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

Size: px
Start display at page:

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

Transcription

1 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, moment of inertia of uniform bodies with simpe geometrica shapes; Anguar momentum; Torque; Conservation of anguar momentum; Dynamics of rigid bodies with fixed axis of rotation; Roing without sipping of rings, cyinders and spheres; Equiibrium of rigid bodies; Coision of point masses with rigid bodies. Q. In absence of torque the rotationa frequency of a body changes from cy/sec to 6 cy/sec, then ratio of radius of gyration in two cases wi be : : : : 4 : Q. A partice of mass m is rotating in a pane is a circuar path of radius r, its anguar momentum is L. The centripita force acting on the partice is : L mr L m r L L mr mr Q. For the same tota mass which of the foowing wi have the argest moment of inertia about an axis passing through its centre of mass and perpendicuar to the pane of the body a disc of radius a a ring of radius a a square amina of side a four rods forming a square of side a Q.4 Find the moment of inertia of a pate cut in shape of a right anged triange of mass M, side AC = BC = a about an axis perpendicuar to the pane of the pate and passing through the mid point of side AB Ma Ma 6 Ma Ma Q.5 Three identica thin rods each of mass m & ength are paced aong x, y & z-axis respectivey they are paced such that, one end of each rod is at origin 'O'. Then moment of inertia of this system about z-axis is m m m m 4 Q.6 Two rods of equa mass m and ength ie aong the x axis and y axis with their centres origin. What is the moment of inertia of both about the ine x=y : m m 4 m m 6

2 Cass (XI) Q.7 Moment of inertia of a rectanguar pate about an axis passing through P and perpendicuar to the pate is I. Then moment of PQR about an axis perpendicuar to the pane of the pate: about P = I/ about R = I/ about P > I/ about R > I/ Q.8 Let I, I and I be the moment of inertia of a uniform square pate about axes AOC, xdx' and yby' respectivey as shown in the figure. The moments of inertia of the pate I : I : I are in the ratio. : 7 : 7 : 7 : 7 : : 7 7 : 7 : 7 Q.9 A thin uniform rod of mass M and ength L has its moment of inertia I about its perpendicuar bisector. The rod is bend in the form of a semicircuar arc. Now its moment of inertia through the centre of the semi circuar arc and perpendicuar to its pane is I. The ratio of I : I wi be < > = can t be said Q.0 The moment of inertia of semicircuar pate of radius R and mass M about axis AA in its pane passing through its centre is MR MR cos 4 MR Q. In the trianguar sheet given PQ = QR =. If M is the mass of the sheet. What is the moment of inertia about PR M 4 M Q. Moment of inertia of a thin semicircuar disc (mass = M & radius = R) about an axis through point O and perpendicuar to pane of disc, is given by : M 6 sin MR 4 M 4 MR MR 8 MR MR Q. Moment of inertia of a semicircuar ring of radius R and mass M ; about an axis passing through A and perpendicuar to the pane of the paper is MR MR 5 MR MR Q.4 A square sheet of edge ength L and uniform mass per unit area is used to form a hoow cyinder. The moment of inertia of this cyinder about the centra axis is 4 L 4 L 4 8 L L 4 Prepared By: Er. Vineet Loomba (IIT Roorkee)

3 Jupiter (XI) Q.5 A rigid body can be hinged about any point on the x-axis. When it is hinged such that the hinge is at x, the moment of inertia is given by I = x x + 7 The x-coordinate of centre of mass is x = x = 0 x = x = Q.6 A square pate of mass M and edge L is shown in figure. The moment of inertia of the pate about the axis in the pane of pate passing through one of its vertex making an ange 5 from horizonta is. ML ML 4 7ML none Q.7 A wire of mass M and ength L is bent in the form of a circuar ring. The moment of inertia of the ring about its axis is 8 ML (8 )ML 4 ML (4 )ML Q.8 The figure shows a uniform rod ying aong the x-axis. The ocus of a the points ying on the xy-pane, about which the moment of inertia of the rod is same as that about O is an eipse a circe a paraboa a straight ine Q.9 Consider the foowing statements Assertion : The moment of inertia of a rigid body reduces to its minimum vaue as compared to any other parae axis when the axis of rotation passes through its centre of mass. Reason (R): The weight of a rigid body aways acts through its centre of mass in uniform gravitationa fied. Of these statements: both A and R are true and R is the correct expanation of A both A and R are true but R is not a correct expanation of A A is true but R is fase A is fase but R is true For more such free Assignments visit Question No. 0 to (4 questions) The figure shows an isoscees trianguar pate of mass M and base L. The ange at the apex is 90. The apex ies at the origin and the base is parae to X axis Q.0 The moment of inertia of the pate about the z-axis is ML ML ML 4 6 Q. The moment of inertia of the pate about the x-axis is none of these ML ML ML ML Q. The moment of inertia of the pate about its base parae to the x-axis is Prepared By: Er. Vineet Loomba (IIT Roorkee)

