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53 Cards in this Set
- Front
- Back
Sound waves are_____ waves which cycle through _____ and ______ |
Longitudinal Compression Decompression |
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angular frequency |
2pi/T |
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Circle velocity |
V=(angular frequency)(radius of circle) Or V= 2(pi)(R)/t |
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General audible hearing for adults |
20-20,000 Hz |
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Speed of sound |
v= root(B/p) B is bulk modulus. Mediums resistance to compression P medium density So Speed is fastest in a solid with low density and slowest in high density gas |
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Frequency is known as |
Pitch |
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Doppler effect and equation |
If source and detector move towards one another then frequency sounds higher and vice versa fprime = (f)(v +_vd)/(v-+vs) Top part is plus over minus and botton is minus over plus. F prime is perceived freq F is actual frequency Vd on top is speed of detector Vs is speed of source SO top sign is used when that thing is moving towards and bottom moving away. So if both are moving towards then top will be plus and bottom will be minus
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Sonic boom |
Always can hear sounds. Waves mitigate behind cuz they destructively interfere with one another |
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Loudness vs intensity |
Loudness subjective Intensity objectively measurable |
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Intensity |
Power transported per unit area I= P/A |
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Standing waves |
Waves that interfere with each other and the wave appears to be standing still. Nodes are places of no displacement Antinodes are the maximum displacement (tip of waves) |
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Standing waves |
Waves that interfere with each other and the wave appears to be standing still. Nodes are places of no displacement Antinodes are the maximum displacement (tip of waves) |
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Closed boundary vs open |
Closed is a object with standing waves with boundaries at both ends (string) Open only a boundary at one end (open pipe) |
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open pipe and string standing wave wavelength and frequency |
WL = 2L/n f = nv/2L L length of string. V is wave speed n is amount of antinodes on a string (count wave peaks) And amount of nodes for open pipe |
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Closed pipe f and WL |
Open in one end only WL = 4L/n f = nv/4L n is number of quarter wavelength and is equal to 1,3, and 5 etc for each quarter |
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Closed pipe f and WL |
Open in one end only WL = 4L/n f = nv/4L n is number of quarter wavelength and is equal to 1,3, and 5 etc for each quarter |
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Doppler ultrasound |
Ultrasound bounces sound waves through and back through body Doppler determines blood flow by detecting frequency shift of stuff moving toward or away |
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Spherical mirror: concave Convex Lens: Concave Convex Name diverging or converging |
Mirrors; concave, converging convex, diverging Lens: concave, diverging convex, converging |
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Forebrain is called the ______encephalon and divides to form_____ and _______ |
Pros Diencephalon (thalamus, hypothalamus, posterior pituitary, pineal gland) Telencephalon( forms cerebral cortex, basal ganglia, limbic) |
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Pet scan |
Position emission tomography Inject radioactive sugar to view target tissue |
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Equation for mirrors and lenses |
1/f= 1/o +1/i = 2/r f focal length o object length i image length r radius of curvature; distance between mirror and center of curvature if curved mirror was one big circle |
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For all mirrors. Positive i (image distance) means image is_____ and _____. Negative i is _______ and ______ |
In front of mirror Real Behind mirror Virtual |
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Magnification equation for mirrors and lenses. Explain key points |
M = -(i/o) Dimensionless ratio of image to object so greater than one image bigger and so on. Negative m is inverted image and positive is upright image |
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What are the two rays for a concave mirror ray diagram. What do they result in if o > f o=f and o |
One ray travels through F and reflects parallel, one travels parallel and reflects back through F o>f Image will be larger, real, and inverted o=f the rays will be parallel and image is at infinity o |
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Ray diagram and info for convex mirror |
Rays look complicated so memorize that image is always a virtual, upright, smaller image (think gas station mirrors) Farther away you get the smaller the image Focal point is on opposite side |
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Where are C and F with regard to concave and convex mirrors. What is the +- of r and f? |
concave they are in same side and r and f are pos Convex they are on opposite side so r and f are negative |
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Index of refraction equation |
n=c/v |
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Index of refraction equation |
n=c/v |
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Critical angle eqn |
For total internal reflection theta(c)=sin^-1(n2/n1) this is the angle when angle 2 is 90 degrees. It needs to be a large enough angle. And. It needs to be going from larger n to smaller n |
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Lens maker equation |
1/f = (n-1)(1/r1-1/r2) This is used for lenses where thickness can’t be neglected n is index of refraction of lens material. r1 and 2 are radius of curvature for first and second lens surface |
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Rays for lens ray diagram Concave and convex |
for convex. Parallel ray runs through F on other side, ray running through F leaves parallel Concave, parallel passes through on a line that when traced backwards would go through F. And ray traveling to opposite F leaves parallel. |
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Rays for lens ray diagram Concave and convex |
for convex. Parallel ray runs through F on other side, ray running through F leaves parallel Concave, parallel passes through on a line that when traced backwards would go through F. And ray traveling to opposite F leaves parallel. |
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Differences and different sign conventions of lenses |
Lenses real side is opposite virtual side is same. pos i is still real and neg i is still virtual. for r and f, just remember that diverging is negative and converging is positive just like mirrors. |
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Lens power |
P=1/f measured in diopters |
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Lens power |
P=1/f measured in diopters |
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What are the two types of vision problems. What types of lenses do they need to correct them? |
Hyperopia, farsighted (can see distant objects clearly), needs converging lenses myopia, nearsighted (can see close objects clearly) needs diverging lenses |
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Lens power |
P=1/f measured in diopters |
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What are the two types of vision problems. What types of lenses do they need to correct them? |
Hyperopia, farsighted (can see distant objects clearly), needs converging lenses myopia, nearsighted (can see close objects clearly) needs diverging lenses |
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Multiple lenses equation for lens in contact |
Behave as a single lens with f 1/f = 1/f1 ...... And P= P1...... |
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Lens power |
P=1/f measured in diopters |
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What are the two types of vision problems. What types of lenses do they need to correct them? |
Hyperopia, farsighted (can see distant objects clearly), needs converging lenses myopia, nearsighted (can see close objects clearly) needs diverging lenses |
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Multiple lenses equation for lens in contact |
Behave as a single lens with f 1/f = 1/f1 ...... And P= P1...... |
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Lens not in contact (telescopes) |
m=(m1)(m2)..... |
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Spherical aberration |
Blurring of image periphery due to inadequate refraction from imperfect lenses and mirrors |
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Spherical aberration |
Blurring of image periphery due to inadequate refraction from imperfect lenses and mirrors |
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Dispersion |
Different light WL travels different speeds in different mediums. Red always on top cuz it experiences least refraction |
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Single slit diffraction equation |
a sin theta= n(lambda) a is slit width, angle is angle between center of lens and selected dark fringe n is number of fringe and bright fringes halfway between dark ones. Lambda WL of incident wave |
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Double slit dark fringe positions |
d sintheta = (n + 1/2)lambda d distance between the slits n is dark fringe number |
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Photoelectric effect |
High frequency light causes metal to eject electrons |
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Photoelectric effect |
High frequency light causes metal to eject electrons |
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Threshold frequency in photoelectric effext |
Minimum freq of light necessary to cause effect (fT) |
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Maximum KE of ejected electrons in photoelectric effect equation |
Kmax= hf-W f is freq of actual light and W is work function (hfT) minumum energy required to eject electrons |
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Fluorescence |
Flourescent substances are things that will light up when exposed to UV |