio signals are used to indirectly monitor solar activity see more here

W

X

Y

Z

Zenith

Point in the sky directly overhead.

Zenithal Hourly Rate

The expected number of meteors that would be observed if the radiant is at the Observers Zenith.

ZHR

Abbreviation for Zenithal Hourly Rate

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Classic Doubles

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By Neil Webster

CASTOR: a six-star system

αGEM Σ 1110

RA 07 35
Dec 31 53

Castor was discovered in 1678 by G.D. Cassini and formally classified as a true “binary” in 1803 by William Herschel. The system lies at a distance of about 52 light years and is a six star system.

The AB components comprise two blue-white stars separated by 5 arc seconds with magnitudes 1.9, 3.0 and spectral types A1V and A2V and an orbital period of 467 years. These are, in turn, spectroscopic binaries giving a four-star configuration.
In addition, a faint orange companion C star (magnitude 8.9 – 9.60) at a separation of 70.5” can be seen. This is, in fact, two orange dwarf stars (Spectral types M0V) that orbit one another in less than a day and is an eclipsing binary to our line of sight known as YY Gem.

The orbital period of the AB to C system is unknown but is thought to be of the order of 10,000 years.
An amazing sextuple system!!

REGULUS

αLEO Σ II 6

RA 10 08
Dec 11 58

Regulus is a four star system comprising two stellar pairs. The blue-white primary (B7V, 3.8 solar masses) pairs with a yet to be visually observed hypothesised White Dwarf star of 0.3 solar masses (detected via spectroscopy). These orbit over a short 40 day period. Regulus is observed to be spinning rapidly with a distorted shape (possible due to gravitational interaction with the white dwarf?).

At a separation of 177 arc seconds lies the secondary which is also a contained binary common proper motion pair with an orbital period of 2000 years. The two components have spectral types K2V and M4V with magnitudes 8.14 and 13.5.

Mizar and Alcor

RA 13 23 55.5
Dec 54 55 31

Mizar (magnitude 2.23, spectral class A1V) was first seen visually by Castelli in 1617 and through a telescope in 1650. It was one of the first double stars to be photographed by Bond in 1857. Its companion can be seen clearly at a separation 0f 14 arc seconds. Mizar A was also the first star found to be a double via spectroscopy (1889) and later its companion B (also A class) was also shown to be a spectroscopic binary making Mizar a quadruple system.

At a larger separation of 707 arc seconds lies Alcor (3.99, A5V) which is also a spectroscopic binary with a red dwarf companion.

Mizar and Alcor’s proper motions have long been observed to be similar but as they are part of the Ursa Major moving group a true gravitational connection between the two was in doubt. However, it has recently been proven (2009) by two separate teams that Mizar and Alcor represent a true binary system at a distance of about 83 light years.

Algieba

Gamma LEO
RA 10 19 58
Dec 19 50 29

Algieba is a true double star comprising two giants with yellow-white colourations at an angular separation of 4 arc seconds. It was first observed by William Herschel in 1782.

The primary star (K0III, 2.28) has a surface temperature of 4, 470 K, a luminosity 180 x that of the Sun and a diameter 23 x the Sun.

The companion star (G5111, 3.64) has a temperature of 4, 980 K a luminosity of 50 Suns and a diameter 10 times the Sun.
The orbital period is 500 years.

Iota Cancri

RA 08 46 42
Dec 28 45 36

The A component lies at a distance of 298 light years and is a G8II spectral type with apparent magnitude 4.02. This yellow/orange star has evolved off the Main Sequence and has a high Fe abundance.

Its companion is a blue-white Main Sequence star (A3V) with magnitude 6.57 and lies at a distance of 2800 A.U.
The angular separation is 30.6 arc seconds and the orbital period is a staggering 65, 000 years!

The pair are often referred to as the “Spring Albireo”.

Cor Caroli

RA 12 56 02
Dec 38 19 06

Cor Caroli (Charles’ Heart) was first observed by William Herschel and named in honour of Charles I (or II?) in 1660. It is a binary system at a distance of 110 light years with an angular separation of 19.6 arc seconds.

The primary is an A0 “chemically peculiar” star whose magnitude varies between 2.84 and 2.98 over a period of 5.47 days. This variability is thought to be due to a powerful magnetic field (5000x that of the Earth) giving rise to starspots that vary in intensity during the star’s rotation period.

