College of Engineering

Similar documents
Objective: To launch a soda bottle rocket, achieve maximum time of flight, and safely land a payload (tennis ball).

Today Mr. Happer told us to use the following physics vocabulary words and relate them to our experiment:

Bottle Rockets. The bottle rocket, like the squid, uses water as the driving agent and compressed air instead of heat to provide the energy.

3, 2, 1, Blast Off! Division A 2019

Very Basic Design Considerations for Water-Bottle Rockets

Give Wings to Imagination

Acceleration= Force OVER Mass. Design Considerations for Water-Bottle Rockets

Bottle Rocket Launcher P4-2000

PHYS 101 Previous Exam Problems

PART 1 Rocket Assembly

Materials: Balloon demo (optional): - balloon, string, drinking straw, flour (optional)

Rocket Activity Foam Rocket

Table of Contents. Career Overview... 4

science-u.org How do you launch a rocket without using Air Pressure Rockets Directions You Will Need ESTIMATED TIME Minutes

Stage 2 Stem Project Term 2, Rocket Design. By Willow, Malia and Sofia

Water Rocket. THE Challenge: Teams (of 2) will design, build and test a water rocket designed to. The competition requirements:th TEAM MEMBERS:

WATER ROCK. Lawndart The rocket goes straight up and comes down nose first at high speed. Disadvantages

Fly Rocket Fly: Rocket Report. Hammerhead X 134

Hang Time Detailed Event Description. Hang Time!

Designing a Model Rocket

End of Chapter Exercises

1 Korean-American Scientists and Engineers Association National Mathematics and Science Competition. 1. Raft Rally

3. A fluid is forced through a pipe of changing cross section as shown. In which section would the pressure of the fluid be a minimum?

Learning Objectives. Key Concepts: Momentum, Pressure, Aerodynamic Forces

Experimental Procedure

Bottle Rockets. Division B only

. In an elevator accelerating upward (A) both the elevator accelerating upward (B) the first is equations are valid

Old-Exam.Questions-Ch-14 T072 T071

Ejection. Boost. Descend WIND. Landing. Takeoff

Lecture 19 Fluids: density, pressure, Pascal s principle and Buoyancy.

End of Chapter Exercises

ACTIVITY 1: Buoyancy Problems. OBJECTIVE: Practice and Reinforce concepts related to Fluid Pressure, primarily Buoyancy

CHM Basics of Gases (r14) Charles Taylor 1/9

Fly Rocket Fly: Design Lab Report. Rocket Name: Wavehog Willie 12/21/16

Rocket Activity Using Dependent and Independent Variables. Constructing the Rocket and Launch System Compressor (LSC)

BOTTLE ROCKET. What you need to make one

wind wobble unstable

The Quarter Pounder A Vehicle to Launch Quarter Pound Payloads to Low Earth Orbit

Quiz name: Chapter 13 Test Review - Fluids

Rocket Activity Rocket Wind Tunnel

ROCKET LABTM. Technology. Fins R Roots! 1. LEARN (First class session)

Bicycles 2. Bicycles 1. Bicycles 4. Bicycles 3. Bicycles 5. Bicycles 6

5.0 Neutral Buoyancy Test

Fly Rocket Fly Design Report

Agood tennis player knows instinctively how hard to hit a ball and at what angle to get the ball over the. Ball Trajectories

How to Do Flight Testing for TARC. Trip Barber NAR TARC Manager

High Altitude Deployment Article By Jim Jarvis Rockets Magazine, June 2011 Edited May 2013

Building a Wind Tunnel

Student name: + is valid for C =. The vorticity

Variation of Pressure with Depth in a Fluid *

The water supply for a hydroelectric plant is a reservoir with a large surface area. An outlet pipe takes the water to a turbine.

Slide 5 / What is the difference between the pressure on the bottom of a pool and the pressure on the water surface? A ρgh B ρg/h C ρ/gh D gh/ρ

Perilous Plunge. Activity Guide PITSCO. Ideas Solutions V0708

Payload Construction Guide

Flying High. HHJS Science Week Background Information. Forces and Flight

mass of container full of air = g mass of container with extra air = g volume of air released = cm 3

2 Available: 1390/08/02 Date of returning: 1390/08/17 1. A suction cup is used to support a plate of weight as shown in below Figure. For the conditio

Physics Acceleration and Projectile Review Guide

LAST NAME First Name(s) Student Number Practical Group as on student card as on student card Code

Figure 1. The distance the train travels between A and B is not the same as the displacement of the train.

