OSCILLATIONS. Syllabus :

Size: px
Start display at page:

Download "OSCILLATIONS. Syllabus :"

Transcription

1 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO OSCILLATIONS Sabus : Periodic otion period, dispaceent as a function of tie. Period functions. Sipe haronic otion (S.H.M.) and its equation; phase; osciations of a sprin - restorin force and force constant; ener in S.H.M. - inetic and potentia eneries; Sipe penduu - derivation of expression for its tie period; Free, forced and daped osciations, resonance.

2 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO CONCEPTS C C Sipe Haronic Motion If a partice oves to and fro about a fixed point (equiibriu position) under the appication of a force or torque (caed restorin force or torque) which is direct proportiona to the dispaceent (inear or anuar), directed towards the fixed point, is caed sipe haronic otion. Equation of SHM The necessar and sufficient condition for the otion to be sipe haronic (inear) is that the force shoud be direct proportiona to the dispaceent i.e. F x d x d x F = x or x dt or x 0 with dt The soution of the above differentia equation representin SHM is iven b : x = A sin (t + ) where A is the apitude of the otion, is the anuar (circuar) frequenc = /T (T = tie period) and is phase constant. Practice Probes : d dt. The equation of S.H.M. of a partice is 0, where is a positive constant. The tie period of otion is iven b. A partice is executin S.H.M. of period 4 s. Then the tie taen b it to ove fro the extree position to haf the apitude is / s / s /4 s 4/ s [Answers : () a () b] d C Veocit of SHM is iven b : v Acos( t ) or v dt A x The axiu and iniu veocit of the partice are v ax = A and V in = 0. Practice Probes :. A partice is vibratin in S.H.M. If its veocities are v and v when the dispaceents fro the ean position are and, respective, then its tie period is v v v. A partice is executin S.H.M. Then the raph of veocit as a function of dispaceent is v straiht ine circe eipse hperboa [Answers : () d () c] v v v v d C4 The acceeration in SHM is a. Thus a ax = A and a in = 0 dt Practice Probes :. A partice is executin S.H.M. Then the raph of acceeration as a function of dispaceent is straiht ine circe eipse hperboa [Answers : () a]

3 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO C5 Ener in SHM (i) Kinetic Ener (K) v (A x ) (ii) Potentia Ener (U) x (iii) Tota ener (E) A = constant Graph for the variation of K, U and E with the position x is iven b : Practice Probes :. A bod executes S.H.M. with an apitude A. Its ener is haf inetic and haf potentia when the dispaceent is A/ A/ A/ A/. When the potentia ener of a partice executin sipe haronic otion is one-fourth of its axiu vaue durin the osciation, the dispaceent of the partice fro the equiibriu position in ters of its apitude a is a/4 a/ a/ a/ [Answers : () c () c] C6 Sipe Penduu The tie period of a sipe penduu of enth L is iven b If enth of the penduu is are, then tie period is iven b : T where R = Radius of the earth L R R so if L, T inutes L. A second penduu is the sipe penduu havin a tie period of s. Practice Probes :. The tie period of a sipe penduu is T. If its enth is increased b %, the new tie period becoes 0.98 T.0 T 0.99 T.0 T

4 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO 4. The enth of a sipe penduu is increased b 44%. The percentae increase in its tie period wi be 44% % 0% %. A ir is swinin on a swin in the sittin position. How wi the period of swin be affected if she stands up? The period wi now be shorter The period wi now be oner The period wi reain unchaned The period a becoe oner or shorter dependin upon the heiht of the ir. 4. For a sipe penduu the raph between enth and tie period wi be a hperboa paraboa straiht ine none of these [Answers : () d () c () a (4) b] C7 Sprin - Boc Sste The tie period of SHM for a boc of ass connected b a sprin of sprin constant as shown in fiure is iven b T Practice Probes :. The bodies M and N of equa asses are suspended fro two separate assess sprins of constants and, respective. If the two osciate vertica such that their axiu veocities are equa, the ratio of the apitude of M to that of N is / / / /. The vertica extension in a iht sprin b a weiht of, in equiibriu, is 9.8 c. The period of osciation of the sprin, in seconds, wi be A assess sprin, havin force constant, osciates with a frequenc n when a ass is suspended fro it. The sprin is cut into two equa haves and a ass is suspended fro it. The frequenc of osciation wi now be n n n/ n [Answers : () d () a () a] C8 Phsica Penduu The tie period of a phsica penduu is iven b : T I Md I : oent of inertia about the rotationa axis passin throuh point of suspension d : distance of the center of ass fro the point of suspension M : tota ass of the bod

5 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 Practice Probes : PO 5. A rod of ass and enth L is suspended fro one of the end point of the rod in vertica pane. The tie period of the rod for sa osciation is iven b L L L L 4 [Answers : () a] C9 C0 Daped Osciation Osciations under the infuence of frictiona force are caed daped osciation. The apitude and hence ener decreases with tie exponentia and eventua the osciator coes to rest. Forced Osciation and Resonance The osciations of a sste under the infuence of an externa periodic force are caed forced osciations. The apitude of these osciations reains constant. If the frequenc of the externa appied force is equa to the natura frequenc of the osciator, resonance is said to occur. If dapin is sa, the apitude of resonant osciations wi becoe ver are. At resonance, the osciator absorbs axiu ener suppied b the externa force.

6 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO 6 INITIAL STEP EXERCISE. A etaic sphere is fied with water and hun b a on thread. It is ade to osciate. If there is a sa hoe in the botto throuh which water sow fows out, the tie period wi o on increasin ti the sphere is ept o on decreasin ti the sphere is ept reain unchaned throuhout first increase, then it wi decrease ti the sphere is ept and the period wi not be the sae as when the sphere was fu of water.. A sipe penduu of enth suspended fro the ceiin of a train is osciatin when the train is at rest. If the train starts ovin with a constant acceeration, the tie period of the penduu wi be a a a. A wea daped haronic osciator of frequenc n is driven b an externa periodic force of frequenc n. When the stead state is reached, the frequenc of the osciator wi be n n (n + n )/ n n 4. The period of a partice in S.H.M. is 8 s. At t = 0 it is at the ean position. The ratio of the distances traveed b it in the first and the second is (C) (D) 5. A bod is on a rouh horizonta surface which is ovin horizonta in S.H.M. of frequenc Hz. The coefficient of static friction between the bod and the surface is 0.5. The axiu vaue of the apitude for which the bod wi not sip aon the surface is approxiate 9 c 6 c 4.5 c c 6. A pan with a set of weiht is attached to a iht sprin. The period of vertica osciations is 0.5 s. When soe additiona weihts are put in the pan, the period of osciations increases b 0. s. The extension caused b the additiona weihts is. c.7 c.8 c 5.5 c 7. A penduu coc, which eeps correct tie at sea eve, oses 5 s per da when taen to the top of a ountain. If the radius of the earth is 6400, the heiht of the ountain is The iniu phase difference between the two sipe haronic osciations sin t cost and = sin t + cos t is /6 /6 / 7/ 9. A sipe penduu is suspended fro the roof of a troe that oves free down a pane of incination. The tie period of osciation of the penduu is sin cos tan 0. A bod executes S.H.M. of period s under the infuence of one force, and S.H.M. of period 4 s under the infuence of a second force. When both the forces act siutaneous in the sae direction, the period of osciation wi be 7 s 5 s s.4 s. The tie period of a sipe penduu easured inside a stationar ift is T. If the ift starts acceeratin upwards with an acceeration /, the tie wi be T T T T

