1. | \(0.15\) m/s2 | 2. | \(0.18\) m/s2 |
3. | \(0.2\) m/s2 | 4. | \(0.1\) m/s2 |
A stone tied to the end of a \(1\) m long string is whirled in a horizontal circle at a constant speed. If the stone makes \(22\) revolutions in \(44\) seconds, what is the magnitude and direction of acceleration of the stone?
1. | \(\pi^2 ~\text{ms}^{-2} \) and direction along the tangent to the circle. |
2. | \(\pi^2 ~\text{ms}^{-2} \) and direction along the radius towards the centre. |
3. | \(\frac{\pi^2}{4}~\text{ms}^{-2} \) and direction along the radius towards the centre. |
4. | \(\pi^2~\text{ms}^{-2} \) and direction along the radius away from the centre. |
1. | The velocity and acceleration both are parallel to \(\vec{r }.\) |
2. | The velocity is perpendicular to \(\vec{r }\) and acceleration is directed towards to origin. |
3. | The velocity is parallel to \(\vec{r }\) and acceleration is directed away from the origin. |
4. | The velocity and acceleration both are perpendicular to \(\vec{r}.\) |
1. | \(\vec v\) is a constant; \(\vec a\) is not a constant. |
2. | \(\vec v\) is not a constant; \(\vec a\) is not a constant. |
3. | \(\vec v\) is a constant; \(\vec a\) is a constant. |
4. | \(\vec v\) is not a constant; \(\vec a\) is a constant. |
In the given figure, \(a=15\) m/s2 represents the total acceleration of a particle moving in the clockwise direction in a circle of radius \(R=2.5\) m at a given instant of time. The speed of the particle is:
1. \(4.5\) m/s
2. \(5.0\) m/s
3. \(5.7\) m/s
4. \(6.2\) m/s
A car is moving at a speed of \(40\) m/s on a circular track of radius \(400\) m. This speed is increasing at the rate of \(3\) m/s2. The acceleration of the car is:
1. \(4\) m/s2
2. \(7\) m/s2
3. \(5\) m/s2
4. \(3\) m/s2
1. | Acceleration is along \((\text{-}\vec R )\). |
2. | Magnitude of the acceleration vector is \(\frac{v^2}{R}\), where \(v\) is the velocity of the particle. |
3. | Magnitude of the velocity of the particle is \(8\) m/s. |
4. | Path of the particle is a circle of radius \(4\) m. |
Two particles \(A\) and \(B\) are moving in a uniform circular motion in concentric circles of radii \(r_A\) and \(r_B\) with speeds \(v_A\) and \(v_B\) respectively. Their time periods of rotation are the same. The ratio of the angular speed of \(A\) to that of \(B\) will be:
1. | \( 1: 1 \) | 2. | \(r_A: r_B \) |
3. | \(v_A: v_B \) | 4. | \(r_B: r_A\) |
1. | \(\dfrac{{v}^{2}}{r}\) | 2. | \(a\) |
3. | \(\sqrt{{a}^{2}{+}{\left({\dfrac{{v}^{2}}{r}}\right)}^{2}}\) | 4. | \(\sqrt{a+\dfrac{v^{2}}{r}}\) |
1. | \(a_{r}=0;\) tangential acceleration \(a_{t}\neq 0.\) | radial acceleration
2. | \(a_{r}=0;\) tangential acceleration \(a_{t}=0.\) | radial acceleration
3. | \(a_{r}\neq 0;\) tangential acceleration \(a_{t}\neq 0.\) | radial acceleration
4. | \(a_{r}\neq 0;\) tangential acceleration \(a_{t}=0\) | radial acceleration