Regras de derivação explicita e implicita-Definição de regra da cadeia

Before this, knowDefinição de regra da cadeia para expoentes racionais

Read · 1 min

The power rule for derivatives is that if the original function is xnx^n, then the derivative of that function is nxn−1n x^{n-1}. To prove this, you use the limit definition of derivatives as hh approaches 00 into the function f(x+h)−f(x)h\frac{f(x+h)-f(x)}{h}, which is equal to (x+h)n−xnh\frac{(x+h)^n - x^n}{h}.

If you apply the Binomial Theorem to (x+h)n(x+h)^n, you get xn+nxn−1h+…x^n + n x^{n-1} h + \dots, and the xnx^n terms cancel!

If the exponent is negative the negative exponents in the numerator get moved to the denominator and become positive exponents. negative exponents in the denominator get moved to the numerator and become positive exponents..

So, the numerator just becomes nxn−1h+…n x^{n-1} h + \dots, where everything in the "…\dots" has at least h2h^2 in it. When we finally divide by hh (the denominator), we get nxn−1+…n x^{n-1} + \dots, where everything in the "…\dots" has at least hh in it. Then, taking the limit h→0h \rightarrow 0, we find that only nxn−1n x^{n-1} remains.

Read · 2 min

There is actually a way of showing that ddx(xr)=rxr−1\frac{d}{dx}(x^r) = r x^{r-1} for all rr directly, without worrying about whether rr is positive or an integer or a rational number or anything. It uses "heavy machinery" to do it, though: natural logarithms (and the exponential function exe^x).

Logarithmic differentiation.

If we take the logarithm of both sides of y=xry = x^r, we end up with ln⁡y=ln⁡(xr)=rln⁡x\ln y = \ln(x^r) = r \ln x. Now we can take the derivative of both sides:

In fact, this is a special case of a technique known as logarithmic differentiation. Whenever you need to differentiate an expression of the form f(x)g(x)f(x)^{g(x)}, a good first step is to take logarithms.

What is xrx^r, anyway?

We can also do things slightly differently. First, write f(x)=xrf(x) = x^r as eln⁡xr=erln⁡xe^{\ln x^r} = e^{r \ln x}. Then, if we differentiate using the chain rule, we get: f′(x)=ddxerln⁡x=erln⁡x⋅ddx(rln⁡x)=erln⁡x⋅rx=xr⋅rx=rxr−1.\begin{align*} f'(x) &= \frac{d}{dx} e^{r \ln x} \\ &= e^{r\ln x} \cdot \frac{d}{dx} (r \ln x) \\ &= e^{r \ln x} \cdot \frac{r}{x} \\ &= x^r \cdot \frac{r}{x} = r x^{r-1}. \end{align*}

This is essentially the same method as before, just in slightly different language. However, it's a good way of thinking about it, because writing xrx^r as erln⁡xe^{r \ln x} helps us answer the slightly awkward question: what do we mean by xrx^r, anyway?

When rr can be any real number, xrx^r isn't just "multiplying xx by itself rr times". How would you multiply 22 by itself π\pi times, for instance? We could take several approaches to answering this... but one common approach is to say "in general, xrx^r is just whatever erln⁡xe^{r\ln x} happens to be".

That way, we only need to say what we mean by exe^x (which can be defined, for example, as the limit lim⁡n→∞(1+xn)n\lim_{n\to \infty} \left(1 + \frac{x}{n}\right)^n) and ln⁡x\ln x (which is, of course, just the inverse of exe^x). Or we could say that ln⁡x\ln x is the anti-derivative of 1x\frac{1}{x}, and exe^x is the inverse of that.

Of course, you'd want to check that this definition actually means something reasonable: if we define 23=e3ln⁡22^3 = e^{3 \ln 2}, which is defined in terms of some hairy limits, we want to know that those hairy limits eventually simplify to 2⋅2⋅2=82 \cdot 2 \cdot 2 = 8. But that's another story.

