Torque_Board720130712 18:17:51localhostconverted to 1.6 markup620130605 18:19:43srnarf520130605 18:01:46srnarf420130605 17:42:40srnarf320121019 15:20:13srnarf220121017 20:50:38srnarf120121017 16:52:00srnarfTable of Mechanics DemonstrationList of Mechanics Equipment & SuppliesLecture Demonstrations
Torque Board, 1J40.25aTopic and Concept: 1J40. Statistics of Rigid Bodies, Static Torque Location: Floor Item: ME, East Wall TorqueBoard01400.jpg Abstract: A whiteboard tear drop shaped wheel is mounted vertically on its CM horizontal axis so that it can spin freely. Various weights can be hung on it at various points. The wheel will then rotate to its new equilibrium. EquipmentLocationID Number

Torque BoardFloor Item: ME, East Wall
Important Setup Notes: Some preparation may be advisable since there are several variables in this demo that can be adjusted. Setup and Procedure: Roll the board to the desired position with the white board side facing the audience. Select which hole you would like the peg (point of the applied force) to go in. String with a loop at the end should already be hanging from the peg. The string should run over the pulley. The vertical position of the pulley can be adjusted to attain the desired effect. Weight hangers should be hung from each of the two dangling strings and weight should be added to the hangars. The board will rotate until it reaches equilibrium. The dryerase markers can be used to sketch out the applied forces and the position vectors as shown in the pictures below. Cautions, Warnings, or Safety Concerns: N/A Discussion: The board is mounted at its center of mass so we don't need to worry about torque due to gravity. There are two other torques in this demonstration: one on either side of the axis of rotation so that the torques oppose each other. The torques are determined by the net weight of the mass hangars and the distance from the rotational axis at which these forces are applied. Our torque equation is Tnet = 0 = r1·W1·sin(θ)  r2·W2 where the r's denote the distance of each force from the axis of rotation, W's denote the force do to gravity acting on the masses (giving rise to the tension in the strings), and θ is the angle between the position vector and the applied tension. The angle is omitted on the second torque since the stage left string is always tangent to the board (i.e. θ2 = 90°). Since the stage left side is circular, r2 is constant. The peg location determines r1. Our choice of weights determines the angle of tilt of the board. sin(θ) = (r2·W2) / (r1·W1). TorqueBoard02250.jpgTorqueBoard04250.jpgTorqueBoard05250.jpgTorqueBoard06250.jpg
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Videos: Lecture Demonstration's Youtube Channel References: Torque  Wikipedia Rigid Body Dynamics  Wikipedia Home