4

5 Jupiter (XI) 5 side AB is horizonta. The reaction at the support A is: mg mg mg mg Q. In an experiment with a beam baance on unknown mass m is baanced by two known mass m is baanced by two known masses of 6 kg and 4 kg as shown in figure. The vaue of the unknown mass m is 0 kg 6 kg 8 kg kg Q. A uniform cube of side b and mass M rest on a rough horizonta tabe. A horizonta force F is appied norma to one of the face at a point, at a height b/4 above the base. What shoud be the coefficient of friction ( ) between cube and tabe so that is wi tip about an edge before it starts sipping? > > > none Q. A homogeneous cubica brick ies motioness on a rough incined surface. The haf of the brick which appies greater pressure on the pane is : eft haf right haf both appies equa pressure the answer depend upon coefficient of friction Q.4 Find minimum height of obstace so that the sphere can stay in equiibrium. R cos R ( sin ) R sin R ( cos ) Q.5 A haow cone of radius R and height R is paced on an incined pane of incination. If is increased graduay, at what vaue of the cone wi toppe. Assume sufficient friction is present to prevent sipping. tan (/) tan (/) sin (/) cos (/) For more such free Assignments visit Q.6 A smooth rod of ength is kept inside a troey at an ange as shown in the figure. What shoud be the acceeration a of the troey so that the rod remains in equiibrium with respect to it? g tan g cos g sin g cot Q.7 A uniform adder of ength 5m is paced against the wa as shown in the figure. If coefficient of friction is the same for both the was, what is the minimum vaue of for it not to sip? = = 4 = = 5 Q.8 A uniform cyinder rests on a cart as shown. The coefficient of static friction between the cyinder and Prepared By: Er. Vineet Loomba (IIT Roorkee)

6 Jupiter (XI) 6 the cart is 0.5. If the cyinder is 4 cm in diameter and 0 cm in height, which of the foowing is the minimum acceeration of the cart needed to cause the cyinder to tip over? m/s 4 m/s 5 m/s the cyinder woud side before it begins to tip over. Q.9 A uniform rod of ength L and weight W is suspended horizontay by two vertica ropes as shown. The first rope is attached to the eft end of the rod whie the second rope is attached a distance L 4 from the right end. The tension in the second rope is W 4 W W W Q.40 The spoo shown in figure is paced on rough horizonta surface and has inner radius r and outer radius R. The ange between the appied force and the horizonta can be varied. The critica ange ( ) for which the spoo does not ro and remains stationary is given by r r r r = cos = cos R = cos R = sin R R Q.4 Two ight vertica springs with equa natura engths and spring constants k and k are separated by a distance. Their upper ends are fixed to the ceiing and their ower ends to the ends A and B of a ight horizonta rod AB. A vertica downwards force F is appied at point C on the rod. AB wi remain horizonta in equiibrium if the distance AC is k k Q.4 Consider the foowing statements Assertion : A cycist aways bends inwards whie negotiating a curve Reason(R) : By bending he owers his centre of gravity Of these statements, both A and R are true and R is the correct expanation of A both A and R are true but R is not the correct expanation of A A is true but R is fase A is fase but R is true Q.4 A cone of radius r and height h rests on a rough horizonta surface, the coefficient of friction between the cone and the surface being. A graduay increasing horizonta force F is appied to the vertex of the cone. The argest vaue of for which the cone wi side before it toppes is = r h = r 5h k k k k k k = h r = r h Q.44 A uniform rod of mass m and ength hinged at its end is reeased from rest when it is in the horizonta position. The norma reaction at the hinge when the rod becomes vertica is : Prepared By: Er. Vineet Loomba (IIT Roorkee)

7

8 Jupiter (XI) 8 mass m o hangs from the end of a ight string wound round the cyinder which does not sip over it. When the system is aowed to move, the acceeration of the descending mass wi be mog m m o mog m m o mog m m o mog m m o Q.5 A uniform rod of ength, hinged at the ower end is free to rotate in the vertica pane. If the rod is hed verticay in the beginning and then reeased, the anguar acceeration of the rod when it makes an ange of 45 o with the horizonta (I = m /) g 6g Q.5 A bock of mass m is attached to a puey disc of equa mass m, radius r by means of a sack string as shown. The puey is hinged about its centre on a horizonta tabe and the bock is projected with an initia veocity of 5 m/s. Its veocity when the string becomes taut wi be m/s.5 m/s 5/ m/s 0/ m/s Q.54 A sma bead of mass m moving with veocity v gets threaded on a stationary semicircuar ring of mass m and radius R kept on a horizonta tabe. The ring can freey rotate about its centre. The bead comes to rest reative to the ring. What wi be the fina anguar veocity of the system? v/r v/r v/r v/r Q.55 A sma object is attached to a ight string which passes through a hoow tube. The tube is hed by one hand and the string by the other. The object is stet into rotation in a circe of radius r. The string is then pued down, shortening the radius of the circe to r. The ratio of the new kinetic energy to origina kinetic energy is r r g r r g r r Q.56 A man, sitting firmy over a rotating stoo has his arms streched. If he fods his arms, the work done by the man is zero positive negative may be positive or negative. Q.57 A partice of mass kg ocated at the position ( î ĵ) m has a veocity ( î ĵ kˆ ) m/s. Its anguar momentum about z-axis in kg-m /s is: zero +8 8 Q.58 A partice is moving in a circuar orbit of radius r with an anguar veocity. It jumps to another circuar orbit of radius r and attains an anguar veocity. If r = 0.5 r and assuming that no externa torque is appied to the system, then the anguar veocity, is given by : = 4 = = = Prepared By: Er. Vineet Loomba (IIT Roorkee)