Read · 1 min

The full power rule is as follows.The derivative of b∗axb*a^x with respect to aa, is bxax−1bxa^{x-1}. We can see why this is true when we take a look at the limit definition of a derivative.

f′(a)=f(a+h)−f(a)hf'(a)=\frac{f(a+h)-f(a)}{h} as hh approaches 00, so then the derivative of baxba^x is b(a+h)x−baxh\frac{b(a+h)^x-ba^x}{h} as hh approaches 00.

The first term of b(a+h)xb(a+h)^x is baxba^x, this will go away when we combine with the −bax-ba^x.

Next it will be xbhax−1xbha^{x-1} and then a bunch of other terms. The important thing to realize is that all of the bunch of other terms will have coefficients with a factor of h2h^2 or higher.

Now the hh on the denominator will bring all the h's on the numerator down by a degree of 11. Now the first term is xbax−1xba^{x-1} and all the other terms will have a factor of hh or higher in their coefficients. Since we say h is approaching 00 (we basically just plug in 00 for hh in this step), all other terms except the first will go away (Because multiplying by 00 causes all except the first term, because the first term doesn't have an hh, to be 00).

Thus the derivative is bxax−1bxa^{x-1}.

Read · 1 min

SQUAD first form of PowerRule was used by Bonaventura Cavalieri in the 17 century and was later improved by Newton and Leibniz who was both working individually. The power rule is used in calculus to differentiate functions.

An example of that would be X^2. This function is one of the more simpler ones because it is a monomial. The forumla to find the deriviative of X^2 is nX^n-1. This forumla works for all types of function to find the deriviative.

To solve X^2 we would use nX^n-1 to find its derivative. N is the exponent. The derivative of X^2 is 2X because The exponent would be moved down to in front of X and the exponent would be subtracted by 1.

A more complex function would be 3X^3 + 4X^2 + 9X + 10. Again we would use the formula nX^n-1. The dervaitive of 3X^3 + 4X^2 + 9X + 10 would be 9X^2 + 8X + 9 + 0 because 3X^3,The 3 would be multipled by the number in front of the X and the exponent would be subtracted by 1, ,4X^2,The exponenet would be multipled by the number in front of the X and the exponent subtracted by 1, and same for 9X. The reason why 10 becomes zero because it has no exponents in it. and the exponent of 0 would equals to zero because anything to the 0 power would equal to 0.

Everything in the PowerRule will eventually become 0. This is because as we keep finding the derivative of the dervaitive the exponehnt will be subtracted by 1 and eventually it will hit 0.

Read · 1 min

The power rule is used to distinguish the form of functions f(x) = x^r, whenever r is the real number. The derivative of a power x is equal to the product of exponent times x with the exponent reduced by 1. The exponent lower a value when change into derivative form. For example x^5=5 x^4. The limits is the value that function or sequence approaches the input and reach to some value. Limits are used to define derivatives, integral and continuity. The limit of sequence was to value the sequence of a function

Read · 1 min

Congratulations, you have just learned the Full Power Rule! Now you can do every single problem on here, best of luck!

Video · + 2 min read

(Video) Power Rule with Post-Its

by Grace Carey

This explanation will focus on how to apply the Power Rule in practice. We will focus more on the method than theory, which is covered by other explanations.

Let's begin with the most basic polynomial function: f(x)=xnf\left(x\right)=x^n

Watch the following video and try to come up with the formula for the derivative with respect to x, that is, dfdx\frac{df}{dx}, or f′(x)f'\left(x\right).

Can you guess the formula for the derivative?

Choose one answer

Video · + 1 min read

(Video) Using the Power Rule to Find Derivatives

by PatrickJMT

Here's a video by patrickJMT showing you how to use the power rule to solve derivative instead of that long and annoying definition.

The power rule is really simple. If you have a function raised to a power and want to take the derivative of it you bring the power out front, and then subtract one from the exponent. In other words: f(x)=xa⇒f′(x)=a⋅xa−1f(x)=x^a\Rightarrow f'(x)=a\cdot x^{a-1}

Now let's see this rule in action. The first problem he finds the derivative for is, f(x)=x10f(x)=x^{10} So our first step is to bring the power, 1010, out front. Then we subtract 11 from the exponent. f′(x)=10x10−1=10x9f'(x)=10x^{10-1}=\boxed{10x^9} Easy right!?