The secondary is an F-type Main Sequence star of magnitude 5.60.

It is suspected that each component may also be a spectroscopic binary.

Virtually no change has been observed in the system’s configuration since 1830 leading to a calculated large orbital period of 7, 900 years.

Iota Bootis

RA 14 16
DEC 51 22

Iota Bootis (Asellus Secundus: Second Donkey Colt??) lies at an approximate distance of 97 light years and is a true double with a third very faint unrelated member,
The primary is an A-type Main Sequence dwarf that is a Delta Scuti variable star. Precise measurements are needed but the magnitude varies between 4.73 and 4.78 over separate pulsation periods of 38.22 and 30.55 minutes.
B is a A2 type star of apparent magnitude 8.27 (7.5).

Kappa Bootis

RA 14 13
DEC 51 47

Kappa Bootis (Asellus Tertius: third donkey colt) lies at a distance of 155 light years and is a triple star system.

The primary is an A7 subgiant (magnitude 4.54) with a surface temperature of 7830K. It is about to end its H-core burning phase and swell to a Red Giant. It is classified as a Delta Scuti variable with a period of 1.56 hours and has a faint binary companion (combined orbital period of 4.9 years).

The secondary (magnitude 6.6) is an F1V dwarf star with an estimated surface temperature of 6835K.

The primary and secondary orbit over at least 6,000 (from observed partial orbit) to 8,700 (theoretical) years.

Mu Bootis

RA 15 24
DEC 37 23

Mu Bootis/Alkalurops (“club”, “shepherd’s Staff”) is a triple system at a distance of 121 light years.

The primary is a yellow-white magnitude 4.31, F-type subgiant that is suspected to be variable and to have an orbiting companion.

At a separation of 109.4 arc-seconds lies the main binary secondary system of two G1 Dwarf stars (magnitudes 7.2, 7.8) orbiting over a 260 year period at an average separation of 2.2 arc-seconds.

Delta Cyg

RA 19 45
DEC 45 08

The dominant primary is a late Main Sequence B class supergiant star of magnitude 2.9, with a luminosity 180 x the Sun, a radius of 4.7 solar radii and a mass of 3.5 solar masses. It is known to be spinning rapidly (135 km/s at the stellar equator) producing an ellipsoidal shape.

The secondary is a yellow-white F-class star with a luminosity 6x the Sun and a mass of 1.5 solar masses. Its magnitude is 6.3 and as it is only 2.5 arc seconds from the primary it can be a challenge requiring steady, clear seeing! The position angle is 217 degrees.

A further two companion stars have been reported consisting of two pairing each 3 arc-seconds apart lying at distances of 42 and 148 arc seconds from the primary. Other sources report a single orange companion however??

AB has an orbital period of 918 years and lies at a distance of 170 light-years.

Albireo (Beta Cyg)

RA 19 30
DEC 27 57

A classic “showcase double” Albireo is actually a triple (or maybe quintuple) system and was first observed by Flamsteed in 1691.

The primary is an orange class K helium fusing star with a temperature of 4400 K, a luminosity 950 x the Sun, a radius of 50 solar radii and a mass 5x that of the Sun. Spectral analysis revealed it to have a varying radial velocity and a companion was clarified by speckle interferometry. It is a late class B9 dwarf star with a temperature of 11,000 K, a luminosity 0f 100 Suns and a mass 3.2 x that of the Sun. Partial orbit measurements have led to period estimates ranging from 100 – 213 years. The two stars are separated by 0.4 arc-seconds.

The secondary blue star is a B8 dwarf with a temperature of 12,100 K, a luminosity of 190 Suns and a mass of 3.3 Suns. It is a rapid rotator (250 km/s at the equator) completing an orbit in 0.6 Earth days. This gives rise to a surrounding disc of gas.

It is not certain that Albireo is a true “binary system” but, if it is, it has an orbital period of around 100,000 years.

Epsilon Lyra: “Double-Double”

RA 18 44
DEC 39 40

This system consists of four A-class white stars organised into two pairs of binaries.

Epsilon 1 has two stars of magnitudes 4.7 and 6.2 separated by 2.6 arc-seconds orbiting one another in around 1200 years.
Epsilon 2 has stars of magnitudes 5.1 and 5.3 orbiting in a period of 600 years (less precise).