1. A cannon shoots a clown directly upward with a speed of 20 m/s. What height will the clown reach?

Questions. theonlinephysicstutor.com. facebook.com/theonlinephysicstutor. Name: Edexcel Drag Viscosity. Questions. Date: Time: Total marks available:

1. The principle of fluid pressure that is used in hydraulic brakes or lifts is that:

Pressure is defined as force per unit area. Any fluid can exert a force

1Pressure 2 21Volume 2 2. or Temperature 2. where the subscript 1 signifies the initial conditions and the subscript 2 signifies the final conditions.

Chapter 9 Fluids and Buoyant Force

Slide 1 / What is the density of an aluminum block with a mass of 4050 kg and volume of 1.5 m 3?

2014 Competition Information & Rules

Rockets. After School STEM Academy 6-8 th Grade Curriculum

Lab 12 Standing Waves

SPH 4C Unit 4 Hydraulics and Pneumatic Systems

PYP 001 First Major Exam Code: Term: 161 Thursday, October 27, 2016 Page: 1

Irrigation &Hydraulics Department lb / ft to kg/lit.

CRITICAL DESIGN REVIEW. Plantation High School Team Optics

Experiment 13: Make-Up Lab for 1408/1420

1. All fluids are: A. gases B. liquids C. gases or liquids D. non-metallic E. transparent ans: C

Design Review Agenda

From and

3. How many kilograms of air is in the room?

Rockets. Student Journal. After School STEM Academy

Fly Rocket Fly: Design Lab Report

Regents Exam Practice: Measurement, Kinematics, Free Fall, PJM, and UCM

Lab 12 Standing Waves

Experiment P18: Buoyant Force (Force Sensor)


Page 1

Grandpa's Homemade Rocket for About a Dollar!

Exploration Series. MODEL ROCKET Interactive Physics Simulation Page 01

STEP 1 A. Lay the two Motor Mount Tubes on a flat surface with ends even and Glue them together with White Glue. Allow Glue to set before moving on.

Exercise 2-3. Flow Rate and Velocity EXERCISE OBJECTIVE C C C

Exam 3 Phys Fall 2002 Version A. Name ID Section

Types of Forces. Pressure Buoyant Force Friction Normal Force

5. Find two numbers whose sum is 48 and whose product is to be a maximum.

Static Fluids. **All simulations and videos required for this package can be found on my website, here:

Unit 2 Kinetic Theory, Heat, and Thermodynamics: 2.A.1 Problems Temperature and Heat Sections of your book.

Applications of Bernoulli s principle. Principle states that areas with faster moving fluids will experience less pressure

The Effect of Twisting Helicopter Blades at an Angle On Duration

3-2-1 POP! Primary Audience: 3 rd 10 th Grade

LAB 7. ROTATION. 7.1 Problem. 7.2 Equipment. 7.3 Activities

Gases. Unit 10. How do gases behave?

Transcription:

College of Engineering Department of Mechanical and Aerospace Engineering MAE-250, Section 001 Introduction to Aerospace Engineering Final Project Bottle Rocket Written By: Jesse Hansen Connor Petersen Jeffrey Balog Date Report Submitted: 12/01/2016

Idea Development: Initial Ideas to Final Concept Through online research and course materials, several bottle rocket designs were proposed, analyzed, and discussed within our group. Our primary concern was obtaining stable flight by ensuring the center of pressure stayed below the center of mass (to prevent the rocket from spinning out of control) and through adding fins to the base of the rocket. We selected a basic 2 liter pop bottle as the pressure chamber and removed the label to reduce drag. A non-contoured bottle was used as it provided a flat surface to attach fins to and with the aid of a nose cone, could be very aerodynamic. To maximize the launch height we used a piece of packaging tape to wrap a compression dressing around the pop bottle s label area on the pressure vessel as this would help keep the bottle s walls from expanding as the air was pumped into it. We then grappled with how to maximize our hang time while delivering our payload (an egg) safely to the ground. Initially we tried to attach a small container containing the egg and built from a second two liter bottle directly to the top of the pressure chamber using tape. This method eliminated the possibility of using a parachute to lengthen the rocket s hang time and also removed any chance of receiving points for the complete detachment of the payload. We then looked for ways to include a parachute, primarily a sleeve attached to the top of the pressure vessel, that could contain the parachute with the egg capsule resting on top. This method relies on the weight of the egg to dislodge the payload container from the sleeve and deploy the parachute at the rocket s peak altitude. Figure 1 loosely demonstrates this concept:

