Download, print and study this document offline |
Page 1 1. (b) 1 n = Frequency of the police car horn observer heard by motorcyclist 1 n = Frequency of the siren heard by motorcyclist. v 2 = Speed of motor cyclist 12 330 330 176; 165 330 22 330 vv nn -+ = ´ =´ - 12 0 22/ n n v ms \ - =Þ= 2. (c) Frequency of first over tone of closed pipe = Frequency of first over tone of open pipe 1 2 1 1 22 3 31 44 vv P PP v LL LL éù g gg Þ = Þ = \= êú r rr ëû 111 2 22 4 4 33 L L L rr Þ== rr 3. (b) For observer note of B will not change due to zero relative motion. Observed frequency of sound produced by A (330 30) 660 600 330 Hz - == \ No of beats = 600 - 596 = 4 4. (c) Open pipe resonanace frequency 1 2 2 v f L = Closed pipe resonance frequency 2 4 nv f L = 21 4 n ff = (where n is odd and 21 ) ff > \ 5 n = 5. (b) 0 () s nvv vv - - 6. (a) Wave number 1 = l but 11 ' s v vv æö = == ç÷ l l- èø and 3 s v v = \ , ( . .) ( . .) 256 /3 2 /3 vv WN WN vv æö = =´ ç÷ èø-u 3 256 384 2 =´= 7. (d) Since there is no relative motion between observer and source, therefore there is no apparent change in frequency. 8. (c) 350 ' 1200 1400 350 50 s v n n cps vv æö æö = =´= ç÷ ç÷ èø -- èø 9. (d) By using 1 ' s n vV nn v v n VS æö = Þ= ç÷ èø -- 10. (a) 0 330 33 ' 100 90 330 vv n n Hz v - - æö = = ´= ç÷ èø 11. (d) The apparent frequency heard by the observer is given by 330 330 ' 450 450 500 330 33 297 s v n x Hz vv = = ´= ´= -- 12. (b) Observer is moving ayay form siren 1 and towards the siren 2. v Stationay Moving Stationay siren 1 observer siren 2 Hearing frequency of sound emitted by siren 1 0 1 330 2 330 328 330 vv n n Hz v - - æö æö = == ç÷ ç÷ èø èø Hearing frequency of sound emitted by siren 2 0 2 330 2 330 332 330 vv n n Hz v - + æö æö = == ç÷ ç÷ èø èø Hence, beat frequency 21 332 328 4 nn = - = -= 13. (b) At point A , source is moving away from observer so apparent frequency 1 nn < (actual frequency). At point B source is coming towards observer so apparent frequency 2 nn > and point C source is moving perpendicular to observer so 3 nn = Hence 2 31 n nn >> 14. (c) According the concept of sound image 3455 ' .272 272 280 3455 person person vv n Hz vv + + = = ´= -- nD = Number of beats = 280 – 272 = 8 Hz 15. (a) The observer will hear two sound, one directly from source and other from reflected image of sound Page 2 1. (b) 1 n = Frequency of the police car horn observer heard by motorcyclist 1 n = Frequency of the siren heard by motorcyclist. v 2 = Speed of motor cyclist 12 330 330 176; 165 330 22 330 vv nn -+ = ´ =´ - 12 0 22/ n n v ms \ - =Þ= 2. (c) Frequency of first over tone of closed pipe = Frequency of first over tone of open pipe 1 2 1 1 22 3 31 44 vv P PP v LL LL éù g gg Þ = Þ = \= êú r rr ëû 111 2 22 4 4 33 L L L rr Þ== rr 3. (b) For observer note of B will not change due to zero relative motion. Observed frequency of sound produced by A (330 30) 660 600 330 Hz - == \ No of beats = 600 - 596 = 4 4. (c) Open pipe resonanace frequency 1 2 2 v f L = Closed pipe resonance frequency 2 4 nv f L = 21 4 n ff = (where n is odd and 21 ) ff > \ 5 n = 5. (b) 0 () s nvv vv - - 6. (a) Wave number 1 = l but 11 ' s v vv æö = == ç÷ l l- èø and 3 s v v = \ , ( . .) ( . .) 256 /3 2 /3 vv WN WN vv æö = =´ ç÷ èø-u 3 256 384 2 =´= 7. (d) Since there is no relative motion between observer and source, therefore there is no apparent change in frequency. 