krit.club logo

Calculus - Kinematics

Grade 12IB_AI

Review the key concepts, formulae, and examples before starting your quiz.

πŸ”‘Concepts

β€’

Kinematics involves the study of motion. The three primary variables are displacement (ss), velocity (vv), and acceleration (aa), all expressed as functions of time (tt).

β€’

Displacement (s(t)s(t)) is the position of an object relative to a fixed origin. Velocity (v(t)v(t)) is the rate of change of displacement over time.

β€’

Acceleration (a(t)a(t)) is the rate of change of velocity over time.

β€’

Relationship via Differentiation: v(t)=sβ€²(t)=dsdtv(t) = s'(t) = \frac{ds}{dt} and a(t)=vβ€²(t)=sβ€²β€²(t)=dvdta(t) = v'(t) = s''(t) = \frac{dv}{dt}.

β€’

Relationship via Integration: v(t)=∫a(t)dtv(t) = \int a(t) dt and s(t)=∫v(t)dts(t) = \int v(t) dt. Note that a constant of integration +C+ C is required when using indefinite integrals.

β€’

A particle is at rest (stationary) when its velocity v(t)=0v(t) = 0. It is moving to the right or upwards when v(t)>0v(t) > 0, and to the left or downwards when v(t)<0v(t) < 0.

β€’

The total distance traveled over the interval [t1,t2][t_1, t_2] is the integral of the absolute value of velocity (speed): ∫t1t2∣v(t)∣dt\int_{t_1}^{t_2} |v(t)| dt.

β€’

Displacement over a time interval is the change in position: s(t2)βˆ’s(t1)=∫t1t2v(t)dts(t_2) - s(t_1) = \int_{t_1}^{t_2} v(t) dt.

πŸ“Formulae

v(t)=dsdtv(t) = \frac{ds}{dt}

a(t)=dvdt=d2sdt2a(t) = \frac{dv}{dt} = \frac{d^2s}{dt^2}

s(t)=∫v(t)dts(t) = \int v(t) dt

v(t)=∫a(t)dtv(t) = \int a(t) dt

Displacement=∫t1t2v(t)dt\text{Displacement} = \int_{t_1}^{t_2} v(t) dt

Total Distance=∫t1t2∣v(t)∣dt\text{Total Distance} = \int_{t_1}^{t_2} |v(t)| dt

πŸ’‘Examples

Problem 1:

A particle moves in a straight line such that its displacement ss (in meters) from a fixed point OO at time tt (in seconds) is given by s(t)=t3βˆ’9t2+24t+5s(t) = t^3 - 9t^2 + 24t + 5 for tβ‰₯0t \ge 0. Find the time(s) when the particle is at rest.

Solution:

The particle is at rest when v(t)=0v(t) = 0. First, find the velocity function by differentiating s(t)s(t): v(t)=sβ€²(t)=3t2βˆ’18t+24v(t) = s'(t) = 3t^2 - 18t + 24 Set v(t)=0v(t) = 0: 3t2βˆ’18t+24=03t^2 - 18t + 24 = 0 Divide by 33: t2βˆ’6t+8=0t^2 - 6t + 8 = 0 Factorize the quadratic: (tβˆ’2)(tβˆ’4)=0(t - 2)(t - 4) = 0 t=2t = 2 or t=4t = 4

Explanation:

To find when a particle is at rest, we calculate the first derivative of displacement to get velocity and solve for tt when velocity equals zero.

Problem 2:

The acceleration of a moving object is given by a(t)=6tβˆ’4a(t) = 6t - 4. At t=0t = 0, the velocity of the object is 10Β mΒ sβˆ’110 \text{ m s}^{-1}. Find an expression for the velocity v(t)v(t) and calculate the velocity at t=3t = 3.

Solution:

Integrate acceleration to find velocity: v(t)=∫(6tβˆ’4)dt=3t2βˆ’4t+Cv(t) = \int (6t - 4) dt = 3t^2 - 4t + C Use the initial condition v(0)=10v(0) = 10 to find CC: 10=3(0)2βˆ’4(0)+Cβ‡’C=1010 = 3(0)^2 - 4(0) + C \Rightarrow C = 10 So, v(t)=3t2βˆ’4t+10v(t) = 3t^2 - 4t + 10 At t=3t = 3: v(3)=3(3)2βˆ’4(3)+10=27βˆ’12+10=25Β mΒ sβˆ’1v(3) = 3(3)^2 - 4(3) + 10 = 27 - 12 + 10 = 25 \text{ m s}^{-1}

Explanation:

Velocity is the integral of acceleration. We use the given initial velocity (the value of vv when t=0t=0) to solve for the constant of integration.

Problem 3:

The velocity of a particle is given by v(t)=2t+5v(t) = 2t + 5. Calculate the displacement of the particle between t=1t = 1 and t=4t = 4.

Solution:

The displacement is the definite integral of the velocity function: ∫14(2t+5)dt\int_{1}^{4} (2t + 5) dt Find the antiderivative: [t2+5t]14[t^2 + 5t]_{1}^{4} Evaluate at the limits: (42+5(4))βˆ’(12+5(1))(4^2 + 5(4)) - (1^2 + 5(1)) (16+20)βˆ’(1+5)(16 + 20) - (1 + 5) 36βˆ’6=3036 - 6 = 30 36βˆ’630\begin{array}{r} 36 \\ - 6 \\ \hline 30 \end{array} The displacement is 30Β m30 \text{ m}.

Explanation:

To find displacement over a specific time interval, we calculate the definite integral of the velocity function.