Figure 1: Initial Rocket Design After construction of this rocket, it was discovered that the egg capsule routinely got jammed in the sleeve containing the parachute, preventing the separation of the payload and deployment of the parachute. To counteract this issue we decided to create the sleeve from a contoured 2 liter pop bottle. The contoured shape would allow the egg capsule to rest in the sleeve without becoming jammed further (see figure 2). Figure 2: Initial Rocket Design with Contoured Sleeve The contoured sleeve design reduced the number of instances of the egg capsule becoming stuck in the sleeve and helps ensure complete separation of the egg capsule and subsequent deployment of the parachute. Our next concern was with the egg capsule itself and designing a system that would allow the egg to remain intact throughout the entire launch, flight, and impact. Our initial instinct was to pad the inside of the capsule with bubble wrap, but the materials list did not include bubble wrap or anything similar. We then set out with a piece of posterboard (or cardboard) and created a cardboard tube (similar to the inner cardboard tube on paper towels or toilet paper) with a diameter that would allow an egg to pass through the tube. This tube kept the egg from sliding horizontally but not vertically (if the tube were positioned vertically - as seen in figure 3). To ensure the egg remained stationary vertically and horizontally, four holes were created on the side of the tube and rubber bands passed through the tube. The egg was then placed in the tube, resting on the rubber bands, and the process repeated a second time to secure the egg from

above. The tube was then cut to a height that would sit securely in the egg capsule. Figure 3 shows the egg capsule: Figure 3: Breakdown of Egg Capsule With an egg capsule in mind, we began looking into parachute design. To maximize our hang time and slow the descent of the egg capsule as much as possible we wanted a parachute with the largest surface area possible. We tested two parachute shapes and decided to use a circular shaped parachute attached using braided nylon cord. Each point where the string attached to the parachute was reinforced with tape to avoid tearing through the parachute during deployment. Figure 4: Parachute Design Lastly, we required some method for stabilizing the rocket during launch. We briefly considered attaching a small, hollow, cardboard cylinder to the side of the rocket, through which a metal rod could be passed through and secured into the ground. This

would provide a guide for the rocket to launch straight upwards. However, we instead opted to use fins as they re more reliable and do not require a metal rod (metal was forbidden in the project statement). Research was required to determine the best shape and placement for fins on a rocket and it was discovered that the best placement for the fins is as far back on the bottle rocket as possible. We placed the fins approximately 9 cm from the base and used three fins (instead of four) as three provides a lot of stabilization while minimizing the drag. In addition, we wanted to avoid adding any unnecessary weight to the rocket and especially to the bottom of the rocket as it is imperative the center of mass of the rocket be above the center of pressure. The fins were chosen to be small relative to the bottle rocket size, so there would be a decrease in drag and an increase in performance. Cardboard was chosen as the material for the fins because of its low weight and high sturdiness. Finally to finish off the design of our fins, we chose to tape the front and sides of all three fins. This will create a more streamlined airfoil body for our fins similar to the airfoil shape for a realistic rocket s fin. The streamlined body for a fin s airfoil allows the rocket to experience less drag as it tries to escape from Earth s atmosphere while providing some protection from potential poor weather. We then moved on from the designing portion of the fins to the attachment phase. All three fins were separated 120 o from each other and directed in a swept back position. They were then attached to the body of the bottle rocket by splitting the ends along the right side on the cardboard crafted fin. The split ends allowed there to be more surface area for the fin to be attached to the bottle rocket. Initially we attached the fins with super glue but later realized that during the pressurizing phase of pre-launch, the expanding walls of the pressure vessel posed the possibility of popping the glue seal and causing the wings to be ripped off during ascension. We then decided to use tape to attach the rocket s fins. Figure 5 shows an outline of the rocket with fins attached.