9 Q.59 A partice of mass m is projected with a veocity u making an ange 45 with the horizonta. The magnitude of the torque due to weight of the projectie, when the partice is at its maximum height, about the point of projectie mu 4 mu 4 mu mu Q.60 Three bodies have equa masses m. Body A is soid cyinder of radius R, body B is a square amina of side R, and body C is a soid sphere of radius R. Which body has the smaest moment of inertia about an axis passing through their centre of mass and perpendicuar to the pane (in case of amina) A B C A and C both Q.6 A point mass m A is connected to a point mass m B by a massess rod of ength as shown in the figure. It is observed that the ratio of the moment of inertia of the system about the two axes BB and AA, which is parae to each other and perpendicuar to the rod is IBB I =. The distance of the centre of mass of the system from the mass A is AA (/4) (/) (/) (/4) Q.6 A chid with mass m is standing at the edge of a disc with moment of inertia I, radius R, and initia anguar veocity. See figure given beow. The chid jumps off the edge of the disc with tangentia veocity v with respect to the ground. The new anguar veocity of the disc is I mv I I mvr I (I mr ) mv I (I mr ) mvr I Q.6 A partice of mass 0.5 kg is rotating in a circuar path of radius m and centrepeta force on it is 9 Newtons. Its anguar momentum (in J sec) is: Question No. 64 & 65 ( questions) A uniform rod is fixed to a rotating turntabe so that its ower end is on the axis of the turntabe and it makes an ange of 0 to the vertica. (The rod is thus rotating with uniform anguar veocity about a vertica axis passing through one end.) If the turntabe is rotating cockwise as seen from above. Q.64 What is the direction of the rod's anguar momentum vector (cacuated about its ower end)? verticay downwards down at 0 to the horizonta up at 0 to the horizonta verticay upwards Q.65 Is there a torque acting on it, and if so in what direction? yes, verticay yes, horizontay yes at 0 to the horizonta no Q.66 A straight rod of ength L is reeased on a frictioness horizonta foor in a vertica position. As it fas + sips, the distance of a point on the rod from the ower end, which foows a quarter circuar ocus is L/ L/4 L/8 None Q.67 Two partices of mass m each are fixed at the opposite ends of a massess rod of ength 5m which is oriented verticay on a smooth horizonta surface and reeased. Find the dispacement of the ower

10 mass on the ground when the rod makes an ange of 7 with the vertica..5 m m.5 m.5 m Q.68 A partice starts from the point (0m, 8m) and moves with uniform veocity of i m/s. After 5 seconds, the anguar veocity of the partice about the origin wi be : 8 89 rad/s 8 rad/s 4 89 rad/s 8 7 rad/s Q.69 A hinged construction consists of three rhombs with the ratio of sides 5::. Vertex A moves in the horizonta direction at a veocity v. Veocity of A is.5 V V.5 V 0.8 V Q.70 A whee of radius r roing on a straight ine, the veocity of its centre being v. At a certain instant the point of contact of the whee with the grounds is M and N is the highest point on the whee (diametricay opposite to M). The incorrect statement is: The veocity of any point P of the whee is proportiona to MP. Points of the whee moving with veocity greater than v form a arger area of the whee than points moving with veocity ess than v. The point of contact M is instantaneousy at rest. The veocities of any two parts of the whee which are equidistant from centre are equa. Q.7 Two points of a rigid body are moving as shown. The anguar veocity of the body is: R R R Q.7 There is rod of ength. The veocities of its two ends are v and v in opposite directions norma to the rod. The distance of the instantaneous axis of rotation from v is: zero v v v v v v R / Q.7 A thin rod of ength L is paced at ange to vertica on a frictioness horizonta foor and reeased. If the center of mass has acceeration = A, and the rod an anguar acceeration = at initia moment, then A = (L ).sin A/ = (L ).sin A = (L ).sin A = L Q.74 A disc of radius R is roing purey on a fat horizonta surface, with a constant anguar veocity. The ange between the veocity and acceeration vectors of point P is zero 45 5 tan (/) Q.75 A adder of ength L is sipping with its ends against a vertica wa and a horizonta foor. At a certain moment, the speed of the end in contact with the horizonta foor is v and the adder makes

11 an = 0 with the horizonta. Then the speed of the adder s center must be v v/ v None ange Q.76 In the previous question, if dv/dt = 0, then the anguar acceeration of the adder when = 45 is v /L v /L [v L ] None Q.77 A ring of radius R ros without siding with a constant veocity. The radius of curvature of the path foowed by any partice of the ring at the highest point of its path wi be R R 4R None Q.78 Two spheres are roing with same veocity (for their C. M.) their ratio of kinetic energy is : & radius ratio is :, their mass ratio wi be : : 4 : 8 : : Q.79 Two identica circuar oops are moving with same kinetic energy one ros & other sides. The ratio of their speed is : : : : 5 : Q.80 Inner and outer radii of a spoo are r and R respectivey. A thread is wound over its inner surface and paced over a rough horizonta surface. Thread is pued by a force F as shown in fig. then in case of pure roing Thread unwinds, spoo rotates anticockwise and friction act eftwards Thread winds, spoo rotates cockwise and friction acts eftwards Thread winds, spoo moves to the right and friction act rightwards Thread winds, spoo moves to the right and friction does not come into existence. For more such free Assignments visit Q.8 Portion AB of the wedge shown in figure is rough and BC is smooth. A soid cyinder ros without sipping from A to B. The ratio of transationa kinetic energy to rotationa kinetic energy, when the cyinder reaches point C is : /4 5 7/5 8/ Q.8 A pank of mass M is paced over smooth incined pane and a sphere is aso paced over the pank. Friction is sufficient between sphere and pank. If pank and sphere are reeased from rest, the frictiona force on sphere is: up the pane down the pane horizonta zero Q.8 A pank with a uniform sphere paced on it rests on a smooth horizonta pane. Pank is pued to right by a constant force F. If sphere does not sip over the pank. Which of the foowing is incorrect. Acceeration of the centre of sphere is ess than that of the pank. Work done by friction acting on the sphere is equa to its tota kinetic energy.