The two systems are thought to orbit one another in about 1000 years and are currently separated by 208 arc seconds.
Precise measurements only began in the 1980s but in 1986 a further companion star was revealed by interferometry giving a five-star system.

However, it is thought that other surrounding faint stars could be part of the system and that the total count could be ten revealing a complex, fascinating gravitational world.

Rasalgethi (α Her)

A 17 14
DEC 14 23

Rasalgethi (Emperor’s Seat) is a triple (quintuple?) system lying 380 light years away.

The primary (magnitude 3.5) is a M5IIvar red bright giant that varies by a magnitude over a 14 year period. It is near the end of its life and undergoing mass-loss giving it an extended gaseous envelope. Speckle interferometry has further hinted at a very close companion star.

The secondary is a double star consisting of a primary yellow giant (G5III) and a secondary yellow-white dwarf (F2V) with a combined magnitude of 5.4).

The overall orbit is around 3600 years.

Nu Draco

RA 17 32
DEC 55 11

Nu Draco consists of two white dwarf stars (A6V, A4m both magnitude 4.9) at a distance of 99 light years and separated by 63.4 arc seconds.

The secondary is also a spectroscopic binary with a low mass companion completing an orbit every 38.6 days.
The overall system has an orbital period of 44,000 years.

61 Cyg

RA 21 07
DEC 38 45

61 Cyg was the first system apart from the Sun to have its stellar parallax and distance measured. The distance measurement of 10.3 light years made by Friedrich Wilhelm Bessel is remarkably close to the current accepted value of 11.4 light years. As the stars are separated by 31 arc-seconds the true binary nature was open to question until 1934 when the orbital parameters were accurately measured confirming the true binary status.

The two stars are orange dwarf main sequence stars (K5V, K7V) with magnitudes 5.2 and 6.05 and a combined orbit of 659 years.

Star A is a BY Draconis variable star and B is a flare type variable star with a measured 11.7 year cycle. Both exhibit notable flare activity with B being 25% more active.

Almaach (γ And)

RA 02 04
DEC 42 20

This double star is actually a quadruple system lying at a distance of 355 light years.

Component A is a bright golden yellow giant star (K3IIb) of magnitude 2.2 separated from an indigo-blue companion (magnitude 4.84) by 9.6 arc seconds and position angle 63 degrees.

However, Wilhelm Struve observed B to be a double in 1842 with the components separated by less than an arc-second. Further spectroscopic analysis between 1957 and 1959 revealed a third star.

B is now known to consist of two B9.5V stars (magnitude 5.5) that orbit in 2.67 days and an A0V star (magnitude 6.3). The two B9.5V stars and the A0V orbit in 64 years.

It is possible that fainter surrounding stars also belong to the system.

95 Her

RA 18 02
DEC 21 36

This is a true binary system with an orbit of about 11,000 years lying at a distance of 470 light years and separated by 6.3 arc-seconds.

Component A is a white A5 giant star (magnitude 4.96) with a temperature 0f 8000K a luminosity of 67 Suns, a diameter of 6.8 Suns and a mass of 2.8 solar masses.

B is a yellow-white giant star (G8) with a temperature of 4900K, a diameter of 19.4 Suns and a mass o £.2 solar masses.
A, due to its smaller size, is the more rapid rotator and is in the transition stage between H and He core burning whereas B has already reached the He burning phase.

Delta Cephei

RA 22 29
DEC 58 25

Delta Cephei lies at a distance of 887 light years and is a triple system (possibly quadruple).

It was discovered by John Goodricke in 1784 and its pale orange primary is the prototype for the Cepheid Variables: vital for distance measurements. It is the second closest Cepheid to the Sun (Polaris being the closest) and varies from magnitude 3.5 – 4.4 over a 5.3 day period. Recent radial velocity measurements revealed a spectroscopic companion B with a tenth of the mass of A. This AB system orbits over a 6 year period.

The visual blue companion C is separated from A by an easy 41 arc-seconds and is strongly suspected to also be a spectroscopic binary. Confirmation is needed but would give Delta Cephei the status of a quadruple system.

56 And

RA 01 56
DEC 37 15

56 And lies at a distance of 360 Light Years and can be found on the SW border of the Open Cluster NGC 752 (distance 1,200 Light Years and unrelated to 56 And).

