Kinetic Energy of 0.2 kg Ball with 20 m/s Velocity

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The kinetic energy of a 0.2 kg ball thrown at 20 m/s at a 30-degree angle is calculated using the horizontal component of the velocity at the top of its path. At this point, the vertical velocity is zero, so only the horizontal component contributes to kinetic energy. The formula used is KE = ½mv_H², where v_H is the horizontal velocity calculated as 20 cos 30 degrees. This emphasizes that even when the vertical component is zero, the horizontal motion still possesses kinetic energy. Understanding the separation of velocity into components is crucial for accurate kinetic energy calculations in projectile motion.
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I realize this problem is like ridiculously easy, but I just don't understand why you get the answer this way.

A 0.2 kg ball is thrown with an initial velocity of 20 m/s at an angle of 30 degrees with respect to the horizontal. What is the kinetic energy of the ball at the top of it's path?

I don't understand why in order to get the answer, you have to use the horizontal velocity componenent, Vx. Shouldn't you just use the velocity as given, and plug it into .5mv^2? Thanks
 
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KE = ½mv², where v is the velocity of the ball.

After projection, the ball's velocity can be resolved into horizontal and vertical components. So it's KE at any particular time is,

KE = \frac{1}{2}mv_H^2 + \frac{1}{2}mv_V^2

But at the top of it's flight, v_V = 0. so only the horizontal velocity needs to be considered.
 
great explanation
 
u must take note that you are projecting the object at an angle of 30 degrees not vertically upwards. Thus, there is velocity also in the horizontal component. Since there is velocity in the horizontal component, there must also be KE in the direction also.
 
K=(1/2) mv^2

Here, v is the speed. That is:

v = \sqrt{{v_H}^2 + {v_V}^2}

where v_H is the horizontal component of the velocity, and v_V is the vertical component.

Plugging this into the formula for kinetic energy, we get Fermat's result (above):

K = (1/2) m ({v_H}^2 + {v_V}^2) = (1/2) m{v_H}^2 + (1/2)m{v_V}^2

In this particular example, at the top of the flight, we have:

v_H = 20\cos 30\deg
v_V = 0
 
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