Let's try a more complicated example: g(x)=x52+3x+4g(x)=x^{\frac52}+3x+4 So one important rule is if a function is broken up by addition or subtraction you just take the derivative of each piece. So let's start with x52x^{\frac52}. It doesn't matter that there's a fraction, we still apply the same rule. g′(x)=52x52−1+...g′(x)=52x32+...g'(x)=\frac52x^{\frac52-1}+...\\ g'(x)=\frac52x^{\frac32}+... Now we take the derivative of 3x3x. In order to understand what happens its a good idea to picture it as 3x13x^1. g′(x)=52x32+3⋅1x1−1+...g′(x)=52x32+3⋅1x0+...g′(x)=52x32+3⋅1⋅1+...g′(x)=52x32+3+...g'(x)=\frac52x^{\frac32}+3\cdot1x^{1-1}+...\\ g'(x)=\frac52x^{\frac32}+3\cdot1x^{0}+...\\ g'(x)=\frac52x^{\frac32}+3\cdot1\cdot1+...\\ g'(x)=\frac52x^{\frac32}+3+...\\ Finally the derivative of a constant is always zero. So, g′(x)=52x32+3+0g′(x)=52x32+3g'(x)=\frac52x^{\frac32}+3+0\\ \boxed{g'(x)=\frac52x^{\frac32}+3}

Here's one final example that can be a little tricky. h(x)=1x3h(x)=\frac{1}{\sqrt[3]{x}} So when it comes to problems like this, the best way to find the derivative is to rewrite them. Remember we can write roots in the form of a rational exponent. h(x)=1x13h(x)=\frac{1}{x^{\frac13}} Also remember that we can write any exponent in the denominator in the numerator but with a negative sign in front. h(x)=x−13h(x)=x^{-\frac13} So we've successfully rewritten our function into a form that we can take the derivative of using the power rule. Again, just put the power out front and subtract one from the exponent. h′(x)=(−13)x−13−1=−13x−43h'(x)=(-\frac13)x^{-\frac13-1}=-\frac13x^{-\frac43} We can even rewrite this to get into a radical form. h′(x)=−13x43=−13x43h'(x)=-\frac{1}{3x^{\frac43}}=\boxed{-\frac{1}{3\sqrt[3]{x^4}}}

Video · + 1 min read

(Videos) Power Rule and Derivatives

by PatrickJMT

Here's a video by patrickJMT where he goes over some examples of finding the derivative using the power rule.

Recall that the power rule states: f(x)=xa⇒f′(x)=axa−1f(x)=x^a\Rightarrow f'(x)=ax^{a-1}

The first problem he finds the derivative of is: p(q)=−3πq4.1p(q)=-\frac{3}{\pi}\sqrt{q^{4.1}} A good practice is to rewrite any radicals as rational exponents. Also don't be thrown off by the −3π-\frac3{\pi}, this is just a constant. p(q)=−3πq4.12=−3πq2.05\begin{align} p(q)&=-\frac3{\pi}q^{\frac{4.1}{2}}\\ &=-\frac3{\pi}q^{2.05} \end{align} From here we can easily take the derivative. p′(q)=−3π⋅2.05q2.05−1=−6.15πq1.05\begin{align} p'(q)&=-\frac3{\pi}\cdot2.05q^{2.05-1}\\ &\boxed{=-\frac{6.15}{\pi}q^{1.05}} \end{align}

Here's another video with another example of find the derivative using the power rule. The function he looks at this time is: f(x)=2x4+3x53−4xf(x)=2x^4+3x^{\frac53}-\frac4x Another good practice is to pull all exponents in the denominator into the numerator, making them negative. f(x)=2x4+3x53−4x−1f(x)=2x^4+3x^{\frac53}-4x^{-1} Now we can start using the power rule. f′(x)=2(4x4−1)+3(53x53−1)−4(−1x−1−1)=8x3+5x23+4x2\begin{align} f'(x)&=2(4x^{4-1})+3(\frac53x^{\frac53-1})-4(-1x^{-1-1})\\ &=\boxed{8x^3+5x^{\frac23}+\frac4{x^2}} \end{align}

Here's another video where he finds a derivative using the power rule. The problem he looks at this time is:

If f(x)=x+3x+4x3f(x)=x+3\sqrt{x}+4\sqrt[3]{x}, what is f′(64)f'(64)?

