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Revision: Kinematics >> Motion in a Plane Physics Science (English Medium) Class 11 CBSE

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Definitions [21]

Definition: Component Vectors

The splitting vectors obtained when a single vector is resolved into two or more vectors in different directions are called component vectors.

Definition: Direction Cosines

The values of cos⁡αcos⁡β, and cosγ which are the cosines of the angles subtended by the rectangular components with the given vector are called direction cosines of a vector.

Definition: Resolution of the Vector

A vector \[\vec V\] can be expressed as the sum of two or more vectors along fixed directions. This process is known as vector resolution.

OR

The process of splitting a single vector into two or more vectors in different directions which together produce same effect as produced by the single vector alone is called resolution of vector.

Definition: Rectangular Components

When a vector is resolved into components along mutually perpendicular directions (like x and y axes in 2D, or x, y, and z axes in 3D), these components are called rectangular or Cartesian components.

Definition: Angular Acceleration (α)

The rate of change of angular velocity of a body is called angular acceleration.

Definition: Radial (Centripetal) Acceleration

The component of acceleration directed towards the centre of the circular path is called centripetal acceleration (or radial acceleration).

Definition: Centripetal Force

The force directed towards the centre along the radius, required to keep a body moving along a circular path at constant speed, is called centripetal force.

Definition: Uniform Circular Motion

When a particle moves with a constant speed in a circular path, its motion is said to be uniform circular motion.

OR

The motion of a body moving with constant speed along a circular path is called uniform circular motion.

OR

The motion of a body moving with constant speed along a circular path, where the velocity is always tangential to the circular path and remains constant in magnitude, is called uniform circular motion.

Define Uniform circular motion.

When a particle moves with a constant speed in a circular path, its motion is said to be the uniform circular motion.

Define angular velocity.

Angular velocity of a particle is the rate of change of angular displacement.

Definition: Angular Displacement

The angle traced out by the radius vector at the centre of the circular path in a given time, expressed as Δθ = θ2 − θ1, is called angular displacement.

Definition: Angular Velocity (ω)

The rate of change of angular displacement of a body undergoing circular motion is called angular velocity.

Definition: Vector

A vector is any quantity that needs both magnitude (size) and direction to be completely described.

Definition: Instantaneous Velocity

Instantaneous velocity of an object is its velocity at a given instant of time. It is defined as the limiting value of the average velocity of the object over a small time interval (Δt) around t when the value of the time interval (Δt) goes to zero.

OR

The limiting value of the average velocity of an object over a small time interval 'Δt' around time t when the value of the time interval goes to zero is called instantaneous velocity.

Definition: Acceleration

Acceleration is defined as the rate of change of velocity with time.

OR

The rate of change of velocity with respect to time — a vector quantity whose direction is the same as that of change in velocity, with dimensional formula [M0L1T−2] and SI unit m/s² — is called acceleration.

Definition: Average Acceleration

The change in velocity of an object divided by the total time required for that change in velocity is called average acceleration.

OR

The ratio of total change in velocity to the total time taken by the particle when the change in velocity results is called average acceleration.

Definition: Instantaneous Acceleration

The limiting value of the average acceleration of an object over a small time interval 'Δt' around time tt when the value of the time interval goes to zero is called instantaneous acceleration.

OR

The acceleration of a particle at a particular instant of time — defined as the limit of average acceleration as time interval Δt→0 — is called instantaneous acceleration.

Definition: Uniform Acceleration

The acceleration when the magnitude and direction of the acceleration remains constant during motion of an object is called uniform acceleration.

Definition: Non-Uniform Acceleration

The acceleration when either magnitude or direction or both change during motion is called non-uniform acceleration.

Definition: Gravitational Acceleration

The acceleration on an object which results due to gravity — where every small body accelerates in a gravitational field at a similar rate towards the centre of mass, irrespective of the mass of the body — is called gravitational acceleration.

Definition: Retardation / Deceleration

The negative acceleration (i.e., uniformly retarded motion where a < 0) that shows slowing down or deceleration of a particle is called retardation.

