What Was the Take Off Speed of the Bike Rider?

AI Thread Summary
The discussion focuses on calculating the take-off speed of a bike rider who leaves a ramp at a 32-degree angle and lands 36 meters away. The equations of motion are applied, with the horizontal distance and vertical motion analyzed separately. The user attempts to derive the time of flight and take-off speed using the equations S=ut+1/2at^2 for both horizontal and vertical components. They express their calculations and seek confirmation on their approach and the next steps. The conversation emphasizes the importance of correctly applying physics principles to solve the problem.
Paul_H
Messages
1
Reaction score
0
1. A bike rider leaves a ramp at an angle of 32 degrees and lands at the same height after traveling a horizontal distance of 36m. What was his take off speed?



2. S=ut+1/2at^2



3. My attempt:
Vertical : s u v a=9.81 t=?
Horizontal: s=36m u v a=0 t=?

Horizontal:
S=ut+1/2at^2
36=(xcos32)t
36/(xcos32) = t

Vertical
S=ut+1/2at^2
xsin32/4.905 = t

36/xcos32 = xsin32/4.905

36*4.905 (xsin32)(xcos32)

Thats my best attempt, hopefully someone can tell me if I am going wrong and what is the next step in order to complete the question. Thanks
 
Physics news on Phys.org
36*4.905 = (xsin32)(xcos32) looks okay to me.
To solve for x, divide both sides by sin(32)*cos(32)
and take the square root of both sides.
 
Thread 'Minimum mass of a block'
Here we know that if block B is going to move up or just be at the verge of moving up ##Mg \sin \theta ## will act downwards and maximum static friction will act downwards ## \mu Mg \cos \theta ## Now what im confused by is how will we know " how quickly" block B reaches its maximum static friction value without any numbers, the suggested solution says that when block A is at its maximum extension, then block B will start to move up but with a certain set of values couldn't block A reach...
Thread 'Calculation of Tensile Forces in Piston-Type Water-Lifting Devices at Elevated Locations'
Figure 1 Overall Structure Diagram Figure 2: Top view of the piston when it is cylindrical A circular opening is created at a height of 5 meters above the water surface. Inside this opening is a sleeve-type piston with a cross-sectional area of 1 square meter. The piston is pulled to the right at a constant speed. The pulling force is(Figure 2): F = ρshg = 1000 × 1 × 5 × 10 = 50,000 N. Figure 3: Modifying the structure to incorporate a fixed internal piston When I modify the piston...
Back
Top