As always, the first thing we should do is rewrite our function. f(x)=x+3x12+4x13f(x)=x+3x^{\frac12}+4x^{\frac13} Now we can take the derivative. f′(x)=1+32x−12+43x−23=1+32x12+43x23\begin{align} f'(x)&=1+\frac32x^{-\frac12}+\frac43x^{-\frac23}\\ &=1+\frac{3}{2x^{\frac12}}+\frac{4}{3x^{\frac23}} \end{align}

Now all we have to do is plug in x=64x=64 into our derivative function. f′(64)=1+32(64)12+43(64)23=1+32(8)+43(16)=1+316+112=6148\begin{align} f'(64)&=1+\frac{3}{2\color{red}{(64)}^{\frac12}}+\frac{4}{3\color{red}{(64)}^{\frac23}}\\ &=1+\frac{3}{2(8)}+\frac{4}{3(16)}\\ &=1+\frac{3}{16}+\frac{1}{12}\\ &=\boxed{\frac{61}{48}} \end{align}

Illustrated · 2 min

(Video) Solving Every Derivative Ever

by PatrickJMT

Okay, maybe it's not EVERY derivative ever but here's a video by patrickJMT going over different derivatives for a whopping 35 minutes.

Let's have a season recap of some formulas before we go in. ddxxn=nxn−1ddxcot⁡x=−csc⁡2xddxk=0ddxsec⁡x=sec⁡xtan⁡xddxsin⁡x=cos⁡xddxex=exddxcos⁡x=−sin⁡xddxax=axln⁡addxtan⁡x=sec⁡2xddxln⁡x=1xddxcsc⁡x=−csc⁡xcot⁡xddxlog⁡ax=1xln⁡a\begin{alignat}{2} & \frac{d}{dx}x^n=nx^{n-1} \quad && \frac{d}{dx}\cot x=-\csc^2 x\\ & \frac{d}{dx}k=0 \quad && \frac{d}{dx}\sec x=\sec x \tan x\\ & \frac{d}{dx}\sin x=\cos x \quad && \frac{d}{dx}e^x=e^x\\ & \frac{d}{dx}\cos x=-\sin x \quad && \frac{d}{dx}a^x=a^x\ln a\\ &\frac{d}{dx}\tan x=\sec^2x \quad && \frac{d}{dx}\ln x=\frac1x\\ &\frac{d}{dx}\csc x=-\csc x\cot x \quad &&\frac{d}{dx}\log_ax=\frac1{x\ln a} \end{alignat}

Also let's recap the product, quotient, and chain rule. [f(x)g(x)]′=f′(x)g(x)+f(x)g′(x)[f(x)g(x)]′=f′(x)g(x)−f(x)g′(x)[g(x)]2[f( g(x) )]′=f′( g(x) )⋅g′(x)\begin{align} [f(x)g(x)]'&=f'(x)g(x)+f(x)g'(x)\\ \bigg[\frac{f(x)}{g(x)}\bigg]'&=\frac{f'(x)g(x)-f(x)g'(x)}{[g(x)]^2}\\ [f(\ g(x)\ )]'&=f'(\ g(x)\ )\cdot g'(x) \end{align}

Problem 1

y=x2+3x+4y′=2x2−1+3(1x1−1)+0=2x+3\begin{align} y&=x^2+3x+4\\ y'&=2x^{2-1}+3(1x^{1-1})+0\\ &=\boxed{2x+3} \end{align}

Problem 2

y=5t−23y′=5(−23t−23−1)=−103t−53=−103t53\begin{align} y&=5t^{-\frac23}\\ y'&=5(-\frac23t^{-\frac23-1})\\ &=-\frac{10}3t^{-\frac53}\\ &=\boxed{-\frac{10}{3t^{\frac53}}} \end{align}

