LECTURE 21 TORQUE Instructor: Kazumi Tolich Lecture 21 2 ¨ Reading chapter 11-1 to 11-2 ¤ Torque ¤ Newton’s 2nd law for rotation Torque about an axis 3 ¨ Torque (𝜏) is a measure of twisting, and the magnitude of torque is defined as 𝐅⃗ 𝜏 = 𝑟𝐹 sin 𝜃 = 𝐹) 𝑟 = 𝐹𝑟* ¨ ¨ ¨ 𝑟* is called moment arm, or lever arm of 𝐅⃗. The SI unit for torque is N·∙m, the same as the unit of work. But torque and work are different physical quantities. If two or more torques act on a rigid object, the net torque is the sum of the torques with correct sign assigned to each torque. 𝜃 𝐅⃗) 𝐫⃗ Axis 𝑟* Line of action Newton’s 2nd law for rotation 4 ¨ Newton’s 2nd law for rotation is given by . 𝜏 = 𝐼𝛼 ¨ ¨ The sign of torque is the same as the sign of angular acceleration it causes if it were the only torque acting in the system. This is analogous to Newton’s 2nd law for linear motion: ∑ 𝐅⃗ = 𝑚𝐚 Quiz: 1 5 Door knobs 6 ¨ Why are all door knobs located farthest from the door hinges? ¤ It gives the longest moment arm, and therefore the most torque, assuming the knobs are always pushed normal to the door. ¤ The more torque you give, the more rotational acceleration of the door you get. Demo: 1 7 ¨ Torque Bar ¤ Demonstration of lever arm dependence of torque Quiz: 2 & 3 8 Example: 1 9 ¨ At the local playground, a child with a mass 𝑚 = 16 kg sits on the end of a horizontal teeter-totter, a distance of 𝐿 = 1.5 m from the pivot point. On the other side of the pivot an adult pushes straight down on the teeter-totter with a force of 𝐹 = 95 N. In which direction does the teeter-totter rotate if the adult applies the force at a distance of a) b) c) 𝐿6 = 3.0 m, 𝐿6 = 2.5 m, or 𝐿6 = 2.0 m from the pivot? Quiz: 4 10 Demo: 2 11 ¨ Hinged Stick and Ball ¤ When the bar is just about to become horizontal, the acceleration of the free-end of the bar is greater than 𝑔. ¤ 𝛼 ¤ 𝑎 8 9 < :;= = => A; = B@ = :@ ? = 𝐿𝛼 = A; B >𝑔 Example: 2 12 ¨ Figure shows the massive shield door at a neutron facility at Lawrence Livermore National Laboratory; this is the world’s heaviest hinged door. The door has a mass of 𝑀 = 44,000 kg, a rotational inertia about an axis through its hinges of 𝐼 = 8.7 × 104 kgm2, and a front face width of 𝑤 = 2.4 m. Neglecting friction, what steady force, applied at its outer edge and perpendicular to the plane of the door, can move it from rest through an angle of 𝜃 = 90º in 𝑡 = 30 s? Example: 3 13 ¨ A wheel on a game show is given an initial angular speed of 𝜔I = 1.22 rad/s. It comes to rest after rotating through ∆𝜃 = 0.75 of a turn. a) b) Find the average torque exerted on the wheel given that it is a disk of radius 𝑟 = 0.71 m and mass 𝑚 = 6.4 kg. If the mass of the wheel is doubled, and its radius is halved, will the angle through which it rotates before coming to rest increase, decrease, or stay the same assuming that the average torque exerted on the wheel is unchanged?
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