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Question: String 1 is connected with string 2. The mass per unit length in string 1 is \({\mu _1}\) and the ma...

String 1 is connected with string 2. The mass per unit length in string 1 is μ1{\mu _1} and the mass per unit length in string 2 is 4μ14{\mu _1} . The tension in the string is TT . A travelling wave is coming from the left. What fraction of the energy in the incident wave goes into string 2?

A) 1/81/8
B) 4/94/9
C) 2/32/3
D) 8/98/9

Explanation

Solution

Some part of the wave will be reflected back and only some part of it will be transmitted to B. First calculate the amplitude of this transmitted wave, and then calculate the power in each of the wires and then their ratio. This ratio will be equal to their energy ratio as time will be the same for both and hence will get cancelled out. This will be the final answer.

Formula Used:
Amplitude of transmitted wave, At=2vBva+vBAi{A_t} = \dfrac{{2{v_B}}}{{{v_a} + {v_B}}}{A_i} where, vB{v_B} is the velocity of wave in string B, vA{v_A}is the velocity of wave in string A, Ai{A_i} is the incident amplitude, or the amplitude of wave in string A
Velocity of a wave in a string, v=Tμv = \sqrt {\dfrac{T}{\mu }} where, TT is the tension in the string and μ\mu is the mass per unit length of the string.
Power of a wave, P=12μvω2A2P = \dfrac{1}{2}\mu v{\omega ^2}{A^2} where, μ\mu is the mass per unit length of the string, vv is the velocity of the wave in string, ω\omega is the angular frequency of the wave, AA is the amplitude of the wave.

Complete step by step solution:
The wave coming from string A will have an amplitude Ai{A_i} , called the incident amplitude. This wave will travel through the string until it meets string B, where a part of it will be reflected back in string A in the opposite direction of the incident wave, and the other part will propagate through B. This wave is called the transmitted wave and its amplitude, At{A_t} is called transmitted amplitude.
From the formula, we have amplitude of transmitted wave, At=2vBva+vBAi{A_t} = \dfrac{{2{v_B}}}{{{v_a} + {v_B}}}{A_i}
Also, we know that velocity of a wave in a string, v=Tμv = \sqrt {\dfrac{T}{\mu }}
Using these two formulas, we get At=2TBμBTAμA+TBμBAi{A_t} = \dfrac{{2\sqrt {\dfrac{{{T_B}}}{{{\mu _B}}}} }}{{\sqrt {\dfrac{{{T_A}}}{{{\mu _A}}}} + \sqrt {\dfrac{{{T_B}}}{{{\mu _B}}}} }}{A_i} where TB{T_B} is tension in string B, TA{T_A} is tension in string A, μA{\mu _A} is mass per unit volume of string A, μB{\mu _B} is mass per unit volume of string B
Since it is given that tension in the strings is equal, we can write above equation as
At=2TμBTμA+TμBAi{A_t} = \dfrac{{2\sqrt {\dfrac{T}{{{\mu _B}}}} }}{{\sqrt {\dfrac{T}{{{\mu _A}}}} + \sqrt {\dfrac{T}{{{\mu _B}}}} }}{A_i}
Now we are given in the question that mass per unit length of string A, μA=μ1{\mu _A} = {\mu _1} and mass per unit length of string B, μB=4μ1{\mu _B} = 4{\mu _1}
Substituting these in above formula, we get At=2T4μ1Tμ1+T4μ1Ai=Tμ1Tμ1+12Tμ1Ai{A_t} = \dfrac{{2\sqrt {\dfrac{T}{{4{\mu _1}}}} }}{{\sqrt {\dfrac{T}{{{\mu _1}}}} + \sqrt {\dfrac{T}{{4{\mu _1}}}} }}{A_i} = \dfrac{{\sqrt {\dfrac{T}{{{\mu _1}}}} }}{{\sqrt {\dfrac{T}{{{\mu _1}}}} + \dfrac{1}{2}\sqrt {\dfrac{T}{{{\mu _1}}}} }}{A_i} (4 comes out of the square root and becomes 2)
At=Tμ1Tμ1(1+12)Ai=23Ai{A_t} = \dfrac{{\sqrt {\dfrac{T}{{{\mu _1}}}} }}{{\sqrt {\dfrac{T}{{{\mu _1}}}} (1 + \dfrac{1}{2})}}{A_i} = \dfrac{2}{3}{A_i} (simplifying the equation)
Now, the power of a wave in string is given by P=12μvω2A2P = \dfrac{1}{2}\mu v{\omega ^2}{A^2}
Power in string A, PA=12μAvAω2Ai2=12μiTμiω2Ai2{P_A} = \dfrac{1}{2}{\mu _A}{v_A}{\omega ^2}{A_i}^2 = \dfrac{1}{2}{\mu _i}\sqrt {\dfrac{T}{{{\mu _i}}}} {\omega ^2}{A_i}^2 (substituting the respective values)
Power in string A, PB=12μBvBω2At2=124μiT4μiω2At2{P_B} = \dfrac{1}{2}{\mu _B}{v_B}{\omega ^2}{A_t}^2 = \dfrac{1}{2}4{\mu _i}\sqrt {\dfrac{T}{{4{\mu _i}}}} {\omega ^2}{A_t}^2 (substituting the respective values)
Now, PAPB=12μiTμiω2Ai2124μiT4μiω2At2=12μiTμiω2Ai2124μiT4μiω2(23Ai)2\dfrac{{{P_A}}}{{{P_B}}} = \dfrac{{\dfrac{1}{2}{\mu _i}\sqrt {\dfrac{T}{{{\mu _i}}}} {\omega ^2}{A_i}^2}}{{\dfrac{1}{2}4{\mu _i}\sqrt {\dfrac{T}{{4{\mu _i}}}} {\omega ^2}{A_t}^2}} = \dfrac{{\dfrac{1}{2}{\mu _i}\sqrt {\dfrac{T}{{{\mu _i}}}} {\omega ^2}{A_i}^2}}{{\dfrac{1}{2}4{\mu _i}\sqrt {\dfrac{T}{{4{\mu _i}}}} {\omega ^2}{{(\dfrac{2}{3}{A_i})}^2}}} (substituting the value of At{A_t} as calculated before)
On cancelling like terms and solving roots, we get PAPB=Tμi4×12×Tμi×49=189=98\dfrac{{{P_A}}}{{{P_B}}} = \dfrac{{\sqrt {\dfrac{T}{{{\mu _i}}}} }}{{4 \times \dfrac{1}{2} \times \sqrt {\dfrac{T}{{{\mu _i}}}} \times \dfrac{4}{9}}} = \dfrac{1}{{\dfrac{8}{9}}} = \dfrac{9}{8}
We know that Energy, E=P×tE = P \times t , where PP is power and tt is time.
Time taken for both wires will be equal and hence, power will be equal to energy.
EAEB=98\Rightarrow \dfrac{{{E_A}}}{{{E_B}}} = \dfrac{9}{8} or, EBEA=89\dfrac{{{E_B}}}{{{E_A}}} = \dfrac{8}{9}
Therefore, 89\dfrac{8}{9} parts of energy in string 1 goes to string 2.

Hence option D is the final answer.

Note: In questions like these, it may not always occur in mind what to do next. Hence, you might need to memorize some important steps of these questions as their steps are not related to each other. It will help you solve this question and also, be faster. Memorizing the power conversion step, or the velocity conversion step will help.