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New answer posted

11 months ago

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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 question posted

11 months ago

0 Follower

New answer posted

11 months ago

0 Follower 4 Views

V
Vishal Baghel

Contributor-Level 10

In galvanometer

( l l g ) S = l g G

I g l = S S + G

1 3 = S S + G S + G = 3 S G = 2 S

New answer posted

11 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

μ B = C v B

v B = 3 * 1 0 8 1 . 4 7 = 2 0 . 4 0 8 * 1 0 7

v A = 2 . 6 * 1 0 7 + 2 0 . 4 0 8 * 1 0 7 = 2 3 * 1 0 7

μ B = C v B & μ A = C v A

= 1.127

1 . 1 3

New answer posted

11 months ago

0 Follower 4 Views

A
alok kumar singh

Contributor-Level 10

Δ z z = 2 Δ A A + 3 Δ B B + 4 Δ C C

New answer posted

11 months ago

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V
Vishal Baghel

Contributor-Level 10

Optical fibre frequency range is 1 THz to 1000 THz.

New answer posted

11 months ago

0 Follower 1 View

V
Vishal Baghel

Contributor-Level 10

Very small change in minority charge carriers produces high value of reverse bias current.

New answer posted

11 months ago

0 Follower 3 Views

V
Vishal Baghel

Contributor-Level 10

  v z n

  v = k z n [K constant]

for 3rd orbit of He+

v H e + = k * 2 3 = 2 k 3  - (1)

v H = k * 1 3 = k 3  - (2)

v H e + v H = 2 : 1

New answer posted

11 months ago

0 Follower 11 Views

A
alok kumar singh

Contributor-Level 10

Y ->And gate

A

B

Y

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1

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New answer posted

11 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

Velocity of light in medium 2

= 1 μ m m

v 2 = 1 μ 0 μ r 0 r

= 1 1 * μ 0 0 * 4

v 2 = 1 2 μ 0 0

By snell's law for total internal Reflection

μ 2 s i n θ C > μ 1 s i n 9 0 °

θ c > 3 0 °

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