organ pipe

a sufficiently long organ pipe has a small hole at the bottom.initially the pipe is empty .water is poured into the pipe at the constant rate .the fundamental frequency of air column in d pipe
(a)cont increase
(b)first increase then constant
(c)cont decrease
(d)first decrease then constant

13 Answers

13
Двҥїяuρ now in medical c ·

is the rate of the water coming out through the bottom is greater/lesser than the the rate of water being poured??

1
vector ·

q me itna hi diya hai

1
vector ·

bt i think as its smll hole rate of wate cming out is very less

13
Двҥїяuρ now in medical c ·

as the length is decreasing...when water is being poured then...the freq will increase....

when the water going out through the hole then it will decrease again.....

1
vector ·

increasing i understand bt why becming constant afterwards

13
Двҥїяuρ now in medical c ·

it will not become constant..
..if we continue pouring water after sometime the pipe will be filled with water[3]

if we stop pouring water then the length will increase again....and freq will decrease....

it will become constant only whan all the water will come out...[3]

1
vector ·

bt that s the ans first increase n then constant

13
Двҥїяuρ now in medical c ·

yes...thats the automatic choice as others are impossible....

bt i think the Q has some flaw...

1
vector ·

even i was cnfused

13
Двҥїяuρ now in medical c ·

[4][4]....[1]

1
vector ·

plzzz see my other doubts too

1
gordo ·

let is be filling at a rate= K (rate of volume increment)..
and the area of the hole be 'a'...the rate of outflow of water is √2gH as a function of height H filled.. so net rate of voulme increment = AdH/dt = (K-a*√2gH) where A is the area of the cylinder... now if H is filled by water, the free height is (L-H) where L is the total height of the cylinder.. now in that case the fundamental freq. f= v/ {2(L-H)} where v=velocity of sound in air..
now df/dt = [2v/{2(L-H)}2]*(dH/dt) {differentiating both sides}
now we know that dH/dt=(K-a*√2gH)/A...so we have
dF/dt = [2v/{2(L-H)}2]*(K-a*√2gH)/A...
looking at this expression we observe that dF/dt is positive only untill
K>a*√2gH or H<K2/(a*√2g)2...
so we observe that F first increases upto a certain limit of H and after that it remains constant as at this instant the rate of increment of volume becomes =0...
so B)
(here it becomes constant after wards becoz after a certain H the rate of volume increase=0 or no height increase or constant height, hence constant frequency)

1
vector ·

@gordo gud wrk thanks

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