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RUDIKE [14]
2 years ago
15

A ball is thrown from a top of a building of height 20m. If the initial velocity of the ball is 15m/s at 370 above the horizonta

l find, a) the velocity of the ball at 2s. b) the position at which the ball strike the ground.​
Physics
1 answer:
Lesechka [4]2 years ago
6 0

Explanation:

Givens:

h = 20 \: m

v _{ix} = 15 \cos(37)  = 11.97

v _{iy} = 15 \sin(37)  = 9.03

a _{y} =  - 9.8

Let t=2 be the final velocity. Since Velocity stays the same horizontal , acceleration due to gravity changes the vertical direction

Use this equation

v _{y} = v _{iy} + a _{y}(t)

Plug in the knowns

v _{y} = 15 \sin(37)  +2 ( - 9.8)

v _{y} =   - 10.57

So the velocity in the y direction at 2 seconds is -10.57

The velocity in the x direction at 2 seconds is 11.97

Use the Pythagorean theorem to find the total velocity

v =  \sqrt{( - 10.57) {}^{2} + (11.97) {}^{2}  }

v = 15.97

b. The range at which it strike the ground.

We need to find when the velocity at the top is zero.

Using the y direction,

0 = v \sin( 37 )  - 9.8(t)

t = 0.921

Next, find the height of the max.

h =  \frac{1}{2} ( 9.8)(0.921) {}^{2}  = 4.16

So the total distance is 4.16+20= 24.16

Next to find the total time it falls

24.16 =  \frac{1}{2} (9.8) {t}^{2}

t = 2.2

So our total flight time is

3.141

Range is

v \cos(37) (3.141) = 37.63

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A block is balanced on top of a frictionless sphere of radius R. When the block is given a slight nudge it starts to slide down
Nataly_w [17]

Answer:\frac{R}{3}

Explanation:

Given

Sphere of Radius R

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At any instant \theta Normal reaction(N) and weight(mg) is acting such that

mg\sin \theta -N=\frac{mv^2}{R}  , where v is velocity of block at any angle \theta

When block is just about to leave then N=0

therefore

mg\sin \theta =\frac{mv^2}{R}

v^2=gR\sin \theta-------------------1

Also by conserving Energy we get

Potential Energy=kinetic Energy of block

mgh=\frac{mv^2}{2}

here h=vertical distance traveled by block

From diagram

h=R-R\sin \theta

h=R(1-\sin \theta )

mgR(1-\sin \theta )=\frac{mv^2}{2}

2gR(1-\sin \theta )=v^2-----------------2

From 1 and  2

2(1-\sin \theta )=\sin \theta

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\sin \theta =\frac{2}{3}

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h=R(1-\frac{2}{3})

h=\frac{R}{3}

3 0
3 years ago
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