CIRCULAR MOTION NOTES
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Text from the first pagesMACRO H2 Physics Topic 6: Motion in a Circle Notes 2 ©MACRO Learning Physics All Rights Reserved under 9836 3500 Copyright Act (Cap. 63) of Singapore Checklist: Motion in a Circle Check (ü) 1. I am able to express angular displacement in radians and use its respective formula. 2. I am able to show an understanding of and use the concept of angular velocity to solve problems. 3. I am able to recall and use 𝑣=𝑟𝜔 to solve problems. 4. I can qualitatively describe the motion due to a constant perpendicular force. 5. I am able to recall and use 𝑎=𝑟𝜔! and 𝑎="!# to solve problems. 6. I am able to recall and use 𝐹=𝑚𝑟𝜔! and 𝐹=$"!# to solve related problems. 7. I am able to distinguish between uniform and non-uniform circular motion by a. Identifying the respective forces acting on an object in non-unform circular motion b. Resolving relevant forces in the intended directions.
MACRO H2 Physics Topic 6: Motion in a Circle Notes 3 ©MACRO Learning Physics All Rights Reserved under 9836 3500 Copyright Act (Cap. 63) of Singapore Introduction Why does water stay at the bottom of a container when it is swung in a vertical circle? Why do we feel weightless in orbit in space? Why are we slightly heavier in the north pole than on the equator? Many phenomenon in our lives can be explained through the topic of circular motion, the study of objects moving in a circular paths, and the conditions required to stay in circular motion. Angular Displacement Angular Displacement is the angle swept out by the radius r joining the body to the centre of a circle. Following the formula for arc length, the angular displacement 𝜃, is given by the ratio of the arc length s, and the radius of the circle, r. One radian is defined as the angle subtended at the centre of the circle by an arc equal in length to the radius of the circle. Conversion from radians(𝑟𝑎𝑑) to degrees: 𝐴𝑛𝑔𝑙𝑒 𝑖𝑛 𝑟𝑎𝑑 ×180°=𝐴𝑛𝑔𝑙𝑒 𝑖𝑛 °×𝜋 Standard conversion formula: Active recall: What is the definition of one joule? 𝜃=𝑠𝑟 𝐴𝑛𝑔𝑙𝑒 𝑖𝑛 𝑢𝑛𝑖𝑡 𝑥×𝑞𝑢𝑎𝑛𝑡𝑖𝑡𝑦 𝑖𝑛 𝑦𝑒𝑞𝑢𝑖𝑣𝑎𝑙𝑒𝑛𝑡 𝑞𝑢𝑎𝑛𝑖𝑡𝑦 𝑖𝑛 𝑢𝑛𝑖𝑡 𝑥 =𝐴𝑛𝑔𝑙𝑒 𝑖𝑛 𝑢𝑛𝑖𝑡 𝑦
MACRO H2 Physics Topic 6: Motion in a Circle Notes 4 ©MACRO Learning Physics All Rights Reserved under 9836 3500 Copyright Act (Cap. 63) of Singapore Angular Velocity, 𝝎 Angular velocity, 𝝎 is the rate of change of angular displacement. This equation represents the instantaneous angular velocity. If the object has a constant angular velocity, the instantaneous value and the average value will be the same. Angular Velocity, 𝝎, in terms of period T Period(T), is the time it takes for an object in circular motion to make one complete revolution, or cycle. Frequency (f) is the number of revolutions, or cycles, made per unit time. The unit of frequency is 𝑠%&, also known as the hertz(Hz). Given the definition: Angular velocity, 𝝎 is the rate of change of angular displacement, for uniform circular motion, the particle in motion has the same tangential speed throughout the motion. Hence, angular velocity is a constant and the time taken for 1 revolution also known as period T can be expressed as: 𝜔=𝑑𝜃𝑑𝑡 𝜔=𝑑𝜃𝑑𝑡=2𝜋𝑇=2𝜋𝑓
MACRO H2 Physics Topic 6: Motion in a Circle Notes 5 ©MACRO Learning Physics All Rights Reserved under 9836 3500 Copyright Act (Cap. 63) of Singapore Relationship between Angular Velocity and Tangential(Linear) Speed A particle moving in a circle has an instantaneous velocity tangential to its circular path. For a constant angular speed, the particle’s orbital or tangential speed v is also constant. At any instant, it is directed tangentially to the circular path at the specific point. From 𝜔='(')='"#') , since radius r is a constant, hence we can get 𝜔=&#('*')), and since speed is the rate of change of distance, we can finally get 𝑣=𝑟𝜔. Uniform Circular Motion In uniform circular motion, although speed is constant, why would there be centripetal acceleration? Ø Although the magnitude of velocity in the circular motion remains constant, its direction changes. Since velocity is a vector quantity, hence there will be changing velocity and a value for acceleration will be present. Ø In addition, by Newton’s Second Law, there must be a resultant force in the direction of acceleration, which is also in the direction of the change in velocity. (Recall: acceleration is the rate of change of velocity) This direction is towards the centre of the circle.
MACRO H2 Physics Topic 6: Motion in a Circle Notes 6 ©MACRO Learning Physics All Rights Reserved under 9836 3500 Copyright Act (Cap. 63) of Singapore Derivation of Centripetal Force and Centripetal Acceleration We need to consider the change in velocity of an object before we derive an equation for acceleration. Hence, from the diagram below we can tell that the change in velocity is given by 𝑣!−𝑣&. ∆𝑣≈𝑣×∆𝜃 ∆𝑣∆𝑡≈𝑣×∆𝜃∆𝑡 𝑎=𝑣×∆𝜃∆𝑡 𝑎=𝑣𝜔=𝑟𝜔!=𝑣!𝑟 𝐹+=𝑚𝑣!𝑟=𝑚𝑟𝜔!
MACRO H2 Physics Topic 6: Motion in a Circle Notes 7 ©MACRO Learning Physics All Rights Reserved under 9836 3500 Copyright Act (Cap. 63) of Singapore Dynamics of uniform circular motion Let’s take a look at common examples of exam questions that ask us to describe why a force towards the centre of the circular motion needs to be present in order for uniform circular motion to take place. Why must the object experience a force that is directed towards the centre of the circle, perpendicular to the motion of the object? Ø Recap Newton’s First Law: In accordance to Newton’s First Law, the object will continue to move in uniform speed in the same direction unless there is a net force acting on it. For a net force to modify the magnitude of velocity, it needs to have a component along the velocity. Hence, if the net force is to only change the direction of velocity and allow the object to remain in uniform motion, it needs to be perpendicular to the velocity. Ø By Newton’s Second Law, there must be a corresponding resultant force acting along the same direction as the change in momentum, which is the same direction as the change in velocity. The equation for centripetal force must be understood as a way to calculate centripetal force needed for uniform circular motion for a mass m moving with speed v in a circle of radius r. ***For an object to move in a circular path, a
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