Explanation
Given,
Velocity {{v}_{1}} achieve in time {{t}_{1}},due to acceleration, {{a}_{1}}=0.2\,m{{s}^{-2}}
{{v}_{1}}={{u}_{1}}+a{{t}_{1}}
\Rightarrow {{v}_{1}}=0+0.2{{t}_{1}}
Velocity reduce to zero in time {{t}_{2}}, due to retardation, {{a}_{2}}=-0.4\,m{{s}^{-2}}
{{v}_{2}}={{v}_{1}}+a{{t}_{2}}
\Rightarrow 0={{v}_{1}}-0.4{{t}_{2}}
Add time
{{t}_{1}}+{{t}_{2}}=\dfrac{{{v}_{1}}}{0.2}+\dfrac{{{v}_{1}}}{0.4}
\Rightarrow 30\times 60={{v}_{1}}\times 7.5
\Rightarrow {{v}_{1}}=240\,m/s
Apply kinematic equation
{{v}^{2}}-{{u}^{2}}=2as
s=\dfrac{{{v}^{2}}-{{u}^{2}}}{2a}
Total distance {{S}_{1}}+{{S}_{2}}=\dfrac{{{v}_{1}}^{2}}{2{{a}_{1}}}+\dfrac{{{v}_{1}}^{2}}{2{{a}_{2}}}=\dfrac{{{240}^{2}}}{2\times 0.2}+\dfrac{{{240}^{2}}}{2\times 0.4}=216\,km
A ball dropped from the top of the tower falls first half height of the tower in 10s. The total time spent by a ball in the air is \left[ {Take\;g = 10m/{s^2}} \right]
Let the height of tower is h. Now considering the equation as
s=ut+\dfrac{1}{2}a{{t}^{2}}
h=ut+\dfrac{1}{2}a{{t}^{2}}...........(1)
here,\,\,h=\dfrac{h}{2}
In 10 sec, object is reaching half the height of tower.
Initially the body is rest so u = 0
It is also given that a = 10 ms-2
Time to reach first half height of tower t = 10 sec
Put the values in (1)
\dfrac{h}{2}=0+\dfrac{1}{2}\times 10\times {{10}^{2}}
h=1000\,\,m
The total time spent by a ball in the air is given by the relation as
1000=\dfrac{1}{2}\times 10\times {{t}^{2}}
t=10\sqrt{2}
t=14.14\,\sec
A body moving along the positive x-axis with uniform acceleration of - 4m{s^{ - 2}}. Its velocity at x=0 is 10m{s^{- 1}}. The time taken by the body to reach a point at x = 12cm is:
Let,
Constant acceleration, a
Initial velocity u
Apply kinematic Equation
v=u+at
a=\dfrac{v-u}{t}
Compare acceleration at both event at time, {{t}_{1}}\,\And \,{{t}_{2}}
\dfrac{{{v}_{2}}-u}{{{t}_{1}}}=\dfrac{{{v}_{3}}-u}{{{t}_{2}}}
\Rightarrow \dfrac{30-u}{2}=\dfrac{60-u}{4}
\Rightarrow u=0
Initial velocity u=zero
The acceleration when the mass is going up is given as,
{v^2} = {u^2} + 2as
{\left( {20} \right)^2} = {\left( 0 \right)^2} + 2as
a = \dfrac{{200}}{s} (1)
The acceleration when the mass is going down is given as,
s = \dfrac{1}{2}a{t^2}
s = \dfrac{1}{2}a{\left( {10} \right)^2}
a = \dfrac{s}{{50}} (2)
From equation (1) and (2), we get
\dfrac{{200}}{s} = \dfrac{s}{{50}}
s = 100\;{\rm{m}}
Substitute the value of s in the equation (2), we get
a = \dfrac{{100}}{{50}}
= 2\;{\rm{m/}}{{\rm{s}}^{\rm{2}}}
The weight is given as,
W = 0.5 \times 2
= 1\;{\rm{N}}
Thus, the weight of the body on that planet is 1\;{\rm{N}}.
Force on crate, F=\,575\,N
Mass of crate, m=50\,kg
Coefficient of friction, \mu =0.25
From the equilibrium of forces
ma=F-\mu mg
a=\dfrac{F-\mu mg}{m}
a=\dfrac{575-0.25\times 50\times 9.81}{50}
a=9.047\,\,m/{{s}^{2}}
Acceleration of block is 9.047\,\,m/{{s}^{2}}
Let distance covered by A be S1
Let distance covered by B be S2
B will catch A when S1 = S2
S = ut + 1/2 * a * t^2
Therefore,
40t + (1/2 * 0 * t^2) = 0t + 1/2 * 4 * t^2
40t = 2t^2
20t = t^2
Therefore, t = 20
Given that,
Mass {{m}_{1}}=3\,kg
Mass {{m}_{2}}=2\,kg
Now, the initial acceleration a of the system
a=\dfrac{3g-2g}{3+2}
a=\dfrac{g}{5}
At 5\ sec
Now, from equation of motion
v=0+\dfrac{g}{5}\times 5
v=9.8\,m/s
When the string breaks at t= 5\ s,
The mass 2\ kg more under gravity
So, height is
h=\dfrac{{{v}^{2}}}{2g}
h=\dfrac{{{\left( 9.8 \right)}^{2}}}{2\times 9.8}
h=4.9\,m
Hence, the height is 4.9\ m
Initial velocity, u=\left( 2\hat{j}+\hat{k} \right)\,m/s
Force, F=\left( 2\hat{i}+\hat{j}+3\hat{k} \right)\,N
\vec{a}=\dfrac{{\vec{F}}}{m}=\dfrac{2\hat{i}+\hat{j}+3\hat{k}}{1}=\left( 2\hat{i}+\hat{j}+3\hat{k} \right)\,m/{{s}^{2}}
\vec{v}=\vec{u}+\vec{a}t
\vec{v}=\left( 2\hat{j}+\hat{k} \right)+\left( 2\hat{i}+\hat{j}+3\hat{k} \right)\times 2
\vec{v}=\left( 4\hat{i}+4\hat{j}+7\hat{k} \right)\,m/s
\left| {\vec{v}} \right|=\sqrt{{{4}^{2}}+{{4}^{2}}+{{7}^{2}}}=9\,m/s
Final velocity is 9\,m/s
Please disable the adBlock and continue. Thank you.