The terminal velocity of a small steel ball of radius \(r\) falling in a fluid is proportional to
\(r^8\)
\(r^7\)
\(r^2\)
\(r^1\)
\(r^5\)
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of