7 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO 7. A second s penduu is paced in a space aborator orbitin around the earth at a heiht R fro the earth s surface where R is the radius of the earth. The tie period of the penduu wi be zero / s 4 s infinite. The percentae chane in radius of the earth is % without chane in its ass. The percentae chane in tie period of the sipe penduu is ½ % % %. % 4. Let the coefficient of inear expansion of the assess strin of sipe penduu is. If the teperature is increased b t then the fractiona chane in tie period of the sipe penduu is t t /4 t / t 5. A sprin of force constant is divided in : :. The force constant of the onest sprin is 6 6. The frequenc of vertica osciations of the three sprin-ass sste, shown in the fiure is FINAL STEP EXERCISE (OBJECTIVE). A sipe penduu has a tie period T. The penduu is copete iersed in a non-viscous iquid whose densit is /0th of that of the ateria of the bob. The tie period of the penduu iersed in the iquid is 9 T T T. A inear haronic osciator of force constant 0 6 N/ and apitude 0.0 has a tota echanica ener of 60 Joue. Its T 0 axiu potentia ener is 00 J axiu inetic ener is 00 J axiu potentia ener is 60 J both and are correct. When a bod is suspended fro two iht sprins separate, the periods of vertica osciations are T and T. When the sae bod is suspended fro the two sprins connected in series, the period wi be T + T T T (T T ) / T T 4. In the above probe if the bod is suspended fro the two sprins connected in parae, the tie period wi be T T T T TT T T TT T T

8 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO 8 5. The dispaceent of a partice executin periodic otion is iven b (M )x / 4cos t sin(000t) This expression a be considered to be a resut of the superposition of two three four five independent haronic otions. 6. A unifor cinder of ass M and cross-sectiona area A is suspended fro a fixed point b a iht sprin of force constant. The cinder is partia subered in a iquid of densit. If it is iven a sa downward push and reeased, it wi osciate with tie period M A M M A M A 7. Two partices execute S.H.M. of the sae apitude and frequenc aon the sae straiht ine. The pass one another when oin in opposite directions each tie their dispaceent is haf their apitude. The phase difference between the is A person nora weihin 60 stands on a patfor which osciates up and down sipe haronica with a frequenc Hz and an apitude 5 c. If a achine on the patfor ives the person s weiht, then ( = 0 /s, = 0), the axiu readin of the achine wi be 08 the axiu readin of the achine wi be 90 the iniu readin of the achine wi be both and are correct 9. A ass M is suspended fro a assess sprin. An additiona ass stretches the sprin further b a distance x. The cobined ass wi osciate on the sprin with tie period /(M ) x (M ) / x ( / ) /(M ) x 0. Eectron in an oscioscope are defected b two utua perpendicuar osciatin eectric fieds such that at an tie the dispaceents due to the are iven b x = A cos t, = A cos t. Then 6 the path of the eectron is a straiht ine havin the equation x = a circe havin the equation x + = A an eipse havin the equation x x A / 4 an eipse havin the equation x x + = A /4. Two inear sipe haronic otions of equa apitudes and frequencies and are ipressed on a partice aon x and axes respective. If the initia phase difference between the is /, the resutant path foowed b the partice is iven b x A x x A x x A 4x x A 8x. A piece of wood has diensions a, b and c. Its reative densit is d. It is foatin in water such that the side a is vertica. If it is pushed down a itte and then reeased, the tie period of osciation wi be abc ad bc d bcd

9 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857. A U tube of unifor bore of cross-sectiona area a is set up vertica with open ends up. A iquid of ass and densit d is poured into it. The iquid coun wi osciate with a period PO 9 ANSWERS (INITIAL STEP EXERCISE) ad a d ad 4. A bod of ass fas fro a heiht h onto the pan of a sprin baance. The asses of the pan and sprin are neiibe. The force constant of the sprin is. The bod stics to the pan and osciates sipe haronica. The apitude of osciation is / ( / ) (h / ) ( / )( (h / )) ( / )( (h / ) ). d. d. b 4. d 5. d 6. b 7. a 8. c 9. b 0. d. b. d. b 4. d 5. c 6. b ANSWERS (FINAL STEP EXERCISE). c. d. d 4. b 5. b 6. a 7. c 8. d 9. a 0. c. c. c. d 4. b

10 PO 0 AIEEE ANALYSIS [00]. If a sprin has tie period T, and is cut into n equa parts, then the tie period of each part wi be 4. A chid swinin on a swin in sittin position, stands up, then the tie period of the swin wi Tn T/n nt T increase decrease. In a sape haronic osciator, at the ean position inetic ener is iniu, potentia ener is axiu both inetic and potentia eneries are axiu inetic ener is axiu, potentia ener is iniu both inetic and potentia eneries are iniu. A sprin of force constant 800 N/ has an extension of 5 c. The wor done in extendin it fro 5 c to 5 c is reain sae increase if the chid is on and decreases if the chid is short 5. A bod executes sipe haronic otion. The potentia ener (P.E.), the inetic (K.E.) and tota ener (T.E.) are easured as a function of dispaceent x. Which of the foowin stateents is true? P.E. is axiu when x = 0 K.E. is axiu when x = 0 T.E. is zero when x = 0 K.E. is axiu when x is axiu 6 J 8 J J 4 J AIEEE ANALYSIS [00] 6. A ass M is suspended fro a sprin of neiibe ass. The sprin is pued a itte and then reeased so that the ass executes SHM of tie period T. If the ass is increased b, the tie period becoes 5T/. Then the ratio of /M is 6/9 5/ /5 5/9 7. Two partices A and B of equa asses are suspended fro two assess sprins of sprin constant and, respective. If the axiu veocities, durin osciation, are equa, the ratio of apitudes of A and B is 8. The enth of a sipe penduu executin sipe haronic otion is increased b %. The percentae increase in the tie period of the penduu of increased enth is 4% 0% % % 9. The dispaceent of a partice varies accordin to the reation x = 4(cos t + sin t). The apitude of the partice is Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857

