CanSat 2019 �Design Review (PDR) Outline �Version 1.1
Team #4053
Lakshya
CanSat 2019 PDR: Team 4053 | Lakshya
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Team Organization
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Tapaswin Padhy
GROUND CONTROL AND SOFTWARE SUBSYSTEM
MECHANICAL SUBSYSTEM
Dr. SURAJ SHARMA (PhD)
FACULTY ADVISER
ELECTRONICS SUBSYSTEM
MANAGEMENT
SUBSYSTEM
BAIVAB KUMAR MISHRA
ALTERNATE
TEAM LEADER
(3rd year)
BONDA
VENKAT SWAMY
IIT BBSR (3rd year)
RAJ KISHORE
PATRA
(2nd year)
DIBYAJYOTI JENA
(2nd year)
SNEHA
SHUKLA
(1st year)
ARIJEET SATAPATHY
(3rd year)
SRIRAM METTA
IIT BBSR(3rd year)
ASHUTOSH
NANDA
(2nd year)
SHUBHAM
SHARMA
(2nd year)
TAPASWIN PADHY
TEAM LEADER
(3rd year)
Systems Overview
Tapaswin Padhy
CanSat 2019 PDR: Team 4053 | Lakshya
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System Level Configuration Selection
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter:Tapaswin Padhy
( Concept 1)
Rationale for selection
Three Wing auto-gyro System
Hollow payload design
(Lowered centre of gravity)
Physical Layout
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter:Tapaswin Padhy
PROPELLERS
HOLLOW
SKELETON
ANTENNA
PCB
POWER
SOURCE
CAMERA
IR SENSORS AND ALTITUDE SENSORS
POWER
SWITCH
Placement of major components
Bottom view
Physical Layout
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter:Tapaswin Padhy
ANTENNA
PCB
POWER SOURCE
CAMERA
ARDUINO NANO
POWER SWITCH
Placement of major components
XBEE S2C PRO
GPS Sensor
Physical Layout
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter:Tapaswin Padhy
Placement of relevant components
PAYLOAD
LAUNCH CONFIGURATION
DEPLOYED
CONFIGURATION
System Concept of Operations
CanSat 2019 PDR: Team 4053 | Lakshya
Presenter: Tapaswin Padhy
CONTAINER
+
PAYLOAD
(IN ROCKET)
CONTAINER GETS SEPARATED ALONG WITH PARACHUTE
20 m/s
PAYLOAD LANDS USING auto-gyro
10m/s
PAYLOAD LANDS/
BUZZER SAFELY START
SERVO MOTOR
DISENGAGED
450
m
725
-
670
m
PARACHUTE
GROUND CONTROL
ROCKET LAUNCHES
Team Logo
Here
(If You Want)
Launch Vehicle Compatibility
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Tapaswin Padhy
310 mm
mm
2.5 mm
310 mm
125 mm
125 mm
NOTE:
Dimensions of the container have been designed such that there is enough clearance and no protrusions for smooth fitting and deployment of payload.
Descent Control Design
Baivab Kumar Mishra
CanSat 2019 PDR: Team 4053 | Lakshya
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Payload Descent Control Strategy Selection and Trade
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Current Design (Chosen) Parachute -1 (Spill Hole Parachute) |
Alternative Design Parachute -2 (Cruciform Parachute) |
Parachute Selection
Advantages (Parachute 1):
|
Disadvantages (Parachute 1):
|
Advantages (Parachute 2):
|
Disadvantages (Parachute 2):
|
Payload Descent Control Strategy Selection and Trade
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Current Design (Chosen): In case of auto-gyro system with three wings the estimated surface area would be distributed more efficiently. That’d help decide the dimensions of the auto-gyro wings more flexibly. |
Alternative Design: In case of auto-gyro system with two wings distribution of the estimated surface area wouldn’t be that efficient. This’d set up constraints while deciding dimensions for the wings of the auto-gyro system. |
auto-gyro System Selection
Rationale: We’ve chosen the three wings design because it gives us more flexibility while deciding the dimensions for our design as well as for the 3D printing.
