Highly Wedged Constraint Motion!!

Find a c c e l e r a t i o n \color{#20A900}{acceleration} of Lowest Hanging Block \color{#20A900}{\text{Lowest Hanging Block}} ( in m / s 2 ) (\text{ in } m/s^2) in above system. If your answer can be expressed of form a b where a , b I + and g c d ( a , b ) = 1 \color{#20A900}{\frac{a}{b}} \color{#333333}{\text{ where } a, b \in I^+ \text{ and } gcd(a, b) = 1} , Enter your answer as a + b \color{#20A900}{a + b} .

Details and Assumptions

  • All surfaces are s m o o t h \color{#20A900}{smooth}

  • All s t r i n g s \color{#20A900}{strings} and p u l l e y s \color{#20A900}{pulleys} are i d e a l \color{#D61F06}{ideal}

  • All W e d g e s \color{#20A900}{Wedges} and b l o c k s \color{#20A900}{blocks} are f r e e \color{#20A900}{free} to move.

  • Take acceleration due to gravity g = 10 m / s 2 \color{#20A900}{g = 10m/s^2}

  • Strings are n o t \color{#D61F06}{not} intermingled.


All of my problems are original


Difficulty: \dagger \dagger \dagger \dagger \color{grey}{\dagger}


The answer is 897.

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1 solution

Aryan Sanghi
Jul 6, 2020

Here is a F.B.D. for all bodies considering only Forces responsible for motion.

We get equations

N s i n θ 5 T = m A 1 Nsin\theta - 5T = mA_1

m g s i n θ = m a x mgsin\theta = ma_x

m g c o s θ N = m a y = m A 1 s i n θ mgcos\theta - N = ma_y = mA_1sin\theta

N = m A 3 N' = mA_3

5 T N = m A 3 5T - N' = mA_3

T m g = m A 4 T - mg = mA_4

4 T m g = m A 2 4T - mg = mA_2

Using Tension trick(Just Work-Energy theorem) to find constraint relation

T . A = 0 \sum T.A = 0

5 T × A 1 + 4 T × A 2 + 5 T × A 3 + T × A 4 = 0 -5T × A_1 + 4T×A_2 + 5T × A_3 + T×A_4 = 0

5 A 1 + 4 A 2 + 5 A 3 + A 4 = 0 \boxed{-5A_1 + 4A_2 + 5A_3 + A_4 = 0}

Solving all equations, we get

T = 40 m g 227 T = \frac{40mg}{227}

A 2 = 67 g 227 = 670 227 A_2 = \frac{67g}{227} = \frac{670}{227}

a + b = 897 \color{#3D99F6}{\boxed{a + b = 897}}

A good problem 👍

Kundan Rathi - 11 months, 1 week ago

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Thanku. :)

Aryan Sanghi - 11 months, 1 week ago

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