11 < [004] Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO AIEEE ANALYSIS [004/005] 0. The bob of a sipe penduu executes sipe haronic otion in water with a period t, whie the period of osciation of the bob is t 0 in air. Neectin frictiona force of water and iven that the densit of the bob is (4/) 000 /. What reationship between t and t 0 is true? t = t 0 t = t 0 / t = t 0 t = 4t 0 [004]. A partice at the end of a sprin executes sipe haronic otion with a period t, whie the correspondin period for another sprin is t. If the period of osciation with the two sprins in series is T, then T = t + t T = t + t T = t + t T = t + t [004]. The tota ener of a partice, executin sipe haronic otion is x x independent of x x ½ where x is the dispaceent fro ean position. [004]. A partice of ass is attached to a sprin (of sprin constant ) and has a neutra anuar frequenc 0. An externa force F(t) proportiona to cos t ( 0 ) is appied to the osciator. The dispaceent of the osciator wi be proportiona to 0 ( 0 ) ( 0 0 ) [004] 4. In forced osciation of a partice the apitude is axiu for a frequenc of the force, whie the ener is axiu for a frequenc of the force, then = > < when dapin is sa and > when dapin is are 5. The function sin (t) represents a sipe haronic otion with a period / a sipe haronic otion with a period / a periodic, but not sipe haronic, otion with a period /. a periodic, but not sipe haronic, otion with a period /. [005] 6. Two sipe haronic otions are represented b the equations = 0. sin 00 t and = 0. cos t. The phase difference of the veocit of partice with respect to the veocit of partice is 6 6 [005] 7. If a sipe haronic otion is represented b d x x 0 dt, its tie period is [005] 8. The bob of a sipe penduu is a spherica hoow ba fied with water. A pued hoe near the botto of the osciatin bob ets sudden unpued. Durin observation, ti water is coin out, the tie period of osciation woud reain unchaned increase towards a saturation vaue first increase and then decrease to the oriina vaue first decrease and then increase to the oriina vaue [005]

12 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO AIEEE ANALYSIS [006] 9. Startin fro the oriin a bod osciates sipe haronica with a period of s. After what tie wi its inetic ener be 75% of the tota ener? s s 6 s Hz 4 0. The axiu veocit of a partice, executin sipe haronic otion with an apitude 7, is 4.4 s. The period of osciation is 0. s 00 s 0.0 s 0 s. A coin is paced on a horizonta patfor which underoes vertica sipe haronic otion of anuar frequenc. The apitude of osciation is radua increased. The coin wi eave contact with the patfor for the first tie for an apitude of / at the hihest position of the patfor at the ean position of the patfor for an apitude of /. AIEEE ANALYSIS [007]. Two sprins, of force constant and, are connected to a ass as shown. The frequenc of osciation of the ass is f. If both and are ade four ties their oriina vaues, the frequenc of osciation becoes f f/4 f/ 4f. A partice of ass executes sipe haronic otion with apitude a and frequenc v. The averae inetic ener durin its otion fro the position of equiibriu to the end is a v a v 4 a v 4 a v 4. The dispaceent of an object attached to a sprin and executin sipe haronic otion is iven b x = 0 cos t etre. The tie at which the axiu speed first occurs is 0.5 s 0.75 s 0.5 s 0.5 s 5. A point ass osciates aon the x-axis accordin to the aw x = x 0 cos (t /4). If the acceeration of the partice is written as a = A cos (t + ), then A = x 0, = /4 A = x 0, = /4 A = x 0, = /4 A = x 0, = /4 ANSWERS AIEEE ANALYSIS. b. c. b 4. b 5. b 6. a 7. a 8. b 9. a 0. c. b. c. b 4. a 5. b 6. c 7. d 8. c 9. c 0. c. d. a. c 4. c 5. a TEST YOURSELF. A sipe penduu is osciatin in a ift. Let the tie period of the osciation is T. Consider the foowin cases : Case. Lift is ovin with constant veocut Tie Period. Lift is ovin with constant acceeration (downward) T 4 Which of the above tie period is iniu : T T T T 4 (upward or downward) T. Lift is ovin with constant acceeration (upward) T

13 Einstein Casses, Unit No. 0, 0, Vardhan Rin Road Paza, Vias Puri Extn., Outer Rin Road New Dehi 0 08, Ph. : 96905, 857 PO. If a hoe is bored aon a diaeter of the earth and a stone is dropped into the hoe, it wi reach the centre of the earth and stop there reach the other side of the earth and stop there execute S.H.M. about the centre of the earth execute osciator, but not sipe haronic, otion about the centre of the earth.. Two asses and are suspended toether b a assess sprin of constant. When the asses are in equiibriu, is ent reoved. Then the anuar frequenc of osciation of and the apit of osciation are respective. /, /,, /( ) /( ), 4. The ratio of the apitudes of the sipe haronic osciations iven b = A sin t and = (A/) sin t + (A/) cos t is / 5. A partice is subjected to two sipe haronic otions aon x and axes : x = a sin t and = a sin t. The resutant trajector is a sine curve circe eipse straiht ine 6. When a partice osciates sipe haronica, its potentia ener varies periodica. If the frequenc of osciation of the partice is n, the frequenc of potentia ener variation is n/ n n 4n 7. A boc of ass is paced on a frictioness horizonta tabe. Sprins of force constants and are attached on either side of it. The other ends of the sprins are fixed as shown in the fiure. If the boc is dispaced a itte horizonta and eft to osciate, the anuar frequenc of osciation wi be. c. c. b 4. d 5. d / ( ) / ( ) ( ) 6. c 7. a 8. b 9. b 0. d / / 8. Sprins of constants,, 4, 8,..., are connected in series. A ass is attached to one end and the sste is aowed to osciate. The tie period is Two sipe penduus havin enths and 6 are both iven sa dispaceents in the sae directions at the sae instant. The wi aain be in phase at the ean position after the shorter penduu has copeted n osciations where n is / A fat horizonta board oves up and down in S.H.M. of apitude A. Then the saest perissibe vaue of tie period, such that an object on the board a not ose contact with the board, is A A A A ANSWERS

Simple Harmonic Motion (SHM)

Simple Harmonic Motion (SHM) Phsics Sipe Haronic Motion (SHM) www.testprepart.co abe of Content. Periodic otion.. Osciator or Vibrator otion. 3. Haronic and Non-haronic osciation. 4. Soe iportant definitions. 5. Sipe haronic otion.

