Animated Solution for Physics - Work, Energy, and Power: Comprehension Passage
A small block of mass M moves on a frictionless surface of an inclined plane, as shown in figure. The angle of the incline suddenly changes from 60∘ to 30∘ at point B. The block is initially at rest at A. Assume that collisions between the block and the incline are totally inelastic(g=10 m/s2).
Visualized Solution
Visualizing the First Incline
The block slides down from point A to point B on a 60∘ incline.
The horizontal distance covered is 3 m.
Calculating Vertical Height h1
We need the vertical height h1 to apply energy conservation.
Using trigonometry: h1=x1tan60∘.
Substituting Values for h1
h1=(3)×(3)
Computing h1
h1=3 m
Conservation of Energy for v1
Velocity just before striking B is v1.
By conservation of mechanical energy: v1=2gh1.
Substituting Values for v1
v1=2×10×3
Computing v1
v1=60 m/s
The Inelastic Collision at B
At point B, the incline angle changes to 30∘.
The collision is totally inelastic.
Velocity Component Conservation
In a totally inelastic collision with a surface, the perpendicular velocity component is lost.
Only the parallel component survives: v2=v1cosθ.
Setting up v2
The angle between v1 and the new incline is 60∘−30∘=30∘.
v2=v1cos30∘
Computing v2
v2=60×23
v2=60×43
Final Answer
v2=45 m/s
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The Sigma Insight: Conservation of Mechanical Energy
Solution Diagram
Imagine you're on a roller coaster. You plunge down a steep drop, building up incredible speed, only to suddenly hit a section where the track levels out slightly. That jarring transition is exactly what our block experiences at point B. Let's break down the physics of this thrilling ride.
Analyzing the First Drop
The block starts from rest at point A and slides down a 60∘ incline. To find its speed at the bottom of this first drop (point B), we need to know how far it has fallen vertically. Gravity only cares about the vertical drop when converting potential energy into kinetic energy.
Using basic trigonometry, the vertical height h1 is related to the horizontal distance x1 by the tangent of the angle:
h1=x1tan60∘
Substituting the given horizontal distance of 3 m:
h1=3×3=3 m
Now, we apply the principle of conservation of mechanical energy. The potential energy lost equals the kinetic energy gained:
v1=2gh1
Plugging in g=10 m/s2 and h1=3 m:
v1=2×10×3=60 m/s
The Inelastic Collision at Point B
Here is where the problem gets interesting. At point B, the incline suddenly changes from 60∘ to 30∘. The block doesn't just smoothly transition; it strikes the new surface. The problem states this collision is totally inelastic.
What does a totally inelastic collision with a fixed surface mean? It means the block doesn't bounce. The component of its velocity that is perpendicular to the new surface is completely absorbed and dissipated as heat and sound. However, the component of its velocity that is parallel to the new surface remains completely unaffected.
To find this surviving parallel component, we need the angle between the incoming velocity vector and the new incline. The incoming velocity is at 60∘ below the horizontal, and the new incline is at 30∘ below the horizontal. The difference between them is:
θ=60∘−30∘=30∘
Final Calculation
The new velocity v2 is simply the parallel component of the incoming velocity v1:
v2=v1cos30∘
Substituting our known values:
v2=60×23
To simplify this, we can bring the 2 inside the square root as a 4:
v2=60×43=45 m/s
And there we have it! The speed of the block immediately after the jarring transition at point B is 45 m/s.