A cyclist needs to exert a centripetal force to move faster around a curve. The amount of force required depends on the speed of the cyclist, mass of the rider and bicycle, radius of the curve, and coefficient of friction between the tires and the road surface. A higher speed or tighter turn will require more force.
As a cyclist goes faster, the force of friction remains relatively constant. The force of friction between the tires and the road depends on the coefficient of friction and the normal force, which do not change significantly with speed.
The primary centripetal force on a car going around a curve is provided by the frictional force between the tires and the road. This force is directed towards the center of the curve, allowing the car to maintain its circular path.
All objects in motion want to travel in a straight line. to get the object to curve in any direction requires a force or pressure to pull or push it around the curve. A string on a rock gravity on a basketball bullet planet or satellite and in this case friction between the tire and the ground. If the rider tried to stay upright he would tip over. This turning force is called "centrifugal force" and when you add it to gravity the direction of up and down change, just like a rock on a string always hangs straight down but as you swing it in a circle faster and faster it swings outward so its "up" looks slanted to us.
The force applied by a cyclist is called pedaling force or pedal force. This force is generated by pushing down on the pedals to propel the bicycle forward.
The force that passengers feel pushing them away from the center of the curve is called centrifugal force. This force is a result of the car's inertia trying to keep moving in a straight line while the car changes direction around the curve.
As a cyclist goes faster, the force of friction remains relatively constant. The force of friction between the tires and the road depends on the coefficient of friction and the normal force, which do not change significantly with speed.
to counter centrifugal force and to take turn faster
The primary centripetal force on a car going around a curve is provided by the frictional force between the tires and the road. This force is directed towards the center of the curve, allowing the car to maintain its circular path.
The force applied by a cyclist is called pedaling force or pedal force. This force is generated by pushing down on the pedals to propel the bicycle forward.
The force that passengers feel pushing them away from the center of the curve is called centrifugal force. This force is a result of the car's inertia trying to keep moving in a straight line while the car changes direction around the curve.
All objects in motion want to travel in a straight line. to get the object to curve in any direction requires a force or pressure to pull or push it around the curve. A string on a rock gravity on a basketball bullet planet or satellite and in this case friction between the tire and the ground. If the rider tried to stay upright he would tip over. This turning force is called "centrifugal force" and when you add it to gravity the direction of up and down change, just like a rock on a string always hangs straight down but as you swing it in a circle faster and faster it swings outward so its "up" looks slanted to us.
Velocity
Yes, a bicycle needs a centripetal force acting towards the center of the curve to change its direction of motion. This force is typically provided by friction between the tires and the road surface, allowing the bike to maintain its trajectory around the curve without sliding out.
Friction
No, the forces acting on a cyclist when decelerating are not balanced. The force of friction between the tires and the road, as well as air resistance, act to slow down the cyclist. The net force in the direction opposite to the movement causes deceleration.
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inertia, centrifugal force