More information

OSCILLATIONS. dt x = (1) Where = k m

OSCILLATIONS. dt x = (1) Where = k m OSCILLATIONS Periodic Motion. Any otion, which repeats itsef at reguar interva of tie, is caed a periodic otion. Eg: 1) Rotation of earth around sun. 2) Vibrations of a sipe penduu. 3) Rotation of eectron

More information

Oscillations Equations 0. Out of the followin functions representin otion of a particle which represents SHM I) y = sinωt cosωt 3 II) y = sin ωt III) IV) 3 y = 5cos 3ωt 4 y = + ωt+ ω t a) Only IV does

More information

14 - OSCILLATIONS Page 1

14 - OSCILLATIONS Page 1 14 - OSCILLATIONS Page 1 14.1 Perioic an Osciator otion Motion of a sste at reguar interva of tie on a efinite path about a efinite point is known as a perioic otion, e.g., unifor circuar otion of a partice.

More information

Convergence P H Y S I C S

Convergence P H Y S I C S +1 Test (Newton s Law of Motion) 1. Inertia is that property of a body by virtue of which the body is (a) Unabe to change by itsef the state of rest (b) Unabe to change by itsef the state of unifor otion

More information

University of Alabama Department of Physics and Astronomy. PH 105 LeClair Summer Problem Set 11

University of Alabama Department of Physics and Astronomy. PH 105 LeClair Summer Problem Set 11 University of Aabaa Departent of Physics and Astronoy PH 05 LeCair Suer 0 Instructions: Probe Set. Answer a questions beow. A questions have equa weight.. Due Fri June 0 at the start of ecture, or eectronicay

More information

Simple Harmonic Motion

Simple Harmonic Motion Chapter 3 Sipe Haronic Motion Practice Probe Soutions Student extboo pae 608. Conceptuaize the Probe - he period of a ass that is osciatin on the end of a sprin is reated to its ass and the force constant

More information

HO 25 Solutions. = s. = 296 kg s 2. = ( kg) s. = 2π m k and T = 2π ω. kg m = m kg. = 2π. = ω 2 A = 2πf

HO 25 Solutions. = s. = 296 kg s 2. = ( kg) s. = 2π m k and T = 2π ω. kg m = m kg. = 2π. = ω 2 A = 2πf HO 5 Soution 1.) haronic ociator = 0.300 g with an idea pring T = 0.00 T = π T π π o = = ( 0.300 g) 0.00 = 96 g = 96 N.) haronic ociator = 0.00 g and idea pring = 140 N F = x = a = d x dt o the dipaceent

More information

Session : Electrodynamic Tethers

Session : Electrodynamic Tethers Session : Eectrodynaic Tethers Eectrodynaic tethers are ong, thin conductive wires depoyed in space that can be used to generate power by reoving kinetic energy fro their orbita otion, or to produce thrust

More information

d x + 2 x = 0 where x is displacement(in m)from (B) 2 (C) 5 10 (D)

d x + 2 x = 0 where x is displacement(in m)from (B) 2 (C) 5 10 (D) J-Physics XRCIS CHCK YOUR GRASP. he equation of otion of a particle of ass is dt ean position. he frequency of oscillation is (in Hz) : d x + x = where x is displaceent(in )fro 5. wo bodies perforin S.H..

More information

THERMAL EXPANSION OF MATERIALS

THERMAL EXPANSION OF MATERIALS HERMAL EXPANSION OF MAERIALS EXPANSION OF SOLIDS PREVIOUS EAMCE QUESIONS ENGINEERING. A cock penduum made of invar has a period of.5 sec, at C. If the cock is used in a cimate where the temperature averaes

More information

Previous Years Problems on System of Particles and Rotional Motion for NEET

Previous Years Problems on System of Particles and Rotional Motion for NEET P-8 JPME Topicwise Soved Paper- PHYSCS Previous Years Probems on Sstem of Partices and otiona Motion for NEET This Chapter Previous Years Probems on Sstem of Partices and otiona Motion for NEET is taken

More information

1) For a block of mass m to slide without friction up a rise of height h, the minimum initial speed of the block must be

1) For a block of mass m to slide without friction up a rise of height h, the minimum initial speed of the block must be v m 1) For a bock of mass m to side without friction up a rise of height h, the minimum initia speed of the bock must be a ) gh b ) gh d ) gh e ) gh c ) gh P h b 3 15 ft 3) A man pus a pound crate up a

More information

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment Forces of Friction When an object is in motion on a surface or through a viscous medium, there wi be a resistance to the motion This is due to the interactions between the object and its environment This

More information

Candidate Number. General Certificate of Education Advanced Level Examination January 2012

Candidate Number. General Certificate of Education Advanced Level Examination January 2012 entre Number andidate Number Surname Other Names andidate Signature Genera ertificate of Education dvanced Leve Examination January 212 Physics PHY4/1 Unit 4 Fieds and Further Mechanics Section Tuesday

More information

CHAPTER 14: Oscillations. Answers to Questions. l. The length, l, is the distance from the center of the tire to the branch.

CHAPTER 14: Oscillations. Answers to Questions. l. The length, l, is the distance from the center of the tire to the branch. CHAPTER 4: Osciations Answers to Questions. Eapes are: a chid s swing (SHM, for sa osciations), stereo speaers (copicated otion, the addition of any SHMs), the bade on a jigsaw (approiatey SHM), the string

More information

PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE)

PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE) Cass XI TARGET : JEE Main/Adv PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE) ALP ADVANCED LEVEL LPROBLEMS ROTATION- Topics Covered: Rigid body, moment of inertia, parae and perpendicuar axes theorems,

More information

PHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I

PHYSICS LOCUS / / d dt. ( vi) mass, m moment of inertia, I. ( ix) linear momentum, p Angular momentum, l p mv l I 6 n terms of moment of inertia, equation (7.8) can be written as The vector form of the above equation is...(7.9 a)...(7.9 b) The anguar acceeration produced is aong the direction of appied externa torque.