Formulae [9]

Formula: Identity of Direction Cosines

The sum of squares of all direction cosines is always equal to 1:

cos2α + cos2β + cos2γ = 1

Formula: Three-Dimensional Resolution of a Vector

When a vector \[\vec A\] is resolved into three-dimensional rectangular components, it is given by:

\[\vec A\] = Ax\[\hat i\] + Ay\[\hat j\] + Az\[\hat k\]
Formula: Magnitude of a 3D Vector

The magnitude of vector \[\vec A\] resolved into three-dimensional components is:

A = \[\sqrt{A_x^2+A_y^2+A_z^2}\]

Formula: Direction Cosines

If αβ, and γ are the angles subtended by the rectangular components with the given vector, then:

cos α = \[\frac {A_x}{A}\], cos β = \[\frac {A_y}{A}\], cos γ = \[\frac {A_z}{A}\]

Formula: Instantaneous velocity

\[\vec{\mathrm{v}}=\lim_{\Delta t\to0}\left(\frac{\Delta\vec{x}}{\Delta t}\right)=\frac{d\vec{x}}{dt}\]

Formula: Velocity of B relative to A

\[\vec{v}_{BA}=\vec{v}_B-\vec{v}_A\]

where:

  • \[\vec v_A\] = Velocity of object A
  • \[\vec v_B\] = Velocity of object B
  • \[\vec v_{AB}\] = Velocity of A relative to B
  • The subscripts indicate the order: for \[\vec v_{BA}\], B is the observer, A is referenced.
Formula: Velocity of A relative to B

\[\vec{v}_{AB}=\vec{v}_A-\vec{v}_B\]

where:

  • \[\vec v_A\] = Velocity of object A
  • \[\vec v_B\] = Velocity of object B
  • \[\vec v_{AB}\] = Velocity of A relative to B
  • The subscripts indicate the order: for \[\vec v_{AB}\], A is the observer, B is referenced.
Formula: Average Acceleration

Average acceleration is calculated when an object has velocities \[\vec v_1\] and \[\vec v_2\] at times t1 and t2:

\[\vec{a}=\frac{\vec{v_2}-\vec{v_1}}{t_2-t_1}\]

where:

  • \[\vec a\] = average acceleration
  • \[\vec v_1\] = velocity at time t1
  • \[\vec v_2\] = velocity at time t2

OR

Average acceleration: \[\vec a_{av}=\frac {\vec v_2-\vec v_1}{t_{2}-t_{1}}=\frac {\Delta\vec v}{\Delta t}\]

Formula: Instantaneous Acceleration

Instantaneous acceleration is the limiting value of average acceleration when the time interval approaches zero:

\[\vec{a}=\lim_{\Delta t\to0}\frac{\Delta\vec{v}}{\Delta t}=\frac{d\vec{v}}{dt}\]

where:

  • \[\vec a\] = instantaneous acceleration
  • \[d\vec{v}\] = infinitesimal change in velocity
  • dt = infinitesimal change in time

The instantaneous acceleration at a given time equals the slope of the tangent to the velocity versus time curve at that time.

Key Points

Key Points: Addition and Subtraction of Vectors
  1. Component Method: Resultant R = A + B is found as Rx = Ax + BxRy = Ay + ByRz = Az + Bz, giving R = Rx\[\hat i\] + Ry\[\hat j\] + Rz\[\hat k\].

  2. Laws of Addition: Triangle law (head-to-tail), Parallelogram law (tail-to-tail, diagonal = resultant), and Polygon law (for multiple vectors, closing side = resultant).

  3. Magnitude (Addition): When A and B are at angle θR = \[\sqrt{A^2+B^2+2AB\cos\theta}\].

  4. Magnitude (Subtraction): Change the sign to minus — ∣R∣ = .

  5. Direction of Resultant: tan⁡α = \[\frac{B\sin\theta}{A+B\cos\theta}\] for addition; tan⁡β = \[\frac{B\sin\theta}{A-B\cos\theta}\] for subtraction.

Key Points: Uniform Circular Motion
  • In UCM, speed is constant, but velocity continuously changes direction, always remaining tangential to the path.
  • Angular displacement is the angle swept by the radius vector; angular velocity is its rate of change.
  • Even at constant speed, centripetal acceleration is never zero — it always acts towards the centre of the circular path.
  • Centripetal force is always directed towards the centre and is essential to maintain circular motion — it does no work on the body.
  • If speed is constant in circular motion, tangential acceleration = 0, but radial acceleration ≠ 0.
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