Figure 5: Rocket Set Up with Fins Experimental Procedure to Tune Concept: In order to tune our initial ideas into the final concept for the bottle rocket design, we had to test multiple designs for both the parachute and containment center for the egg in the capsule. We tested two parachute shapes: rectangle and a circle, by tossing the parachute and capsule off the third floor balcony inside Engineering Building 3. When we tested the rectangular parachute, the egg had a fast descent and wobbled vigorously back and forth, exhibiting a very unstable descent that could result in a damaged egg. We discovered that a circular parachute worked best for safely delivering the capsule to the ground as it had a steadier flight path and a longer hang time in the air. Once we figured out the best shape for the parachute, we also had to test the best method on the containment center for the egg. We tested the several different capsules with the egg inside by dropping the egg capsule and parachute off the third floor balcony inside Engineering Building 3. We experimentally determined the best egg capsule to be one that used a paper towel roll and rubber bands cut to secure the egg. Unfortunately we did not have a means for testing the rocket as a whole prior to the actual launch. To compensate we mathematically determined a few key things as shown below.

Mathematical Performance Estimates Bottle Rocket Performance Estimates To optimize our rocket s performance we performed a mathematical analysis of the system to determine several characteristics of our rocket s flight path and flight time. The constants used in these calculations can be found in Table 1. Table 1: Powered Ascent Constants Used in Calculations Variable Metric Units Relevant English Units Gage Pressure at Launch Time, P 0 Water Density, ρ Initial Air Volume in Pop Bottle, V 0 Atmospheric Pressure, P atm Diameter of Pop Bottle Hole, D h Diameter of the Pressure Cylinder, D r Mass of the Rocket, M r V r dv dm 4.137e5 Pa 1000 kg/m^3 1.13e-3 m^3 1.013e5 Pa 2.2 e-2 m.1088 m 1 kg 2 e-3 m^3 3e-5m^3 3e-2 kg 60psi

To start off, the velocity of the water leaving the bottle rocket, u, was calculated using Equation 1. The initial air volume in the pressure cylinder was 1.13e-3 m 3, which is 65% of the 2 Liter bottle (45% filled with water). A change in volume of.03 Liters (3e-5 m 3 ) was selected and the value V for each iteration was found by adding the change in air volume to the previous air volume. Equation 1 models this relationship where all variables can be found in Table 1. Equation 1 The total change in volume of the air in the pressure cylinder was then calculated using the values obtained from Equation 1 plugged into Equation 2. ΔV 1 2 ΔT = 4 υπdr ΔV ΔT = 1 uπd 2 4 h Equation 2 The change in velocity for each iteration was then calculated using Equation 3 where a C D value of 0.3 was used and the area of the pressure chamber found using the known diameter and height of the bottle. The change in mass was determined by multiplying the density of water by the consistent change in volume. was replaced with the particular iteration s value of u calculated in the first step and M is the mass of the rocket. The calculated change in velocity was added to the last iteration of velocity to update the velocity of the bottle rocket. V f ( mg C AρV )Δt + Δm(V +V ) 2 d Δ V = M 1 2 f Equation 3 Finally, the total time taken for the powered ascent was calculated by adding the change in time to the previous time iteration and the total time for this stage was calculated to be 0.112 seconds.

The additional height gained after the powered ascent stage can then be calculated using the following equation: V 2 f = V 2 i + 2 * a * Δ y Equation 4 Where V f is the final velocity of the coasting stage (zero) and V i is the initial velocity of the coasting stage (also the final velocity of the powered stage which was calculated to be 10.16 m/s). The additional vertical distance travelled after the powered ascent is then calculated to be 5.26 meters and the total time of this period calculated using the following equation: V f = V i + a * t Equation 5 The time for this period was calculated to be 1.03 seconds. These calculations were carried out in an excel spreadsheet which is shown below in Figure 6. All the units are SI units. Figure 6: Figure depicting excel spreadsheet used to carry out the iterative calculations. SI Units.

Discussion of Estimates Right after the bottle rocket launches, the velocity of the water coming out of the bottle is highest and decreases as time goes on and less water is left in the bottle. For this reason, the change in volume over the change in time decreases as time goes on. Effectively, the flow rate of the water out of the bottle decreases as time passes. The change in velocity just as the rocket launches is largest, and therefore the acceleration is greatest just when the rocket launches and decreases as time goes on and as the rocket runs out of fuel. The maximum velocity that the rocket is projected to achieve is about 10.3 m/s. After the powered ascent stage, there is a period where the bottle will continue to gain height in the coasting ascent stage. It was calculated that the rocket will travel an additional 5.26 meters in this stage, for a calculated 1.03 seconds. Dimensioned Drawings:

Figure 7: Final, dimensioned drawing of bottle rocket showing breakdown of each part from an exterior view.

Figure 8: Dimensioned Drawing of Parachute and Egg Capsule Interior Sources: https://sites.google.com/site/gjhsrockets/building