A particle at rest starts moving along a horizontal line with an acceleration a in a particular direction. After time t it changes the sign of its acceleration . At what time T will it come back to its initial position?
Let that time be T = K t . Find K .
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I really like this intuitive approach, Ujjwal. I should try and use graphic methods more often; I'm too much in the habit of using algebra as my default approach. :)
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But algebra ALWAYS works while these methods are applicable/cheaper sometimes - especially when the graphs are straight lines (constant or zero acceleration patches) I will try to find and post some old problems that yielded quick solutions this way . . .
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Yes, I suppose that is part of the reason I usually try algebra first, (even if it ends up being messy). I'll keep an eye out for any problems you post. :)
Root 2 can not be simplified to 1.414, as it is irrational
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You are right. Only here, the expected answer was a decimal approximation. So I used this value for root(2)
After time t the particle will have traveled a distance ( 2 1 ) a t 2 and be traveling at a speed of a t .
Now reset the clock to t 1 = 0 . The acceleration is now − a , and with an initial speed of a t the distance D from the original starting point is given by the formula
D = ( 2 1 ) a t 2 + a t t 1 − ( 2 1 ) a t 1 2 .
Now the particle will have returned to its starting point when D = 0 , i.e., when
( 2 1 ) a t 1 2 − a t t 1 − ( 2 1 ) a t 2 = 0 ⟹ t 1 2 − t t 1 − t 2 = 0
⟹ t 1 = 2 2 t ± 4 t 2 + 4 t 2 = ( 1 + 2 ) t ,
where we took the positive root since we must have t 1 > 0 .
To find the total time of travel T we just add this result to t to find that
T = ( 2 + 2 ) t , giving us K = 2 + 2 = 3 . 4 1 4 to 3 decimal places.
Let us say for convenience time is in sec and distance in m. It moves, say a distance D m in t sec, D = 2 1 ∗ a ∗ t 2 . ....(1)
After changing the sign of a, the particle will come to rest before starting back movement. The distance moved from start to change of sign is D m in t sec, then it will move further D m in t sec before coming to rest, just symmetrical.
So, it has to move - 2D m distance with -a, the time taken is (T - 2t) sec.
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Nice approach, Niranjan. :)
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Brian, Prof. Khanderia taught me kinematics and dynamics of machines 30 years back and has remained ever since a lifelong guide and source of inspiration. Feels so good to share this space with him!
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@Ujjwal Rane – In that case I am honored as well. :) Small world that the two of you are on this site together; did one of you let the other know about it, or did you find it independently?
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@Brian Charlesworth – In fact it was Ujjwal who showed me this site. He has always been adding something. We meet when I go to India, and are in touch by e.mail. It is a joy to have contact with some one like Ujjwal.
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@Niranjan Khanderia – I'm impressed that the two of you have kept in touch all these years. You clearly have a high regard for one another. :)
Thank you.
Nice solution sir ! :)
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There are two great solutions here already, so just adding the visual approach using velocity v/s time graph - the area under which is the distance covered.
Consider three areas or distances covered
A1 - covered while speeding up
A2 - covered while slowing down
A3 - covered in the return journey
A1 = A2 . . . congruent right triangles <=identical height and slope of hypotenuse
For a round trip, A3 = A1 + A2 = 2 A2
Because they are both right angled triangles and share a pair of vertically opposite angles, the blue and the red triangles are similar.
Similar triangles with areas 1:2 must have sides t : t ′ = 1 : 2 Hence T = t + t + t ′ = ( 2 + 2 ) t = 3 . 4 1 4 t