More information

OSCILLATIONS

OSCILLATIONS OSCIAIONS Important Points:. Simple Harmonic Motion: a) he acceleration is directly proportional to the displacement of the body from the fixed point and it is always directed towards the fixed point in

More information

Module 22: Simple Harmonic Oscillation and Torque

Module 22: Simple Harmonic Oscillation and Torque Modue : Simpe Harmonic Osciation and Torque.1 Introduction We have aready used Newton s Second Law or Conservation of Energy to anayze systems ike the boc-spring system that osciate. We sha now use torque

More information

PHYS 1443 Section 003 Lecture #22

PHYS 1443 Section 003 Lecture #22 PHYS 443 Section 003 Lecture # Monda, Nov. 4, 003. Siple Bloc-Spring Sste. Energ of the Siple Haronic Oscillator 3. Pendulu Siple Pendulu Phsical Pendulu orsion Pendulu 4. Siple Haronic Motion and Unifor

More information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #8-3 Oscillations, Simple Harmonic Motion Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.

More information

XI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com

XI PHYSICS. M. Affan Khan LECTURER PHYSICS, AKHSS, K. https://promotephysics.wordpress.com XI PHYSICS M. Affan Khan LECTURER PHYSICS, AKHSS, K affan_414@ive.com https://promotephysics.wordpress.com [TORQUE, ANGULAR MOMENTUM & EQUILIBRIUM] CHAPTER NO. 5 Okay here we are going to discuss Rotationa

More information

Wave Motion: revision. Professor Guy Wilkinson Trinity Term 2014

Wave Motion: revision. Professor Guy Wilkinson Trinity Term 2014 Wave Motion: revision Professor Gu Wiinson gu.wiinson@phsics.o.a.u Trinit Ter 4 Introduction Two ectures to reind ourseves of what we earned ast ter Wi restrict discussion to the topics on the sabus Wi

More information

Measurement of acceleration due to gravity (g) by a compound pendulum

Measurement of acceleration due to gravity (g) by a compound pendulum Measurement of acceeration due to gravity (g) by a compound penduum Aim: (i) To determine the acceeration due to gravity (g) by means of a compound penduum. (ii) To determine radius of gyration about an

More information

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations P Physics Multiple Choice Practice Oscillations. ass, attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is.

More information

A we connect it in series with a capacitor of capacitance C 160 F. C The circuit thus carries an alternating sinusoidal current i.

A we connect it in series with a capacitor of capacitance C 160 F. C The circuit thus carries an alternating sinusoidal current i. I-(7 points) Deterination of a characteristic of a coil In order to deterine the resistance r of a coil of inductance 0 03 H, A we connect it in series with a capacitor of capacitance C 160F across the

More information

INDIAN ASSOCIATION OF PHYSICS TEACHERS NATIONAL STANDARD EXAMINATION IN PHYSICS

INDIAN ASSOCIATION OF PHYSICS TEACHERS NATIONAL STANDARD EXAMINATION IN PHYSICS INDIAN ASSOCIATION OF PHYSICS TEACHERS NATIONAL STANDARD EXAMINATION IN PHYSICS 009-00 Tota tie : 0 inutes (A-, A- & ) PART - A (Tota Marks : 80) SU-PART A- Q. The Schrodinger equation for a free eectron

More information

Parallel-Axis Theorem

Parallel-Axis Theorem Parae-Axis Theorem In the previous exampes, the axis of rotation coincided with the axis of symmetry of the object For an arbitrary axis, the paraeaxis theorem often simpifies cacuations The theorem states

More information

11 - KINETIC THEORY OF GASES Page 1. The constituent particles of the matter like atoms, molecules or ions are in continuous motion.

11 - KINETIC THEORY OF GASES Page 1. The constituent particles of the matter like atoms, molecules or ions are in continuous motion. - KIETIC THEORY OF GASES Page Introduction The constituent partices of the atter ike atos, oecues or ions are in continuous otion. In soids, the partices are very cose and osciate about their ean positions.

More information

Chapter 32 Inductance

Chapter 32 Inductance Chapter 3 nductance 3. Sef-nduction and nductance Sef-nductance Φ BA na --> Φ The unit of the inductance is henry (H). Wb T H A A When the current in the circuit is changing, the agnetic fux is aso changing.

More information

Experiment 1: Simple Pendulum

Experiment 1: Simple Pendulum COMSATS Institute of Information Technoloy, Islamabad Campus PHY-108 : Physics Lab 1 (Mechanics of Particles) Experiment 1: Simple Pendulum A simple pendulum consists of a small object (known as the bob)

More information

PERIODIC MOTION. 1/ f 1/220 Hz s. = s and the angular frequency is ω = 2π. f = 880 Hz. This is equal to 1/T. f = 0.

PERIODIC MOTION. 1/ f 1/220 Hz s. = s and the angular frequency is ω = 2π. f = 880 Hz. This is equal to 1/T. f = 0. PERIODIC MOTION IDENTIFY and SET UP: The taret variables are the period T and anular frequency ω We are iven the frequency f, so we can find these usin Eqs() and () EXECUTE: (a) f Hz T / f / Hz 454 s ω

More information

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz ecture 8-1 Oscillations 1. Oscillations Simple Harmonic Motion So far we have considered two basic types of motion: translational motion and rotational motion. But these are not the only types of motion

More information

NSEP EXAMINATION

NSEP EXAMINATION NSEP 009-00 EXAMINATION INDIAN ASSOCIATION OF PHYSICS TEACHERS NATIONAL STANDARD EXAMINATION IN PHYSICS 009-00 Tota tie : 0 inutes (A-, A- & ) PART - A (Tota Marks : 80) SU-PART A- Q. The Schrodinger equation

More information

Join discussion of this test paper at

Join discussion of this test paper at SECTION - 1. This question consists of TWENTY-FIVE sub-questions (1.1 1.5) of ONE ark each. For each of these sub-questions, four possibe aternatives (,, C and D) are given, out of which ONLY ONE is correct.

More information

Vector Spaces in Physics 8/6/2015. Chapter 4. Practical Examples.

