physics ncert solutions class 11th

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New answer posted

5 months ago

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Vishal Baghel

Contributor-Level 10

Length of the pipe, l = 20 cm = 0.2 m

Source frequency = nth normal mode frequency is given by the relation

νn = (2n-1) ν4l , n is an integer = 0,1,2,3, ….

430 = (2n-1) *3404*0.2

n = 1

Hence, the first mode of vibration frequency is resonantly excited by the given source. In a pipe open at both ends, the nth mode of vibration frequency is given by the relation:

νn=nv2l , n = 2lνnv = 2*0.2*430340 = 0.5

Since the number of the node of vibration (n) has to be an integer, the given source does not produce a resound vibration in an open pipe.

New answer posted

5 months ago

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Vishal Baghel

Contributor-Level 10

Length of the steel rod, l = 100 cm = 1 m

Fundamental frequency of vibration,  ν = 2.53 kHz = 2.53 *103 Hz

When the rod is plucked at its middle, an antinode (A) is formed at the centre, and the nodes (N) are formed at its two ends, as shown in the figure.

The distance between two successive nodes is λ /2

l = λ/2 λ = 2l = 2 m

The speed of sound in steel is given by the relation

v = νλ = 2.53 *103*2 = 5.06 *103 m/s = 5.06 km/s

New answer posted

5 months ago

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Vishal Baghel

Contributor-Level 10

Frequency of the tuning fork,  ν = 340 Hz

Since the given pipe is attached with a piston at one end, it will behave as a pipe with one end closed and the other end open, as shown in this figure.

l1 = λ4, wherelength of the pipe l1 = 25.5 cm = 0.255 m

λ=4l1 = 4 *0.255 m = 1.02 m

The speed of sound is given by the relation, v = νλ = 340 *1.02 = 346.8 m/s

New answer posted

5 months ago

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V
Vishal Baghel

Contributor-Level 10

Mass of the wire, m = 3.5 *10-2 kg

Linear mass density,  μ=ml = 4 *10-2 kg/m

Frequency of vibration,  ν = 45 Hz

Length of the wire, l = mμ = 3.5*10-24*10-2 = 0.875 m

The wavelength of the stationary wave λ = 2ln , where n = number of nodes in the wire

For fundamental node, n = 1,  λ = 2l = 2 *0.875=1.75m

(a) The speed of the transverse wave in the string is given as v = νλ = 45 *1.75 = 78.75 m/s

 

(b) The tension produced in the string is given by the relation, T = v2μ =  (78.75)2 * 4 *10-2 = 248.06 N

New answer posted

5 months ago

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V
Vishal Baghel

Contributor-Level 10

(a) The given equation represents a stationary wave because the harmonic terms kx and ωt appear separately in the equation.

 

(b) The given equation does not contain any harmonic term. Therefore, it does not represent either a travelling wave or a stationary wave.

 

(c) The given equation represents a travelling wave as the harmonic terms kx and ωt are in the combination of kx – ωt .

 

(d) The given equation represents a stationary wave because the harmonic terms kx and ωtapearseparately in the equation. This equation represents the superposition of two stationary waves.

New answer posted

5 months ago

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Vishal Baghel

Contributor-Level 10

(i)

(a) All the points on the string oscillates with the same frequency, except at the nodes, which have zero frequency

 

(b) All the points in any vibrating loop have the same phase, except at the nodes.

 

(c) All the points in any vibrating loop will have different amplitudes of vibration.

(ii)

The given equation is: y (x, t) = 0.06 sin ( 2π3x) cos (120 πt)

For x = 0.375 and t =0

Amplitude = Displacement = 0.06 sin ( 2π3**0.375) cos (0 ) = 0.06sin ( π4) = 0.042 m

New answer posted

5 months ago

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Vishal Baghel

Contributor-Level 10

(a) The general equation representing a stationary wave is given by the displacement function y(x,t) = 2asin kx cos ωt

The equation is similar to the give equation y(x, t) = 0.06 sin ( 2π3x) cos (120 πt)

Hence, the given function represents a stationary wave.

A wave travelling along the positive x-direction is given as: y1 = asin ( ω t – kx)

The wave travelling along the negative x-direction is given as: y2 = asin ( ω t + kx)

 

(b) The superposition of these two waves yields:

y = y1+y2 = asin ( ω t – kx) + asin ( ω t + kx)

= a sin( ω t)cos(kx) – a sin(kx)cos(&nbs

...more

New answer posted

5 months ago

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Vishal Baghel

Contributor-Level 10

The equation for a travelling harmonic wave is given by

y(x, t) = 2.0 cos 2 π (10t – 0.0080 x + 0.35) or

= 2.0 cos (20 π t – 0.016 π x + 0.70 π )

Comparing with classical equation y (x, t) = a sin?(ωt+kx+φ) , we get

Amplitude a = 2.0 cm. Propagation constant, k = 0.016 π , angular frequent, ω=20πrad/s

From the relation φ=kx=2πλx

(a) For x = 4 m = 400 cm, we have φ = 0.016 π*400 = 6.4 π rad

 

(b) For x = 0.5 m = 50 cm, we have φ = 0.016 π*50 = 0.8 π rad

 

(c) For x = λ2 , we have φ=2πλ* λ2 = π rad

 

(d) For x = 3λ4 , we have φ=2πλ* 3λ4&nbs

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New answer posted

5 months ago

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V
Vishal Baghel

Contributor-Level 10

All the waves have different phases. The given transverse harmonic wave is:

y(x, t) = 3.0 sin (36t + 0.018x + π4 ) ………(i)

For x = 0, the equation reduces to

y (0,t) = 3.0 sin (36t + π4 )

Also ω = 2πT , so T = 2πω = 2π36 = π18 s

For plotting y vs., t graphs using different values of t, we get

When t = 0, y = 2.12

t = T8 = π18*8 , y = 3

t = 2T8 = 2*π18*8 , y = 2.12

t = 3T8 = 3*π18*8 , y = 0

t = 4T8 = 4*π18*8 , y = -2.12

t = 5T8 = 5*π18*8 , y = -3

t = 6T8 = 6*π18*8 , y = -2.12

t = 7T8 = 7*π18*8 , y = 0

For x = 2 and x = 4.

...more

New answer posted

5 months ago

0 Follower 5 Views

V
Vishal Baghel

Contributor-Level 10

The equation of a progressive wave travelling from right to left is given by the displacement function:

y (x, t) = a sin?(ωt+kx+φ) ……….(i)

The given equation is

y(x, t) = 3.0 sin (36 t + 0.018 x + π /4) …….(ii)

On comparing equations (i) and (ii), we find that the equation (ii) represents a travelling wave, propagating from right to left. Now, using equations (i) and (ii), we can write

ω=36rad/s , k = 0.018 m-1

From the relation ν=ω2π and λ=2πk and v = νλ , we can write

v = ω2π* 2πk = ωk = 360.018 = 2000 cm /s = 20 m/s

Hence, the speed of the given travelling wave is 20 m/s

The frequency ν=ω2π&

...more

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