A block slides down a frictionless plane having an inclination of 0 = 15.0°. The block starts from rest at the top, and the length of the incline is 2.00 m. (a) Draw a free-body diagram of the block. Find (b) the acceleration of the blockand (c) its speed when it reaches the bottom of the incline
(a) The figure represents the free-body diagram of the block that slides on frictionless inclined surface.
(b) The weight of the block is resolved into two components. The component
mg cos θ
is equal to the normal force and the component
mg sin θ
is the force that slides the block on the inclined surface. Here
θ
is angle of inclination. From Newton’s law the net force is equal to the product of mass
(m)
and acceleration
(a)
Therefore,
"F_{net} = mg sin \u03b8 \\\\\n\nma=mg sin \u03b8 \\\\\n\na = g sin \u03b8"
The angle of inclination,
θ = 15.0 °
Therefore acceleration of the block is:
"= 9.80 \\times sin 15.0\u00b0 \\\\\n\n= 2.54 \\;m\/s^2"
We can find the speed of the block when it reaches the bottom of the incline by using kinematic equation,
"v_f^2 -v_i^2 = 2as"
v_f is the final speed of the block at the bottom of incline
s is the length of the incline
The block starts from rest at the top of inclined surface. So, the initial speed of the block at the top of inclined surface,
"v_i=0"
Length of the inclined surface,
s=2.00 m
Acceleration of the block,
"a=2.54 \\; m\/s^2"
Substituting the values in above equation we can find the speed of the block when it reaches the bottom of incline.
"v_f^2 -v_i^2 = 2as \\\\\n\nv_f^2 -0 = 2 (2.54)(2.00) \\\\\n\nv_f = \\sqrt{2 \\times 2.54 \\times 2.00} \\\\\n\n= 3.18 \\;m\/s"
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