12

13 Q.9 A sender uniform rod of ength is baanced verticay at a point P on a horizonta surface having some friction. If the top of the rod is dispaced sighty to the right, the position of its centre of mass at the time when the rod becomes horizonta : ies at some point to the right of P ies at some point to the eft of P must be / to the right of P ies at P Q.9 A soid sphere with a veocity (of centre of mass) v and anguar veocity is genty paced on a rough horizonta surface. The frictiona force on the sphere: must be forward (in direction of v) must be backward (opposite to v) cannot be zero none of the above Q.9 A cyinder is pure roing up an incine pane. It stops momentariy and then ros back. The force of friction on the cycinder is zero throughout the journey is directed opposite to the veocity of the centre of mass throughout the journey is directed up the pane throughout the journey is directed down the pane throughout the journey Q.94 A uniform circuar disc paced on a rough horizonta surface has initiay a veocity v 0 and an anguar veocity 0 as shown in the figure. The disc comes to rest after moving some distance in v the direction of motion. Then 0 r is 0 Q.95 On a soid sphere ying on a horizonta surface a force F is appied at a height of R/ from the centre of mass. The initia acceeration of a point at the top of the sphere is (there is no sipping at any point) 5F 7M 5F 4M 0 F 7M M F Q.96 A ba ros down an incined pane, figure. The ba is first reeased from rest from P and then ater from Q. Which of the foowing statement is/ are correct? (i) The ba takes twice as much time to ro from Q to O as it does to ro from P to O. (ii) The acceeration of the ba at Q is twice as arge as the acceeration at P. (iii) The ba has twice as much K.E. at O when roing from Q as it does when roing from P. i, ii ony ii, iii ony i ony iii ony Question No. 97 to 0 (6 questions) In the foowing probems, indicate the correct direction of friction force acting on the cyinder, which is pued on a rough surface by a constant force F. Q.97 A cyinder of mass M and radius R is pued horizontay by a force F. The

14 friction force can be given by which of the foowing diagrams (B ) cannot be interpreted Q.98 A cyinder is pued horizontay by a force F acting at a point beow the centre of mass of the cyinder, as shown in figure. The friction force can be given by which of the foowing diagrams (B ) cannot be interpreted Q.99 A cyinder is pued horizontay by a force F acting at a point above the centre of mass of the cyinder, as shown in figure. The friction force can be given by which of the foowing diagrams (B ) cannot be interpreted Q.00 A cyinder is paced on a rough pank which in turn is paced on a smooth surface. The pank is pued with a constant force F. The friction force can be given by which of the foowing diagrams canot be interpreted For more such free Assignments visit Maths Notes and Assignments for IIT-JEE: Physics Notes and Assignments for IIT-JEE: Chemistry Notes and Assignments for IIT-JEE: New Chapters and Assignments are being reguary updated. Share it with your friends because Sharing is Caring. Discuss among yoursef or with your teachers in case of doubts. You can post your doubts on website comment section too and I wi try to answer as eary as possibe. SHARING IS CARING!! I AM SHARING WITH YOU. YOU HAVE TO SHARE WITH YOUR FRIENDS AND HELP THEM.

15 ANSWER KEY Q. D Q. D Q. D Q.4 B Q.5 B Q.6 C Q.7 C Q.8 D Q.9 A Q.0 D Q. B Q. B Q. D Q.4 B Q.5 D Q.6 B Q.7 C Q.8 B Q.9 B Q.0 C Q. A Q. C Q. C Q.4 B Q.5 B Q.6 B Q.7 D Q.8 A Q.9 D Q.0 B Q. C Q. A Q. A Q.4 D Q.5 B Q.6 D Q.7 C Q.8 B Q.9 D Q.40 A Q.4 D Q.4 B Q.4 C Q.44 C Q.45 B Q.46 A Q.47 C Q.48 C Q.49 C Q.50 C Q.5 A Q.5 A Q.5 D Q.54 C Q.55 C Q.56 B Q.57 D Q.58 A Q.59 D Q.60 B Q.6 D Q.6 D Q.6 C Q.64 B Q.65 B Q.66 B Q.67 A Q.68 C Q.69 D Q.70 D Q.7 B Q.7 C Q.7 C Q.74 B Q.75 C Q.76 A Q.77 C Q.78 A Q.79 C Q.80 B Q.8 B Q.8 D Q.8 D Q.84 C Q.85 A Q.86 C Q.87 C Q.88 D Q.89 D Q.90 A Q.9 A Q.9 D Q.9 C Q.94 A Q.95 A Q.96 D Q.97 A Q.98 A Q.99 D Q.00 B

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

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

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

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

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

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

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

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

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

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

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

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

PROBLEMS. Apago PDF Enhancer

PROBLEMS. Apago PDF Enhancer PROLMS 15.105 900-mm rod rests on a horizonta tabe. force P appied as shown produces the foowing acceerations: a 5 3.6 m/s 2 to the right, a 5 6 rad/s 2 countercockwise as viewed from above. etermine 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

ELASTICITY PREVIOUS EAMCET QUESTIONS ENGINEERING

ELASTICITY PREVIOUS EAMCET QUESTIONS ENGINEERING ELASTICITY PREVIOUS EAMCET QUESTIONS ENGINEERING. If the ratio of engths, radii and young s modui of stee and brass wires shown in the figure are a, b and c respectivey, the ratio between the increase

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

Physics Dynamics: Springs

Physics Dynamics: Springs F A C U L T Y O F E D U C A T I O N Department of Curricuum and Pedagogy Physics Dynamics: Springs Science and Mathematics Education Research Group Supported by UBC Teaching and Learning Enhancement Fund

More information

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s

More information

Solution Set Seven. 1 Goldstein Components of Torque Along Principal Axes Components of Torque Along Cartesian Axes...