Vector Spaces in Physics 8/6/2015. Chapter 4. Practical Examples. Vector Spaces in Physics 8/6/15 Chapter 4. Practical Exaples. In this chapter we will discuss solutions to two physics probles where we ae use of techniques discussed in this boo. In both cases there are

More information

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2! Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached

More information

University of California, Berkeley Physics 7A Spring 2009 (Yury Kolomensky) SOLUTIONS TO PRACTICE PROBLEMS FOR THE FINAL EXAM

University of California, Berkeley Physics 7A Spring 2009 (Yury Kolomensky) SOLUTIONS TO PRACTICE PROBLEMS FOR THE FINAL EXAM 1 University of Caifornia, Bereey Physics 7A Spring 009 (Yury Koomensy) SOLUIONS O PRACICE PROBLEMS FOR HE FINAL EXAM Maximum score: 00 points 1. (5 points) Ice in a Gass You are riding in an eevator hoding

More information

Simple Harmonic Motion

Simple Harmonic Motion Reading: Chapter 15 Siple Haronic Motion Siple Haronic Motion Frequency f Period T T 1. f Siple haronic otion x ( t) x cos( t ). Aplitude x Phase Angular frequency Since the otion returns to its initial

More information

Physics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14

Physics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14 Physics 07, Lecture 18, Nov. 3 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand

More information

Phase Diagrams. Chapter 8. Conditions for the Coexistence of Multiple Phases. d S dt V

Phase Diagrams. Chapter 8. Conditions for the Coexistence of Multiple Phases. d S dt V hase Diaras Chapter 8 hase - a for of atter that is unifor with respect to cheica coposition and the physica state of areation (soid, iquid, or aseous phases) icroscopicay and acroscopicay. Conditions

More information

Sure Shot 2016 Electric Current By M K Ezaz

Sure Shot 2016 Electric Current By M K Ezaz Sure Shot 06 Eectric Current B M K Ezaz. A 0 V batter of negigibe interna resistance is connected across a 00 V batter and a resistance of 38 Ω. Find the vaue of the current in circuit. () E 00 0 A: I

More information

Page 1. Physics 131: Lecture 22. SHM and Circles. Today s Agenda. Position. Velocity. Position and Velocity. Acceleration. v Asin.

Page 1. Physics 131: Lecture 22. SHM and Circles. Today s Agenda. Position. Velocity. Position and Velocity. Acceleration. v Asin. Physics 3: ecture Today s enda Siple haronic otion Deinition Period and requency Position, velocity, and acceleration Period o a ass on a sprin Vertical sprin Enery and siple haronic otion Enery o a sprin

More information

AAPT UNITED STATES PHYSICS TEAM AIP 2009

AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS DO NOT OPEN THIS TEST UNTI YOU ARE TOD TO BEGIN Use = 10 N/k throuhout this contest.

More information

Physics 201 Lecture 29

Physics 201 Lecture 29 Phsics 1 ecture 9 Goals ecture 9 v Describe oscillator otion in a siple pendulu v Describe oscillator otion with torques v Introduce daping in SHM v Discuss resonance v Final Ea Details l Sunda, Ma 13th

More information

Remove this page when instructed to do so. Work written on this page will not be marked. UNIVERSITY OF TORONTO

Remove this page when instructed to do so. Work written on this page will not be marked. UNIVERSITY OF TORONTO Reove this page when instructed to do so. Work written on this page wi not be arked. UNIVERSITY OF TORONTO FULTY OF PPLIED SIENE ND ENGINEERING Ter Test, February 0, 05 First Year MSE0 INTRODUTION TO MTERILS

More information

Problem Set 14: Oscillations AP Physics C Supplementary Problems

Problem Set 14: Oscillations AP Physics C Supplementary Problems Proble Set 14: Oscillations AP Physics C Suppleentary Probles 1 An oscillator consists of a bloc of ass 050 g connected to a spring When set into oscillation with aplitude 35 c, it is observed to repeat

More information

MODELLING, SIMULATION AND OPTIMIZATION OF DAMPING

MODELLING, SIMULATION AND OPTIMIZATION OF DAMPING MODELLNG SMULAON AND OPMZAON O DAMPNG Jiří Vondřich Evžen hőnde Departent of Eectric Drives and raction acut of Eectrica Engineering zech echnica Universit in Prague Astract Modeing siuation and optiization

More information

14-6 The Equation of Continuity

14-6 The Equation of Continuity 14-6 The Equation of Continuity 14-6 The Equation of Continuity Motion of rea fuids is compicated and poory understood (e.g., turbuence) We discuss motion of an idea fuid 1. Steady fow: Laminar fow, the

More information

PHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #9 Solutions November 12/13

PHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #9 Solutions November 12/13 PHY 4Y FOUNDAIONS OF PHYSICS - utorial Questions #9 Solutions Noveber /3 Conservation of Ener and Sprins. One end of a assless sprin is placed on a flat surface, with the other end pointin upward, as shown

More information

Candidate Number. General Certificate of Education Advanced Level Examination June 2010

Candidate Number. General Certificate of Education Advanced Level Examination June 2010 Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initias Genera Certificate of Education Advanced Leve Examination June 2010 Question 1 2 Mark Physics

More information

Student Book pages

Student Book pages Chapter 7 Review Student Boo pages 390 39 Knowledge. Oscillatory otion is otion that repeats itself at regular intervals. For exaple, a ass oscillating on a spring and a pendulu swinging bac and forth..

More information

N N N ( N

N N N ( N Copyriht Glencoe/McGraw-Hill, a division of The McGraw-Hill Copanies, Inc. Chapter 4 1. You and your bike have a cobined ass of 80 k. How uch brakin force has to be applied to slow you fro a velocity of

More information

Problem Set 6: Solutions

Problem Set 6: Solutions University of Aabama Department of Physics and Astronomy PH 102 / LeCair Summer II 2010 Probem Set 6: Soutions 1. A conducting rectanguar oop of mass M, resistance R, and dimensions w by fas from rest

More information

SIMPLE HARMONIC MOTION PREVIOUS EAMCET QUESTIONS ENGINEERING. the mass of the particle is 2 gms, the kinetic energy of the particle when t =

SIMPLE HARMONIC MOTION PREVIOUS EAMCET QUESTIONS ENGINEERING. the mass of the particle is 2 gms, the kinetic energy of the particle when t = SIMPLE HRMONIC MOION PREVIOUS EMCE QUESIONS ENGINEERING. he displacement of a particle executin SHM is iven by :y = 5 sin 4t +. If is the time period and 3 the mass of the particle is ms, the kinetic enery

More information

Simple Harmonic Motion

Simple Harmonic Motion Siple Haronic Motion Physics Enhanceent Prograe for Gifted Students The Hong Kong Acadey for Gifted Education and Departent of Physics, HKBU Departent of Physics Siple haronic otion In echanical physics,

More information

Part B: Many-Particle Angular Momentum Operators.

