Let us consider, a physical quantity y depends on another physical quantity x i.e., y = .
The graph shown in figure represents the variation of y with respect to x and A and B are two points on the graph. We draw two perpendiculars on OX from point A and B.
AC and BC are two mutually perpendiculars which represents the small change in x i.e x and corresponding change in y i.e y respectively.
The rate of change of y with respect to x is = slope of the line AB = tan.
But the rate of change is not same at all points on the graph because at point B the slope is more. So, to get the rate of change of y with respect to x at point A, x should be very small and points A and B are very close.
The slope or the tangent at point A gives the rate of change of y with respect to x at point A is = . Where is the differentiation operator.
Some common formulas of differentiations are respectively:
(i)
(ii)
(iii)
(iv) = cosx
(v) = -sinx
(vi)
(vii) = secxtanx
(viii)
(ix) = - cosecxcotx
(x)
Some common rules of differentiations are respectively:
(i) where A is a constant.
If u and v are then,
(ii)
(iii)
(iv)
(v)
(vi) this is chain rule.
Applications of differential calculus to solve physics problems:
1. The velocity-displacement graph of a particle is given in figure. What is the acceleration when displacement is 2m?
From graph slope is = tan 30 =
Acceleration a = = ( )( ) = v( ) =
When s = 2m then v = 3m
∴ a = = = m
2. One dimensional motion of body:
A particle is moving in a straight line and its displacement is x = (3 – 1.5 + 2) m. What is the velocity and acceleration of the particle in 2s? What is the displacement when velocity of the particle is zero?
Velocity of the particle is v = = = 9 – 3t. At t = 2s v = 30 m .
Acceleration of the particle is a = = = 18t – 3. At t = 2s a = 33 m .
Now v = 0 so, 9 – 3t = 0 or, t = s. At t = s displacement is x = 3 – 1.5 + 2 = m.
3. Pulley problem using differential calculus:
A ring initially at rest can slide downward through a vertical wire. The ring is connected with a block by a massless inextensible string through a fixed pulley as shown in figure. What is the ratio of velocities of ring and the block if the string creates an angle at pulley with the initial horizontal position?
Let us consider when string creates angle , the displacement of ring and block are respectively x and y. The length between ring and pulley is l which remain constant.
The length of the string is L = + y = constant
The velocity of the ring is = and the velocity of the block is = (taking downward motion is positive and upward motion is negative)
Now, + =
Or, × 2x + = 0
Or, sin =
∴ = cosec
4. Pulley 1 is fixed and block A is connected by a mass less inextensible string with a movable pulley 2 as shown in figure. Another block B is connected with a string over the pulley 2 and the other end of the string is fixed with horizontal surface. Mass of block B is more than that of block A. What is the relation of acceleration of block A and block B?
We consider a reference line on pulley 1 and the distance of block A, pulley 2, block B and horizontal surface are respectively , , , and y.
If is the length of the string over pulley 1 and is the total length of string which connects
body A and pulley 2 then, + + =
Differentiating the equation with respect to time t we get + + =
Or, – + 0 + = 0 (as and are constant then differentiation is 0 and taking upward
motion is negative)
Or, =
Or, =
Or, =
If is the length of the string over pulley 2 and is the total length of string connected between body B and horizontal surface then
(y – ) + + ( – ) = or, y – 2 + + =
Differentiating the equation with respect to time t we get, – 2+ + =
Or, 0 – 2 + 0 + = 0 (as and are constant then differentiation is 0)