Projectile Motion

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New answer posted•a year ago
S
a year ago

y = α x − β x 2

⇒ d y d x = α − 2 β x = 0

⇒ x = α 2 β

y m a x = α × α 2 β − β × ( α 2 β ) 2 = α 2 4 β

Range = 2 x = α β = 2 u 2 s i n θ . c o s θ g

On comparing with

y = x tan θ - g x 2 2 u 2 c o s 2 θ

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New answer posted•a year ago
S
a year ago

y = x5 (1 – x) = x tan θ (1−xR)

tan = 5, R = 1

sinθ=526, cosθ=126

R=u2sin2θg=1

⇒u2=26⇒u=26m/s

y – component of initial velocity

= u sin θ

= =26×526

= 5 m/s

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

For climbing downward

50 g – T = 50a

T = 500 – 50 * 4

= 300 N < 350 N

for climbing upwards

T – 50 g = 50 a

T – 500 = 50 * 5

T = 750 N > 350 N

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New answer posted•a year ago
S
a year ago

h = 1 2 g t 2

or x = v 2 h g

So, x = vt

or, x = v 2 h g

So, dist of man from helicopter is

h 2 + x 2 = h 2 + v 2 2 h g = 2 v 2 h g + h 2

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New answer posted•a year ago
S
a year ago

First angle, θ1= θ, R = u 2 s i n 2 θ g      

Another angle (θ2 = 90 - θ) for which range will be Same as that of θ1 =θ

R 1 = u 2 s i n 2 ( 9 0 − θ ) g = u 2 g s i n 2 θ = R

at θ 1 = θ ,           h 1 = u 2 s i n 2 θ 2 g

&       θ 2 = 9 0 − θ , h 2 = u 2 s i n 2 θ 2 2 g = u 2 c o s 2 θ 2 g

⇒ h 1 h 2 = 1 4 2 [ u 2 s i n 2 θ g ] 2

h 1 h 2 = 1 4 2 R 2

R = 4 h 1 h 2

So, Both statement is true & Reason is correct explanation for statement 1.

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New answer posted•a year ago
S
a year ago

d = R

6 0 = R [ 3 π 4 ]

R = 6 0 × 4 3 π = 8 0 π m

Displacement = R 2 + R 2 − 2 R 2 c o s 1 3 5

= 2 R 2 − 2 R 2 ( − 0 . 7 )

= 3 . 4 R 2

= 3 . 4 ( 8 0 4 ) 2

47 m

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New answer posted•a year ago
S
a year ago

H=u2sin2θ2g  and  R=u2sin2θg

According to question

R=H⇒u2sin2θ2g=2u2snθcosθg⇒tanθ=4

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

after 2 sec, v = 20 m/sec

v→=ucos45°i^+ (usin45°−gt)j^v=20= (ucos45°)2+ (usin45°−20)2

⇒400=u2+400−40usin45°

u = 40 sin 45°

Hmax=u2sin2452g=402sin245°×sin2452g

=40×402×10×12×12=20m

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