| Class XII |
Accountancy |
Computerised Accounting System |
2 |
January 1, 1900. Numbers to the right of the decimal point in the serial number represent the time; numbers to the left represent the date. For exa... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
C HAPTER F OURTEEN W AVES 14.1 INTRODUCTION In the previous Chapter, we studied the motion of objects oscillating in isolation. What happens in a s... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
that propagate from one point to another. All our communications essentially depend on transmission of signals through waves. Speech means producti... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
on. The disturbance moves Light, radiowaves, X-rays, are all electromagnetic from one end to the other; but each spring only waves. In vacuum, all ... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
a region is compressed, the molecules first scientific analysis of wave motion dates back in that region are packed together, and they tend to move... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
wave propagation. involves oscillations of constituents of the position as the pulse or wave passes through medium. If the constituents of the medi... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
periodic sinusoidal up Fig. 14.4 Longitudinal waves (sound) generated in a and down jerk to one end of the string. The pipe filled with air by movi... |
|
| Class XI |
Physics |
Physics Part-II |
7 |
14.3 DISPLACEMENT RELATION IN A PROGRESSIVE WAVE sustain shearing stress, such as solids and not in fluids. Fluids, as well as, solids can sustain ... |
|
| 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... |
|
| 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... |
|
| 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... |
|
| 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... |
|
| 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... |
|
| 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... |
|
| 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... |
|
| 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... |
|
| 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 ... |
|
| 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... |
|
| 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 |
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... |
|
| 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,... |
|
| 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... |
|
| 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.... |
|
| 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... |
|
| 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... |
|