Solution Set Seven. 1 Goldstein Components of Torque Along Principal Axes Components of Torque Along Cartesian Axes... : Soution Set Seven Northwestern University, Cassica Mechanics Cassica Mechanics, Third Ed.- Godstein November 8, 25 Contents Godstein 5.8. 2. Components of Torque Aong Principa Axes.......................

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

TAM 212 Worksheet 9: Cornering and banked turns

TAM 212 Worksheet 9: Cornering and banked turns Name: Group members: TAM 212 Worksheet 9: Cornering and banked turns The aim of this worksheet is to understand how vehices drive around curves, how sipping and roing imit the maximum speed, and how banking

More information

IIT JEE, 2005 (MAINS) SOLUTIONS PHYSICS 1

IIT JEE, 2005 (MAINS) SOLUTIONS PHYSICS 1 IIT JEE, 5 (MINS) SOLUTIONS YSIS iscaimer: Tis booket contains te questions of IIT-JEE 5, Main Examination based on te memory reca of students aong wit soutions provided by te facuty of riiant Tutorias.

More information

Term Test AER301F. Dynamics. 5 November The value of each question is indicated in the table opposite.

Term Test AER301F. Dynamics. 5 November The value of each question is indicated in the table opposite. U N I V E R S I T Y O F T O R O N T O Facuty of Appied Science and Engineering Term Test AER31F Dynamics 5 November 212 Student Name: Last Name First Names Student Number: Instructions: 1. Attempt a questions.

More information

RIGID BODIES - MOMENT OF INERTIA

RIGID BODIES - MOMENT OF INERTIA IID DIES - ET F IETI The inabiity of a body to change by itsef its position of rest or uniform motion is caed Inertia. The greater the mass of the body, the greater its inertia as greater force is required

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

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

APPENDIX C FLEXING OF LENGTH BARS

APPENDIX C FLEXING OF LENGTH BARS Fexing of ength bars 83 APPENDIX C FLEXING OF LENGTH BARS C.1 FLEXING OF A LENGTH BAR DUE TO ITS OWN WEIGHT Any object ying in a horizonta pane wi sag under its own weight uness it is infinitey stiff or

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

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

Numerical simulation of javelin best throwing angle based on biomechanical model

Numerical simulation of javelin best throwing angle based on biomechanical model ISSN : 0974-7435 Voume 8 Issue 8 Numerica simuation of javein best throwing ange based on biomechanica mode Xia Zeng*, Xiongwei Zuo Department of Physica Education, Changsha Medica University, Changsha

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

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String

Lecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary

More information

Class XI Chapter 7- System of Particles and Rotational Motion Physics

Class XI Chapter 7- System of Particles and Rotational Motion Physics Page 178 Question 7.1: Give the location of the centre of mass of a (i) sphere, (ii) cylinder, (iii) ring, and (iv) cube, each of uniform mass density. Does the centre of mass of a body necessarily lie

More information

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on

More information

Laboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis

Laboratory Exercise 1: Pendulum Acceleration Measurement and Prediction Laboratory Handout AME 20213: Fundamentals of Measurements and Data Analysis Laboratory Exercise 1: Penduum Acceeration Measurement and Prediction Laboratory Handout AME 20213: Fundamentas of Measurements and Data Anaysis Prepared by: Danie Van Ness Date exercises to be performed:

More information

O9e Fringes of Equal Thickness

O9e Fringes of Equal Thickness Fakutät für Physik und Geowissenschaften Physikaisches Grundpraktikum O9e Fringes of Equa Thickness Tasks 1 Determine the radius of a convex ens y measuring Newton s rings using ight of a given waveength.

More information

PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE) 60 Best JEE Main and Advanced Level Problems (IIT-JEE). Prepared by IITians.

PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE) 60 Best JEE Main and Advanced Level Problems (IIT-JEE). Prepared by IITians. www. Class XI TARGET : JEE Main/Adv PREPARED BY: ER. VINEET LOOMBA (B.TECH. IIT ROORKEE) ALP ADVANCED LEVEL PROBLEMS Straight Lines 60 Best JEE Main and Advanced Level Problems (IIT-JEE). Prepared b IITians.

More information

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18

Quantum Mechanical Models of Vibration and Rotation of Molecules Chapter 18 Quantum Mechanica Modes of Vibration and Rotation of Moecues Chapter 18 Moecuar Energy Transationa Vibrationa Rotationa Eectronic Moecuar Motions Vibrations of Moecues: Mode approximates moecues to atoms

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

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

Physics 235 Chapter 8. Chapter 8 Central-Force Motion

Physics 235 Chapter 8. Chapter 8 Central-Force Motion Physics 35 Chapter 8 Chapter 8 Centra-Force Motion In this Chapter we wi use the theory we have discussed in Chapter 6 and 7 and appy it to very important probems in physics, in which we study the motion

More information

CE601-Structura Anaysis I UNIT-IV SOPE-DEFECTION METHOD 1. What are the assumptions made in sope-defection method? (i) Between each pair of the supports the beam section is constant. (ii) The joint in

More information

Exam 3 Practice Solutions

Exam 3 Practice Solutions Exam 3 Practice Solutions Multiple Choice 1. A thin hoop, a solid disk, and a solid sphere, each with the same mass and radius, are at rest at the top of an inclined plane. If all three are released at

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

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z Chapter W3 Mechanica Systems II Introduction This companion website chapter anayzes the foowing topics in connection to the printed-book Chapter 3: Lumped-parameter inertia fractions of basic compiant

