1.29.2012

[The Tenth Blog] Electrostatic.

Today I went to a first birthday party for my mother's co-worker's daughter. Her name is Leura (after the city in Australia) and she's really cute. :] But anyway, since it was a birthday party, there were lots of balloons, which of course reminded me of...physics!
Objects can become charged by friction if they are rubbed together. I would not have done this at the party (sorry, not even for physics) because I would have looked ridiculous as well as made my hair all frizzy and such, so I'll just speak theoretically. If I had rubbed the balloon against my hair, both my hair and a balloon would have become charged. Since the rubber balloon has a greater electron affinity (Yay for chemistry. :P) than hair, it would pull electrons away from my hair (It is always the electrons that move! :]), making the balloon negatively charged and my hair positively charged.  Also, since charge is conserved, the net charge would be constant throughout the process. The balloon and my hair were both neutral at the beginning, and since electrons are simply transferred to make one object positive and the other negative, the total number of electrons and protons remains the same (equal), so the net charge is still zero. Now that we have created two objects of opposite charge, guess what? They'll attract! Because opposites don't only attract in real life; opposites attract in physics too. :] We would actually be able to calculate the electrostatic force that my hair would exert on the balloon using the equation 
F = kQ1Q2 /rwhere k is equal to 8.99 x 109 N • m2/C2, Q1 and Q2 are the charges of my hair and the balloon, and r is the distance between them. I actually recall doing this as an experiment back in elementary school, but only now do I actually know the physics behind it (after, like, six years... Haha.)

1.16.2012

[The Ninth Blog] Thermodynamics.

Since finals ended, I haven’t really thought about school. At all. Even though it’s only been, like, five days since we’ve been in physics class, I’ve basically forgotten everything. Well, not everything, but quite a bit. I’m forgetful, what can I say? :] 

I baked some pumpkin muffins this weekend. For Christmas, one of our neighbors gave us a jar of pumpkin bread/muffin mix with raisins in it that I finally decided to use on Saturday. They actually turned out to be pretty good. And the process involved physics, so all the better, right?

From the very beginning, physics was at play: when I set the oven to 350°, heat was added to the system in order to bring it up to temperature. Such a process is isochoric, as the volume of the oven cannot be changed. According to the ideal gas law PV = nRT, as temperature rose, so too did pressure. Also occurring due to the added heat was an increase in the system’s entropy.


Once the oven had reached 350°, it was time to put in the muffins. Since heat readily flows from hot to cold, heat was transferred from the surrounding air to the muffins, causing them to undergo a temperature and phase change. At this point, the muffins were taking part in an isobaric process. As the temperature of the muffins increased, it caused them to rise as they baked, with temperature and volume varying but pressure constant. Once the muffins were brought up to the same temperature as the oven, they finished baking in an isothermal process. [I think...] The muffins dropped slightly in height (volume decreased) as they continued to cook, since pressure was increasing as the batter became more dense, completing its change from a liquid-like substance to a solid, and temperature was being held constant.

And voila! The result: delicious pumpkin-raisin muffins and a nice lesson in physics. :]

 

[What Was Supposed To Be...The Eighth Blog] Sound.

Wow, it’s been a while... So here’s the response on sound from December that I just never got around to posting:
Values/Calculations
Instrument
Violin
Properties
Chosen string: D
- Frequency: 294 Hz
- Vibrating length: 0.32 m
- Mass density: 9.375 x 10-4 kg/m [mass = 0.30 g]
- Tension: 33.191 N
      



Frequencies Of Next Highest Harmonics
- Second harmonic: 588.00 Hz
- Third harmonic: 882.00 Hz
    

Analysis
Fingering Positions
The fingering positions correspond to where the frequencies for the next notes can be found.  When you press the string down with your finger, it decreases the vibrating length of the string.  This shorter length results in a higher frequency.  When placed in the correct position, the new frequency is that of a new note.  For example, in first position, placing your first finger on the D-string gives the note E while your second finger can give either the For F#, depending on where it is placed.

To play an E on the D-string, the vibrating length is reduced by about 0.03 m, making the new length 0.29 m.  So when the new frequency is calculated, it comes out to 324.412 Hz (which is fairly close to the established 329.63 Hz...).



Plucking/Bowing Location
The plucking/bowing location is close to the bottom (by the bridge) node of the string.  At this location...all (or most of...many of...) the harmonics are likely to be heard! :]

Plucking Versus Bowing
When a string is plucked, energy is only applied for an instant so the sound diminishes quickly.  When it is bowed, energy is constantly applied so the note can be heard for a longer period.  After the initial sound of a plucked note is heard (with all of its frequencies), some of the higher frequencies are lost so only lower and fundamental frequencies can be heard until the sound is stopped altogether.  However, when a note is bowed, all frequencies are being heard together continuously, giving it greater depth.