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Circular Motion.

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Presentation on theme: "Circular Motion."β€” Presentation transcript:

1 Circular Motion

2 Uniform Circular Motion
Uniform Circular Motion – Traveling with a constant speed in a circular path Even though the speed is constant, the acceleration is non-zero The acceleration responsible for uniform circular motion is called centripetal acceleration We can calculate π‘Ž 𝑐 by relating Ξ” 𝑣 to Δ𝑑

3 𝑣 π‘Ÿ

4 𝑣 = ? π‘Ÿ 𝑓 Ξ”πœƒ π‘Ÿ 0

5 Ξ” 𝑣 𝑣 𝑓 𝑣 0 π‘Ÿ 𝑓 𝑣 0 Ξ”πœƒ π‘Ÿ 0

6 Centripetal Acceleration
When an object travels with uniform circular motion, the acceleration always points towards the center of the circular path with: π‘Ž 𝑐 = 𝑣 2 π‘Ÿ

7 Period, Frequency, & Angular Frequency
Period (𝑇)– The time it takes to complete one full rotation Frequency (𝑓)– Rotations per second (or per minute) Angular Frequency (πœ”) – Radians per second

8 Period, Frequency, & Angular Frequency
Period and frequency are related by: 𝑓= 1 𝑇 There are 2πœ‹ radians in one rotation, therefore: πœ”=2πœ‹ 𝑓

9 Angular Frequency Equations
If an object rotates through an angle πœƒ with a radius π‘Ÿ, how far does the object travel? Ξ”s πœƒ

10 Angular Frequency Equations
In general: Ξ”s=r πœƒ and 𝑣=π‘Ÿ πœ”

11 Angular Frequency Equations
Combining π‘Ž 𝑐 = 𝑣 2 π‘Ÿ and 𝑣=π‘Ÿ πœ” gives: π‘Ž 𝑐 =π‘Ÿ πœ” 2

12 Centripetal Acceleration - Example
A centrifuge creates a centripetal acceleration of π‘š 𝑠 2 . The average radius of the arm of the centrifuge is π‘Ÿ=5 π‘π‘š. How fast does the centrifuge spin in revolutions per second?

13 π‘Ž 𝑐 =61250 π‘š 𝑠 𝑣= ? π‘Ÿ=0.05 π‘š 𝑓= ?

14 Centripetal Acceleration - Example
A car drives around a level turn. The tires have a coefficient of friction of πœ‡ 𝑠 =0.8, and the turn has a radius of 90 π‘š. How fast can the car go around the turn without sliding?

15 𝑣 = ? π‘Ÿ

16 Centripetal Acceleration - Example
A car drives around an banked turn with a radius of 90 π‘š. The turn is designed so that a car traveling 10 π‘š/𝑠 will be able go around the turn even when the coefficient of friction is reduced to πœ‡ 𝑠 =0. What angle is the turn banked at?

17 𝑣 = ? π‘Ÿ πœƒ

18 Circular Motion with Gravity
The centripetal force is any force that holds an object in circular motion. That is, any force that points inwards towards the center of a circular path. As an object goes around a loop, the forces that make up the centripetal force change.

19 Circular Motion with Gravity

20 Circular Motion with Gravity
How fast does a rollercoaster need to be traveling when it goes through a vertical loop with a radius of 4.0 π‘š ?

21 π‘Ÿ=4.0 π‘š

22 Newton’s Law of Universal Gravity
Every particle exerts an attractive force all other particles The force is given by: 𝐹 𝐺 = 𝐺 π‘š 1 π‘š 2 π‘Ÿ 2 𝐺 is the universal gravitational constant: 𝐺= βˆ’11 𝑁 π‘š 2 π‘˜ 𝑔 2

23 Newton’s Law of Universal Gravity
𝐹 𝐺 = 𝐺 π‘š 1 π‘š 2 π‘Ÿ 2 Note that π‘Ÿ, is the distance between the centers of the two masses Therefore, when standing on the surface of the Earth: π‘Ÿ= 𝑅 𝐸 +β„Ž β‰ˆ 𝑅 𝐸

24 Using Newton’s Law of Universal Gravity, we can show that 𝑔=9
𝑀 𝐸 = kg 𝑅 𝐸 = π‘š Using this formula, we can calculate the acceleration due to gravity on planets other than Earth.

25 Universal Gravity - Example
Another planet is discovered. The new planet has a radius half the radius of the Earth, R p =0.5 𝑅 𝐸 , and one-tenth the mass of Earth 𝑀 𝑝 =0.1 𝑀 𝐸 . What is the acceleration due to gravity on this planet?

26 𝑅 𝑝 =0.5 𝑅 𝐸 𝑀 𝑝 =0.1 𝑀 𝐸 𝑔 𝑝 =?

27 Orbit Any force can supply the centripetal force required to keep an object in uniform circular motion. When a satellite obits the Earth, the centripetal force is supplied by the gravitational force. 𝐹 𝑔

28 Universal Gravity - Example
How fast is the satellite moving when it is placed in a circular orbit around the Earth with a radius of π‘š? The Earth has a mass of π‘˜π‘”.

29 π‘Ÿ= π‘š 𝑀 𝐸 = π‘˜π‘” 𝐺= βˆ’11 𝑁 π‘š 2 π‘˜ 𝑔 𝑣= ?

30 Kepler’s Third Law of Planetary Motion
Kepler’s Third Law relates the period 𝑇 to the radius of the orbit 𝑅

31 Kepler’s Third Law of Planetary Motion
Kepler’s Third Law of Planetary Motion Says: 𝑇 2 𝑅 3 =π‘π‘œπ‘›π‘ π‘‘.

32 Kepler’s Third Law - Example
An asteroid orbits the Sun with a radius that is exactly twice the radius of the Earth’s orbit around the Sun. How long does it take this asteroid to orbit the Sun?

33 Kepler’s Third Law - Example
𝑇 𝐸 =1 π‘¦π‘’π‘Žπ‘Ÿ 𝑅 𝐴 =2 𝑅 𝐸 𝑇 𝐴 = ?


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