Problem 3

y=3x−1x=3x−1x12=3xx12−1x12=3x12−x−12y′=3(12x−12)−(−12x−32)=32x12+12x32=3x+12x32\begin{align} y&=\frac{3x-1}{\sqrt x}\\ &=\frac{3x-1}{x^{\frac12}}\\ &=\frac{3x}{x^{\frac12}}-\frac{1}{x^{\frac12}}\\ &=3x^{\frac12}-x^{-\frac12}\\ y'&=3(\frac12x^{-\frac12})-(-\frac12x^{-\frac32})\\ &=\frac{3}{2x^{\frac12}}+\frac{1}{2x^{\frac32}}\\ &=\boxed{\frac{3x+1}{2x^{\frac32}}} \end{align}

Problem 4

y=(x+4)(x−4)=x2−4x+4x−16=x2−16y′=2x2−1−0=2x\begin{align} y&=(x+4)(x-4)\\ &=x^2-4x+4x-16\\ &=x^2-16\\ y'&=2x^{2-1}-0\\ &=\boxed{2x} \end{align}

Problem 5

y=x−1x+1=x12−1x12+1y′=(x12−1)′(x12+1)−(x12−1)(x12+1)′(x12+1)2=12x−12(x12+1)−(x12−1)(12x−12)(x12+1)2=12x−12[(x12+1)−(x12−1)](x12+1)2=(x12+1)−(x12−1)2x(x12+1)2=22x(x12+1)2=1x(x12+1)2\begin{align} y&=\frac{\sqrt x-1}{\sqrt x+1}\\ &=\frac{x^{\frac12}-1}{x^{\frac12}+1}\\ y'&=\frac{\color{red}{(x^{\frac12}-1)'}(x^{\frac12}+1)-(x^{\frac12}-1)\color{red}{(x^{\frac12}+1)'}}{(x^{\frac12}+1)^2}\\ &=\frac{\frac12x^{-\frac12}(x^{\frac12}+1)-(x^{\frac12}-1)(\frac12x^{-\frac12})}{(x^{\frac12}+1)^2}\\ &=\frac{\frac12x^{-\frac12}[(x^{\frac12}+1)-(x^{\frac12}-1)]}{(x^{\frac12}+1)^2}\\ &=\frac{(x^{\frac12}+1)-(x^{\frac12}-1)}{2\sqrt x(x^{\frac12}+1)^2}\\ &=\frac{2}{2\sqrt x(x^{\frac12}+1)^2}\\ &=\boxed{\frac{1}{\sqrt x(x^{\frac12}+1)^2}} \end{align}

Problem 6

y=2x−x⋅xx2=2x−x32x2=2xx2−x32x2=2x−1x12=2x−1−x−12y′=2(−1x−2)−(−12x32)=12x32−2x2\begin{align} y&=\frac{2x-\sqrt{x}\cdot x}{x^2}\\ &=\frac{2x-x^{\frac32}}{x^2}\\ &=\frac{2x}{x^2}-\frac{x^{\frac32}}{x^2}\\ &=\frac{2}{x}-\frac{1}{x^{\frac12}}\\ &=2x^{-1}-x^{-\frac12}\\ y'&=2(-1x^{-2})-(-\frac12x^{\frac32})\\ &=\boxed{\frac{1}{2x^{\frac32}}-\frac{2}{x^2}} \end{align}

Problem 7

y=(sin⁡x)(x12)y′=(sin⁡x)′(x12)+(sin⁡x)(x12)′=(cos⁡x)(x12)+(sin⁡x)(12x−12)=xcos⁡x+sin⁡x2x\begin{align} y&=(\sin x)(x^{\frac12})\\ y'&=\color{red}{(\sin x)'}(x^{\frac12})+(\sin x)\color{red}{(x^{\frac12})'}\\ &=(\cos x)(x^{\frac12})+(\sin x)(\frac12x^{-\frac12})\\ &=\boxed{\sqrt{x}\cos x+\frac{\sin x}{2\sqrt x}} \end{align}

