Motion in a Plane

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New answer posted

2 months ago

0 Follower 3 Views

V
Vishal Baghel

Contributor-Level 10

R = l θ

T i m e = 4 * 2 π R V = 4 * 2 π x V ( l θ )

Time = 4 * 2 π * 4 . 4 * 9 . 6 4 * 1 0 1 5 8 * 1 . 5 * 1 0 1 1 * 4 3 6 0 0 * π 1 8 0

T i m e = 4 . 5 * 1 0 1 0 s o c s

New answer posted

2 months ago

0 Follower 3 Views

V
Vishal Baghel

Contributor-Level 10

Let's say | O A | = | O B | = | O C | = l

O A = l c o s 3 0 ° i ^ + l s i n 3 0 ° j ^

O A + O B O C

= [ l c o s 3 0 ° i ^ + l s i n 3 0 ° j ^ ] + [ l c o s 6 0 ° i ^ + l s i n 6 0 ° ( j ^ ) ] [ l c o s 4 5 ° ( i ^ ) + l s i n 4 5 ° ( + j ^ ) ]

= l ( 3 2 + 1 2 + 1 2 ) i ^ + l [ 1 2 3 2 1 2 ] j ^

t a n θ = l [ 1 2 3 2 2 2 ] l [ 3 2 + 1 2 + 2 2 ] = 1 3 2 1 + 3 + 2

New answer posted

2 months ago

0 Follower 2 Views

R
Raj Pandey

Contributor-Level 9

First angle, 1 = R = u 2 s i n 2 ? g

 

Another angle (2 = 90 - ) for which range will be

Same as that of 1 =

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

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

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

? h 1 h 2 = 1 4 2 [ u 2 s i n 2 ? 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.

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

  | A ^ + B ^ | = A 2 + B 2 + 2 A B c o s θ

= 1 + 1 + 2 c o s θ

= 2 ( 1 + c o s θ )

= 2 * 2 c o s 2 θ 2

| A ^ + B ^ | = 2 c o s θ 2  -(1)

| A ^ B ^ | = A 2 + B 2 2 A B c o s θ

= 1 + 1 2 c o s θ

= 2 s i n θ 2  -(2)

(2) ÷  (1)

| A ^ B ^ | | A ^ + B ^ | = 2 s i n θ 2 2 c o s θ 2

| A ^ B ^ | = | A ^ + B ^ | t a n θ 2

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

A * A = A A s i n θ n ^

= A A s i n 0 ° n ^

= 0 [since Angle between the vectors are zero degree]

A * A = 0

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

We know that horizontal speed will remain constant

20 cos = v cos ……… (i)

Along y-axis

U y = 2 0 s i n α , V y = v s i n β

V y = V y + a y t

V s i n β = 2 0 s i n α 1 0 * 1 0  ……. (ii)

( i i ) ÷ ( i )

t a n β = t a n α 5 s e c α

 

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

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

New answer posted

2 months ago

0 Follower 3 Views

A
alok kumar singh

Contributor-Level 10

| P ? + Q ? | = | P ? |

P 2 + Q 2 + 2 P Q c o s ? θ = P 2

Q + 2 P c o s ? θ = 0

c o s ? θ = - Q 2 P

t a n ? α = 2 P s i n ? θ 2 P c o s ? θ + Q =

? [ 2 P c o s ? θ + Q = 0 ]

α = 90 ?

 

New answer posted

2 months ago

0 Follower 5 Views

V
Vishal Baghel

Contributor-Level 10

From conservation of Energy

1 2 m v 0 2 = m g h

v 0 = 1 0 2

For A to B

a = g s i n 4 5 ° = 1 0 2

T = t1 + t2

= 2 2 + 2 = 2 ( 2 + 1 )

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

R = u 2 s i n ( 2 * 4 5 ° ) g = u 2 g

R 2 = u 2 2 g = u 2 s i n 2 0 g

s i n 2 θ = 1 2

2 θ = 3 0 ° θ = 1 5 °

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