Part B: Many-Particle Angular Momentum Operators. Part B: Man-Partice Anguar Moentu Operators. The coutation reations deterine the properties of the anguar oentu and spin operators. The are copete anaogous: L, L = i L, etc. L = L ± il ± L = L L L L =

More information

Periodic Motion is everywhere

Periodic Motion is everywhere Lecture 19 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand and use energy conservation

More information

before the collision and v 1 f and v 2 f after the collision. Since conservation of the linear momentum

before the collision and v 1 f and v 2 f after the collision. Since conservation of the linear momentum Lecture 7 Collisions Durin the preious lecture we stared our discussion of collisions As it was stated last tie a collision is an isolated eent in which two or ore odies (the collidin odies) exert relatiely

More information

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1 PHYS12 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 1 OSCILLATIONS Sections: 1.5 1.6 Exaples: 1.6 1.7 1.8 1.9 CHECKLIST Haronic otion, periodic otion, siple haronic

More information

(A) (B) (C) (D) None of these

(A) (B) (C) (D) None of these Exercise OBJECTIVE PROBLEMS. Action and reaction (A) act on two different objects (C) have opposite directions. Which fiure represents the correct F.B.D. of rod of mass m as shown in fiure : (B) have equal

More information

SE-514 (OPTIMAL CONTROL) OPTIMAL CONTROL FOR SINGLE AND DOUBLE INVERTED PENDULUM. DONE BY: Fatai Olalekan ( Ayman Abdallah (973610)

SE-514 (OPTIMAL CONTROL) OPTIMAL CONTROL FOR SINGLE AND DOUBLE INVERTED PENDULUM. DONE BY: Fatai Olalekan ( Ayman Abdallah (973610) SE-54 (OPTIAL CONTROL OPTIAL CONTROL FOR SINGLE AND DOUBLE INVERTED PENDULU DONE BY: Fatai Oaekan (363 Ayman Abdaah (9736 PREPARED FOR: Dr. Sami E-Ferik Tabe of contents Abstract... 3 Introduction... 3

More information

Dynamics - Midterm Exam Type 1

Dynamics - Midterm Exam Type 1 Dynaics - Midter Exa 06.11.2017- Type 1 1. Two particles of ass and 2 slide on two vertical sooth uides. They are connected to each other and to the ceilin by three sprins of equal stiffness and of zero

More information

COUPLED OSCILLATORS. Two identical pendulums

COUPLED OSCILLATORS. Two identical pendulums COUPED OSCIATORS A real physical object can be rearded as a lare nuber of siple oscillators coupled toether (atos and olecules in solids. The question is: how does the couplin affect the behavior of each

More information

which proves the motion is simple harmonic. Now A = a 2 + b 2 = =

which proves the motion is simple harmonic. Now A = a 2 + b 2 = = Worked out Exaples. The potential energy function for the force between two atos in a diatoic olecules can be expressed as follows: a U(x) = b x / x6 where a and b are positive constants and x is the distance

More information

LECTURE 10. The world of pendula

LECTURE 10. The world of pendula LECTURE 0 The word of pendua For the next few ectures we are going to ook at the word of the pane penduum (Figure 0.). In a previous probem set we showed that we coud use the Euer- Lagrange method to derive

More information

MA 201: Partial Differential Equations Lecture - 10

MA 201: Partial Differential Equations Lecture - 10 MA 201: Partia Differentia Equations Lecture - 10 Separation of Variabes, One dimensiona Wave Equation Initia Boundary Vaue Probem (IBVP) Reca: A physica probem governed by a PDE may contain both boundary

More information

The mechanical energy balance equation used for the mh-b correlation 1 (2-6) sg u

The mechanical energy balance equation used for the mh-b correlation 1 (2-6) sg u Modified Haedron and Brown Method (mh-b) This is an empirica two-phase fow correation, the core of which is correation for iquid hod-up. Griffith correation is used for fow in the bubbe fow reion. The

More information

Unit - 10 Ocsillations And Waves

Unit - 10 Ocsillations And Waves Unit - 0 Ocsillations And Waves 3 SUMMARY. Waves : he otion o the disturbance in the ediu (or in ree space) is called wave pulse or enerally a wave.. Aplitude o a wave : Aplitude o oscillation o particles

More information

SRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES

SRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES SRI LANKAN PHYSICS OLYMPIAD - 5 MULTIPLE CHOICE TEST QUESTIONS ONE HOUR AND 5 MINUTES INSTRUCTIONS This test contains ultiple choice questions. Your answer to each question ust be arked on the answer sheet

More information

PHYS 102 Previous Exam Problems

PHYS 102 Previous Exam Problems PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal

More information

Mechanics 3. Elastic strings and springs

Mechanics 3. Elastic strings and springs Chapter assessment Mechanics 3 Eastic strings and springs. Two identica ight springs have natura ength m and stiffness 4 Nm -. One is suspended verticay with its upper end fixed to a ceiing and a partice

More information

Bohr s atomic model. 1 Ze 2 = mv2. n 2 Z

Bohr s atomic model. 1 Ze 2 = mv2. n 2 Z Bohr s atomic mode Another interesting success of the so-caed od quantum theory is expaining atomic spectra of hydrogen and hydrogen-ike atoms. The eectromagnetic radiation emitted by free atoms is concentrated

More information

Newton's laws of motion

Newton's laws of motion Episode No - 5 Date: 03-04-2017 Faculty: Sunil Deshpande Newton's laws of motion * A plank with a box on it at one end is slowly raised about the other end. As the anle with the horizontal slowly reaches

More information

Simple Harmonic Motion of Spring

Simple Harmonic Motion of Spring Nae P Physics Date iple Haronic Motion and prings Hooean pring W x U ( x iple Haronic Motion of pring. What are the two criteria for siple haronic otion? - Only restoring forces cause siple haronic otion.

