
The distance x covered in time t by a body having initial velocity u and having constant acceleration a is given by \[x=ut+\dfrac{1}{2}a{{t}^{2}}\] . This result follows from
a) Newton’s first law
b) Newton’s second law
c) Newton’s third law
d) None of the above
Answer
570.9k+ views
Hint: Newton's second Law of motion states that the rate of change of momentum of a body is equal to the force applied on the body. Also, momentum is defined as the product of mass and velocity of a body.
Complete step by step answer:
From Newton's second Law of motion, we have: \[F=ma......(1)\] ,
where m is mass of the body and a is the acceleration.
Also, we know that: \[F=\dfrac{dp}{dt}......(2)\]
Therefore,
\[\Rightarrow \dfrac{dp}{dt}=ma......(3)\]
Since, \[p=mv\]
So, we have:
\[\begin{align}
& \Rightarrow \dfrac{d\left( mv \right)}{dt}=ma \\
& \Rightarrow m\dfrac{dv}{dt}=ma \\
& \Rightarrow \dfrac{dv}{dt}=a \\
& \Rightarrow \dfrac{dv}{dt}=a \\
& \Rightarrow dv=adt......(4) \\
\end{align}\]
Now, integrate both the sides of equation (4), we get:
\[\begin{align}
& \Rightarrow \int{dv}=\int{adt} \\
& \Rightarrow v=at+c......(5) \\
\end{align}\]
Here \[c=u\] , which is u initial velocity.
Therefore,
\[v=at+u......(6)\]
Since\[v=\dfrac{ds}{dt}\] , where s is the distance covered by the body.
So, we can write equation (5) as:
\[\begin{align}
& \Rightarrow \dfrac{ds}{dt}=at+u \\
& \Rightarrow ds=atdt+udt......(6) \\
\end{align}\]
Now, integrate both sides of equation (6), we get:
\[\begin{align}
& \Rightarrow \int{d}s=\int{atdt}+\int{udt} \\
& \Rightarrow s=\dfrac{a{{t}^{2}}}{2}+ut+C......(7) \\
\end{align}\]
Here C is constant of integration which is distance at \[t=0\] .
Since, the distance at \[t=0\] is zero.
Thus, C = 0.
Hence, the equation becomes
\[\begin{align}
& \Rightarrow s=\dfrac{a{{t}^{2}}}{2}+ut+0 \\
& \Rightarrow s=ut+\dfrac{1}{2}a{{t}^{2}} \\
\end{align}\]
So, the correct answer is “Option B”.
Note:
While integration always takes constant integration which always gives the initial value of the physical quantity which is getting integrated.Also remember the concept of Newton's second law of motion.
Complete step by step answer:
From Newton's second Law of motion, we have: \[F=ma......(1)\] ,
where m is mass of the body and a is the acceleration.
Also, we know that: \[F=\dfrac{dp}{dt}......(2)\]
Therefore,
\[\Rightarrow \dfrac{dp}{dt}=ma......(3)\]
Since, \[p=mv\]
So, we have:
\[\begin{align}
& \Rightarrow \dfrac{d\left( mv \right)}{dt}=ma \\
& \Rightarrow m\dfrac{dv}{dt}=ma \\
& \Rightarrow \dfrac{dv}{dt}=a \\
& \Rightarrow \dfrac{dv}{dt}=a \\
& \Rightarrow dv=adt......(4) \\
\end{align}\]
Now, integrate both the sides of equation (4), we get:
\[\begin{align}
& \Rightarrow \int{dv}=\int{adt} \\
& \Rightarrow v=at+c......(5) \\
\end{align}\]
Here \[c=u\] , which is u initial velocity.
Therefore,
\[v=at+u......(6)\]
Since\[v=\dfrac{ds}{dt}\] , where s is the distance covered by the body.
So, we can write equation (5) as:
\[\begin{align}
& \Rightarrow \dfrac{ds}{dt}=at+u \\
& \Rightarrow ds=atdt+udt......(6) \\
\end{align}\]
Now, integrate both sides of equation (6), we get:
\[\begin{align}
& \Rightarrow \int{d}s=\int{atdt}+\int{udt} \\
& \Rightarrow s=\dfrac{a{{t}^{2}}}{2}+ut+C......(7) \\
\end{align}\]
Here C is constant of integration which is distance at \[t=0\] .
Since, the distance at \[t=0\] is zero.
Thus, C = 0.
Hence, the equation becomes
\[\begin{align}
& \Rightarrow s=\dfrac{a{{t}^{2}}}{2}+ut+0 \\
& \Rightarrow s=ut+\dfrac{1}{2}a{{t}^{2}} \\
\end{align}\]
So, the correct answer is “Option B”.
Note:
While integration always takes constant integration which always gives the initial value of the physical quantity which is getting integrated.Also remember the concept of Newton's second law of motion.
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