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2. Now, change the location of the pivot point- moving it to the right of the center of mass a distance r3. Solve the system pictured below using equation (2) for the mass of the meter stick. This will be equation (3). otar cm. sam N aquor r ure mg mg mcomg

2. Now, change the location of the pivot point- moving it to the right of the center of mass a distance r3. Solve the system pictured below using equation (2) for the mass of the meter stick. This will be equation (3). otar cm. sam N aquor r ure mg mg mcomg

College Physics
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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Can you help me solve number 2? Equation 2 is on expg2_1.jpg.

1. Starting with equation (2) above and given values on the picture below, solve the force body diagram pictured for the ratio m,/m2 loon N dlamps wi First be 2 Insert the (COM) of Record the lc r2 mg m2g mcomg 2. Now, change the location of the pivot point - moving it to the right of the center of mass a distance r3. Solve the system pictured below using equation (2) for the mass of the meter stick. This will be equation (3). notar Record om. rst 5 g Record added AN r2 m g mag mcomg CS Scan nke WheCOM position so that it achieved. Record the
Transcribed Image Text:1. Starting with equation (2) above and given values on the picture below, solve the force body diagram pictured for the ratio m,/m2 loon N dlamps wi First be 2 Insert the (COM) of Record the lc r2 mg m2g mcomg 2. Now, change the location of the pivot point - moving it to the right of the center of mass a distance r3. Solve the system pictured below using equation (2) for the mass of the meter stick. This will be equation (3). notar Record om. rst 5 g Record added AN r2 m g mag mcomg CS Scan nke WheCOM position so that it achieved. Record the
This experiment will investigate the rotational analog of forces in equilibrium – i.e. torques in equilibrium. Here we will consider the net Torque acting on a rotating mass, Et around a specified pivot point. A single torque, t, is directly related to an individual force acting on a rotating object: T =rx F; |t| = Ir||F|sine = rF1, (1) where r is the position vector indicating the distance from where the force acts to the pivot point. Only perpendicular components of force with respect to the r vector will contribute to torque. Generally speaking net torque will give rise to an angular acceleration a. Στ- Ια (general equation) Equilibrium problems consider the subset of the general equation where there is no rotation; i.e. a=0. Στ -0 (equilibrium equation) (2) CS Scanned
Transcribed Image Text:This experiment will investigate the rotational analog of forces in equilibrium – i.e. torques in equilibrium. Here we will consider the net Torque acting on a rotating mass, Et around a specified pivot point. A single torque, t, is directly related to an individual force acting on a rotating object: T =rx F; |t| = Ir||F|sine = rF1, (1) where r is the position vector indicating the distance from where the force acts to the pivot point. Only perpendicular components of force with respect to the r vector will contribute to torque. Generally speaking net torque will give rise to an angular acceleration a. Στ- Ια (general equation) Equilibrium problems consider the subset of the general equation where there is no rotation; i.e. a=0. Στ -0 (equilibrium equation) (2) CS Scanned
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