Question
Question: The acceleration of a particle is \(a = 3{t^2}\hat i + 5t\hat j - (8{t^3} + 400)\hat k{\text{ }}m/{s...
The acceleration of a particle is a=3t2i^+5tj^−(8t3+400)k^ m/s2. What is the change in velocity from t=0 to 10 s given as n1i^+n2j^−n3k^?
(A) n1=1000m/s
(B) n2=250m/s
(C) n3=24000m/s
(D) All of these
Solution
Hint
The acceleration of a particle is given as the rate of change of its velocity. Since velocity is a vector quantity, acceleration is also a vector, and is measurable in all the principle directions.
Complete step by step answer
In this question, we are provided with the acceleration vector of a particle. This vector tells us the acceleration of the particle in the X, Y and Z direction independently as:
a=3t2i^+5tj^−(8t3+400)k^ m/s2
We are required to find the velocity of the particle from
Initial time t=0s
Final time t=10s
Now, we know that the acceleration of a body is given as the rate of change of its velocity. Mathematically this can be written as:
a=dtdV
To find the velocity, we cross-multiply and perform integration as:
V=∫dV=∫adt and the limits of this integral range from 0 to 10 seconds.
Substituting the known values gives us:
V=0∫10(3t2i^+5tj^−(8t3+400)k^)dt
Following the linearity property of the integral in the principle direction gives us:
V=0∫103t2dti^+5tdtj^−(8t3+400)dtk^
Performing the integration according to the specified rules:
V=33t3i^+25t2j^−(48t4+400t)k^010
Simplifying this further:
V=t3i^+25t2j^−(2t4+400t)k^010
Putting the values of the initial and final time gives us:
V=103i^+25×102j^−(2×104+400×10)k^ [As any value multiplied by 0 will be equal to 0]
V=1000i^+250j^−(20000+4000)k^
This is equivalent to:
V=1000i^+250j^−24000k^
Now comparing this vector with the general vector n1i^+n2j^−n3k^, we get the values as:
n1=1000m/s
n2=250m/s
n3=24000m/s
All of these match with the options provided, hence the correct answer is option D: All of these.
Note
The components of a vector undergo mathematical operations individually. This property is particularly helpful in determining the behaviour of a vector quantity in a certain direction. For example, if a vector is multiplied by a constant A, all of the components in all the directions will be multiplied by the same factor A.