Question #42019

Hey
And its,a physics ques
From laws of motion-motion in connected bodies

There was a,ques of 2 bodies suspended from a pully m1>m2 with acceleration a
Find a
And tension

Ans was a=(m1-m2)g/(m1+m2)

And T=2m1m2g/(m1+m2)



For mass m1
T=m1g-m1a (i)

For m2
T =m2a+m2g

My doubt
Why acc is taken in opp dir.?
Since in m1 acc is downward thus eqn should be
For mass m1
T=m1g+m1a (i)

and for m2 acc is upward
T =m2g-m2a

Then f=ma is taken opp
In direction
When it is along the direction of mg in m1 case and along t in m2 case

Expert's answer

Answer on Question #42019 – Physics - Mechanics | Kinematics | Dynamics

Hey

And its, a physics ques

From laws of motion-motion in connected bodies

There was a, ques of 2 bodies suspended from a pully m1>m2m1 > m2 with acceleration a

Find a

And tension

Ans was a=(m1m2)g/(m1+m2)a = (m1 - m2)g / (m1 + m2)

And T=2m1m2g/(m1+m2)T = 2m1m2g / (m1 + m2)

For mass m1

T=m1g-m1a (i)

For m2

T = m2a + m2g

My doubt

Why acc is taken in opp dir.?

Since in m1 acc is downward thus eqn should be

For mass m1

T=m1g+m1a (i)

and for m2 acc is upward

T = m2g - m2a

Then f=maf = ma is taken opp

In direction

When it is along the direction of mgmg in m1m1 case and along tt in m2m2 case

Solution:

Forces acting on the two masses and pulley:



mg - the force of gravity,

T - string tension force,

a - acceleration of the system;

Accelerations is taken in opposite directions because acceleration of the heavy bodie m1\mathfrak{m}_1 is directed downward (bodie is moving down) and the other's bodie m1\mathfrak{m}_1 is directed upward (moving up).

Tension force to each end of the string:


T1=T1;T2=T2;a=a\left| \overrightarrow {\mathrm {T} _ {1}} \right| = \left| \overrightarrow {\mathrm {T} _ {1} ^ {\prime}} \right|; \left| \overrightarrow {\mathrm {T} _ {2}} \right| = \left| \overrightarrow {\mathrm {T} _ {2} ^ {\prime}} \right|; \left| \overrightarrow {\mathrm {a} ^ {\prime}} \right| = | \vec {\mathrm {a}} |


If we consider that we have ideal pulley:


T1=T2\overrightarrow {\mathrm {T} _ {1} ^ {\prime}} = \overrightarrow {\mathrm {T} _ {2} ^ {\prime}}


Newton's second law for the first mass:


T1+m1g=m1a\overrightarrow {\mathrm {T} _ {1}} + \overrightarrow {\mathrm {m} _ {1} \vec {\mathrm {g}}} = \mathrm {m} _ {1} \vec {\mathrm {a}}y:m1gT1=m1ay: m _ {1} g - T _ {1} = m _ {1} aT1=m1gm1aT _ {1} = m _ {1} g - m _ {1} a


Newton's second law for the second mass:


T2+m2g=m1a\overrightarrow {T _ {2}} + \overrightarrow {m _ {2} g} = m _ {1} \vec {a}y:T2m2g=m2ay: T _ {2} - m _ {2} g = m _ {2} aT2=m2am2g=T1 (from (1)) (2)T _ {2} = m _ {2} a - m _ {2} g = T _ {1} \text{ (from (1)) (2)}(1)=(2):(1) = (2):m2am2g=m1gm1am _ {2} a - m _ {2} g = m _ {1} g - m _ {1} aa(m1+m2)=g(m1m2)a (m _ {1} + m _ {2}) = g (m _ {1} - m _ {2})a=g(m1m2)m1+m2a = \frac {g \left(m _ {1} - m _ {2}\right)}{m _ {1} + m _ {2}}


We do not know the values of the masses but we know that m1>m2m_{1} > m_{2}, so we can take the absolute difference m1m2m_{1} - m_{2} for the positive value of the acceleration:


(3)in(1):(3) \text{in}(1):T1=T2=T=m1gm1g(m1m2)m1+m2=m1g(m1+m2m1+m2m1+m2)=T _ {1} = T _ {2} = T = m _ {1} g - m _ {1} \frac {g (m _ {1} - m _ {2})}{m _ {1} + m _ {2}} = m _ {1} g \left(\frac {m _ {1} + m _ {2} - m _ {1} + m _ {2}}{m _ {1} + m _ {2}}\right) ==2m1m2gm1+m2= \frac {2 m _ {1} m _ {2} g}{m _ {1} + m _ {2}}


Answer: a=g(m1m2)m1+m2,T=2m1m2gm1+m2a = \frac{g(m_1 - m_2)}{m_1 + m_2}, T = \frac{2m_1m_2g}{m_1 + m_2}

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