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Standard Derivatives

Dalam dokumen Maths for Physics (Halaman 92-98)

6.2 Standard Derivatives

Example:

Differentiatey=x12.

Solution: So using the rule that if y = xn then dy

dx =nxn−1. We have n = 1

2. This gives the answer:

dy dx = 1

2×x12−1=x12 2 = 1

2 x

So far we have only considered polynomials which have a coefficient of 1. But how do we differentiate y= 4x2where the coefficient is equal to 4? When we have a coefficientawe have the rule:

Ify=axn then dy

dx =a×n×xn−1

Note: The first rule that we discussed is just a special case of the above rule whena= 1.

So going back toy= 4x2 we can see that the coefficienta= 4 andxis raised to the power ofn= 2. So using the rule, ify=axn then dy

dx =a×n×xn−1. We have:

dy

dx = 4×2×x2−1= 8x1= 8x

IMPORTANT:When differentiating any functionf(x) multiplied by some constanta, findingdxd [af(x)], we can take the constantaout of the derivative so:

d dx

af(x)

=a d dx

f(x)

For example d

dx(2x3) = 2× d

dx(x3) = 2×3x2= 6x2.

Example:

Differentiatey= 4x12

Solution: This example combines everything we have looked at so far. So using the rule:

Ify=axn then dy

dx =a×n×xn−1 we havea= 4 and n=−1

2. This gives the answer:

dy

dx = 4× −1

2×x12−1=−2x32

Physics Example:

Coulomb’s Law states that the magnitude of the attractive forceF be- tween two charges decays according to the inverse square of the separating distancer:

F = 1 r2

If we plot a graph ofF on they-axis againstr on thex-axis, what is the gradient?

Solution: To find the gradient we find the derivative with respect tordenoted dF dr of:

F = 1 r2 =r−2

All the examples so far have only containedxandyhowever in this question we have the variables dy

Below we have the rules for differentiating trigonometric functions:

Ify= sin(x) then dy

dx = cos(x)

Ify= cos(x) then dy

dx =−sin(x)

Ify= tan(x) then dy

dx = sec2(x)

When we have constants multiplying the trigonometric functions and coefficients multiplying our xwe can use the following rules:

Ify=asin(bx) then dy

dx =a×b×cos(bx)

Ify=acos(bx) then dy

dx =−a×b×sin(bx)

Ify=atan(bx) then dy

dx =a×b×sec2(bx) Note: These rules only work whenxis being measured in radians.

Example:

Differentiate:

1. y= sin(9x) 2. y= 4 cosx

2 3. y=−2 tan (−7x)

Solution: Using the rules above:

1. Ify=asin(bx) then dy

dx =a×b×cos(bx)

Note that we havey= sin(9x) soa= 1 and b= 9. So dy

dx = 9 cos(9x) 2. Ify=acos(bx) then dy

dx =−a×b×sin(bx) Note that we havey= 4 cosx

2

soa= 4 andb= 1 2

dy

dx =−4× ×1

2×sinx 2

=−2 sinx 2

3. Ify=atan(bx) then dy

dx =a×b×sec2(bx)

Note that we havey=−2 tan (−7x) soa=−2 andb=−7 dy

dx = (−2)× −7 sec2(−7x)

=

−14 sec2(−7x) = 14 sec2(7x)

Physics Example:

In X-ray crystallography, the Bragg equation relates the distance d be- tween successive layers in a crystal, the wavelength of the X-raysλ, an integer nand the angle through which the X-rays are scatteredθin the equation:

λ= 2d n sinθ What is the rate of change ofλwithθ?

Solution: The question is asking us to find dλ

dθ. So asnanddare constants we can use the rule:

Ify=asin(bx) then dy

dx =a×b×cos(bx) So we havea=

2d n

andb= 1 with λas y andθasxtherefore:

dλ dθ =

2d n

×1×cosθ= 2d n cosθ.

Differentiating Exponential Functions

The exponential function ex is special, since when we differentiateex, we just obtainex again. This is shown in the rule below:

Ify=exthen dy

dx =ex

We can also differentiate when thexhas a coefficient, for exampley=e4x, and also when the exponential is multiplied by a constant, for exampley= 3ex. We combine these into the rule below:

Ify=aebx then dy

dx =a×b×ebx

Example:

Differentiate the following with respect tox:

1. y=e2x 2. y= 8 exp

−x 3

Solution:

1. Using the rule

Ify=aebx then dy

dx =a×b×ebx note y=e2x soa= 1 andb= 2 hence dy

dx = 2e2x 2. Using the rule

Ify=aebx then dy

dx =a×b×ebx −x

−1 dy

× −1

×

−x

−8 x

Ify= ln(x) then dy

dx = 1 x

We can differentiate when thexhas a coefficient, for exampley= ln(4x), and also when the logarithmic function has a coefficient, for exampley= 3 ln(x). We combine these into the rule below:

Ify=aln(bx) then dy

dx = a x

Note: In the above rule, the b disappears and it forms a nice exercise in the practice of using the laws of logarithms hence we have included the algebra in the next example. We do have to differenti- ate a sum however so if you are unsure on that step then check out the next section for more information.

Example:

Fory=aln(bx) find dy dx

Solution: Using laws of logarithms we can writey=aln(bx) as:

y=a(ln(x) + ln(b)) Now differentiating this as a sum gives:

dy dx = d

dx[a(ln(x) + ln(b))]

=⇒ dy dx =a d

dx[ln(x)] +a d dx[ln(b)]

Now as d

dx[ln(x)] = 1

x and d

dx[ln(b)] = 0 as ln(b) is a constant, we have:

dy dx = a

x

Note: This derivation is included as it provides an advanced example of the use of the laws of logarithms with differentiation.

Example:

Differentiate:

1. y= ln(3x) 2. y=−4

5ln x

2

Solution:

1. We use the rule:

Ify=aln(bx) then dy dx = a

x Note that we havey= ln(3x) soa= 1 andb= 3. Hence dy

dx = 1 x 2. We use the rule:

Ify=aln(bx) then dy dx = a

x Note that we havey=−4

ln x

soa=−4

andb=1

. Hence dy

=−4

×1

=− 4

Differentiating Hyperbolic Functions

Below we have the rules for differentiating hyperbolic functions:

Ify= sinh(x) then dy

dx = cosh(x)

Ify= cosh(x) then dy

dx = sinh(x)

Ify= tanh(x) then dy

dx = sech2(x)

When we have constants multiplying the hyperbolic functions and coefficients multiplying ourxwe can use the following rules:

Ify=asinh(bx) then dy

dx =a×b×cosh(bx)

Ify=acosh(bx) then dy

dx =a×b×sinh(bx)

Ify=atanh(bx) then dy

dx =a×b×sech2(bx)

Note: that the derivative of cosh(x) is sinh(x) and NOT−sinh(x). We can prove these derivatives by differentiating the exponential forms of the hyperbolic functions:

Example:

Differentiate cosh(x) by converting to the exponential form.

Solution: Begin by writing cosh(x) as

cosh(x) = ex 2 +e−x

2 Differentiating each term:

d

dxcosh(x) = ex 2 −e−x

2

= sinh(x)

6.3 Differentiation Techniques

Dalam dokumen Maths for Physics (Halaman 92-98)