Payload Descent Stability Control Strategy Selection and Trade
CanSat 2019 PDR: Team 4053 | Lakshya
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Descent Stability Control Selection
CHOSEN DESIGN FOR DESCENT STABILITY CONTROL
ALTERNATE DESIGN FOR DESCENT STABILITY CONTROL
Presenter: Baivab Kumar Mishra
Descent Rate Estimates (1/11)
1. D = 𝑫 = Drag force acting on the probe
𝑊 = Weight of CanSat / Probe
𝝆 = Air density = 1.2 kg/m3
𝒗 = Terminal descending velocity
𝑪d = Drag coefficient = 1.124
𝑺 = Projected surface area of
descending object.
W = mag
2. ma = 350 g
g = 9.8m/s2
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Descent rate estimation of Science Payload
Descent Rate Estimates (2/11)
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Descent Rate Estimates (3/11)
Therefore,
The circular area then has been assumed to be the area upon which fluid concepts work. Hence, the area would be the surface area of the auto-gyro.
Surface area = 3 x ( surface area of 3 identical rectangles ) + surface area of centre circle
s1= surface area of rectangles
s2= surface area of the circle
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Descent Rate Estimates (4/11)
d = 4 cm(From our design), 𝝿 = 22/7
S = total surface area of the auto-gyro
; where l = length of each rectangular wing.
b = breadth of each rectangular wing.
(Here l = 30 cm)
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s2 = 12.57 cm2
∵ S = 3s1 + s2
⇒ 325.5 = 3s1+12.57
⇒ s1 = 104.31 cm2
lb = s1
⇒ b = =
⇒ b = 3.48 cm
104.31 cm2
30 cm
Presenter: Baivab Kumar Mishra
Descent Rate Estimates (5/11)
In case of circular motion of the auto-gyro
r = radius of the circle
Equation (1) w = angular speed
v = linear speed
d = diameter of the circle
𝝿 = 22/7
n = no. of complete revolutions per minute
Here the linear speed v has been assumed to be peripheral speed of the fluid (atmospheric air).
But, W = Weight of the descending object.
ρ = Air density
V = Peripheral speed of the fluid
Cd = Drag coefficient
S = Surface area of the descending object
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Descent Rate Estimates (6/11)
*But earlier V is the terminal descending speed of the payload .
So here,
V = Peripheral speed of the fluid = Terminal descending speed of payload.
V = 12.5 m/s
Substituting this assumption in Equation (1) we get,
12.5 x 100 =
⇒ n = 1172.66
⇒ n ≈ 1173 rpm
Hence, the rpm (no. of complete rotations per minute) is 1173.
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Descent Rate Estimates (7/11)
Descent Rate Estimation of Container
⇒ Sc =
⇒ Sc = 0.01635 m2
⇒ Sc = 163.5 cm2
CanSat 2019 PDR: Team 4053 | Lakshya
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Where,
container = 450 g
container system = 20 m/s
2 x mcg
𝝆V2CDc
Presenter: Baivab Kumar Mishra
Descent Rate Estimates (8/11)
Descent Rate Estimation of Container
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Baivab Kumar Mishra
Area of parachute = 163.5 x 104% = 170 cm2
Descent Rate Estimates (9/11)
𝑊 = Weight of CanSat/Probe
𝝆 = Air density
𝒗 = Descent velocity
𝑪𝑫 = Drag coefficient
𝑺 = Projected surface area of
descending object.
