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Motion in A Plane question

2015 · Q129
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Motion in A Plane question

2015 · Q129

NEETPhysicsMotion in A PlaneMCQ+4 / −1
If vectors A→=cos⁡ωti^+sin⁡ωtj^\overrightarrow A = \cos \omega t\widehat i + \sin \omega t\widehat jA=cosωti+sinωtj​ and B→=cos⁡ωt2i^+sin⁡ωt2j^\overrightarrow B = \cos {{\omega t} \over 2}\widehat i + \sin {{\omega t} \over 2}\widehat jB=cos2ωt​i+sin2ωt​j​ are functions of time, then the value of t at which they are orthogonal to each other is
  1. A
    t=πωt = {\pi \over \omega }t=ωπ​
  2. B
    t === 0
  3. C
    t=π4ωt = {\pi \over {4\omega }}t=4ωπ​
  4. D
    t=π2ωt = {\pi \over {2\omega }}t=2ωπ​
View written solutionFree

Correct answer: A

Two vectors A‾\overline A A and B‾\overline B B are orthogonal to each other, if their scalar product is zero i.e. A‾\overline A A.B‾\overline B B = 0.

Here, A‾=cos⁡ωti^+sin⁡ωtj^\overline A = \cos \omega t\widehat i + \sin \omega t\widehat jA=cosωti+sinωtj​

and B‾=cos⁡ωt2i^+sin⁡ωt2j^\overline B = \cos {{\omega t} \over 2}\widehat i + \sin {{\omega t} \over 2}\widehat jB=cos2ωt​i+sin2ωt​j​

∴A‾.B‾=(cos⁡ωti^+sin⁡ωtj^)(cos⁡ωt2i^+sin⁡ωt2j^) \therefore \overline A .\overline B = \left( {\cos \omega t\widehat i + \sin \omega t\widehat j} \right)\left( {\cos {{\omega t} \over 2}\widehat i + \sin {{\omega t} \over 2}\widehat j} \right)∴A.B=(cosωti+sinωtj​)(cos2ωt​i+sin2ωt​j​)

= cos⁡ωtcos⁡ωt2+sin⁡ωtsin⁡ωt2\cos \omega t\cos {{\omega t} \over 2} + \sin \omega t\sin {{\omega t} \over 2}cosωtcos2ωt​+sinωtsin2ωt​
    (∵i^.i^=j^.j^=1 and i^.j^=j^.i^=0) \left( \because {\widehat i.\widehat i = \widehat j.\widehat j = 1\,and\,\widehat i.\widehat j = \widehat j.\widehat i = 0} \right)(∵i.i=j​.j​=1andi.j​=j​.i=0)

= cos⁡(ωt−ωt2)\cos \left( {\omega t - {{\omega t} \over 2}} \right)cos(ωt−2ωt​)
    (∵cos⁡(A−B)=cosAcosB+sinAsinB \because \cos (A - B) = cosAcosB + sinAsinB∵cos(A−B)=cosAcosB+sinAsinB)

But A‾.B‾=0\overline A .\overline B = 0A.B=0 (as A‾\overline A A and B‾\overline B B are orthogonal to each other)

∴cos⁡(ωt−ωt2)=0 \therefore \cos \left( {\omega t - {{\omega t} \over 2}} \right) = 0∴cos(ωt−2ωt​)=0

cos⁡(ωt−ωt2)=cos⁡π2  or ωt−ωt2=π2\cos \left( {\omega t - {{\omega t} \over 2}} \right) = \cos {\pi \over 2}\,\,or\,\omega t - {{\omega t} \over 2} = {\pi \over 2}cos(ωt−2ωt​)=cos2π​orωt−2ωt​=2π​

ωt2=π2 or t=πω{{\omega t} \over 2} = {\pi \over 2}\,or\,t = {\pi \over \omega }2ωt​=2π​ort=ωπ​

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