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\(\pi\)
e
\(\frac{a}{b}\)
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→
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\(\sqrt{\,}\)
\(a^{b}\)
7
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9
\(\div\)
log
ln
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\(\times\)
cos
cos⁻¹
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sin
sin⁻¹
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tan
tan⁻¹
A ball of mass \(m=2\) kg is thrown into the air. Near the Earth's surface, the only significant force acting on it is the force of gravity, \(\Vect{F_g}\).
Assuming the y-axis points vertically upwards and the acceleration due to gravity is \(g=9.8\) m/s², calculate the gravitational force vector \(\Vect{F_g}\) and use Newton's Second Law to find the acceleration vector \(\Vect{a}\) of the ball.
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