2. g = 9.8m/s2
𝝆 = 1.2 kg/m2
CanSat 2019 PDR: Team 4053 | Lakshya
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1
2
x = Distance from ground (Altitude)
v = Descent speed
t = Time required for descent
Presenter: Baivab Kumar Mishra
Formulae used for Descent Rate Estimations
Descent Rate Estimates (10/11)
CanSat 2019 PDR: Team 4053 | Lakshya
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v = Linear speed
r = Radius of the circle
⍵ = Angular speed
5.
v = Linear speed
d = Diameter of the circle
n = no. of complete revolutions per minute
Presenter: Baivab Kumar Mishra
Descent Rate Estimates (11/11)
CanSat 2019 PDR: Team 4053 | Lakshya
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Assumptions
Presenter: Baivab Kumar Mishra
Descent Rate Estimates
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Final Summarized Results
163.5 cm2 x 104%= 170 cm2
Presenter: Baivab Kumar Mishra
Mechanical Subsystem Design
Sriram Metta
CanSat 2019 PDR: Team 4053 | Lakshya
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Mechanical Subsystem Overview
Container
Payload
Electronics
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Sriram Metta
Payload Mechanical Layout of Components Trade & Selection
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Presenter: Sriram Metta
CONCEPT 1 (CHOSEN):-
Hollow payload design using 3 wing auto-gyro system
Location of Electrical Components
Mechanical Parts such as hinges and springs
auto-gyro
Attachment
Point
Structure of Payload
Payload Pre Deployment�Configuration Trade & Selection
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Sriram Metta
Payload inside the container, with the servo motor holding on to the container in place
The Folded auto-gyro is put inside the container and the lid was closed .
Natural Position of the wings of the auto-gyro
The wings are folded to be stowed inside the container using springs and hinges
Chosen Pre Deployment Configuration
Payload Deployment
Configuration Trade & Selection
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Sriram Metta
Current Design: |
Alternative Design: |
Payload Deployment Configuration Selection
Rationale: The current design is chosen because of micro servo lightweight and non interference with any other sensors providing better alternative
Using an electromagnetic system for the container opening is a bit more complex. Secondly It needs huge amount of current for this system to work. Again, the presence of electromagnet causes interference in the GPS module and other sensors’ working.
The opening of the container using micro servo motor is simple to make and it’s mechanically more feasible.
Payload Deployment
Configuration Trade & Selection
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Sriram Metta
The Selected design for the payload deployment configuration employes hinges on each wing of the auto-gyro system and the hinges use springs which will try to restore themselves to their natural lengths once the payload is deployed from the container and the springs will straighten the wings thereafter.
PAYLOAD
SPRING MECHANISM FOR FOLDING AND DEPLOYMENT OF PROPELLERS
Electronics Structural Integrity
Container Drop Test Simulation
Stress variation Strain variation
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Sriram Metta
Electronics Structural Integrity
(Simulation)
Payload Drop Test Simulation
Strain Variation Stress Variation
CanSat 2019 PDR: Team 4053 | Lakshya
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Note:-
Drop test simulations were done in ANSYS 16.0 and the results are above.
It shows the structure survives 30Gs of acceleration and 15Gs of shock.
Presenter: Sriram Metta
Electronics Structural Integrity
CanSat 2019 PDR: Team 4053 | Lakshya
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(Experimental)
Drop Test from Drone
Presenter: Sriram Metta
Mass Budget
35
Communication and Data Handling (CDH) Subsystem Design
Raj Kishore Patra
CanSat 2019 PDR: Team 4053 | Lakshya
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Probe Telemetry Format
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Raj Kishore Patra
Telemetry Data
Real Time Plotting |
<ALTITUDE>(m) |
<PRESSURE> (Pa) |
<TEMP>(C) |
<VOLTAGE>(V) |
<GPS ALTITUDE>(m) |
<PITCH> |
<ROLL> |
<BLADE SPIN RATE> (rpm) |
Displayed |
<TEAM ID> |
<MISSION TIME>(s) |
<PACKET COUNT> |
<GPS TIME> |
<GPS SATS> |
<SOFTWARE STATE> |
<BONUS> |
Team Logo
Here
(If You Want)
Electrical Power Subsystem (EPS) Design
Dibyajyoti Jena
CanSat 2019 PDR: Team 4053 | Lakshya
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Payload Electrical Block Diagram
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Dibyajyoti Jena
Power Source(9V)
Switch
Microcontroller (9V)
Voltage Regulator(3.3v)
Audio Beacon (3.3 v)
Power Led(3.3V)
DS1307 (5V)
SD Module
Infrared Sensor
XBEE
CMOS
AdaFruit IMU
UBLOX Neo
Flight Software (FSW) Design
Shubham Sharma
CanSat 2019 PDR: Team 4053 | Lakshya
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Team Logo
Here
Team Logo
Here
(If You Want)
PROBE FSW STATE DIAGRAM
CanSat 2019 PDR: Team 4053 | Lakshya
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Power On
All system initialization
Read data from sensors & collect
Store data to SD card
Send data at 1Hz via XBEEs
Launch?
