Jurong Junior College 2014 JC1 H1 and H2 Physics (8866 and 9646) Tutorial Topic: 5. Work, Energy and Power Learning Outcomes (Candidates should be able to:) (a) show an understanding of the concept of work in terms of the product of a force and displacement in the direction of the force. (b) calculate the work done in a number of situations, including the work done by a gas which is expanding against a constant external pressure: W = pV. (c) give examples of energy in different forms, its conversion and conservation, and apply the principle of energy conservation to simple examples. (d) derive, from the equations of motion, the formula Ek = ½ m v2. (e) (f) (g) (h) (i) (j) (k) Questions 1 2 3, 7, 9, 10, 11, . 11, refer to lecture notes. recall and apply the formula Ek = ½ m v2. 3, 11, . distinguish between gravitational potential energy, electric potential Refer to lecture energy and elastic potential energy. notes. show an understanding of and use the relationship between force and 4 potential energy in a uniform field to solve problems. derive, from the defining equation W = Fs, the formula Ep = mgh for 11, refer to potential energy changes near the Earth’s surface. lecture notes. recall and use the formula Ep = mgh for potential energy changes near 5, 8, 11, . the Earth’s surface. show an appreciation for the implications of energy losses in practical 5 devices and use the concept of efficiency to solve problems. define power as work done per unit time and derive power as the product 5, 6, refer to of force and velocity. lecture notes. Section A: Fundamental/conceptual questions F 1. θ s A object is pulled by force F over a horizontal distance s. Calculate the work done if (i) (ii) (iii) (iv) F is 1 N, θ is 0 and s is 2 m. [W = F s cos θ] (1)(2) cos 0o = 2 J [2 J] F is 4 N, θ is 30 and s is 5 m. [W = F s cos θ] (4)(5) cos 30o = 17.3 J [17.3 J] F is 7 N, θ is 60 and s is 8 m. [W = F s cos θ] (7)(8) cos 60o = 28 J [28 J] F is 10 N, θ is 90 and s is 11 m. [W = F s cos θ] (10)(11) cos 90o = 0 J Page 1 [0 J] 2. A gas expands by 100 cm3 against a constant pressure of 1.25 × 105 Pa. Calculate the work done by the gas. [12.5 J] [W = pV] (1.25 × 105)(100)(10-2)3 = 12.5 J 3. On braking, 500 kJ of heat was produced when a vehicle of total mass 1600 kg was brought to rest on a level road. What was the speed of the vehicle just before the brakes were applied? [25 m s-1] Loss in KE of the vehicle = heat dissipated 1 2 (1600)v 2 500 103 v = 25 m s-1 4. 5. A charged body placed in a uniform electric field experiences an electric force of 10 N. (i) What is the change in the electric potential energy of the body if it moves a displacement of 5.0 cm in the direction of the electric force? [Fx = U] [0.5 J] U = Fx = (10)(0.05) = 0.5 J (ii) Is there an increase or a decrease in the electric potential energy of the charged body? U is negative means there is a decrease in the electric potential energy of the charged body A crane lifts a load of 8000 N at constant speed through a vertical distance of 20 m in a time of 4 s. (i) (ii) What is the average useful power during this operation? Average useful power total useful work done 8000 20 40 kW total time taken 4 If the efficiency of the motor is 20%, what is the electrical power supplied to the motor? [200 kW] useful output energy useful output power Efficiency x100% x100% total input energy total input power 40 103 100% total input power Total input power = 200 kW 20% 6. [40 kW] TYS Page 67 Question 9 [N09/I/12] At constant velocity, resultant force on boat is zero, hence applied force from boat engine = total resistive force experienced by boat = kv2 power required from boat engine = applied force from boat engine × velocity of boat = (kv2)(v) = kv3 72000 = kv3 = k(123) eqn 1 Page 2 With only 1 engine, power = 36000 W, hence 36000 = kv3 eqn 2 1 Dividing eqn 1 by eqn 2 gives v3 = 2(123) So, v = 9.5 ms-1 Section B: Short examination-style questions 7. The diagram on the right shows an arrangement used to find the output power of an electric motor. The wheel attached to the motor's axle has a circumference of 0.5 m and the belt which passes over it is stationary when the weights have the values shown. If the wheel makes 20 revolutions per second, what is the output power? [300 W] P 8. Fs (20)(0.5) s F 50 20 300 W t 1 t The diagram shows two bodies X and Y connected by a light cord passing over a light, free-running pulley. X starts from rest and moves on a smooth plane inclined at 30 to the horizontal. Calculate the total kinetic energy of the system when X has travelled 2.0 m along the plane. [59 J] Using conservation of energy, KE gain by X + KE gain by Y + GPE gain by X = GPE loss by Y Total KE of system + (4.0)(9.81)(2.0 sin 30o) = (5.0)(9.81)(2.0) Total KE of system = 59 J 9. Discuss the energy changes which take place for a system comprising a mass suspended from the end of a spring and then made to oscillate vertically. You need to refer to the different forms of energy involved. (Assume the oscillation is small enough so that the spring is never