I want important notes and equations in physics 1
Related topics:
chapter 6 :
topic:
1. description of uniform circular motion
2. radial acceleration
chapter 7:
topic:
1. unbanked and banked curves
2. angular acceleration
Chapter 6
1)Uniform circular motion can be described as the motion of an object in a circle at a constant speed. As an object moves in a circle, it is constantly changing its direction. At all instances, the object is moving tangent to the circle. Since the direction of the velocity vector is the same as the direction of the object's motion, the velocity vector is directed tangent to the circle as well. The animation at the right depicts this by means of a vector arrow.
An object moving in a circle is accelerating. Accelerating objects are objects which are changing their velocity - either the speed (i.e., magnitude of the velocity vector) or the direction. An object undergoing uniform circular motion is moving with a constant speed. Nonetheless, it is accelerating due to its change in direction. The direction of the acceleration is inwards. The animation at the right depicts this by means of a vector arrow.
The final motion characteristic for an object undergoing uniform circular motion is the net force. The net force acting upon such an object is directed towards the center of the circle. The net force is said to be an inward or centripetal force. Without such an inward force, an object would continue in a straight line, never deviating from its direction. Yet, with the inward net force directed perpendicular to the velocity vector, the object is always changing its direction and undergoing an inward acceleration.
2) Let's say an object is tied at A, one end of a string OA and rotated keeping the other end O as center. When the string is rotated fast, the string gets completely stressed out and the length of the string becomes the radius of rotation. It means a force is exerted on the object from the center to the end and there by an acceleration ao in a radial direction is faced by the object. To counter this force, a tension force develops in the string acting in the opposite direction. This tension force is called the centripetal force and the acceleration generated on the object is called the radial acceleration and denoted as ar.
a = v^2/R where v is the tangential velocity and R is the radius of the circle.
I want important notes and equations in physics 1 Related topics: chapter 6 : topic: 1....
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Physics 1 One of the main topics this week is circular, or centripetal, motion looking at its acceleration and associated force. For the centripetal force, is this a NEW force, explain? Often times, CENTRIFUGAL force is used in describing circular motion, is this an appropriate alternative to centripetal force, explain? One example of centripetal force is its application to curves - flat & banked - in terms of the maximum speed one can make the curve, what happens when the...
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2. The equations of motion for a system of reduced mass moving subject to a force derivable from a spherically symmetric potential U(r) are AF –102) = (2+0 + rē) = 0 . (3) Using the second of these equations, show that the angular momentum L r 8 is a constant of the motion (b) Then use the first of these equations to derive the equation for radial motion in the form dU L i=- What is the significance of...
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PHYS 141-Physies Kaul Lecture Supplement/Worksheet 6Intre Cireular Motion A 1. Define and provide an example of each of the qeantisies belorw and discess their differences. Alvo, draw a vector diagram for each example showing any change in velocity vectors, and showing the centripetal acceleration vector wr to your velocity vectors if i. son mo. b) c) 2. Circular Motion Quantities. Define each of the following quantities used in circular motion and state the base units used in each...