Problem 8

y=(sin⁡x)(cos⁡x)y′=(sin⁡x)′(cos⁡x)+(sin⁡x)(cos⁡x)=(cos⁡x)(cos⁡x)+(sin⁡x)(−sin⁡x)=cos⁡2x−sin⁡2x=cos⁡(2x)\begin{align} y&=(\sin x)(\cos x)\\ y'&=\color{red}{(\sin x)'}(\cos x)+(\sin x)\color{red}{(\cos x)}\\ &=(\cos x)(\cos x)+(\sin x)(-\sin x)\\ &=\cos^2x-\sin^2x\\ &=\boxed{\cos(2x)} \end{align}

Problem 9

y=sin⁡(cos⁡x)y′=cos⁡(cos⁡x)⋅[cos⁡x]′=cos⁡(cos⁡x)⋅(−sin⁡x)=−sin⁡xcos⁡(cos⁡x)\begin{align} y&=\sin(\cos x)\\ y'&=\cos(\cos x)\cdot\color{red}{[\cos x]'}\\ &=\cos(\cos x)\cdot(-\sin x)\\ &=\boxed{-\sin x\cos(\cos x)} \end{align}

Problem 10

y=sec⁡[(1+x2)12]y′=sec⁡[(1+x2)12]⋅tan⁡[(1+x2)12]⋅[(1+x2)12]′=sec⁡[(1+x2)12]⋅tan⁡[(1+x2)12]⋅12(1+x2)−12⋅(1+x2)′=sec⁡[(1+x2)12]⋅tan⁡[(1+x2)12]⋅12(1+x2)−12⋅(2x)=xsec⁡[(1+x2)12]tan⁡[(1+x2)12]1+x2\begin{align} y&=\sec[(1+x^2)^{\frac12}]\\ y'&=\sec[(1+x^2)^{\frac12}]\cdot\tan[(1+x^2)^{\frac12}]\cdot\color{red}{[(1+x^2)^{\frac12}]'}\\ &=\sec[(1+x^2)^{\frac12}]\cdot\tan[(1+x^2)^{\frac12}]\cdot\frac12(1+x^2)^{-\frac12}\cdot\color{red}{(1+x^2)'}\\ &=\sec[(1+x^2)^{\frac12}]\cdot\tan[(1+x^2)^{\frac12}]\cdot\frac12(1+x^2)^{-\frac12}\cdot(2x)\\ &=\boxed{\frac{x\sec[(1+x^2)^{\frac12}]\tan[(1+x^2)^{\frac12}]}{\sqrt{1+x^2}}} \end{align}

Problem 11

y=tan⁡2[sin⁡(θ3)]y′=2tan⁡[sin⁡(θ3)]⋅[ tan⁡[sin⁡(θ3)] ]′=2tan⁡[sin⁡(θ3)]⋅sec⁡2[sin⁡(θ3)]⋅[sin⁡(θ3)]′=2tan⁡[sin⁡(θ3)]⋅sec⁡2[sin⁡(θ3)]⋅cos⁡(θ3)⋅(θ3)′=2tan⁡[sin⁡(θ3)]⋅sec⁡2[sin⁡(θ3)]⋅cos⁡(θ3)⋅3θ2=6θ2tan⁡[sin⁡(θ3)]sec⁡2[sin⁡(θ3)]cos⁡(θ3)\begin{align} y&=\tan^2[\sin(\theta^3)]\\ y'&=2\tan[\sin(\theta^3)]\cdot\color{red}{[\ \tan[\sin(\theta^3)]\ ]'}\\ &=2\tan[\sin(\theta^3)]\cdot\sec^2[\sin(\theta^3)]\cdot\color{red}{[\sin(\theta^3)]'}\\ &=2\tan[\sin(\theta^3)]\cdot\sec^2[\sin(\theta^3)]\cdot\cos(\theta^3)\cdot\color{red}{(\theta^3)'}\\ &=2\tan[\sin(\theta^3)]\cdot\sec^2[\sin(\theta^3)]\cdot\cos(\theta^3)\cdot3\theta^2\\ &=\boxed{6\theta^2\tan[\sin(\theta^3)]\sec^2[\sin(\theta^3)]\cos(\theta^3)} \end{align}

