Coefficient of Friction Experiment Notes

Objectives

  • Determine the static (μ<em>s\mu<em>s) and kinetic (μ</em>k\mu</em>k) coefficients of friction using an inclined plane.

  • Determine μ<em>k\mu<em>k and μ</em>s\mu</em>s using a horizontal setup with a pulley and applied forces.

  • Compare the values of μ<em>k\mu<em>k and μ</em>s\mu</em>s obtained by the two methods.

  • Demonstrate that the coefficients are independent of the normal force and that \mus > \muk.

Theory

  • Friction is a force resisting motion between two surfaces.

  • The normal force (FNF_N) acts perpendicularly to the surface of contact.

    • For a horizontal surface: F<em>N=F</em>g=mgF<em>N = F</em>g = mg

  • On an inclined plane with angle θ\theta: F<em>N=F</em>gcosθ=mgcosθF<em>N = F</em>g \cos \theta = mg \cos \theta

Static and Kinetic Friction

  • Static friction (f<em>sf<em>s) occurs between surfaces not in motion: f</em>sμsNf</em>s \le \mu_s N

    • If the applied force is less than the maximum static friction, there is no motion.

    • If the applied force exceeds the maximum static friction, the object moves.

  • Kinetic friction (f<em>kf<em>k) occurs when surfaces are moving relative to each other: f</em>k=μkNf</em>k = \mu_k N

    • μk\mu_k is assumed to be constant at slow speeds.

Inclined Plane

  • At the angle where the block just begins to slip (θ<em>s\theta<em>s):μ</em>s=tanθs\mu</em>s = \tan \theta_s

  • When the block slides down at constant velocity (angle θ<em>k\theta<em>k): μ</em>k=tanθk\mu</em>k = \tan \theta_k

Horizontal Plane with Pulley

  • For static friction (M<em>1M<em>1 is the block mass, M</em>2M</em>2 is the mass needed to start movement):M<em>2=μ</em>sM1M<em>2 = \mu</em>s M_1

  • For kinetic friction (M<em>2M<em>2 is the mass needed to maintain constant velocity): M</em>2=μ<em>kM</em>1M</em>2 = \mu<em>k M</em>1

Experimental Procedure: Inclined Plane

  • Incline the plane until the block slides on its own to determine static friction.

  • Measure Y (height of block) and X (distance from pivot line).

  • Repeat with added masses.

  • Calculate μ<em>s=YX=tanθ</em>s\mu<em>s = \frac{Y}{X} = tan \theta</em>s for each mass.

  • Repeat the procedure to find the angle at which the block moves at constant speed after a slight push to determine kinetic friction.

  • Calculate μ<em>k=YX=tanθ</em>k\mu<em>k = \frac{Y}{X} = tan \theta</em>k for each mass.

Experimental Procedure: Horizontal Plane with Pulley

  • Place the board horizontally with a pulley at the edge.

  • Attach a string to the block, run it over the pulley, and attach a mass holder.

  • Add mass to the holder until the block just moves (static friction) or moves at constant velocity (kinetic friction).

  • Record M<em>1M<em>1 (block mass) and M</em>2M</em>2 (mass on holder).

  • Calculate μ<em>s\mu<em>s and μ</em>k\mu</em>k using the equations M<em>2=μ</em>sM<em>1M<em>2 = \mu</em>s M<em>1 and M</em>2=μ<em>kM</em>1M</em>2 = \mu<em>k M</em>1 respectively.

  • Perform a linear least squares fit of M<em>2M<em>2 vs. M</em>1M</em>1 to determine the slopes, which are equal to μ<em>s\mu<em>s and μ</em>k\mu</em>k.

Inclined Plane Setup (Alternative Method)

  • Set up the inclined plane.

  • Attach a string to the block, over the pulley, and attach a weight hanger to the other end.

  • Adjust the string to be parallel to the inclined plane.

  • Add masses to the hanger until the block moves at a constant velocity after using the vibration part of the apparatus.

  • Record the total hanging weight in the Data Table 5.

  • Add different amounts of mass to the block for different values of Fg and repeat step 5.

  • Empty all the mass out of the block before proceeding to the next step.

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