Is altitude between 670 &725m?
Sensor sampling, telemetry at 1Hz & store data to SD card
Yes
No
State 1:Pre-Launch
State 2: Ascent
Deployment from rocket
Sensor sampling, telemetry at 1Hz & store data to SD card
Is
Alt.=450m?
Release heat shield
Descend under auto-gyro control
& begin capturing video
Is
Altitude=5m
?
Sensor sampling, telemetry at 1Hz & store data to SD card
Release
OK?
Initialize backup release mechanism
Activate audio beacon & stop telemetry
State 3:Descent
No
Yes
No
Yes
Yes
No
System State Recovery:
EEPROM memory will be read in order to recover the state of the software in case of sudden processor resets.
It will also store time for telemetry update
Presenter: Shubham Sharma
Team Logo
Here
(If You Want)
Ground Control System (GCS) Design
Raj Kishore Patra
CanSat 2019 PDR: Team 4053 | Lakshya
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GCS Overview
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Raj Kishore Patra
PROBE
XBEE
HANDHELD
2.4GHz
YAGI
ANTENNA
RP-SMA to SMA ADAPTER
GCS
XBEE
ARDUINO NANO (MPU)
LAPTOP (GUI)
XBEE USB Adaptor Board
GCS Software
Selected prototype of the GUI using LabVIEW.
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Raj Kishore Patra
CanSat Integration and Test
Tapaswin Padhy
CanSat 2019 PDR: Team 4053 | Lakshya
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Subsystem Level Testing Plan
CanSat 2019 PDR: Team 4053 | Lakshya
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DESCENT CONTROL SUBSYSTEM PLAN
Presenter: Tapaswin Padhy
A proposed CanSat design connected to a
Quadcopter for drop test from different heights
A Picture while the CanSat is descending under auto-gyro mechanism.
Subsystem Level Testing Plan
CanSat 2019 PDR: Team 4053 | Lakshya
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DESCENT CONTROL SUBSYSTEM PLAN
Presenter: Tapaswin Padhy
The simulations related to the parachute are done.
The auto-gyro system connected to a dummy container and dropped from an altitude of 30m
Integrated Level Functional Test Plan
The parachute opening, the impact test and the working of the auto-gyro mechanisms will be tested in this test plan. We have some methods such as releasing from a quadcopter or dropping it from the roof of our administration building and from different altitudes.
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Tapaswin Padhy
DESCENT TESTING
Impact test and the working of the auto-gyro mechanism when dropped from a height of about 40 metres.
Management
Arijeet Satapathy
CanSat 2019 PDR: Team 4053 | Lakshya
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Program Schedule Overview
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Arijeet Satapathy
Program Schedule Overview
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Presenter: Arijeet Satapathy
Social Media and Publicity
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Presenter: Arijeet Satapathy
We have our social outreach with a growing number of followers and constant support will help us grow
We Constantly keep updating videos in YouTube to share our daily progress.
Conclusions
Major Accomplishments:
2. Finance was secured.
3. Airline tickets sponsors were found.
4. PDR was completed.
Unfinished Work
The Preliminary Design Phase is complete for Mechanical and Electronics setup. Design and hardware, both are finalized and we are ready to move to the next phase i.e. the Critical Design Phase.
CanSat 2019 PDR: Team 4053 | Lakshya
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Presenter: Arijeet Satapathy