8. (c) 350 ' 1200 1400 350 50 s v n n cps vv æö æö = =´= ç÷ ç÷ èø -- èø 9. (d) By using 1 ' s n vV nn v v n VS æö = Þ= ç÷ èø -- 10. (a) 0 330 33 ' 100 90 330 vv n n Hz v - - æö = = ´= ç÷ èø 11. (d) The apparent frequency heard by the observer is given by 330 330 ' 450 450 500 330 33 297 s v n x Hz vv = = ´= ´= -- 12. (b) Observer is moving ayay form siren 1 and towards the siren 2. v Stationay Moving Stationay siren 1 observer siren 2 Hearing frequency of sound emitted by siren 1 0 1 330 2 330 328 330 vv n n Hz v - - æö æö = == ç÷ ç÷ èø èø Hearing frequency of sound emitted by siren 2 0 2 330 2 330 332 330 vv n n Hz v - + æö æö = == ç÷ ç÷ èø èø Hence, beat frequency 21 332 328 4 nn = - = -= 13. (b) At point A , source is moving away from observer so apparent frequency 1 nn < (actual frequency). At point B source is coming towards observer so apparent frequency 2 nn > and point C source is moving perpendicular to observer so 3 nn = Hence 2 31 n nn >> 14. (c) According the concept of sound image 3455 ' .272 272 280 3455 person person vv n Hz vv + + = = ´= -- nD = Number of beats = 280 – 272 = 8 Hz 15. (a) The observer will hear two sound, one directly from source and other from reflected image of sound 84 DPP/ P 30 Hence number of beats heard per second ss vv nn vv vv æ ö æö =- ç ÷ ç÷ -+ è ø èø 22 2 2 2563305 7.8 335 325 s s n Hz uu ´ ´´ = == ´ u -u 16. (a) In closed pipe only odd harmonics are present. 17. (a) Maximum pressure at closed end will be atmospheric pressure adding with acoustic wave pressure So max0 A P PP =+ and min0 A P PP =- Thus max0 min0 A A P PP P PP + = - 18. (b) 11 ( ) 320 160 22 = =´= closed open n n Hz 19. (a) 1.21Å l= N N N A A 1.21 Å 20. (a) 211 21 122 1 270 50 13.5 1000 lnn n l l cm llnn æö µÞ = Þ= = ´= ç÷ èø 21. (c) Loudness depends upon intensity while pitch depends upon frequency . 22. (d) Using ( ) ( ) 21 21 2ll v 2nll l= -Þ=- 2 215(63.2 30.7) 33280cm / s Þ´ -= Actual speed of sound v 0 = 332m / s = 33200cm / s Hence error = 33280 – 33200 = 80cm / s 23. (c) 3 7 1 2 5 300 301 303 308 8 3 7 5 2 1 300 305 307 308 8 24. (a) Doppler shift doesn't depend upon the distance of listner from the source. 25. (b) Since the edges are clamped, displacement of the edges (, )0 uxy = for line - y C B (L,L) A x O (0, 0) (0,L) OA i.e y = 0, 0 xL ££ AB i.e. ,0 y L yL = ££ BC i.e. ,0 y L xL = ££ OC i.e. 0,0 x yL = ££ The above conditions are satisfied only in alternatives (b) and (c). Note that (, )0 uxy = for all four values e.g. in alternative (), (, )0 d uxy = for 0, y yL == But it is not zero for 0 x = or xL = . Similarly in option (a) (,)0 uxy = at , x LyL == but it is not zero for 0 x = or 0 y = , while in options (b) and (c), (,)0 uxy = for 0, 0, x y xL = == and yL = 26. (b), 27. (d). For fundamental force, s 2s 2 l = Þl= V elocity of waves is, v = Y r where Y is Y oung's modu- lus of quartz and r is its density . From f 0 = 4 v 2.87 10 s ´ = l Þ 4 Y 1 2.87 10 2ss ´ ´= r Þ Y = 8.76 × 10 12 N/m 2 For 3rd harmonic, f = 3f 0 = 1.2 × 10 6 Hz Þ 4 3 2.87 10 s ´´ = 1.2 × 10 6 Þ s = 0.07175 cm. 28. (d) As emission of light from atom is a random and rapid phenomenon. The phase at a point due to two independent light source will change rapidly and randomly. Therefore, instead of beats, we shall get uniform intensity . However, if light sources are LASER beams of nearly equal frequencies, it may possible to observe the phenomenon of beats in light. 29. (d) The person will hear the loud sound at nodes than at antinodes. We know that at anti-nodes the displacement is maximum and pressure change is minimum while at nodes the displacement is zero and pressure change is maximum. The sound is heared due to variation of pressure. Also in stationary waves particles in two different segment vibrates in opposite phase. 30. (a) Stationary wave N N N A A A node is a place of zero amplitude and an antinode is a place of maximum amplitude.Read More
97 videos|378 docs|103 tests
|
|
Explore Courses for NEET exam
|