Sections | |||
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Intro to Moment of Inertia | 30 mins | 0 completed | Learn |

Moment of Inertia via Integration | 19 mins | 0 completed | Learn |

More Conservation of Energy Problems | 55 mins | 0 completed | Learn |

Moment of Inertia of Systems | 23 mins | 0 completed | Learn |

Conservation of Energy in Rolling Motion | 45 mins | 0 completed | Learn |

Moment of Inertia & Mass Distribution | 10 mins | 0 completed | Learn |

Intro to Rotational Kinetic Energy | 17 mins | 0 completed | Learn |

Energy of Rolling Motion | 18 mins | 0 completed | Learn |

Types of Motion & Energy | 24 mins | 0 completed | Learn |

Parallel Axis Theorem | 14 mins | 0 completed | Learn |

Conservation of Energy with Rotation | 36 mins | 0 completed | Learn |

Torque with Kinematic Equations | 59 mins | 0 completed | Learn |

Rotational Dynamics with Two Motions | 51 mins | 0 completed | Learn |

Rotational Dynamics of Rolling Motion | 27 mins | 0 completed | Learn |

Concept #1: Intro to Rotational Kinetic Energy

**Transcript**

Hey guys! In this video, we're going to talk about rotational kinetic energy, which is the energy associated with the motion of spinning. Let's check it out. If you remember, if you had linear speed which is V, you had kinetic energy. There's going to be two types of kinetic energy so we're going to specify that this is linear kinetic energy. You're used to this equation KL = _ mv^2. I put a little L there to indicate this is the linear type of kinetic energy that's because now, we have a new one which is if you have rotational speed, instead of V, it's w or Omega. You have rotational kinetic energy and instead of KL, we call it KR. Now, the equation is very similar, it's half. Instead of using m, we're going to use the rotational equivalent of m which is I, moment of inertia and instead of V, we're going to use the rotational equivalent of V, which is w (omega) so I get this. So if you remember the first equation, it should be easy to remember the second one. On a special case, there's a special situation when you're moving and rotating so you have a V and a w. This is called rolling motion. One example of this is if you have a toilet paper roll that is sort of moving this way while rolling around itself. It's a toilet paper that's rolling on the floor. It has both kinds of motion, therefore it has both kinds of kinetic energy. IÕm going to say that the K total is KL plus KR. The last thing I wanna remind you, weÕll do a quick example is that for point masses, point masses are tiny objects that don't have a shape that have negligible size and radius. They have no volume. The moment of inertia, I, is mr^2 (squared) where r is a distance between the object and the axis. Remember also that if you have shape or a rigid body, an object with non-negligible radius and volume, we're going to get the moment of inertia from a table lookup. For example if you have a solid cylinder or a solid disk, same thing, the equation for that is _ mr2 (squared). Point mass is always this and some sort of shape will have a different equation each time. Let's do a very quick example here. I have a basketball player that spins a basketball around itself on top of his finger. I'm going to try to draw this, it's going to come out terrible. Here's a basketball player. Here's his finger, exaggerating some stuff and here's a basketball and he's rotating the basketball around itself so it looks kind of like this. The basketball is spinning around itself on top of your finger. It says here the ball has a mass of 0.62, a diameter of 24 centimeters so point 0.24 meters and it spins at 15 radians per second. Radians per second is angular velocity omega, 15. We want to know the ballÕs linear rotational and total kinetic energy. In other words, we want to know what is KL, what is KR and what is KTotal. First things first, you may already have caught this in physics. We never use diameter we always use radius, so when you see the diameter you immediately convert it to radius. Radius is half so it's 0.12. We're going to plug into the equation here. Kinetic energy is _ mv^2 (squared) and this ball has no kinetic energy, no linear kinetic energy I should say and that's because it spins in place. It's rotating but it's not actually moving. It has rotational motion but it doesn't have linear motion. It doesn't have translational motion. It just stays in place spinning around itself. We're going to say that it has no linear kinetic energy. It does have rotational kinetic energy because it's spinning around itself and that's given by _ Iw^2 (half I omega squared). A basketball has moments of inertia, the moment of inertia of a hollow sphere. I didn't give you the equation for that. I didn't explicitly say it was a hollow sphere but you should know that a basketball is a shell and then there's air inside, so it is a hollow sphere. I for a hollow sphere, you would look it up or it would be given to you, is 2/3 mr^2 (squared). What I'm going to do is I'm going to plug that in here, 2/3 mr^2 (squared) and then w2 (omega squared) which I have. Now we can just plug in numbers. The two cancels with the two and IÕm left with one-third. The mass is 0.62, the radius is 0.12^2 (squared) and w (omega), we have it right here 15, so 15^2 (squared). If you multiply all of this, I got it here. You get a 0.67 Joules. That's it. For the last part, we want to do the total kinetic energy. Remember the total kinetic energy is just an addition of the two types, kinetic linear plus kinetic rotational. There is no kinetic linear so the total kinetic energy is just the 0.67 that's coming from the rotational kinetic energy. That's how this stuff works. Hopefully this made sense. Let me know if have any questions and let's keep going.