More information

Exam 2: Tonight 8:20-10:10pm

Exam 2: Tonight 8:20-10:10pm xa : Toniht 8:0-0:0p oo ssinents: ast Nae oo - NN 7 F-K TU 007 -O 064 P-S CB C0 T-Z CCC 00 Breakdown o the 0 Probles aterial # o Probles Chapter 6 Chapter 7 4 Chapter 8 5 Chapter 9 6 Chapter 0 Crib Sheet:

More information

PY241 Solutions Set 9 (Dated: November 7, 2002)

PY241 Solutions Set 9 (Dated: November 7, 2002) PY241 Solutions Set 9 (Dated: Noveber 7, 2002) 9-9 At what displaceent of an object undergoing siple haronic otion is the agnitude greatest for the... (a) velocity? The velocity is greatest at x = 0, the

More information

WileyPLUS Assignment 3. Next Week

WileyPLUS Assignment 3. Next Week WileyPLUS Assignent 3 Chapters 6 & 7 Due Wednesday, Noveber 11 at 11 p Next Wee No labs of tutorials Reebrance Day holiday on Wednesday (no classes) 24 Displaceent, x Mass on a spring ωt = 2π x = A cos

More information

A body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of

A body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of Chapter 14 [ Edit ] Overview Suary View Diagnostics View Print View with Answers Chapter 14 Due: 11:59p on Sunday, Noveber 27, 2016 To understand how points are awarded, read the Grading Policy for this

More information

Experiment 2: Hooke s Law

Experiment 2: Hooke s Law COMSATS Institute of Inforation Technology, Islaabad Capus PHYS-108 Experient 2: Hooke s Law Hooke s Law is a physical principle that states that a spring stretched (extended) or copressed by soe distance

More information

Experiment 3 The Simple Pendulum

Experiment 3 The Simple Pendulum PHY191 Fall003 Experiment 3: The Simple Pendulum 10/7/004 Pae 1 Suested Readin for this lab Experiment 3 The Simple Pendulum Read Taylor chapter 5. (You can skip section 5.6.IV if you aren't comfortable

More information

1. Measurements and error calculus

1. Measurements and error calculus EV 1 Measurements and error cacuus 11 Introduction The goa of this aboratory course is to introduce the notions of carrying out an experiment, acquiring and writing up the data, and finay anayzing the

More information

(C) 7 s. (C) 13 s. (C) 10 m

(C) 7 s. (C) 13 s. (C) 10 m NAME: Ms. Dwarka, Principal Period: #: WC Bryant HS Ms. Simonds, AP Science Base your answers to questions 1 throuh 3 on the position versus time raph below which shows the motion of a particle on a straiht

More information

Announcements. Last year s final exam has been posted. Final exam is worth 200 points and is 2 hours: Quiz #9 this Wednesday:

Announcements. Last year s final exam has been posted. Final exam is worth 200 points and is 2 hours: Quiz #9 this Wednesday: Announceents sartphysics hoework deadlines have been reset to :0 PM on eceber 15 (beinnin of final exa). You can et 100% credit if you o back and correct ANY proble on the HW fro the beinnin of the seester!

More information

g L Simple Pendulum, cont Simple Pendulum Period of Simple Pendulum Equations of Motion for SHM: 4/8/16 k m

g L Simple Pendulum, cont Simple Pendulum Period of Simple Pendulum Equations of Motion for SHM: 4/8/16 k m Simple Pendulum The simple pendulum is another example of simple harmonic motion The force is the component of the weiht tanent to the path of motion F t = - m sin θ Simple Pendulum, cont In eneral, the

More information

Easticity. The strain produced in the stretched spring is ) Voume Strain ) Shearing Strain 3) Tensie Strain 4) None of the above. A body subjected to strain a number of times does not obey Hooke's aw due

More information

27 Oscillations: Introduction, Mass on a Spring

27 Oscillations: Introduction, Mass on a Spring Chapter 7 Oscillations: Introduction, Mass on a Spring 7 Oscillations: Introduction, Mass on a Spring If a siple haronic oscillation proble does not involve the tie, you should probably be using conservation

More information

Control of an Inverted Pendulum Johnny Lam

Control of an Inverted Pendulum Johnny Lam Contro of an Inverted Penduu Johnny a Abstract he baancin of an inverted enduu by ovin a cart aon a horizonta track is a cassic robe in the area of contro his aer wi describe two ethods to swin a enduu

More information

2. Which of the following best describes the relationship between force and potential energy?

2. Which of the following best describes the relationship between force and potential energy? Work/Energy with Calculus 1. An object oves according to the function x = t 5/ where x is the distance traveled and t is the tie. Its kinetic energy is proportional to (A) t (B) t 5/ (C) t 3 (D) t 3/ (E)

More information

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ). Reading: Energy 1, 2. Key concepts: Scalar products, work, kinetic energy, work-energy theore; potential energy, total energy, conservation of echanical energy, equilibriu and turning points. 1.! In 1-D

More information

Question 1. [14 Marks]

Question 1. [14 Marks] 6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is

More information

Physics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Tuesday, December 7, Stress Strain. For the rest of the semester

Physics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Tuesday, December 7, Stress Strain. For the rest of the semester ics day, ember 7, 004 Ch 17: Kinetic Theory Stress Strain Ch 18: 1st Law of Thermodynamics nd Law of Thermodynamics or the rest of the semester Thursday,. 9, 3-5pm and 7-9pm Monday,. 13, 004 10:30 am 1:30

More information

Chapter 11 Simple Harmonic Motion

Chapter 11 Simple Harmonic Motion Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion

More information

Version 2.2 NE03 - Faraday's Law of Induction

Version 2.2 NE03 - Faraday's Law of Induction Definition Version. Laboratory Manua Department of Physics he University of Hong Kong Aims o demonstrate various properties of Faraday s Law such as: 1. Verify the aw.. Demonstrate the ighty damped osciation

More information

22 - ELECTRON AND PHOTONS Page 1 ( Answers at the end of all questions )

22 - ELECTRON AND PHOTONS Page 1 ( Answers at the end of all questions ) 22 - ELECTRON AND PHOTONS Page 1 1 ) A photocell is illuinated by a sall source placed 1 away. When the sae source of light is placed 1 / 2 away, the nuber of electrons eitted by photocathode would ( a

More information

m potential kinetic forms of energy.

m potential kinetic forms of energy. Spring, Chapter : A. near the surface of the earth. The forces of gravity and an ideal spring are conservative forces. With only the forces of an ideal spring and gravity acting on a ass, energy F F will

More information

00 Elasticity Mechanical Properties of olids tress and train. When a weight of 0kg is suspended fro a copper wire of length 3 and diaeter 0.4. Its length increases by.4c. If the diaeter of the wire is

More information

IX Mechanics of Rigid Bodies: Planar Motion

IX Mechanics of Rigid Bodies: Planar Motion X Mechancs of Rd Bodes: Panar Moton Center of Mass of a Rd Bod Rotaton of a Rd Bod About a Fed As Moent of nerta Penduu, A Genera heore Concernn Anuar Moentu puse and Coson nvovn Rd Bodes. Rd bod: dea

More information