Phys211C6 p1 Work: a measure of the change produced by a force Work = force through the displacement W = F s(assuming force is constant!) Units: 1 Newton. 1 meter = 1 joule = 1J = 1 N. m x FF W = F x Work and Kinetic Energy

Phys211C6 p2 Ex: A car is pushed by a constant 200 N force across a level street for a distance of 20 m. How much work is done by the person pushing on the car?

Phys211C6 p3 Work: portion of the force along displacement * displacement W = F cos  x F cos  x FF W = F cos  |x| x FF W = F |x| x F cos 90 = F  FF W = 0 Total Work = F net cos  x where  is the angle between net force and displacement What is net work done on an object moving at constant velocity?

Phys211C6 p4 Ex: An object with weight 15,000 N is dragged for a distance of 20.0 m across level ground. The force is exerted through a cable with a tension of 5,000 N which makes an angle of 36.9º above the horizontal. There is a 3,500 N frictional force opposing the motion. What is the work done by gravity, the force applied by the tension and friction?

Phys211C6 p5 Kinetic Energy motion in a straight line from constant acceleration (and force)

Phys211C6 p6 Ex: Take previous example of the 15,000 N dragged across level ground. Determine the final speed via the Work- Energy Theorem and via Newton’s Laws. Take the initial speed to be 3.00 m/s. Example: A pile driver uses a 200 kg hammer is dropped from a height of 3m above a beam that is being driven into the ground. The rails which guide the hammer exert a 60.0 N frictional force on the falling hammer-head. The beam is driven 7.4 cm further into the ground with each impact. What is the speed of the hammer as it hits the beam? What is the average force of the hammer on the pile when struck?

Phys211C6 p7 Interpreting Kinetic Energy accelerating an object from rest W net = K – 0 = K Kinetic Energy is the total work necessary to accelerate an object from rest to its final speed. conversely Kinetic Energy is the total work an object can do in the process of being brought to rest.

Phys211C6 p8 Example: Consider two objects of mass m and 2m are accelerated from rest. Compare the work done on them, their final kinetic energies and their final speeds if they are under the influence of identical forces acting over the same distances. Compare the work done on them, their final kinetic energies and the distances they must have traveled if they are under the influence of identical forces and end up with the same final speed.

Phys211C6 p9 F x Work and Energy with varying forces Take average force, small sub-intervals  x i F1F1 x2x2 x3x3 x4x4 xNxN … F2F2 F3F3 Constant Force – near trivial example W = F. (x 2  x 1 ) F x x2x2 x1x1

Phys211C6 p10 F x Varying Force Example: Force of a Spring |F| = kx (Hooke’s “Law”) k is spring constant or force constant note that force and displacement are in opposite directions! From origin to x: area under curve = area of right triangle W = ½ “height”. “width” = ½ kx x = ½ kx 2 From x1 to x2: area is difference between two triangles W = ½ kx 2 2  ½ kx 1 2 these results are for the work done on the spring F x2x2 x1x1

Phys211C6 p11 Example: A 600 N individual steps upon a spring scale which is compressed by 1.00 cm under her weight. What is the force constant? How much work is done on the spring?

Phys211C6 p12 mv v Work-Energy for a varying Force

Phys211C6 p13 Example: A.100 kg mass is attached to the end of a spring which has a force constant of 20.0 N/m. The spring is initially unstretched. The mass is given an initial speed of 1.50 m/s to the right. Find the maximum distance the mass moves to the right if the surface is frictionless the coefficient of kinetic friction between the mass and the surface is.47

Phys211C6 p14 Work and energy along a curve: small increment of work along a small displacement dW = F cos  dl = F. dl Add up increments of work along all such displacements

Phys211C6 p15 Example: A small child of weight w is push slowly by a horizontal force until the swing chain makes an angle  f with respect to the vertical. Determine the work done by the tension in the chain (near trivial), the “push” force (needs calculus), and the force of gravity ff

Phys211C6 p16 Power: the rate at which work is done

Phys211C6 p17 Example: A 50.0 kg marathon runner is to run up the stairs of the 443 m tall Sears Tower in Chicago in 15 minutes. What is the runner’s average power exerted in this effort?