More information

Chap. 10: Rotational Motion

Chap. 10: Rotational Motion Chap. 10: Rotational Motion I. Rotational Kinematics II. Rotational Dynamics - Newton s Law for Rotation III. Angular Momentum Conservation (Chap. 10) 1 Newton s Laws for Rotation n e t I 3 rd part [N

More information

O -x 0. 4 kg. 12 cm. 3 kg

O -x 0. 4 kg. 12 cm. 3 kg Anwer, Key { Homework 9 { Rubin H andau 1 Thi print-out houd have 18 quetion. Check that it i compete before eaving the printer. Ao, mutipe-choice quetion may continue on the net coumn or page: nd a choice

More information

DYNAMICS MOMENT OF INERTIA

DYNAMICS MOMENT OF INERTIA DYNAMICS MOMENT OF INERTIA S TO SELF ASSESSMENT EXERCISE No.1 1. A cylinder has a mass of 1 kg, outer radius of 0.05 m and radius of gyration 0.03 m. It is allowed to roll down an inclined plane until

More information

Chapter 8, Rotational Equilibrium and Rotational Dynamics. 3. If a net torque is applied to an object, that object will experience:

Chapter 8, Rotational Equilibrium and Rotational Dynamics. 3. If a net torque is applied to an object, that object will experience: CHAPTER 8 3. If a net torque is applied to an object, that object will experience: a. a constant angular speed b. an angular acceleration c. a constant moment of inertia d. an increasing moment of inertia

More information

Question 7.1: Answer. Geometric centre; No

Question 7.1: Answer. Geometric centre; No Question 7.1: Give the location of the centre of mass of a (i) sphere, (ii) cylinder, (iii) ring,, and (iv) cube, each of uniform mass density. Does the centre of mass of a body necessarily lie inside

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

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed

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

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.

More information

1D Heat Propagation Problems

1D Heat Propagation Problems Chapter 1 1D Heat Propagation Probems If the ambient space of the heat conduction has ony one dimension, the Fourier equation reduces to the foowing for an homogeneous body cρ T t = T λ 2 + Q, 1.1) x2

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

c 2007 Society for Industrial and Applied Mathematics

c 2007 Society for Industrial and Applied Mathematics SIAM REVIEW Vo. 49,No. 1,pp. 111 1 c 7 Society for Industria and Appied Mathematics Domino Waves C. J. Efthimiou M. D. Johnson Abstract. Motivated by a proposa of Daykin [Probem 71-19*, SIAM Rev., 13 (1971),

More information

Webreview Torque and Rotation Practice Test

Webreview Torque and Rotation Practice Test Please do not write on test. ID A Webreview - 8.2 Torque and Rotation Practice Test Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A 0.30-m-radius automobile

More information

Pendulum with a square-wave modulated length

Pendulum with a square-wave modulated length Penduum with a square-wave moduated ength Eugene I. Butikov St. Petersburg State University, St. Petersburg, Russia Abstract Parametric excitation of a rigid panar penduum caused by a square-wave moduation

More information

Chemical Kinetics Part 2

Chemical Kinetics Part 2 Integrated Rate Laws Chemica Kinetics Part 2 The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates the rate

More information

Cluster modelling. Collisions. Stellar Dynamics & Structure of Galaxies handout #2. Just as a self-gravitating collection of objects.

Cluster modelling. Collisions. Stellar Dynamics & Structure of Galaxies handout #2. Just as a self-gravitating collection of objects. Stear Dynamics & Structure of Gaaxies handout # Custer modeing Just as a sef-gravitating coection of objects. Coisions Do we have to worry about coisions? Gobuar custers ook densest, so obtain a rough

More information

Multiple Beam Interference

Multiple Beam Interference MutipeBeamInterference.nb James C. Wyant 1 Mutipe Beam Interference 1. Airy's Formua We wi first derive Airy's formua for the case of no absorption. ü 1.1 Basic refectance and transmittance Refected ight

More information

Newton s Law of motion

Newton s Law of motion 5-A 11028 / 9, WEA, Sat Nagar, Karol Bagh New Delhi-110005 M : 9910915514, 9953150192 P : 011-45660510 E : keshawclasses@gmail.com W: www.keshawclasses.com Newton s Law of motion Q. 1. Two sphere A and

More information

Figure 1 Answer: = m

Figure 1 Answer: = m Q1. Figure 1 shows a solid cylindrical steel rod of length =.0 m and diameter D =.0 cm. What will be increase in its length when m = 80 kg block is attached to its bottom end? (Young's modulus of steel

More information

Physics. TOPIC : Rotational motion. 1. A shell (at rest) explodes in to smalll fragment. The C.M. of mass of fragment will move with:

Physics. TOPIC : Rotational motion. 1. A shell (at rest) explodes in to smalll fragment. The C.M. of mass of fragment will move with: TOPIC : Rotational motion Date : Marks : 120 mks Time : ½ hr 1. A shell (at rest) explodes in to smalll fragment. The C.M. of mass of fragment will move with: a) zero velocity b) constantt velocity c)

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics Physics 111.6 MIDTERM TEST #2 November 16, 2000 Time: 90 minutes NAME: STUDENT NO.: (Last) Please Print (Given) LECTURE SECTION

More information

arxiv: v1 [physics.flu-dyn] 2 Nov 2007

arxiv: v1 [physics.flu-dyn] 2 Nov 2007 A theoretica anaysis of the resoution due to diffusion and size-dispersion of partices in deterministic atera dispacement devices arxiv:7.347v [physics.fu-dyn] 2 Nov 27 Martin Heer and Henrik Bruus MIC

