"T=2\\pi\\sqrt{\\frac{l}{g}}\\to l=\\frac{T^2\\cdot g}{4\\pi^2}=\\frac{3.5^2\\cdot 9.81}{4\\cdot3.14^2}=3m"
So,
"\\sin\\alpha=0.3\/3=0.1\\to \\alpha\\approx5.7\u00b0"
The period of oscillation of a simple pendulum does not depend on the mass of the pendulum and the amplitude (if the angle of deviation of the pendulum does not exceed 6 °)
if the length is extended by 20% then "l_1=l+0.2l=1.2l"
We get that
"\\frac{T}{T_1}=\\frac{1}{\\sqrt{1.2}}\\to T_1=\\sqrt{1.2}T=\\sqrt{1.2}\\cdot3.50=3.8s"
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