Moment and angular momentum

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Moment and angular momentum TEP Related topics Circular motion, angular velocity, angular acceleration, moment of inertia, Newton s Laws, rotation. Principle The angle of rotation and angular velocity are measured as a function of time on a body which is pivoted so as to rotate without friction and which is acted on by a moment. The angular acceleration is determined as a function of the moment. Equipment 1 Turntable with angle scale 02417-02 1 Aperture plate for turntable 02417-05 1 Holding device w. cable release 02417-04 1 Air bearing 02417-01 1 Precision pulley 11201-02 1 Pressure tube, l 1.5 m 11205-01 1 Blower 230V/50Hz 13770-97 1 Power supply 5 V DC/2.4 A with 4 mm plugs 11076-99 1 Light barrier with counter 11207-30 1 Capacitor 100 nf/250v, G1 39105-18 1 Adapter, BNC-plug/socket 4 mm. 07542-26 1 Weight holder 1 g 02407 20 Slotted weight, 1 g, natur.colour 03916 1 Silk thread,200m 02412 1 Connecting cord, 32 A, 1000 mm, blue 07363-04 1 Connecting cord, 32 A, 1000 mm, red 07363-01 1 Circular level, d = 36 mm 02123 1 Tripod base -PASS- 02002-55 1 Barrel base -PASS- 02006-55 2 Bench clamp -PASS- 02010 Fig. 1: P2131500 www.phywe.com P2131500 PHYWE Systeme GmbH & Co. KG All rights reserved 1

TEP Moment and angular momentum Tasks Determine the following with uniformly accelerated rotary motion: 1. the angle of rotation as a function of time, 2. the angular velocity as a function of time. 3. the angular acceleration as a function of the force, 4. the angular acceleration as a function of the lever arm. Set-up The experimental set-up is arranged as shown in Fig. 1. Please refer to the manual of 02417-88 for details about the installation of the turntable with air bearing. By means of a spirit level, and with the blower switched on, the rotary bearing is aligned horizontally with the two adjusting feet on the support base. The release switch should be adjusted so that it touches the curve of the sector mask. The triggering range and the electrical switching point can be adjusted with the knurled screw. The angular range to be measured is fixed by moving the light barrier. The release switch and light barrier should be connected as shown in Fig. Fig. 2: Connection of the light barrier (Lb). 2. The precision pulley is clamped so that the thread is suspended horizontally over the plate and is flush with the pulley. Adjust the tripod s feet such that the turntable is horizontal. Adjust the air supply in such a manner that the rotor is just lifted by the air pressure and rotates without vibration on its cushion of air. Procedure It is suitable to perform task 1 and 2 simultaneously. After determining the time of a certain angle of rotation φ, the corresponding angular velocity ω is measured directly afterwards. Then, the light barrier is moved to the next position. 1. Measurement of the angle of rotation φ as a function of time t: Place the selection key of the fork type light barrier on. Install the light barrier in a desired angle φ with the shutter release. Press the wire release and lock in place. Press the Reset key of the light barrier. Loosening the wire release stopper sets in motion the plate of rotation with the screen and the counter starts. After the screen has passed the pin of the shutter release, the wire release is pressed again and locked. As soon as the screen enters the light path of the light barrier, the counter stops. Note If the counter stops on loosening, viz. pressing the wire release, a capacitor of high capacitance should be connected parallel to the wire release. 2 PHYWE Systeme GmbH & Co. KG All rights reserved P2131500

