The force that keeps a ball moving in a circle is called centripetal force. This force acts towards the center of the circle and prevents the ball from moving in a straight line.
The centripetal force, directed towards the center of the circle, keeps the ball on a string moving in a circle. This force is provided by the tension in the string, which constantly pulls the ball towards the center, preventing it from moving in a straight line. The ball's velocity remains tangential to the circle due to the centripetal force acting perpendicular to the velocity vector, resulting in circular motion.
The net force on the ball is directed towards the center of the circle, providing the centripetal force required to keep the ball moving in a circular path. This force is perpendicular to the velocity of the ball at any given moment.
The magnitude of the tension in the string at the bottom of the circle is equal to the sum of the gravitational force acting on the ball and the centripetal force required to keep the ball moving in a circular path.
The centripetal force is what causes a ball to accelerate around a pole. It is directed towards the center of the circular path and keeps the ball moving in a curved trajectory.
The force of gravity pulls the ball downhill, causing it to accelerate as it moves. As long as there is a slope for it to roll on, the ball will continue moving downhill until it reaches a flat surface or encounters a force that slows it down.
The centripetal force, directed towards the center of the circle, keeps the ball on a string moving in a circle. This force is provided by the tension in the string, which constantly pulls the ball towards the center, preventing it from moving in a straight line. The ball's velocity remains tangential to the circle due to the centripetal force acting perpendicular to the velocity vector, resulting in circular motion.
The roulette ball stays in motion due to centrefugal force. Since the ball is moving fast it "wants" to just go straight (Newton's 1st law) but the contact force of the metal track exerts an inward force that keeps it moving in a circle. Eventually, as the ball loses momentum, the force of gravity will be greater and the ball will then fall into a pocket.
The roulette ball stays in motion due to centrefugal force. Since the ball is moving fast it "wants" to just go straight (Newton's 1st law) but the contact force of the metal track exerts an inward force that keeps it moving in a circle. Eventually, as the ball loses momentum, the force of gravity will be greater and the ball will then fall into a pocket.
The ball keeps moving forward because of its momentum, which is not a force.
centripetal
It's not that there is some force keeping the planets from falling into the sun; the sun's gravity prevents the planets from travelling in a straight line out of the solar system. If you throw a ball in a straight line then it keeps going, but if you throw a ball on a rope tied to a pole then the rope pulls the ball toward the pole and keeps the ball moving in a circle.
The net force on the ball is directed towards the center of the circle, providing the centripetal force required to keep the ball moving in a circular path. This force is perpendicular to the velocity of the ball at any given moment.
The magnitude of the tension in the string at the bottom of the circle is equal to the sum of the gravitational force acting on the ball and the centripetal force required to keep the ball moving in a circular path.
The centripetal force is what causes a ball to accelerate around a pole. It is directed towards the center of the circular path and keeps the ball moving in a curved trajectory.
The force of gravity pulls the ball downhill, causing it to accelerate as it moves. As long as there is a slope for it to roll on, the ball will continue moving downhill until it reaches a flat surface or encounters a force that slows it down.
The critical velocity of a ball moving in a vertical circle is the minimum velocity required at the top of the circle to prevent the ball from losing contact with the track. Below the critical velocity, the ball will fall off the track at the top of the circle.
Picture a ball on a string being whirled about the head of an experimenter. If the string breaks, the centripetal force disappears. The ball leaves on a tangent path form its (previous) circular path. Yes, it's that simple. The string provided centripetal force, by virtue of its tensile strength, to the ball to keep that ball moving in a circle. When the string broke, there was no force left to accelerate the ball "in" and keep it moving in an arc.