Radial Acceleration: Definition, Derivation, Formula and Units

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Radial Acceleration includes its main usage in terms of movement, velocity and direction of the objects. All these phenomena are measured in the relative context. The acceleration could also be defined as a changing velocity of any object at any particular time. Acceleration is referred to as a vector quantity that confines in itself both magnitude and the direction.

What is Radial Acceleration?

As per Newton's law of motion, any object or body which is under motion tends to undergo a change in its speed through movement and this varies on the basis of the amount of force applied to an object. 

Therefore, the measure of the rate of change in the speed of an object along with that of its direction and with respect to time is called acceleration. Although, the motion of the object can be either linear or circular.

The type of acceleration that is involved in linear motion is called linear acceleration. While the type of acceleration that is involved in a circular motion is called angular acceleration. The angular acceleration can be classified as follows:

  • Radial Acceleration
  • Tangential Acceleration

Radial acceleration shall be defined as an acceleration of an object that is directed towards the centre. This acceleration takes place in a uniform circular motion and the movement is concerned along the radius of an object. 

On the other hand, tangential acceleration measures the rate of change of tangential velocity of a point at a certain radius with respect to time. Tangential acceleration is similar to linear acceleration but is relevant to circular motion.

Units of the Radial Acceleration

Radial acceleration is measured in terms of Radians per second square which is represented as ωs-2

Formulas Related to Radial Acceleration

In the above figure, an object M is tied to a string and then it is made to rotate at a fixed axis around the point ‘C’ which is the centre of the circle. The object when rotated fast, the string CM appears like the radius of the circle. A force is exerted on the object from the centre, thereby an acceleration a0 acts along the radial direction, that is, along the radius of the circle towards the centre.

In order to counter this force, the tension is developed along the string in the opposite direction. This force which emerges due to the tension is called centripetal force. And the acceleration that is generated on an object is called the centripetal acceleration or radial acceleration ar.

The above figure represents the two objects which are infinitesimally closer to each other and the specific diagram of an equivalent triangle having a centripetal velocity vector.

On applying the property of the similar triangles, it could be seen that 

\(\frac {AB} {OA} = IR\) 

Since, the points A and B are infinitesimally closer, it could be assumed as AB to the length of arc AB as 

AB = v × dt

The points A and B are very close, therefore,

v + dv ≈ dv × \(\frac {AB} {OA}\)

\(\frac {dv} {v}\) ×\(\frac {v x dt} {r}\)

 → \(\frac {dv} {v}\)

Now, on rearranging,

\(\frac {dv} {v} = \frac {v^2} {r}\)

Hence, dv / dt represents the radial acceleration of an object which is under the uniform circular motion. Therefore, the final equation for the above proving is given below.

ar = \(\frac {v^2} {r}\)

Tangential Acceleration

The tangential acceleration is generally defined as the component of angular acceleration tangential to the circular path. The unit of measurement of the tangential acceleration is represented as ms-2. And the mathematical equation for the same is given as:

at = \(\frac {v_2 - v_1} {t}\)

Here,

at → The tangential component

t → Time period

v1 and v2 → Respective velocities of the two objects which are given in a circular motion

Things to Remember based on Radial Acceleration

  • Angular acceleration can be classified into Radial and Tangential acceleration
  • Radial acceleration shall be defined as an acceleration of an object that is directed towards the centre.
  • Radial acceleration is measured in terms of Radians per second square which is represented as ωs-2 
  • Centripetal acceleration is also called radial acceleration.
  • The tangential acceleration is generally defined as the component of angular acceleration tangential to the circular path. 

Sample Questions based on Radial Acceleration

Ques. What defines centripetal acceleration? (2 marks) 

Ans. Centripetal acceleration is simply another name for radial acceleration which defines the acceleration or movement towards the centre of the circle.

Ques. What is acceleration and deceleration?  (2 marks) 

Ans. Both acceleration and deceleration refer to the change in the velocity of an object at any unit of time.

Ques. A cyclist starts from centre O of a circular park of radius 1 km and moves along the path OPRQO as shown in figure. If he maintains a constant speed of 10 ms”1, what is his acceleration at point R in magnitude and direction?  (3 marks) 

Ans. According to the problem the path of the cyclist is O-P- R-Q-O.

