cuspaceflight.co.uk Report : Visit Site


  • Server:Apache/2.4.18 (Ubunt...

    The main IP address: 131.111.179.82,Your server United Kingdom,Cambridge ISP:University of Cambridge  TLD:uk CountryCode:GB

    The description :cambridge university spaceflight a student society aiming to get a rocket into space for less than £1000 per launch spaceflight-- -- search -- main menu skip to primary content skip to secondary conte...

    This report updates in 13-Jun-2018

Created Date:15-Nov-2012
Changed Date:26-Oct-2017

Technical data of the cuspaceflight.co.uk


Geo IP provides you such as latitude, longitude and ISP (Internet Service Provider) etc. informations. Our GeoIP service found where is host cuspaceflight.co.uk. Currently, hosted in United Kingdom and its service provider is University of Cambridge .

Latitude: 51.733329772949
Longitude: -2.3666698932648
Country: United Kingdom (GB)
City: Cambridge
Region: England
ISP: University of Cambridge

HTTP Header Analysis


HTTP Header information is a part of HTTP protocol that a user's browser sends to called Apache/2.4.18 (Ubuntu) containing the details of what the browser wants and will accept back from the web server.

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Date:Wed, 13 Jun 2018 05:53:06 GMT
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DNS

soa:ns1.digitalocean.com. hostmaster.cuspaceflight.co.uk. 1412272717 10800 3600 604800 1800
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cambridge university spaceflight a student society aiming to get a rocket into space for less than £1000 per launch spaceflight-- -- search -- main menu skip to primary content skip to secondary content home projects martlet 1 nova comet wombat autorotator quasar outreach sponsorship launches about contact predictor wiki post navigation ← older posts cambridge university spaceflight featured posted on 26/10/2011 by jon sowman from the edge of space a tiny camera captures the dramatic curvature of the earth, during a test flight that is one small step for cambridge university students aiming to launch a rocket into space for under £1,000. – the guardian cambridge university spaceflight is a student run society founded in 2006 comprising undergraduates and postgraduates from many disciplines. we design, build and test high altitude balloons, high powered rockets, and other related experiments. our main aims are to inspire and provide practical experience to cambridge university students. posted in news recovery system forces posted on 05/09/2016 by david walker when designing the recovery system for a rocket the maximum forces must estimated. there are two main considerations, the deceleration of the separating parts of the rocket as the shock cord goes tight and the deceleration of the rocket as the main parachute deploys (in dual deployment systems). firstly the separation velocity must be found. this can be calculated if the pressure causing separation and therefore force acting to accelerate the components of the rocket are known using newton’s laws (remembering there are two parts of the rocket being accelerated). estimating the pressure for standard black powder charges is tricky, there are some approximations to a gas equation around (eg http://www.vernk.com/ejectionchargesizing.htm ). i’d really like to set up a controlled experiment with some bp charges and a pressure sensor. next consider the deceleration as the shock cord goes tight, this can be model as two mass connected by a spring of stiffness k, length l and extension delta. using the velocities from the previous calculation and iterating the differential equations using this matlab script listed below produces the below graph of force against time (should also work in octave). the graph is for a shock cord 3m long and made of 5mm diameter nylon cord. the next consideration is when the main deploys, the rocket is descending at the terminal velocity of the drogue. the main then deploys, the velocity is higher than the new terminal velocity therefore the rocket decelerates. the force is simply given by the drag from the main at the terminal velocity of the drogue. posted in rocket calculations canard aerodynamics posted on 05/09/2016 by david walker my final year project was on building a guided rocket using canards during which i was fortunate enough to get access to a large wind tunnel for a week at very short notice. this proved extremely enlightening as the aerodynamics were much more complicated than i had been assuming. firstly the lift from the canards was much lower than anticipated based on 2d values (see graph). this was due to the extremely low aspect ratio (span/chord) of the canards, this meant the flow was dominated by the tip vortex. due to the pressure differential between the top and bottom of the aerofoil a vortex is generated at the tip (see diagram) this vortex induces downwash which reduces the effective angle of attack delaying stall (the canards stalled above 30°) and reducing lift. however the lift forces back calculated from the rolling moment are much lower again. to explain this requires consideration of how the vortices interact with the aft fins. as can be seen in the diagram below the vortices generated by the canards resulting in an opposing roll moment from the aft fins. source: the effect of tail fin parameters on the induced roll of a canard-controlled missile by melissa mcdaniel, christine evans and dan lesieutre. my full report can be read here: final report posted in canards sizing static ports for altimeter sampling posted on 05/09/2016 by david walker it is important that vents are drilled in the rocket so that the barometer on the flight computer can sample the atmospheric pressure (and calculate the altitude). there are various rules of thumb for sizing such ports but few explanations from first principles. intuitively (or based on dimensional analysis if you will) there must be a ratio between the volume to be vented and the area of the vents. one rule of thumb is one 1/4” diameter hole for every 100 cubic inches. an approach based on first principles goes like this. first decide on the maximum allowable error in the altitude, say 10m. this provides the pressure difference between the altimeter bay and the free stream. next find the maximum flight speed, this gives the maximum rate of change of pressure. modelling the altimeter bay as a volume v with an orifice area a and pressure drop delta p this gives all the information needed based on bernoulli’s equation for the flow through the orifice and mass conservation. this mathcad sheet calculates the size of the vent holes. (mathcad prime express can be download for free). based on an error of 10m and a flight velocity of mach 2 the calculation yields a 0.176″ hole for every 100 cubic inches, a fair bit less than the rule of thumb above. posted in rocket calculations vacuum packing parachutes?! posted on 05/09/2016 by david walker due to a late minute design change we could not get the parachutes to fit inside the booster section of martlet 3. perhaps inspired by his phd on dyson vacuum cleaners jack suggested that vacuum bags might help, no one thought it would work. a short trip to asda and some experimentation later and the chutes were in the rocket. what’s more they could be pulled out with negligible force! the technique involves fitting the parachute bay and parachute (in it’s deployment bag) inside a large vacuum bag. the vacuum then assists the packing of the chute into the bay. posted in martlet 3 smokeless powder for deployment charges? posted on 04/09/2016 by david walker the standard in model rocketry is to use a small (about 2 grams) black powder (bp) charge to deploy the parachutes. the black powder can be ignited with an e-match which can be fired from a flight computer. the rapid combustion produces hot gases which pressurise the sealed parachute bay causing the rocket to separate at a specially designed section. smokeless powder (sp) has been designed as a replacement for bp in firearms applications. it does not require an explosives license where as bp does, which makes its use attractive. however the chemistry of sp is quite different to bp, in particular its reaction rate is far more sensitive to pressure. when used as an ejection charge the powder is far less contained than in the barrel of a gun. after learning this i made some aluminium charge holders. the first one had an internal diameter of 7mm, this proved too small as the holder was fired through the 5mm plywood bulkhead during the deployment test. the second version had the below dimensions. i made up a charge with the tip of the e-match positioned at the bottom, about 2 grams of sp, masking tape acting as wadding and a section of old inner tube cable tied over the top as a burst diaphragm. the ground test worked perfectly. as it was a launch day i jumped in the car and headed to the launch site where i made up 3 identical charges (one for the drogue, two for the main). but the main failed to deploy. both charges had fired but had not produced enough pressure to break the shear pins. on closer inspection of the failed charges the inner tube (burst diaphragm) had slipped past the cable tie rather than rupturing. this must have reduce the containment just enough to curtail the combustion. in conclusion sp can be used for rocket deployment charges but it is very sensitive to how it is confined. black powder is much more f

