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Term Project Presentation on Dec. 9

(To volunteer, drag and drop your slides as images

by 23:59 pm, Sat, Nov. 30, 2019.)

6-page limit including the title page.

You will later have a chance to modify your slides

if selected to present.

DO NOT MAKE DOCUMENT-WIDE CHANGES SUCH AS CHANGING THE MASTER BACKGROUND!

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Student Name: 유진우

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Student Name : 곽호성

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Student name: 김도연

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Student name: 변성민

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Student name: 고광현

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Student name: 김형모

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Student name: 고성민

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Student Name: 김성수

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Dancing t-handle

2019-19668 김성수

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Dancing t-handle

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EOM

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EOM

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NUTATION PERIOD

초기 각속도에 반비례

초기 각속도에 반비례 각운동량의 미소 변화량에 의존하지 않음

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NUTATION PERIOD

p=I2/I3 에 대해 복잡한 형태로 증가

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Student Name : 백두현

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Student Name: 황준상

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우주선의 궤도

물리천문학부 황준상

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고려할 점

  • 중심력
  • 중력 편차
  • 지구 자전
  • 공기 저항
  • 태양 복사압

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지구 중심 궤도

  • LEO
  • GPS
  • GEO
  • 몰니냐
  • 태양동기
  • 정지 궤도

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달 탐사 궤도

  • 지구 대기궤도
  • 달 전이궤도
  • 달 도착궤도

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화성 탐사 궤도

  • 지구 이탈 궤도
  • 화성 도착궤도
  • 화성 전이궤도

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감사합니다

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Student name: 김기완

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Student name: 김현용

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우주항공공학과 2018-19828 김현용

Calculating The Trajectory

Including The Coriolis force with python!

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Missile and Rocket

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Recap: Coriolis Effect

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Problem 10.18�Battle of the Falkland Islands

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Problem 2.6-bale of hay

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Coriolis Effect In Neutron star

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Student name: 황은오

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Student name: 김다솔

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Student name: 박희인

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Terminology

•Euler angles

  • Why 321 Euler Angles?

•Reference Frames

  • Why not Principal Axes?

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Equations of Motion

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Dynamic Characteristics of Aircrafts

•Longitudinal: Short Period & Phugoid

•Lateral: Spiral, Rolling, Dutch Roll

https://www.youtube.com/watch?v=Zmjam1evDD4

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Including Feedback Control

•Control Surface depends on attitude

•Kind of passive Control System

https://www.youtube.com/watch?v=XWhGjxdug0o

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Student name:김태호

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Thermal Conduction in 2D Lattice Using the Loaded String Model

Dept. of Physics & Astronomy

Taeho Kim

https://www.youtube.com/watch?v=OoKDC1AMMwg

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https://www.youtube.com/watch?v=OoKDC1AMMwg

MATLAB!!

 

 

 

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https://www.youtube.com/watch?v=OoKDC1AMMwg

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https://www.youtube.com/watch?v=OoKDC1AMMwg

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https://www.youtube.com/watch?v=OoKDC1AMMwg

p=0.15

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https://www.youtube.com/watch?v=OoKDC1AMMwg

Q&A

Thank You!

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Student Name : 김재환

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More Examples and Codes are in Github: https://github.com/sshskjh/Physics-Engine

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Student name: 조성주

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Student Name: 고상범

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Stability and Modes of Aircraft’s Oscillatory Motion,

and How to Counteract

Dept. of Physics and Astronomy

Ko Sang Bum

2019.12.9

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Lift and Basic Aircraft Structure

Caused by pressure difference

Depends on Angle of Attack (AOA)

Acts on Center of Pressure (CP)

CP moves forward as AOA increases

Fuselage, Wing, Vertical and Horizontal Stabilizers

Lift, Drag, Weight, Thrust: 4 Forces

Rotates about COM, Torques on each CPs

Pitch: Elevators Roll: Ailerons Yaw: Rudders

From FAA Pilot’s Handbook of Aeronautical Knowledge, Public Domain

Lift

Aircraft Structure

(Only for Airfoils)

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Longitudinal (Pitch) Oscillatory Motion

Long Period Mode, Big Altitude Change

Exchange between potential energy and kinetic energy

Very small damp, easy to counter

Dangerous when left uncontrolled

Shorter period.

Heavily damped primarily due to horizontal stabilizers

Least concern for pilot

Phugoid Mode

Short Period Mode

Phugoid osc., From Wikipedia user “Andrzejmat”, released as Public Domain

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Lateral (Roll & Yaw) Motion Modes and Coupling

Role Damping Mode

Damp of high roll rate

No restoration force

Spiral Mode

Coupled, Divergent or poorly damped

Slow buildup, easy to counter

Dangerous when unattended

Dutch Roll Mode

Coupled, cause dizziness

In straight wings, heavily damped In other wings, small damp or no damp

Stressful to counter

Small Period

From Wikipedia user, “Picascho”, released as Public Domain

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Pilot’s Actions and Instruments to Damp Motions

Wrong technique can worsen the Motions!!!

Do NOT blindly Counteract the displacement!

Expect lag

Sometimes rough control input creates another oscillations

Engine effects (torques, airflows) considered

Instruments such as Roll Dampers and Fly by Wire system (computer assist) help pilots

Example of technique. US Air Force, Public Domain

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Conclusion (and other materials)

Longitudinal:

Lateral:

Some simplification

Is possible.

Equations of Motion: , where normal modes are from: =0 where Matrices are:

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Student name : 이정현

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Order of magnitude: λ~ 2cm~2m

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Student Name: 박진우

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Student Name : 정승원

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N=1, 111Hz(max)

N=2, 68Hz(max)

N=3, 49Hz(max)

N=4, 38Hz(max)

N=5, 31Hz(max)

N=6, 30Hz(max)

N=7, 24Hz(max)

N=8, 21Hz(max)

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Student name : 권의준

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Student name: 서원우

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Student name: 이강민

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Student name: 손호성

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Student name: 이준영

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How does a Sphere Oscillate?

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Hydrodynamics in solar interior

Nodes and normal mode

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Python Plot: Solar model

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Lamb & Buoyancy Frequency

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Oscillation Modes

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Student name: 정정우

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여기까지 쓸게요

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Student name: 김한솔

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Student name: 심진우

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Student name: 정은우

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Student name: 김세훈

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Motion of the Tippe Top

물리천문학부 2018-19745 김세훈

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What is the Tippe Top?

-구 모양의 몸통과 막대기 모양의 손잡이를 가진 팽이

-팽이를 돌리면, 대칭축이 서서히 기울어지고, 결국, 뒤집어진 채로 돌게 된다.

관련 영상: https://www.youtube.com/watch?v=AyAgeUneFds

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step1-

-유효 퍼텐셜

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step2-

-오일러 운동 방정식

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step3-

-유효 퍼텐셜

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Conclusion

-유효 퍼텐셜 그래프를 이용해 Tippe Top의 운동을 설명할 수 있었다.

-step1에서 유효 퍼텐셜로부터 θ가 증가하는 것을 확인하였다.

-step2에서 Tippe Top이 뒤집어질 조건을 확인하였다.

-step3에서 유효 퍼텐셜로부터 θ가 증가하다 감소하는 것을 확인하였다.

-마찰력을 고려한다면 보다 정확한 논의가 가능하다.

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Student name: 김상하

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