Moment and angular momentum TEP 2. Measurement of the angular velocity ω as a function of time t. The dark time of the sector mask in the light barrier is used (gate time Δt) for measuring velocity. Directly after the measurement of the time of rotation t for a certain angle of rotation φ, the corresponding angular velocity ω is determined by the following steps Place the selection key to the light barrier at. Press the Reset key of the light barrier. set the plate of rotation with the screen into motion by loosening the locked wire release, the counter indicates 0000. As soon as the screen enters the path of the light of the fork type light barrier, the counter starts; it stops when the screen moves out of the light path Thus, Δt is measured that you need to determine the angular velocity form Δt and Δϕ (the angle of the sector mask). See evaluation. Task3: Measurement of the angular acceleration as a function of the force To determine the acceleration as a function of the force, the mass on the weight pan is increased by 1 g at a time. The instantaneous velocities are measured at a fixed location. Determine ω and t for each weight. Task 4: Measurement of the angular acceleration as a function of the lever arm The dependence of the acceleration on the radius is determined at constant mass. The instantaneous velocities are measured at a fixed location. The precision pulley must be aligned to the corresponding radius (height, alignment). The light barrier is not moved. Determine ω and t for each radius. Three different lever arms can be adjusted (15/30/45 mm). Theory The relationship between the angular momentum L of a rigid body in a stationary coordinate system with its origin at the centre of gravity, and the moment T acting on it, is The angular momentum is expressed by the angular velocity ω and the inertia tensor Î from (1) that is the reduction of the tensor with the vector. In the present case, ω has the direction of a principal inertia axis (z-axis), so that L has only one component: where I Z is the z-component of the principal inertia tensor of the plate. For this case, equation (1) reads: www.phywe.com P2131500 PHYWE Systeme GmbH & Co. KG All rights reserved 3

TEP Moment and angular momentum The moment of the force F (see Fig. 2) gives, as shown in Fig. 3, where: r = Radius of the axle bolt or of the driving wheel used m = Accelerated mass g = 9.81 m/s 2 Acceleration of gravity Fig. 3: Moment of a weight force on the rotary plate. The equation of motion now reads With the initial condition (2) one obtains (3) and for the angle of rotation φ with the initial condition (4) 4 PHYWE Systeme GmbH & Co. KG All rights reserved P2131500

Moment and angular momentum TEP Evaluation and results Task 1: The results from task one are plotted logarithmically as in Fig 4. Simplifying Equation 4 gives Y = A X B The slope of the regression line in the logarithmic diagram in Fig 4 is the exponential statement B. The exponent is: B = 2.005 which confirms equation (4). Task 2: The angular velocity ω is calculated from the following equation ω = Δϕ / Δt where Δϕ is the angle of the sector mask and Δt is the time that this mask needs to cross the light barrier. (In this sample result Δϕ = 0,262 rad). Thus, Fig. 4: Angle of rotation as a function of time with uniformly accelerated rotary motion for m = 0.01 kg, r = 0.015 m. where t 1 is the time from the start until the sector mask reaches the light barrier (angle time). In an ω(t) graph (Fig 5) the ω(t) relationship is exactly the slope of the regression line (see (3)). To calculate I Z, the accelerating mass m and the radius r of the rotational axis around which the thread is wound must be taken into consideration. In this exemplary measurement the following is valid: m (slope) = mgr / I z = 0.114 rad/s 2 (see (3)) Thus the moment of inertia is I Z = 0.0129 kgm 2. Remark: The accelerated mass m becomes increasingly more rapid in the course of the experiment and thus receives an increasing kinetic energy. However, this energy is extremely small compared to the two other energy forms present and can thus be neglected in the calculation. Fig. 5: Angular velocity as a function of time in uniformly accelerated rotary motion, with m = 0.01 kg, r = 0.015 m. www.phywe.com P2131500 PHYWE Systeme GmbH & Co. KG All rights reserved 5

TEP Moment and angular momentum Task 3: Angular acceleration α is determined using the following equation α = ω/t 1 where ω is the velocity after the angle time t 1 (see task 2). For a uniformly accelerated rotary movement, the angular acceleration as a function of time is constant. The results of Task 3 are plotted in Fig. 6. Fig. 6: Angular acceleration α = ω/t 1 as a function of the active force with uniformly accelerated rotary motion for r = 0.03 m. Task 4: Calculate the angular acceleration α as in Task 3. The results of Task 4 are plotted in Fig. 7. Fig. 7: Angular acceleration as a function of the lever arm with uniformly accelerated rotary motion for m = 0.016 kg. 6 PHYWE Systeme GmbH & Co. KG All rights reserved P2131500