The primary A is a K0 giant star separated from the M0 giant secondary B by 207 arc seconds (PA 298 degrees). Burnham noticed the large proper motion of A and observed a further C star (magnitude 11.9 at 18 arc seconds, PA 77 degrees). In addition, there is a further star D of magnitude 9.77 lying at 204 arc seconds from A (PA 258 degrees).

The present magnitudes of A and B are 5.7 and 5.9 but there has been dispute in the past as to which is the primary in this system implying some magnitude variations and possibly variable-like activity?

However, A and B are not physically connected and are an Optical Double star system.

ɳ Persei

RA 02 51
DEC 55 54

The primary of this multiple star system is a K3 (originally reported as M3?) orange-yellow supergiant (magnitude 3.8) with a luminosity of 13, 000 Suns and an estimated radius of 210 solar radii. Also known as “Miram” it lies at 1, 300 Light years and its light will have undergone significant dust absorption due to its location deep in the Milky Way. It has at least five companions although all are probably line of sight coincidences.

The secondary is a B9 dwarf star of magnitude 8.5 and its blue hue together with the yellow tints of the primary make this a “mini-Albireo”. If this is a true binary system then the orbital period would be a staggering 350,000 years which makes a true binary connection unlikely.

Ʃ 2816

RA 21 39
DEC 57 29

This, at first sight, appears to be a neat triple system found in the heart of the nebulous H11 Open Cluster (IC 1396).
However, things are far more complex and the following systems are now verified:

A (a magnitude 5.73 06F star) and C (magnitude 7.48) are separated by 11.8 arc-seconds (PA 120 degrees)
A and D (magnitude 7.53) are separated by 19.8 arc seconds (POA 338 degrees).
D and E (magnitude 13.19) are separated by 55.2 degrees (PA 351 degrees).
Another B star of magnitude 13.3 was identified by Burnham in 1889 and is separated from A by 1.7 arc-seconds (PA 320 degrees).

Very high resolution observations revealed a further companion to A at a distance 0f 0.1 arc seconds…………..and this is further shown to be a spectroscopic binary making A on its own a very close triple system.

I think that makes Ʃ 2816 a seven-star system……..at least!!

And, close by is the double Ʃ 2819 system consisting of magnitude 7.4, 8.6 stars separated by 13 arc seconds.

A multiple star feast!!!

Beta Cepheus

RA 21 29
DEC 70 34

Beta Cepheus was first observed by William Herschel and Piazzi and is also known by the Arabic name of “Alfirk” meaning Flock of Sheep.

The primary (A: magnitude 3.2) is the prototype of the Beta Cepheid Variable Stars that are similar to the Cepheids but with lower amplitudes and magnitude variations. In this case the magnitude varies from 3.15 to 3.21 over a 4 – 4.567 hour period. It was also itself found to be a binary (a: companion magnitude 8) by speckle interferometry techniques in the 1970s. The Aa system displays an inclined orbit and separations ranging from 0.33 to 0.01 arc seconds. A is a young (50 million years) B3 white/blue giant.

The secondary B is an 8th magnitude A2V star with colours recorded as blue/green. It is separated from A by 14 arc seconds and a position angle between 249 and 251 degrees.

The whole system lies at a distance between 595 and 700 light years according to recent Hipparcos measurements.

λ Ari

RA 01 58
DEC 23 36

First discovered by Christian Mayer and certainly observed by William Herschel Lambda Ari lies at a distance of 129 light years. The angular separation of 37.4 arc seconds has barely changed since Herschel first measured it given an estimated orbital period of 33, 000 years.

The primary is a yellow-white F0 V Main Sequence star with an estimated mass of 1.8 solar masses, a surface temperature of 7200 K, and an apparent magnitude of 4.95.

The secondary is a green-blue G1 V main sequence star with a smaller estimated mass of 1.25 solar masses, a temperature of 5930 K and a magnitude of 7.75.

Also in the field of view are λ Ari C (magnitude 9.7 at a separation of 189 arc seconds from the primary) and λ Ari D (magnitude 9.9 at a separation of 271 arc seconds). These are purely “optical” and are in no way physically related to the main double.

Xi CEP

RA 22 04
DEC 64 38

This is a relatively close double (80 Lyr, 30 pc???) with an orbital period of 3800 years. The spectral designations are A3 and F7/8 with contrasting magnitudes of 4.4 and 6.4. The colours seem to have divided opinion.