The cyclist is in uniform circular motion and it is given that linear velocity = 10 m/s, R = 1 km = 1000 m. As we know whenever an object is performing circular motion, acceleration is called centripetal acceleration and is always directed towards the centre.So cyclist experiences a centripetal force (acceleration) at point R towards centre.

Ques. What is the unit of radial acceleration? (2 marks) 

Ans. Radial Acceleration has the unit that is similar to that of the angular acceleration, that is radian / sec2. This unit is represented as ωs-2.

Ques. Earth can be thought of as a sphere of radius 6400 km. Any object (or a person) is performing circular motion around the axis of the earth due to the earth rotation (period 1 day). What is the acceleration of an object on the surface of the earth (at equator) towards its centre? What is it at latitude 9? How does these accelerations compare with g = 9.8 m/s2?  (3 marks) 

Ans.  

Ques. What is radial acceleration? (2 marks) 

Ans. The radial acceleration shall be defined as an acceleration of an object that is directed towards the centre in context of the radius of the circle.

Ques. What are the two types of angular motion? (2 marks) 

Ans. The two types of angular motions are radial acceleration and tangential acceleration.

Ques. Earth also moves in circular orbit around the sun once every year with an orbital radius of 1.5 x 1011 What is the acceleration of the earth (or any object on the surface of the earth) towards the centre of the sun? How does this acceleration compare with g = 9.8 m/s2? (3 marks) 

Ans. 

Ques. Mention some examples of some incidents and the cause of centripetal force involved. (3 marks) 

Ans. Some of the examples are

  • Orbital motion of planets and the gravitational force between them.
  • Orbital motion of electrons and the electrostatic forces between the electrons and nucleus.
  • When vehicles take a turn and the frictional force that acts between the tyre and the road.
  • When a stone is tied with a string, it revolves around. The tension in the string is an example of centripetal force.

Ques. What is angular velocity? (2 marks) 

Ans. The time rate of change of angular displacement (Δθ) is called angular velocity.

Angular velocity (ω) = (Δθ/Δt)

Angular velocity is a vector quantity and its unit is rad/s.

Relation between linear velocity (v) and angular velocity (ω) is given by

v = rω

CBSE CLASS XII Related Questions

  • 1.
    If Bohr’s quantization postulate (angular momentum \( = \frac{nh}{2\pi} \)) is a basic law of nature, it should be equally valid for the case of planetary motion also. Why, then, do we never speak of quantization of orbits of planets around the Sun? Explain.


      • 2.
        The figure shows three point charges kept at the vertices of triangle ABC. The net electric field, due to this system of charges, at the midpoint M of base BC will be:

          • \( \frac{q}{4 \pi \epsilon_0 l^2} \) pointing along MA
          • \( \frac{q}{\pi \epsilon_0 l^2} \) pointing along AM
          • \( \frac{q}{2 \pi \epsilon_0 l^2} \) pointing along AM
          • Zero

        • 3.
          Assertion (A) : All atoms have a net magnetic moment. Reason (R) : A current loop does not always behave as a magnetic dipole.

            • Both Assertion (A) and Reason (R) are true and Reason (R) is the correct explanation of the Assertion (A).
            • Both Assertion (A) and Reason (R) are true, but Reason (R) is not the correct explanation of the Assertion (A).
            • Assertion (A) is true, but Reason (R) is false.
            • Both Assertion (A) and Reason (R) are false.

          • 4.
            A light copper ring is freely suspended by a light string. A bar magnet is held horizontally with its length along the axis of the ring. The magnet is moved towards the ring with its N pole facing the loop. What will happen to the ring and its position? Explain.


              • 5.
                If both the number of protons and the neutrons are conserved in each nuclear reaction, in what way is mass converted into energy (or vice versa) in a nuclear reaction? Explain.


                  • 6.
                    Two heaters rated as \((P_1,V)\) and \((P_2,V)\) are connected in series across a dc source of \(V/2\) volt. The power consumed by the combination will be –

                      • \((P_1+P_2)\)
                      • \(\dfrac{P_1+P_2}{2}\)
                      • \(\dfrac{P_1P_2}{2(P_1+P_2)}\)
                      • \(\dfrac{P_1P_2}{4(P_1+P_2)}\)
                    CBSE CLASS XII Previous Year Papers

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