URL analysis for cuspaceflight.co.uk


http://www.cusf.co.uk/2016/09/recovery-system-forces/recovery-loading/
http://www.cusf.co.uk/launches/
http://www.cusf.co.uk/2014/11/quasar-machining-in-progress/
http://www.cusf.co.uk/category/uncategorized/
http://www.cusf.co.uk/category/news/
http://www.cusf.co.uk/2016/09/smokeless-powder-for-deployment-charges/ejection_charge/
http://www.cusf.co.uk/2013/03/
http://www.cusf.co.uk/wombat/
http://www.cusf.co.uk/2016/09/sizing-static-ports-of-altimeter-sampling/
http://www.cusf.co.uk/2016/09/sizing-static-ports-of-altimeter-sampling/shock-load-2/
http://www.cusf.co.uk/2016/09/canard-aerodynamics/roll_vorticies/
http://www.cusf.co.uk/2014/11/
http://www.cusf.co.uk/2016/09/canard-aerodynamics/markham/
http://www.cusf.co.uk/2014/08/
http://www.cusf.co.uk//#content
cambridge-circuit.co.uk
ukhas.org.uk

Whois Information


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Domain name:
cuspaceflight.co.uk

Data validation:
Nominet was not able to match the registrant's name and/or address against a 3rd party source on 23-Dec-2012

Registrar:
eNom LLC [Tag = ENOM]
URL: http://www.enom.com

Relevant dates:
Registered on: 15-Nov-2012
Expiry date: 15-Nov-2018
Last updated: 26-Oct-2017

Registration status:
Registered until expiry date.

Name servers:
ns1.digitalocean.com
ns2.digitalocean.com
ns3.digitalocean.com

WHOIS lookup made at 06:53:05 13-Jun-2018

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  REFERRER http://www.nominet.org.uk

  REGISTRAR Nominet UK

SERVERS

  SERVER co.uk.whois-servers.net

  ARGS cuspaceflight.co.uk

  PORT 43

  TYPE domain

DOMAIN

SPONSOR
eNom LLC [Tag = ENOM]
URL: http://www.enom.com
Relevant dates:

  CREATED 15-Nov-2012

  CHANGED 26-Oct-2017

STATUS
Registered until expiry date.

NSERVER

  NS1.DIGITALOCEAN.COM 173.245.58.51

  NS2.DIGITALOCEAN.COM 173.245.59.41

  NS3.DIGITALOCEAN.COM 198.41.222.173

  NAME cuspaceflight.co.uk

DISCLAIMER
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