Webb found them White and Tawny, Smyth thought them both to be bluish whereas Haas states them to be Lemon-White and Royal-Blue.

17/16 Draconis

RA 16 36
DEC 52 55

17 Dra is a 5.38 B9 dwarf star and a 6.42 A1 dwarf star separated by 3.3 arc-seconds. The combined magnitude is 5.03 with as calculated distance of 412 light years.

16 Dra is a B9.5 Hydrogen-fusing dwarf with a magnitude 5.53 lying at a distance of 423 light years. The motions of the two systems (separated by 90 seconds of arc) are similar so this is a true binary/triple system.

However, 16 Dra is also suspected to be a double with a White Dwarf companion: never seen but revealed by the healthy UV/X-ray radiation measured around the system.

65 UMa

RA 11 55.1
DEC 46 29

Visually this appears to be a neat triple system consisting of a primary star (A) with a close companion (C) 3.7 arc seconds (PA 42 degrees) and a further companion (D) 63.2 arc seconds (PA 114 degrees).

However, this is a seven-star system.

Robert Aitken in 1908 found a star (B) orbiting A at a very close 0.2 arc seconds (PA 329 degrees) over a period of 118 years.
A itself is triple consisting off an eclipsing binary system 0.3 milli arc-seconds apart with a period of 1.7 days. This pair (Aa1 and Aa2) orbits with a third star (Ab) at a separation of 11 miili arc-seconds over a 640 day period. This system is known as DN Uma.

Furthermore, interferometry has revealed D to itself be a double system with a separation of 0.1 arc-seconds.
A fascinating, rare septuple system!!

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Double Star Primer

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A double star primer covering types of double star, how to observe them and their history, essential reading for anyone interested in observing double stars.

Double Stars History etc (PowerPoint presentation) 

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Jim goes up a ladder and comes down a hero

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THIS WAS A SPOOF

Meteor camera success features in BAA newsletter.

JimGoesUpALadderAndComesDownAHero

In all seriousness, there are a lot of people to thank for going up and down the ladder and providing input into getting the Meteor Cam working, so many that I daren't not mention anyone because I'm bound to miss someone - you know who you are - we still have a small bug that Simon is working on to prevent the sorted meteor files from reappearing on the myCloud drive.

 

 

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Making Dew Heater Bands and Controller

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Introduction:

Dew heaters warm the optics of a telescope to prevent dew forming. Commercial control units and heater elements are available, however with a couple of hours, a soldering iron and a few tools, the control units and heaters can easily be constructed at home. As well as being a satisfying experience building astronomical accessories building these is also financially viable with a controller and as many heating elements as you need costing the price of a mid to low range control unit.

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Control Unit

The control unit provides the ability to alter the amount of heat passing through the heater bands and the most efficient method is to switch the power to the heater elements on and off using a DC to pulse width converter, this varies the time the power is applied to change the average power to the heater bands. Fortunately, DC to pulse width converter circuits are available as simple kits from Velleman so do not require any electronics knowledge. The K8004 kit is specifically designed for the control of heaters, motors and lights and has short circuit protection and a maximum load of 6.5A - plenty for our purposes, this kit is about £13 (2010)

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ATM-dewHeater1

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ATM_Dew_03

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ATM_Dew_04

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Heater Elements

Heater elements are made by passing a current through a resistive wire, the more current the more heat produced and the overall power can be calculated using Ohm’s law, Volts = Current x Resistance and Power = Current squared x Resistance.

Resistance wire is usually measured in Ohms per meter, and our heater bands have to be a specific length dictated by the overall circumference of the object the heater has to go around, although by looping the wire or connecting in parallel it is usually possible to get the correct length of wire for the power desired.

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The simplest way to enclose the heater elements is to sow them onto floor foam, the type used on kitchen floors is ideal, this provides some substance to your heater bands and insulates them on the outside, I cut mine 100mm longer than the element to provide enough space to sow the lead on ensuring no force is put on the soldered connections.
The element is then encased in a sleeve of hook and loop fabric.

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ATM_Dew_08

Cable sown onto element for high strength

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ATM_Dew_09

Heater element sown into foam, as much as possible is kept on the side that will touch the telescope

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Some commercial dew bands suffer from low quality, short leads and/or low quality connectors so don't scrimp here, High quality cable (road cable) and connectors will only cost a few pounds but really make your dew bands look superior to commercial equivalents.

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ATM_Dew_10

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