compressed but always stretched by different extent during the oscillation.) Assume the oscillation is started by displacing the mass vertically downwards from its equilibrium position thus stretching the spring and giving it elastic potential energy (EPE). When the Page 3 mass is released and the oscillation begins, the EPE stored in the spring is converted into kinetic energy (KE) and gravitational potential energy (GPE) of the mass as it moves upwards. The KE of the mass is maximum when it moves at maximum speed past the equilibrium position. After the mass passes the equilibrium position, its KE and the EPE stored in the spring are converted into GPE as it continues to move upwards. When the mass reach the highest point in the oscillation, its KE is zero and its GPE is maximum whereas the EPE stored in the spring is minimum. As the mass move from the highest point to the equilibrium position, its GPE is converted to its KE and EPE stored in the spring. As it moves from the equilibrium position to the lowest point, its KE and GPE are converted to EPE stored in the spring, thus completing one oscillation. Dissipative forces will gradually convert the mechanical energy into thermal energy so the amplitude of the oscillation will decrease with time and eventually become zero. Section C: Long examination-style questions 10. (a) Starting with the definition of work, deduce the change in the gravitational potential energy of a mass m, when moved a distance h upwards against a gravitational field of field strength g. (b) By using the equations of motion, show that the kinetic energy Ek of an object of mass m travelling with speed v is given by Ek = ½mv2. Page 4 (c) A cyclist, together with his bicycle, has a total mass of 90 kg and is travelling with a constant speed of 15 m s1 on a flat road at A, as shown below. He then goes down a small slope to B, descending 4.0 m in doing so. Calculate (i) the kinetic energy at A, ½mv2 = ½(90)(15)2 = 10.1 kJ [10.1 kJ] (ii) the loss of potential energy between A and B, mgh = (90)(9.81)(4.0) = 3.53 kJ [3.53 kJ] (iii) the speed at B, assuming that all the lost potential energy is transformed into kinetic energy of the cyclist and bicycle. Loss in GPE = gain in KE [17.4 m s1] 2 2 (90)(9.81)(4.0) = ½(90)v ½(90)(15) v = 17.4 m s-1 (d) (i) A cyclist traveling at a constant speed of 15 m s1 on a level road provides a power of 240 W. Calculate the total resistive force. For constant speed motion, [16 N] force provided by cyclist = total resistive force F. Power from cyclist = (Force provided by cyclist)(velocity of cyclist) 240 = (F)(15) F = 16 N Page 5 (ii) (c) The cyclist now travels at a higher constant speed. Explain why the cyclist needs to provide a greater power. 1. Higher speed also means larger value for total resistive force F since air resistance increases with speed. 2. Since the cyclist is moving at constant speed, force by the cyclist is equal to total resistive force, force by cyclist increase. 3. The power required of the cyclist is the product of F and v so it will be higher. It is often stated that many forms of transport transform chemical energy into kinetic energy. Explain why the cyclist travelling at constant speed is not making this transformation. Explain what transformations of energy are taking place. Since the cyclist is travelling at constant speed, there is no increase in kinetic energy. The chemical energy from the cyclist is being converted to thermal energy in the gears, tyres, road and air when overcoming resistive forces. Some of the chemical energy is also converted to sound energy. 11. (a) The minimum flying speed for a bird called house-martin is 9.0 m s1. It reaches this speed by falling from its nest before swooping away. Calculate the minimum distance its nest must be above the ground. [4.13 m] Loss in GPE = gain in KE m(9.81)h = ½m(9.0)2 h = 4.13 m (b) A house-martin has a mass of 120 g. When it returns to its nest, it is travelling horizontally at P with a speed of 13.0 m s1 and at a distance 7.5 m below its nest. It then glides upwards to the nest, as shown in the figure below. Neglecting any air resistance, calculate (i) (ii) the kinetic energy of the house-martin at P, KE at P = ½(120 x 10-3)(13.0)2 = 10.1 J [10.1 J] the gain in potential energy as it glides upwards to its nest, gain in GPE = (120 x 10-3)(9.81)(7.5) = 8.83 J [8.83 J] Page 6 (iii) (iv) (c) its kinetic energy as it reaches its nest, Gain in GPE = loss in KE 8.83 = 10.1 KE as it reaches its nest KE as it reaches its nest = 1.27 J its speed as it reaches its nest, ½(120 x 10-3)v2 = 1.27 v = 4.60 ms-1 [1.27 J] [4.60 m s-1] Discuss qualitatively how air resistance affects, if at all, each of your answers in (b). (b)(i) No effect. (b)(ii) No effect (but the house-martin may not reach its nest if its KE at P is less than the sum of GPE required to gain that height and the energy required to overcome air resistance). (b)(iii) Decreased (since there is work done to overcome air resistance). (b)(iv) Decreased (since it reaches its nest with less KE). Page 7