-
$\text{A}\omega^2$
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$\frac{\text{A}\omega^2}{2}$
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$\frac{\text{A}\omega^2}{\sqrt{2}}$
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$\text{Zero}.$
$\text{A}\omega^2$
$\frac{\text{A}\omega^2}{2}$
$\frac{\text{A}\omega^2}{\sqrt{2}}$
$\text{Zero}.$
Explanation:
The acceleration changes its direction (to opposite direction) after every half oscillation. Thus, net acceleration is given as,
$\text{A}\omega^2+(-\text{A}\omega^2)=0$
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(a) Motion remains S.H.M. with time period = 2T |
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(b) Motion remains S.H.M. with time period = 4T |
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(c) Motion remains S.H.M. and period remains nearly constant |
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(d) Motion remains S.H.M. with time period = |
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(a) 1.11 |
(b) 9.11 |
(c) 7.11 |
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(a) A straight line |
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(a) |
(b) |
(c) |
(d) |
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(a) 4.5 A |
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(c) 3.0 A |
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(a) 1 : 2 |
(b) 1 : 1 |
(c) 2 : 1 |
(d) 1 : 4 |