More information

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003 FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Saturday, 14 December 2013, 1PM to 4 PM, AT 1003 NAME: STUDENT ID: INSTRUCTION 1. This exam booklet has 14 pages. Make sure none are missing 2. There is

More information

PHYSICS 221, FALL 2011 EXAM #2 SOLUTIONS WEDNESDAY, NOVEMBER 2, 2011

PHYSICS 221, FALL 2011 EXAM #2 SOLUTIONS WEDNESDAY, NOVEMBER 2, 2011 PHYSICS 1, FALL 011 EXAM SOLUTIONS WEDNESDAY, NOVEMBER, 011 Note: The unit vectors in the +x, +y, and +z directions of a right-handed Cartesian coordinate system are î, ĵ, and ˆk, respectively. In this

More information

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym

FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym FALL TERM EXAM, PHYS 1211, INTRODUCTORY PHYSICS I Thursday, 11 December 2014, 6 PM to 9 PM, Field House Gym NAME: STUDENT ID: INSTRUCTION 1. This exam booklet has 13 pages. Make sure none are missing 2.

More information

(1) Class Test Solution (STRUCTURE) Answer key. 31. (d) 32. (b) 33. (b) IES MASTER. 34. (c) 35. (b) 36. (c) 37. (b) 38. (c) 39.

(1) Class Test Solution (STRUCTURE) Answer key. 31. (d) 32. (b) 33. (b) IES MASTER. 34. (c) 35. (b) 36. (c) 37. (b) 38. (c) 39. () ass Test Soution (STRUTUR) 7-09-07 nswer key. (b). (b). (c). (a) 5. (b) 6. (a) 7. (c) 8. (c) 9. (b) 0. (d). (c). (d). (d). (c) 5. (d) 6. (a) 7. (c) 8. (d) 9. (b) 0. (c). (a). (a). (b) (b) 5. (b) 6.

More information

Lecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling

Lecture 9. Stability of Elastic Structures. Lecture 10. Advanced Topic in Column Buckling Lecture 9 Stabiity of Eastic Structures Lecture 1 Advanced Topic in Coumn Bucking robem 9-1: A camped-free coumn is oaded at its tip by a oad. The issue here is to find the itica bucking oad. a) Suggest

More information

Technical Data for Profiles. Groove position, external dimensions and modular dimensions

Technical Data for Profiles. Groove position, external dimensions and modular dimensions Technica Data for Profies Extruded Profie Symbo A Mg Si 0.5 F 25 Materia number.206.72 Status: artificiay aged Mechanica vaues (appy ony in pressing direction) Tensie strength Rm min. 245 N/mm 2 Yied point

More information

Please Visit us at:

Please Visit us at: Q # 1. What do you know about the circular motion? CIRCULAR MOTION Ans. When a body is moving in a circle, its motion is called circular motion. Q # 2. Define the term angular displacement. Also describe

More information

Code No: R Set No. 1

Code No: R Set No. 1 Code No: R05010302 Set No. 1 I B.Tech Supplimentary Examinations, February 2008 ENGINEERING MECHANICS ( Common to Mechanical Engineering, Mechatronics, Metallurgy & Material Technology, Production Engineering,

More information

Chapter Rotational Motion

Chapter Rotational Motion 26 Chapter Rotational Motion 1. Initial angular velocity of a circular disc of mass M is ω 1. Then two small spheres of mass m are attached gently to diametrically opposite points on the edge of the disc.

More information

b) 2/3 MR 2 c) 3/4MR 2 d) 2/5MR 2

b) 2/3 MR 2 c) 3/4MR 2 d) 2/5MR 2 Rotational Motion 1) The diameter of a flywheel increases by 1%. What will be percentage increase in moment of inertia about axis of symmetry a) 2% b) 4% c) 1% d) 0.5% 2) Two rings of the same radius and

More information

International Journal of Advance Engineering and Research Development

International Journal of Advance Engineering and Research Development Scientific Journa of Impact Factor (SJIF): 4.4 Internationa Journa of Advance Engineering and Research Deveopment Voume 3, Issue 3, March -206 e-issn (O): 2348-4470 p-issn (P): 2348-6406 Study and comparison

More information

if the initial displacement and velocities are zero each. [ ] PART-B

if the initial displacement and velocities are zero each. [ ] PART-B Set No - 1 I. Tech II Semester Regular Examinations ugust - 2014 ENGINEERING MECHNICS (Common to ECE, EEE, EIE, io-tech, E Com.E, gri. E) Time: 3 hours Max. Marks: 70 Question Paper Consists of Part- and

More information

High Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings

High Efficiency Development of a Reciprocating Compressor by Clarification of Loss Generation in Bearings Purdue University Purdue e-pubs Internationa Compressor Engineering Conference Schoo of Mechanica Engineering 2010 High Efficiency Deveopment of a Reciprocating Compressor by Carification of Loss Generation

More information

Chemical Kinetics Part 2. Chapter 16

Chemical Kinetics Part 2. Chapter 16 Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates

More information

ROTATIONAL & ROLLING MOTION

ROTATIONAL & ROLLING MOTION PR ROTATIONA & ROING MOTION CA CB TYPES OF MOTION Motion of an object can be of three kinds : Translational Motion Rotational Motion Rolling Motion ROTATIONA MOTION Here we examine the rotation of a rigid

More information

CHAPTER 9. Columns and Struts

CHAPTER 9. Columns and Struts CHATER 9 Coumns and Struts robem. Compare the ratio of the strength of soid stee coumn to that of the hoow stee coumn of the same cross-sectiona area. The interna diameter of the hoow coumn is /th of the

