This document discusses key concepts related to projectile motion. It defines a projectile as an object that is thrown or projected such that it moves through the air in a parabolic path, affected only by gravity. It notes that the horizontal motion of a projectile is independent of its vertical motion affected by gravity. It then provides equations for projectile motion relating variables like displacement, velocity, acceleration due to gravity, and time.

2. kpman (ho-Un-tbm)

3. XcwKNew
am[y-a-¯nsâ Hcp `mK-¯p-­m-
Ip¶
hnt£m`w aäp `mKങ്ങfnte¡v hym]n-¡p¶
coXn

4. Ap-{ ]Ø XcwKങ്ങÄ
am[y-a-¯nse IWn-I-I-fpsS I¼w
Xcw-K-¯nsâ k©mc Znibv¡v ew_w

5. Ap-{ ]Ø XcwKw, Xcw-K-N-ew (hoUntbm)

6. Ap-{]Ø XcwK¯nsâ Ne {]tXy-IX
Hcp XcwKw DuÀÖs¯ am[y-a-¯nsâ Hcp
`mK¯p n¶v asämcp `mK-t¯-¡v F¯n-¡p-¶p.
am[y-a-¯nse IW-MvMÄ¡v Xcw-K-N-e Zni-bnÂ
ØmmvXc New D­m-
hp-¶n-Ã.

7. BbXn
Xpe Øm-¯p-n¶pÅ ]c-am-
h[n AIew

8. XcwKssZÀLyw ( )
kam I¼-m-h-Ø-bn-epÅ ASp-¯-Sp¯ c­p
_nμp-¡Ä X½n-epÅ AIew

9. Bhr¯n
Hcp sk¡³n-ep-­m-
Ip¶ Xcw-K-MvMfpsS
F®-amWv Bhr-¯n. (f)

10. ka-hmIyw
V = f
V = XcwK { ]thKw
f = Bhr¯n
= XcwK ssZÀLyw

11. D¯cw ]d-bpI
XcwKNew F¶m Fന്ത്?
Ap-{ ]Ø XcwKw F¶m Fന്ത്?

12. XcwK {]thKw 20 m/s Dw
XcwK ssZÀLyw 20 m/s Dw
Bb Xcw-K-¯nsâ Bhr¯n F{X?