| Class XI |
Physics |
Physics Part-II |
7 |
diminishing amplitude to the very bottom. The y(x,t) = Asin(kx − ω t)+ Bcos(kx − ωt) (14.3) particle motion in water waves involves a From Equation... |
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| Class XI |
Physics |
Physics Part-II |
7 |
k : angular wave number positivedirectionofx-axisatdifferenttimes. kx– t+ : initial phase angle (a+x = 0, t = 0) Using the plots of Fig. 14.6, we n... |
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| Class XI |
Physics |
Physics Part-II |
7 |
x = 0 origin oscillates about its mean position as the wave progresses. This is true for any other and t = 0. Hence, is called the initial phase lo... |
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| Class XI |
Physics |
Physics Part-II |
7 |
distance between points with the same –1 displacement (at any given instant of time) is Its SI unit is rad s . The frequency ν is the obtained by t... |
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| Class XI |
Physics |
Physics Part-II |
7 |
could be dropped and the units could be written merely as m . Thus, k reprπsents 2 times the number of waves (or the total phase difference) that c... |
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| Class XI |
Physics |
Physics Part-II |
7 |
speed v (otherwise the wave pattern will not λ = 2π/k remain fixed). The motion of a fixed phase point on the wave is given by 2π = −1 kx – ωt = co... |
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| Class XI |
Physics |
Physics Part-II |
7 |
2026-27 WAVES 285 the speed; Eq. (14.12) then relates wavelength to arising due to an external force). It does not frequency for the given speed. O... |
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| Class XI |
Physics |
Physics Part-II |
7 |
–1 therefore, use dimensional analysis. We already know that dimensional analysis alone can never Tension, T = 60 N yield the exact formula. The ov... |
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| Class XI |
Physics |
Physics Part-II |
7 |
inspection reveals and µ (T is a property of the stretched string that quantity B/ ρ has the relevant dimension: Reprint 2026-27 286 PHYSICS −2 −2 ... |
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| Class XI |
Physics |
Physics Part-II |
7 |
case is the same that as before and yields a relation like Eq. (14.18), V∆P + P∆V = 0 with an undetermined C, which the exact derivation shows to b... |
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| Class XI |
Physics |
Physics Part-II |
7 |
was pointed out by Laplace that the pressure variations in the propagation of sound waves are so fast that there is little time for the heat flow t... |
|
| Class XI |
Political Science |
India Constitution at Work |
1 |
decide? The constitution has to provide an answer to this question. It specifies the basic allocation of power in a society. It decides who gets to... |
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| Class XI |
Physics |
Physics Part-II |
7 |
waves arrive in a region OFWAVES simultaneously, and therefore, overlap, the net displacement y (x,t) is given by What happens when two wave pulses... |
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| Class XI |
Physics |
Physics Part-II |
7 |
in phase, and y 2x, t) = a sin (kx – t + ) (14.28) y t 2a sin k t (14.33) The net displacement is then, by the principle of superposition,... |
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| Class XI |
Physics |
Physics Part-II |
7 |
completely free to move (such as in completely rigid or is an interface between two the case of a string tied to a freely moving ring different ela... |
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| Class XI |
Physics |
Physics Part-II |
7 |
waves differ by a phase of π, so that yr(x, t) = a sin (kxω–t + 0). the resultant displacement is zero. This = a sin (kx –ω t) (14.36) reasoning is... |
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| Class XI |
Physics |
Physics Part-II |
7 |
t) + sin (kx + t)] nodes; the points at which the amplitude is the Using the familiar trigonometric identity largest are called antinodes. Fig. 14.... |
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| Class XI |
Physics |
Physics Part-II |
7 |
is different at different locations. The points at which the amplitude is n zero (i.e., where there is no motion at all) are x = ; n = 0, 1, 2, 3... |
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| Class XI |
Physics |
Physics Part-II |
7 |
case of a stretched string of length L fixed at both ends. Taking one end to be at x = 0, the boundary conditions are that x = 0 and x = L are posi... |
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| Class XI |
Physics |
Physics Part-II |
7 |
with the same source be water to be x = 0, the node condition (Eq. 14.38) observed if one end of the pipe is closed ? is already satisfied. If the ... |
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| Class XI |
Physics |
Physics Part-II |
7 |
easily seen that an open air column at both ends generates all harmonics (See Fig. 14.15). The systems above, strings and air columns, can also und... |
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| Class XI |
Physics |
Physics Part-II |
7 |
, 5= , and so on. Using the familiar trigonometric identity for 4L 4L cos A + cosB, we get –1 For L = 30 cm and v = 330 m s , the ( - )t ( + ... |
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| Class XI |
Physics |
Physics Part-II |
7 |
ν 2 (14.48) Fig. 14.16 illustrates the phenomenon of beats for two harmonic waves of frequencies 11 Hz and 9 Hz. The amplitude of the resultant wav... |
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| Class XI |
Physics |
Physics Part-II |
7 |
the original frequency The musical pillars of Nelliappar and of B (νB) were greater than that of AνA), further several other temples in southern In... |
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| Class XI |
Physics |
Physics Part-II |
7 |
through the relation 2π T = ω 8. Frequency v of a wave is defined as 1/T and is related to angular frequency by ω ν = 2 π ω λ 9. Speed of a progres... |
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