Gravitational Potential and Escape Velocity, Lecture notes of Physics

A comprehensive exploration of gravitational potential, escape velocity, and related concepts in physics. It covers topics such as the universal law of gravitation, gravitational fields, potential energy, and the motion of objects in gravitational fields. Various examples and formulas to illustrate these concepts, making it a valuable resource for students and researchers in physics.

Typology: Lecture notes

2023/2024

Available from 06/04/2024

vikramjeet-rajora
vikramjeet-rajora 🇮🇳

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Gravitation

→ :

Universal law

of gravitation ?'É~ (^) Gravitational face (^) of

attraction

~ b/w these two (^) masses (E)

f ✗^ MIMZ

Fam :# ✗ ¥ f- = Gm~-?÷ G→^ universal^ Gravitational^ comet

9=6.67× 15

" mmHg

Direction of gravitational^ foeee

is

always attractive → ^.

Vector four of universal law^ of (^) gravitation . Y ' am, Ñte→=→z

  • is^ i=ñ_ñ ñ

§ .

M

☐ F- (^) i=μ÷=ri >

×

Hi-FI f%→ force^ due^ to^ mass^ ② on^ mats^ ① f→μ→ ✗ 71 "^ "^ ①^ " (^) In ② ñi-9:;÷_i=G;;÷-¥y=amˢˢlñ-ñ ) F-ñP

Faia ;;÷ =-¥m;÷¥,=-;÷;→ñ fi,=

  • f? So gravitational faeces^ fans^ action reaction (^) pair. force due^ to^ multiple masses Supn# pup : (^) Gravitational fare of attraction b/w any

two masses^ in^

system is independent on presence of

other masses in

system

. but resultant (^) Joke on a mass is^ vector^ fun^ of all^ the^ faeces.

Éet= (^) Ñ+É=fi8G

§) ↑ = -3-

② find location where Inky mess must^ be^ placed on line joining

bar mass So that

experience

net Reece (^). 9.7-a (^) 7.2-a47 liter __

f, 2kg

Fry

R -^ Fz

oh , =

§ (5)

= 3m

G¥#

G←Yj a = ¥

(5) 22m

9-

I z=¥

0 £? Three^ messes^ ace^ placed To (^) on vertices F, of equilateral jF ① ʰf?¥FsF^

Aref side e.^.^ find neem c- a→m force on

any

one of the mass. ☒ HE/^

= Gma

=F

a- (^) fie

  • (^) Ba :'-( ↑ (^) ) ① ② Of M (^) - a -

masses are (^) places on § a^ 7- (^) a

vertices

of square

.^ find 7 Fr ✓zf=F%

net

fake on^ mass^ Ma Mo ¥ ,

F. = Gma7- i Eet (^) = FT^ c-^ FT^ c-^ f)

= a

?_? / (

'ñ)↑+ (

¥r§]

  • %?-(^

E) (^ i + ↑ ) Gravitation field (^) Intensity Mo É

  • , L

Gravitation field Intensity

due to a^ mass at

some (^) distance is fake pee^

wit mais^

placed at that point^ . → É=Gm→- (^) E=f÷

it

IÉ/

GAME unity field (^) %

Ys

Direction of field^

is

always in (^) the (^) direction of force acting on a^ mess^ at^ Thet point .

at

/ Ek G- el

  • m
> I

Eat

-^ it

zing

find

point

i

e' siren.'S 2- honk ' E- on line joining Fe

= EL

| Ig a ¥ 1 liter __^ yo.^ two^ masses where met G (^) field :÷=9÷ (^) is deco . 4=gI(407= dr=3_g( (^48215) -

Plot graph b/w^ field^ due to^ masses^ and^ distance on line joining both mass.es (^) - I (^) I ¥,^ ←^ Er ←Er 25

%

E- (^) É - É = (^0) - G÷(-imE3^ i s¥ E- Gang

m① ( " [③ find net^ field at^ A. a i^ ¥ 1 __^ =aˢ

É at

> E.

,^ =^ *?

' ÷ ) (^) too. > Ez

> F}

1%1--11%

§÷→

> Ey E. =%÷c :^) E- = 9, . ↑ = GIT in Fiera Et^ Et^ Est^ ET +^

  • É mu (^) arm = (^). + (^) EI (^) + ¥
  • (^) ( E. (^) +7,9=+927) ↑

E=fdE= (^) 97-2%1=47-1-1- "

L

=

  • Gy / E- (^) E) = -1% E- a :-, " oil Rod^ of

lined mass

F-

  • (^) l & " density 4--40×^2

'"° ,,

✗=L > (^) ✗

✗◦^ →^ Constant

find field at point

A.

dim -_^ ✗^ die^

≥ Xok2dk

= "%¥÷, 0

field due to

uniform (^) ring at (^) point on^ its^ axis. dm ↑

M→ Total^ mass

grig R ᵈÉ (^) andesite (^) R→ Radius of (^) tiny ◦ dE% 0 I %__ᵈ¥fd☒μ

Is Ñ+Ñ

DE

d

' 'm