Practice: A flywheel is a rotating disc used to store energy. What is the maximum energy you can store on a flywheel built as a solid disc with mass 8 x 10^{4} kg and diameter 5.0 m, if it can spin at a max of 120 RPM?

Example #1: Mass of re-designed flywheel

**Transcript**

Hey guys! Here we have a rotational kinetic energy problem of the proportional reasoning type and what that means, it's one of those questions where I ask you how changing one variable affects another variable. It's one of those. Let's check out. IÕm going to show you what I think is the easiest way to solve these.

It says you're tasked with redesigning a solid disk flywheel and you want to decrease the radius by half. First things first, solid disk means that the moment of inertia is 1/2 mr^2. That's the equation for a solid disk or solid cylinder. You want the new radius, IÕm going to call this R2 to be _ R1. I want to know by how much mass must the new flywheel have. It's the new mass relative to the original mass so that you can store the same amount of energy. You want the amount of energy that you stored to be the same. The amount of energy you stored is given by KR, that's energy stored which is given by _ Iw^2. This is energy stored as rotational kinetic energy in a flywheel. You want this number not to change. Yu want this number to be constants. How do you do this? If R changes, then I is going to change and if I changes, K is going to change and that's bad news. How do we change something else so that the K doesn't change? For the K not to change, you have to make sure that the I doesn't change. For the I not to change, you have to cancel out changing R with changing M. What I'm going to do here is I'm going to expand this equation, _, I is _ MR^2 w^2. Now I see all the variables that affect my K and again the K has to remain constant. If my radius is becoming half as large, it means that it is decreasing by a factor of 2. But the R is squared which means that when I reduce R by a factor of two, I also have to square this and R is becoming half as large but then the whole thing R^2 is becoming four times smaller. What that means is that if you want to keep everything constant, my mass has to grow by a factor of 4x. My new mass has to be four times my old mass and that's the answer. Again, R decreases by the factor of two but then you have to square because there's a square here. You get a four. If one variable decreases by four, the other one has to increase by four. Notice there are no squares in the M, so it's just a four not a two. Nothing crazy like that. That's it for this one let me know you have any questions.

Practice: When solid sphere 4 m in diameter spins around its central axis at 120 RPM, it has 10,000 J in kinetic energy. Calculate the sphere’s mass.

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Concept #1: Intro to Rotational Kinetic Energy

Practice #1: Max storing energy in flywheel

Example #1: Mass of re-designed flywheel

Practice #2: Mass of spinning sphere

A square, with a side length of 40 cm, has a 5 kg mass at each of its corners. If the square rotates about an axis through its center, perpendicular to the plane of the square, with an angular speed of 5 rad/s, how much kinetic energy does the square have?

A grinding wheel in the shape of a solid disk is 0.200 m in diameter and has a mass of 3.0 kg. The wheel is rotating at 2200 rpm about an axis through its center.
a) What is its kinetic energy?
b) How far would it have to drop in free fall to acquire the same amount of kinetic energy?

The L-shaped object shown in the figure below right consists of the masses connected by light rods. How much work must be done to accelerate the object from rest to an angular speed of 3.25 rad/s about the x-axis?
a) 62.3 J
b) 23.7 J
c) 17.6 J
d) 47.4 J
e) 34.2 J

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