Open Query 14

course phys 202

014. `Query 12

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Question: `qquery doppler shift experiment (experiment was to be read and viewed only) **** explain why the frequency

of the sound observed when the buzzer moves toward you is greater than that of the stationary buzzer and why this

frequency is greater than that observed when the buzzer is moving away from you

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Your solution:

When the buzzer moves towards the observer the frequency of the emitted sound is being added to make the observed

frequency seem higher. This is because sound is being emitted by the buzzer but because it is moving closer the sound

emitted after it has travelled a little while is adding to the original emitted sound that has also been travelling towards the

observer. These frequencies add together to make the overall observed frequency seem higher that the emitted frequency

of the stationary buzzer. When the object is moving away from the observer the opposite effect is observed. The initial

emitted frequency reaches the observer faster than the emitted frequency as the buzzer moves further away causing the

overall frequency to sound lower by subtracting from the initial frequency.

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Given Solution:

`a** The 'pulses' emitted by an approaching source in a certain time interval are all received in a shorter time interval,

since the last 'pulse' is emitted closer to the source than the first and therefore arrives sooner than if the source was still.

So the frequency is higher.

If the source is moving away then the last 'pulse' is emitted further from the source than if the source was still, hence

arrives later, so the pulses are spread out over a longer time interval and the frequency is lower.

GOOD EXPLANATION FROM STUDENT:

Well, for the purposes of this explanation, I am going to explain the movement of the buzzer in one dimention which will

be towards and away. The buzzer is actually moving in a circle which means it exists in three dimentions but is moving in

two dimentions with relation to the listener. However, using trigonometry we can determine that at almost all times the

buzzer is moving either towards or away from the listener so I will explain this in terms of one dimention.

}When a buzzer is 'buzzing' it is emitting sound waves at a certain frequency. This frequency appears to change when the

buzzer moves toward or away from the listener but the actual frequency never changes from the original frequency. By

frequency we mean that a certain number of sound waves are emitted in a given time interval (usually x number of cycles

in a second). So since each of the waves travel at the same velocity they will arrive at a certain vantage point at the same

frequency that they are emitted. So If a 'listener' were at this given vantage point 'listening', then the listener would

percieve the frequency to be what it actually is. Now, if the buzzer were moving toward the listener then the actual

frequency being emitted by the buzzer would remain the same. However, the frequency percieved by the listener would

be higher than the actual frequency. This is because, at rest or when the buzzer is not moving, all of the waves that are

emitted are traveling at the same velocity and are emitted from the same location so they all travel the same distance. But,

when the buzzer is moving toward the listener, the waves are still emitted at the same frequency, and the waves still travel

at the same velocity, but the buzzer is moving toward the listener, so when a wave is emitted the buzzer closes the

distance between it and the listener a little bit and there fore the next wave emitted travels less distance than the previous

wave. So the end result is that each wave takes less time to reach the listener than the previously emitted wave. This

means that more waves will reach the listener in a given time interval than when the buzzer was at rest even though the

waves are still being emitted at the same rate. This is why the frequency is percieved to be higher when the buzzer is

moving toward the listener.

By the same token, if the same buzzer were moving away from the listener then the actual frequency of the waves emitted

from the buzzer would be the same as if it were at rest, but the frequency percieved by the listener will be lower than the

actual frequency. This is because, again at rest the actual frequency will be the percieved frequency. But when the buzzer

is moving away from the listener, the actual frequency stays the same, the velocity of the waves stays the same, but

because the buzzer moves away from the listener a little bit more each time it emits a wave, the distance that each wave

must travel is a little bit more than the previously emitted wave. So therefore, less waves will pass by the listener in a given

time interval than if the buzzer were not moving. This will result in a lower percieved frequency than the actual frequency.

**

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Self-critique (if necessary): OK

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Self-critique Rating: OK

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Question: `qquery General College Physics and Principles of Physics: what is a decibel?

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Your solution: A decibel is a measure of the level of intensity of a sound. It is equal to 10 log (I/I0) which is the Intensity

observed over the lowest audible intensity.

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Given Solution:

`a** dB = 10 log( I / I0 ), where I is the intensity of the sound in units of power per unit area and I0 is the 'hearing

threshold' intensity.

