Physics!
Monday, January 31, 2011
Blog 9: Dryer Sheets
In class we were talked about how sometimes when your clothes come out of the dryer they cling to you or each other because of static electricity. Static electricity is more common in dry places with low humidity like dyers becase objects can keep their charge imbalaces longer. When we were talking about this, I wondered why my clothes are never usually never clingy and I figured it was just because Hawaii is pretty humid but this weekend I found out that my mom uses dryer sheets when she does laundry. I guess the fact that I didnt know what dryer sheets even were before this shows how rarely I do my own laundry... Usually in dryers, clothes become charged because the different materials of the the different clothes have different affinities for electron so they transfer electrons as the rub against each other (charging by friction). Dryer sheets are useful because not only are they the explanation for why my clothes are always magically soft and smell delightful after my mom washes them, they also reduce static cling by lubricating all the clothes with the same chemical so that all the clothes have the same affinity for electrons and none of them will become charged. They will be even more useful next in college on the mainland because of the drier environment. Yay for dryer sheets! For all the people in my class who didnt know what dryer sheets were, GET SOME AND USE THEM, they make your clothes so soft its so wonderful!!!!! I know it looks a little weird and gross in the picture, but seriously they are great.
Monday, January 10, 2011
Blog 8: Center of Mass & Torque
This is a picture I took this summer of a catherdral in Spain which is still under construction even though it's super old. The carthedral is pretty amazing but it was pretty irritating that there was so much construction equiptment and noise from power tools etc. Beyond that I never really gave much thought to all the cranes around the cathedral. At first glace, it seems amazing that the cranes can balance even though they have one really long end sticking out that is obviously not over the support base. If the horizontal part of the crane was uniform then the weight of it would create a torque(force x lever arm) in the middle of its arm, and it would tip over because of unblanced torques. However, when you look at this picture, you can see that the short end of the crane's arm has a lot of weight on the end of it. This makes it so the center of mass is closer to the right side and the center of mass is therefore over the support base. Now the crane wont tip over!
Monday, December 13, 2010
Blog 7: Circular Motion
Sunday night, 11:49pm. I'm sitting at home, studying my physics notes as I do every night, when I suddenly realize we have a blog due. Panic mode commence. I frantically search my humble abode for signs of circular motion. None to be found. I curl up I my bed, about ready to accept defeat, when suddenly a bikini hits me in the face. I stare up angrily at my fan where I had hung my bikini earily today so it could dry. So there I am, looking at the rotating fan blades, when I suddenly realize I am staring straight into the eyes of circular motion. I said a quick prayer to the physics gods for blessing me with the perfect example of cirular motion despite my procrastination as I took this video of my fan. In this video I turned the speed of my fan up so that the other bikinis I was drying on my fan flew off as well. Because it is on a high speed, it has higher centripetal accleration than it did when it was roatating slower because centripetal accleration = velocity squared / radius. The radius of the fan is constant during every speed so as the velocity increase or decreases, so does the centripetal acceleration. The centripetal force that was keeping the bikinis on the fan blades was friction. Centripetal force is equal to (mass)(centripetal acceleration). As the velocity increased, so did centripetal accleration untill mac was greater than the centripetal force which was keeping the bikinis in circular motion. The bikinis flew off in a path the was tangent to the circle. Thanks to physics I know to keep my fan on a low speed so that I dont get hit with things flying off my fan when their centriptal acceleration becomes too great.
Sunday, November 28, 2010
Blog 6: Collisions
This weekend my friends and I decided to have a friendly volleyball tournament. I was super excited because even though I'm horrible at volleyball, I knew I'd see a lot of examples of momentum and collisions that I could blog about! In this picture you can see the Bret (left) has hit the ball toward Sean (in the red) who is trying to block it. The volleyball's momentum is equal to its mass times its velocity. After Bret hit it, the ball then collided with Sean's hands and bounced back towards Bret. A bouncy collision! The collision created an impulse which is equal to change in momtum or force times mass. The ball experienced a large change in momentum so it its impulse must have been pretty big. Because the time that the ball was in contact with Sean's hands was extremely short, that must mean the the force was very large (J=F t ) . Ouch, his hands must've hurt after this from all the force...
Monday, November 8, 2010
Blog 4: Energy, Work and Power
Once we climbed up to the platform, we ziplined down. We could calculate the speed at which we ziplined down by using the conservation on total energy. Because out kinetic energy on the platform = 0 and out potential energy at the end of the zipline = 0, our potential energy (mgh) at the platform would equal our kinetic energy (1/2mv^2) at the bottom. Solving for v would tell us how fast we were going.
Monday, October 4, 2010
Blog 3: Defying Newton's Laws
Today my mom asked me to burn her a CD of all the pictures I took on our trip this past summer. While I was doing this, I came across this picture I took of a man I saw on a street in Barcelona who was floating in mid air! At the time I was flabbergasted and wondered how it was physcially possible. However, I have learned a lot since then and when I saw this today I thought, "Physics must have an answer!" I turned to Newton and his trusty laws to explain it.
Newton's first law of motion states that an object at rest stays at rest and an object in motion continues moving at a constant velocity unless acted upon by a net external force. If this is true, the man should accelerate downards because the force of gravity is acting on him. However, he just floated there, motionless.
Newton's second law states that Accleration = Net Force / Mass. Because the acceleration of the man is zero, that must mean that the net force also is equal to zero. In order for net force to be zero, there must be another force acting on the man that is equal in magnitude but opposite in direction of gravity to make Fnet = 0. So I guess he is pushing up on his stick with a force of 9.8 N? But it still seems impossible. Maybe gravity just doesn't affect him. I wish Newton was here to see this...
Monday, September 20, 2010
Blog 2: Projectiles
One one the sections on the back of the cereal box asked "Do you have enough projectile pop to push your Penguin over the top of the box?" Being a good physics student, I took the challenge and decided to see if I could launch my penguin over the box. It took me a couple tries but I finally got the pengin to go oever the box. The trick is to launch it really hard so it has an initial vertical velocity great enough to reach a height greater than the cereal box. If I timed the amount of time it was in the air and how high the penguin went, I could calculate its inital vertical velocity using the equation y = (initial velocity)(time)+ 1/2 (vertical acceleration)(time squared).
Notice the parabolic shape of the projectile motion!
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