Untitled Flashcards Set

Recap of the course to date 2 Definition and Formula sheet Formulas β€’ 𝑣 𝑑 =𝑣 , +π‘Žπ‘‘ β€’ π‘₯𝑑 =π‘₯+𝑣 , 𝑑+β„π‘Žπ‘‘ β€’ 𝑣 , =𝑣 , +2π‘Žβˆ†π‘₯ β€’ 𝑔= 9.8 m/sΒ² β€’ βˆ†βƒ— 𝑝=βƒ— π‘βˆ’βƒ— 𝑝=0 β€’ βˆ†π‘ˆ =π‘šπ‘”βˆ†π‘¦ Definitions β€’ βˆ†βƒ— π‘Ÿβ‰‘βƒ— π‘Ÿ βˆ’βƒ— π‘Ÿ=βƒ— π‘Ÿ(𝑑)βˆ’βƒ— π‘Ÿ(𝑑) β€’ βƒ— 𝑣≑ lim βˆ†β†’ βˆ†βƒ— βˆ† 𝑣=βƒ— 𝑣 =βˆ†βƒ— βˆ† β€’ π‘Ž=βƒ— π‘Ž β‰‘βˆ† βˆ† β€’ βƒ— π‘β‰‘π‘šβƒ— 𝑣 β€’ Kβ‰‘β„π‘šπ‘£ β€’ E≑K+Eint β€’ Emech≑K+U 3 Definition and Formula sheet Formulas β€’ 𝑣 𝑑 =𝑣 , +π‘Žπ‘‘ β€’ π‘₯𝑑 =π‘₯+𝑣 , 𝑑+β„π‘Žπ‘‘ β€’ 𝑣 , =𝑣 , +2π‘Žβˆ†π‘₯ β€’ 𝑔= 9.8 m/sΒ² β€’ βˆ†βƒ— 𝑝=βƒ— π‘βˆ’βƒ— 𝑝=0 β€’ βˆ†π‘ˆ =π‘šπ‘”βˆ†π‘¦ Definitions β€’ βˆ†βƒ— π‘Ÿβ‰‘βƒ— π‘Ÿ βˆ’βƒ— π‘Ÿ=βƒ— π‘Ÿ(𝑑)βˆ’βƒ— π‘Ÿ(𝑑) β€’ βƒ— 𝑣≑ lim βˆ†β†’ βˆ†βƒ— βˆ† 𝑣=βƒ— 𝑣 =βˆ†βƒ— βˆ† β€’ π‘Ž=βƒ— π‘Ž β‰‘βˆ† βˆ† β€’ βƒ— π‘β‰‘π‘šβƒ— 𝑣 β€’ Kβ‰‘β„π‘šπ‘£ β€’ E≑K+Eint β€’ Emech≑K+U β€’ 𝑣 𝑑 =𝑣 , +π‘Ž 𝑑 β€’ 𝑦𝑑 =𝑦+𝑣 , 𝑑+β„π‘Ž 𝑑 β€’ 𝑣 , =𝑣 , +2π‘Žβˆ†π‘¦ 4 11/23/20 Chapters 1-3 β€’ Essentially describing motion Β§ Displacement Β§ Velocity Β§ Acceleration β€’ Predictive tool: kinematic equations (for constant acceleration) Chapter 4: Momentum β€’ Observation: before and after collisions π‘š π‘š =βˆ’βˆ†π‘£ βˆ†π‘£ β€’ Concept introduced: momentum βƒ— 𝑝 ≑ π‘šβƒ— 𝑣 β€’ System defined Β§ Isolated system: where momentum is conserved. 5 6 Chapter 5: Kinetic Energy β€’ Observation: reversible and irreversible collisions Β§ Elastic and inelastic collisions β€’ Concept: kinetic energy K ≑ β„π‘šπ‘£ β€’ Closed system: conservation of energy Chapter 7: Interactions β€’ Observation: disappearing kinetic energy β€’ Elastic and inelastic collisions β€’ Concept: potential energy Β§ Gravitational Β§ Elastic 7 β€’ Conservation of mechanical energy (Emech ≑ K+U): βˆ†Emech = 0 8 2 11/23/20 3 Going forward β€’ Combined description β€’Why do we need another description?? 9 2 steps 1) transfer of momentum (at contact) 2) KβŸΊπ‘ˆ Non-dissipative interaction: reversible (Newton’s cradle keeps going and going) 10 2 steps 1) transfer of momentum (at contact) 2) KβŸΊπ‘ˆ Non-dissipative interaction: reversible (Newton’s cradle keeps going and going) Would it keep going forever? Why would it stop? 11 23 steps 1) transfer of momentum (at contact) 2) KβŸΊπ‘ˆ Non-dissipative interaction: reversible (Newton’s cradle keeps going and going) Would it keep going forever? Why would it stop? β€’ Seems non-dissipative on short timescales β€’ Does not carry on forever β€’ Actually dissipative interactions Β§ Air resistance (friction) 12 11/23/20 4 Going forward β€’ Combine everything into one theory Β§Newtonian Mechanics aka Newton’s laws Β§Not covering everything in detail Β§Concept introduced: forces 13 Forces β€’ Abstract concept Β§Does not cause the motion... Β§Motion is caused by objects, but ... Β§Objects exert forces β€’ Thus forces can describe the motion Β§Much more versatile description, Β§Every object is treated on same footing Β§Irrespective of physical attributes 14 PHYS101 Pedagogy Knowing and understanding β€’ Knowing Newton’s Laws is differ from understanding them Delayed introduction of forces and Newton’s Laws to β€’ give a fuller picture, β€’ in-depth motivation, β€’ make the application more intuitive. 15 Recap of the video β€’ Orientation with regards what we have done, and, β€’where we are going. 1