More information

Get Solution of These Packages & Learn by Video Tutorials on EXERCISE-1

Get Solution of These Packages & Learn by Video Tutorials on  EXERCISE-1 OBJECTIVE PROBLEMS EXERCISE-. A force of 98 N is require to just start moving a body of mass 00 kg over ice. The coefficient of static friction is : (A) 0.6 0.4 (C) 0. (D) 0.. The maximum static frictional

More information

Add Math (4044/02) (+) x (+) 2. Find the coordinates of the points of intersection of the curve xy 2 the line 2y 1 x 0. [5]

Add Math (4044/02) (+) x (+) 2. Find the coordinates of the points of intersection of the curve xy 2 the line 2y 1 x 0. [5] Add Math (444/) Requirement : Answer a questions Tota mars : 7 Duration : hour 45 minutes. Sove the inequaity 5 and represent the soution set on the number ine. [4] 5 4 From the setch on number ine, we

More information

AAPT UNITED STATES PHYSICS TEAM AIP 2012 DO NOT DISTRIBUTE THIS PAGE

AAPT UNITED STATES PHYSICS TEAM AIP 2012 DO NOT DISTRIBUTE THIS PAGE 2012 Semifina Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2012 Semifina Exam DO NOT DISTRIBUTE THIS PAGE Important Instructions for the Exam Supervisor This examination consists of two parts. Part A has

More information

TOPIC D: ROTATION EXAMPLES SPRING 2018

TOPIC D: ROTATION EXAMPLES SPRING 2018 TOPIC D: ROTATION EXAMPLES SPRING 018 Q1. A car accelerates uniformly from rest to 80 km hr 1 in 6 s. The wheels have a radius of 30 cm. What is the angular acceleration of the wheels? Q. The University

More information

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method. Version 2 CE IIT, Kharagpur

Module 2. Analysis of Statically Indeterminate Structures by the Matrix Force Method. Version 2 CE IIT, Kharagpur odue 2 naysis of Staticay ndeterminate Structures by the atri Force ethod Version 2 E T, Kharagpur esson 12 The Three-oment Equations- Version 2 E T, Kharagpur nstructiona Objectives fter reading this

More information

(Refer Slide Time: 2:34) L C V

(Refer Slide Time: 2:34) L C V Microwave Integrated Circuits Professor Jayanta Mukherjee Department of Eectrica Engineering Indian Intitute of Technoogy Bombay Modue 1 Lecture No 2 Refection Coefficient, SWR, Smith Chart. Heo wecome

More information

Problem Set x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. 1. Moment of Inertia: Disc and Washer

Problem Set x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. 1. Moment of Inertia: Disc and Washer 8.01x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology Problem Set 10 1. Moment of Inertia: Disc and Washer (a) A thin uniform disc of mass M and radius R is mounted on an axis passing

More information

THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS

THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS ECCM6-6 TH EUROPEAN CONFERENCE ON COMPOSITE MATERIALS, Sevie, Spain, -6 June 04 THE OUT-OF-PLANE BEHAVIOUR OF SPREAD-TOW FABRICS M. Wysocki a,b*, M. Szpieg a, P. Heström a and F. Ohsson c a Swerea SICOMP

More information

Circle the correct answer. For those questions involving calculations, working MUST be shown to receive credit.

Circle the correct answer. For those questions involving calculations, working MUST be shown to receive credit. Dynamics Assignment 3 Name: Multiple Choice. Circle the correct answer. For those questions involving calculations, working MUST be shown to receive credit. 1. Which statement is always true regarding

More information

1. An object is dropped from rest. Which of the five following graphs correctly represents its motion? The positive direction is taken to be downward.

1. An object is dropped from rest. Which of the five following graphs correctly represents its motion? The positive direction is taken to be downward. Unless otherwise instructed, use g = 9.8 m/s 2 Rotational Inertia about an axis through com: Hoop about axis(radius=r, mass=m) : MR 2 Hoop about diameter (radius=r, mass=m): 1/2MR 2 Disk/solid cyllinder

More information

DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE

DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE 3 th Word Conference on Earthquake Engineering Vancouver, B.C., Canada August -6, 4 Paper No. 38 DYNAMIC RESPONSE OF CIRCULAR FOOTINGS ON SATURATED POROELASTIC HALFSPACE Bo JIN SUMMARY The dynamic responses

More information

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

PHYS 110B - HW #1 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased PHYS 110B - HW #1 Fa 2005, Soutions by David Pace Equations referenced as Eq. # are from Griffiths Probem statements are paraphrased [1.] Probem 6.8 from Griffiths A ong cyinder has radius R and a magnetization

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

Laws of Motion. Multiple Choice Questions

Laws of Motion. Multiple Choice Questions The module presented herein is a sequel to MCQs on different units in Physics, a few viz. Rotational motion and Oscillations etc. posted earlier. The contents of the documents are intended to give the

More information

3.10 Implications of Redundancy

3.10 Implications of Redundancy 118 IB Structures 2008-9 3.10 Impications of Redundancy An important aspect of redundant structures is that it is possibe to have interna forces within the structure, with no externa oading being appied.

More information

CHAPTER 8: ROTATIONAL OF RIGID BODY PHYSICS. 1. Define Torque

CHAPTER 8: ROTATIONAL OF RIGID BODY PHYSICS. 1. Define Torque 7 1. Define Torque 2. State the conditions for equilibrium of rigid body (Hint: 2 conditions) 3. Define angular displacement 4. Define average angular velocity 5. Define instantaneous angular velocity

More information