Teacher Notes
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Atwood’s MachineDemonstration Kit
Publication No. 13926
IntroductionAccurately measuring the acceleration of a falling object due to gravity is difficult because a falling object travels short, laboratory-scale distances very quickly. However, by slowing down an object’s fall according to the rules of Newton’s second law of motion, the acceleration due to gravity can be accurately determined by an indirect method. A device that is used to indirectly measure the acceleration due to gravity is called an Atwood’s machine. Concepts
MaterialsAtwood’s machine*
Clamp holder Digital timer or stopwatch Heavy books Hooked masses, 200-g, 2 (or equivalent) Meter sticks, 2, or tape measure Pulley cord* Slotted masses, 1-g, 5† Slotted mass, 5-g† Slotted mass, 10-g† Slotted mass, 20-g† Support stand Table or platform, 1.5 m or higher Towel, soft *Materials included in kit. †Suggested (may use others) Safety PrecautionsPlease follow normal laboratory safety guidelines. Make sure the weights are tightly secured to the pulley cord so they will not come loose during the experiment. If one weight falls off one end of the pulley system, one side will crash down to the ground while the other side flies up. The quickly falling and/or rising masses could cause injury. The masses may also be damaged if they hit the floor too hard. Prelab Preparation
ProcedureSimple Atwood’s Machine
The results from the Simple Atwood’s Machine Procedure are generally not as good as expected (about 30–40% error). This is because the simplified Atwood’s equation (Equation 5 from the Discussion section) assumes the pulleys are massless and frictionless, and that the mass of the string is negligible. However, the results indicate this is obviously not the case. Better results are obtained from the same data by using a more realistic Atwood’s equation (Equation 10 from the Discussion section). Equation 10 accounts for the mass of the pulley sheave as well as the friction in the axles of the pulley.
Teacher Tips
Correlation to Next Generation Science Standards (NGSS)†Science & Engineering PracticesAnalyzing and interpreting dataUsing mathematics and computational thinking Developing and using models Disciplinary Core IdeasMS-PS2.B: Types of InteractionsHS-PS2.A: Forces and Motion HS-PS2.B: Types of Interactions Crosscutting ConceptsSystems and system modelsPerformance ExpectationsHS-PS1-8: Develop models to illustrate the changes in the composition of the nucleus of the atom and the energy released during the processes of fission, fusion, and radioactive decay. Sample DataRelease height (h): 163.5 cm {13926_Data_Table_1_Time Trials}
Determining the acceleration due to gravity Simple Equation (Equation 5) g = 0.259 m/s2 x (200 g + 220 g)/(220 g – 200 g) = 5.44 m/s2 Percent error from the accepted value of g: [(9.81 m/s2 – 5.44 m/s2)/9.81 m/s2] x 100% = 44.5% error Accounting for Friction and Pulley Mass (Equation 10) “Frictional” mass (measured) (mf): 8.3 g Mass of pulley sheave (ms): 5.3 g g = 0.259 m/s2 x (200 g + 220 g + 5.3 g)/(220 g – 200 g – 8.3 g) = 9.41 m/s2 Percent error from the accepted value of g: [(9.81 m/s2 – 9.41 m/s2)/9.81 m/s2] x 100% = 4.1% error DiscussionThe Atwood’s Machine was developed by Reverend George Atwood in the late 18th century to indirectly measure the acceleration of gravity. When two unequal masses are tied to the ends of a length of string and hung over a pulley, the larger mass will accelerate down, while the smaller mass accelerates up at the same rate. If the pulleys are assumed to be massless and frictionless, the acceleration of both masses is the same and it depends on the acceleration due to gravity, as well as the total mass of the system and the difference in mass between the two hanging masses. This follows Newton’s second law of motion, force equals mass times acceleration (F = ma). Refer to Figure 2 and the following equations for the derivation of the theoretical Atwood’s machine equation. {13926_Discussion_Figure_2}
{13926_Discussion_Equation_1}
{13926_Discussion_Equation_2}
{13926_Discussion_Equation_3}
{13926_Discussion_Equation_4}
{13926_Discussion_Equation_5}
Where: T1 = tension in string 1 A rotating object experiences a torque that is equal to its rotational moment of inertia times its angular acceleration (τ = Iα). A torque is equal to a force times the distance of the lever arm where the force is applied (τ = F x r). In the case of Atwood’s machine, the lever arm is the radius (R) of the pulley sheave (see Figure 3). Therefore, the torque is equal to the net force on the outer rim of the pulley sheave times the radius, R, of the pulley. Rotational moment of inertia is equivalent to the “rotational” mass of the object about an axis of rotation. Assuming the pulley sheave is a solid cylinder with mass ms and radius R, its rotational moment of inertia about the center is equal to ½msR2. Angular acceleration is simply the linear acceleration divided by the radial distance from the center of rotation (α = a/R). {13926_Discussion_Figure_3}
The friction along the axle of the pulley sheave produces a torque that acts against the rotation. Since the torque produced by friction acts against the motion, it can be assumed that an additional mass has been added to the smaller mass which causes the acceleration of the masses to be less than expected compared to the ideal situation. The torque produced by this “frictional” mass, mf, is equal to mfgR. Since the “frictional” mass is a measure of the total friction produced by the two-pulley Atwood’s machine in this experiment, it is assumed that each pulley produces half the total measured amount of friction. The net force on the outer edge of the pulley sheave is therefore: {13926_Discussion_Equation_6}
{13926_Discussion_Equation_7}
Equation 7 reduces to:
{13926_Discussion_Equation_8}
Substitute for T1 and T2 from Equations 1 and 2:
{13926_Discussion_Equation_9}
Rearrange to solve for g:
{13926_Discussion_Equation_10}
The pulley sheave’s mass is a constant. For the Atwood’s machine in this experiment the mass of the pulley sheave is 5.3 ±0.1 grams. The “frictional” mass will be measured during the experiment and is dependent on the total mass hanging from the pulleys. The masses acceleration is determined by the following equation:
{13926_Discussion_Equation_11}
h = distance the masses move (heavy mass falls, lighter mass rises) References“Making Atwood’s Machine ‘Work.’” The Physics Teacher, Vol. 39. March 2001, pp. 154–158. Recommended Products
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