The magnitude of displacement of a particle moving in a circle of radius 'a' with constant angular speed ω \omega ω varies with time 't' as :
(A) 2 a sin ω t \omega t ω t ;
(B) 2 a sin ω t / 2 \omega t / 2 ω t /2 ;
(C) 2 a cos ω t \omega t ω t ;
(D) 2 a cos ω t / 2 \omega t / 2 ω t /2 ;
Please do specify the method by which u got ur answer...
Particle position:
R ⃗ = acos ( ω t ) ı ⃗ + asin ( ω t ) j ⃗ \vec {R} = \operatorname {a c o s} (\omega t) \vec {\imath} + \operatorname {a s i n} (\omega t) \vec {j} R = acos ( ω t ) + asin ( ω t ) j
At t = 0 t = 0 t = 0 :
R 0 → = a ı ⃗ \overrightarrow {R _ {0}} = a \vec {\imath} R 0 = a
Displacement:
d ⃗ = R ⃗ − R 0 → = a cos ( ω t ) ı ⃗ + a sin ( ω t ) j ⃗ − a ı ⃗ = a ( cos ( ω t ) − 1 ) ı ⃗ + a sin ( ω t ) j ⃗ d = ( a ( cos ( ω t ) − 1 ) ) 2 + ( a sin ( ω t ) ) 2 = a 2 − 2 cos ( ω t ) = a 2 ( 1 − cos ( ω t ) ) 1 − cos ( ω t ) = 2 ( sin ( ω t / 2 ) ) 2 d = a 2 ∗ 2 ( sin ( ω t / 2 ) ) 2 = 2 a sin ( ω t / 2 ) \begin{array}{l}
\vec {d} = \vec {R} - \overrightarrow {R _ {0}} = a \cos (\omega t) \vec {\imath} + a \sin (\omega t) \vec {j} - a \vec {\imath} = a (\cos (\omega t) - 1) \vec {\imath} + a \sin (\omega t) \vec {j} \\
d = \sqrt {\left(a (\cos (\omega t) - 1)\right) ^ {2} + (a \sin (\omega t)) ^ {2}} = a \sqrt {2 - 2 \cos (\omega t)} = a \sqrt {2 (1 - \cos (\omega t))} \\
1 - \cos (\omega t) = 2 (\sin (\omega t / 2)) ^ {2} \\
d = a \sqrt {2 * 2 (\sin (\omega t / 2)) ^ {2}} = 2 a \sin (\omega t / 2) \\
\end{array} d = R − R 0 = a cos ( ω t ) + a sin ( ω t ) j − a = a ( cos ( ω t ) − 1 ) + a sin ( ω t ) j d = ( a ( cos ( ω t ) − 1 ) ) 2 + ( a sin ( ω t ) ) 2 = a 2 − 2 cos ( ω t ) = a 2 ( 1 − cos ( ω t )) 1 − cos ( ω t ) = 2 ( sin ( ω t /2 ) ) 2 d = a 2 ∗ 2 ( sin ( ω t /2 ) ) 2 = 2 a sin ( ω t /2 )
Answer d = 2 a sin ( ω t / 2 ) d = 2a\sin (\omega t / 2) d = 2 a sin ( ω t /2 ) (B)
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