MORE EXTENSIVE EXPLANATION FROM STUDENT:

Sound is possible because we exist in a medium of air. When a sound is emitted, a concussive force displaces the air

around it and some amount energy is transferred into kinetic energy as air particles are smacked away from the force.

These particles are now moving away from the initial force and collide into other air particles and send them moving and

ultimately through a series of collisions the kinetic energy is traveling out in all directions and the air particles are what is

carrying it. The behavior of this kinetic energy is to travel in waves. These waves each carry some amount of kinetic

energy and the amount of energy that they carry is the intensity of the waves. Intensities of waves are given as a unit of

power which is watts per square meter. Or since the waves travel in all directions they move in three dimentions and this

unit measures how many watts of energy hits a square meter of the surface which is measuring the intensity. But we as

humans don't percieve the intensities of sound as they really are. For example, a human ear would percieve sound B to be

twice as loud as sound A when sound B is actually 10 times as loud as sound A. Or a sound that is ...

1.0 * 10^-10 W/m^2 is actually 10 times louder than a sound that is

1.0 * 10^-11 W/m^2 but the human ear would percieve it to only be twice as loud.

The decibel is a unit of intensity for sound that measures the intensity in terms of how it is percieved to the human ear.

Alexander Graham Bell invented the decibel. Bell originally invented the bel which is also a unit of intensity for waves. The

decibel is one tenth of a bel and is more commonly used. The formula for determing the intensity in decibels is ...

Intensity in decibles = the logarithm to the base 10 of the sound's intensity/ I base 0

I base 0 is the intensity of some reference level and is usually taken as the minimum intensity audible to an average person

which is also called the 'threshold of hearing'.

Since the threshold of hearing is in the denominator, if a sound is this low or lower the resulting intensity will be 0 decibles

or inaudible. **

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Self-critique (if necessary): OK

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Self-critique Rating: OK

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Question: `qgen phy what is the difference between the node-antinode structure of the harmonics a standing wave in a

string and in an organ pipe closed at one end

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Your solution:

A string has nodes at both ends, with antinodes in between each node. For example a fundamental frequency would have

a node on each end with 1 antinode in the middle, the first overtone would have a node, antinode, node, antinode, and

node. This pattern would continue for each subsequent overtone. A closed organ pipe has a node at the closed end and

an antinode at the open end. The fundamental would be node antinode, while the first overtone would be node antinode

node antinode.

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Given Solution:

`a** in a string there are nodes at both ends so the harmonics are described the the configurations NAN, NANAN,

NANANAN, etc.. In a pipe closed at one end there is a node at one end and an antinode at the other so the possible

configurations are NA, NANA, NANANA, etc..

displacement nodes are at both ends of the string, so the structure is N &&& N, where &&& is any sequence of nodes

and antinodes that results in an alternating sequence.

The possibilities are NAN, NANAN, NANANAN, ... , containing 1, 2, 3, 4, ..., half-wavelengths in the length of the

string. Possible wavelengths are therefore 2 L, 1 L, 2/3 L, ..., where L is string length.

For an open organ pipe the configuration must be N &&& A. Possibilities include NA, NANA, NANANA,

NANANANA, ..., containing 1, 3, 5, 7, ..., quarter-wavelengths. Possible wavelengths are therefore 4 L, 4/3 L, 4/5 L,

4/7 L, ... **

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Self-critique (if necessary): OK

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Self-critique Rating: OK

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Question: `q **** gen phy what are beats?

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Your solution:

Beats occur when two sources emit sounds close in frequency whose waves interfere with each other. Sometimes the

waves are in phase and sometimes they are out of phase. This produces intensity changes that are regularly spaced apart.

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Given Solution:

`a** Beats are what happens when the two sounds are close in frequency. Beats occur when the combined sound gets

louder then quieter then louder etc. with a frequency equal to the differences of the frequencies of the two sounds. **

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Self-critique (if necessary): OK

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Self-critique Rating: OK

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Question: `q **** query univ phy 16.54 (20.32 10th edition) steel rod 1.5 m why hold only at middle to get fund? freq

of fund? freq of 1st overtone and where held? **** why can the rod be held only at middle to get the fundamental?

"

&#Good work. Let me know if you have questions. &#