359630 The imaginary angular velocity of the earth for which the effective acceleration due to gravity at the equator shall be zero is equal to (take, \(g=10 \mathrm{~ms}^{-2}\) for the acceleration due to gravity, if the earth were at rest and radius of earth equal to \(6400 \mathrm{~km}\).)
359631 The acceleration due to gravity on the earth's surface at the poles is \(g\) and angular velocity of the earth about the axis passing through the pole is \(\omega\). An object is weighed at the equator and at a height \(h\) above the poles by using a spring balance. If the weights are found to be same, then \(h\) is : (\(h < < R\), where \(R\) is the radius of the earth)
359630 The imaginary angular velocity of the earth for which the effective acceleration due to gravity at the equator shall be zero is equal to (take, \(g=10 \mathrm{~ms}^{-2}\) for the acceleration due to gravity, if the earth were at rest and radius of earth equal to \(6400 \mathrm{~km}\).)
359631 The acceleration due to gravity on the earth's surface at the poles is \(g\) and angular velocity of the earth about the axis passing through the pole is \(\omega\). An object is weighed at the equator and at a height \(h\) above the poles by using a spring balance. If the weights are found to be same, then \(h\) is : (\(h < < R\), where \(R\) is the radius of the earth)
359630 The imaginary angular velocity of the earth for which the effective acceleration due to gravity at the equator shall be zero is equal to (take, \(g=10 \mathrm{~ms}^{-2}\) for the acceleration due to gravity, if the earth were at rest and radius of earth equal to \(6400 \mathrm{~km}\).)
359631 The acceleration due to gravity on the earth's surface at the poles is \(g\) and angular velocity of the earth about the axis passing through the pole is \(\omega\). An object is weighed at the equator and at a height \(h\) above the poles by using a spring balance. If the weights are found to be same, then \(h\) is : (\(h < < R\), where \(R\) is the radius of the earth)
359630 The imaginary angular velocity of the earth for which the effective acceleration due to gravity at the equator shall be zero is equal to (take, \(g=10 \mathrm{~ms}^{-2}\) for the acceleration due to gravity, if the earth were at rest and radius of earth equal to \(6400 \mathrm{~km}\).)
359631 The acceleration due to gravity on the earth's surface at the poles is \(g\) and angular velocity of the earth about the axis passing through the pole is \(\omega\). An object is weighed at the equator and at a height \(h\) above the poles by using a spring balance. If the weights are found to be same, then \(h\) is : (\(h < < R\), where \(R\) is the radius of the earth)