Problem 12

y=xsin⁡(3x−1)y′=(x)′[sin⁡(3x−1)]+(x)[sin⁡(3x−1)]′=(1)sin⁡(3x−1)+(x)cos⁡(3x−1)⋅(3x−1)′=sin⁡(3x−1)+(x)cos⁡(3x−1)⋅3(−1x−2)=sin⁡(3x−1)−3xcos⁡(3x−1)x2=sin⁡(3x)−3cos⁡(3x)x=xsin⁡(3x)−3cos⁡(3x)x\begin{align} y&=x\sin(3x^{-1})\\ y'&=\color{red}{(x)'}[\sin(3x^{-1})]+(x)\color{red}{[\sin(3x^{-1})]'}\\ &=(1)\sin(3x^{-1})+(x)\cos(3x^{-1})\cdot\color{red}{(3x^{-1})'}\\ &=\sin(3x^{-1})+(x)\cos(3x^{-1})\cdot3(-1x^{-2})\\\\ &=\sin(3x^{-1})-\frac{3x\cos(3x^{-1})}{x^{2}}\\ &=\sin(\frac3x)-\frac{3\cos(\frac3x)}{x}\\ &=\boxed{\frac{x\sin(\frac3x)-3\cos(\frac3x)}{x}} \end{align}

Problem 13

y=(x3+4)2(x2+1)4y′=[(x3+4)2]′(x2+1)4−(x3+4)2[(x2+1)4]′[(x2+1)4]2=2(x3+4)(x3+4)′(x2+1)4−4(x3+4)2(x2+1)3(x2+1)′(x2+1)8=6x2(x3+4)(x2+1)4−8x(x3+4)2(x2+1)3(x2+1)8=6x2(x3+4)(x2+1)4−8x(x3+4)2(x2+1)3(x2+1)8=2x(x3+4)(x2+1)3[3x(x2+1)−4(x3+4)](x2+1)8=2x(x3+4)[3x(x2+1)−4(x3+4)](x2+1)5=2x(x3+4)[(3x3+3x)−(4x3+16)](x2+1)5=2x(x3+4)(−x3+3x−16)(x2+1)5\begin{align} y&=\frac{(x^3+4)^2}{(x^2+1)^4}\\ y'&=\frac{\color{red}{[(x^3+4)^2]'}(x^2+1)^4-(x^3+4)^2\color{red}{[(x^2+1)^4]'}}{[(x^2+1)^4]^2}\\ &=\frac{2(x^3+4)\color{red}{(x^3+4)'}(x^2+1)^4-4(x^3+4)^2(x^2+1)^3\color{red}{(x^2+1)'}}{(x^2+1)^8}\\ &=\frac{6x^2(x^3+4)(x^2+1)^4-8x(x^3+4)^2(x^2+1)^3}{(x^2+1)^8}\\ &=\frac{6x^2(x^3+4)(x^2+1)^4-8x(x^3+4)^2(x^2+1)^3}{(x^2+1)^8}\\ &=\frac{2x(x^3+4)(x^2+1)^3[3x(x^2+1)-4(x^3+4)]}{(x^2+1)^8}\\ &=\frac{2x(x^3+4)[3x(x^2+1)-4(x^3+4)]}{(x^2+1)^5}\\ &=\frac{2x(x^3+4)[(3x^3+3x)-(4x^3+16)]}{(x^2+1)^5}\\ &=\boxed{\frac{2x(x^3+4)(-x^3+3x-16)}{(x^2+1)^5}} \end{align}

Problem 14

y=ln⁡(x)+x3y′=1x+3x2=3x3+1x\begin{align} y&=\ln(x)+x^3\\ y'&=\frac1x+3x^2\\ &=\boxed{\frac{3x^3+1}{x}} \end{align}

Problem 15

y=x2exy′=(x2)′ex+x2(ex)′=2xex+x2ex=xex(x+2)\begin{align} y&=x^2e^x\\ y'&=\color{red}{(x^2)'}e^x+x^2\color{red}{(e^x)'}\\ &=2xe^x+x^2e^x\\ &=\boxed{xe^x(x+2)} \end{align}

Problem 16

y=et⋅cos⁡(2t)y′=et⋅cos⁡(2t)⋅[t⋅cos⁡(2t)]′=et⋅cos⁡(2t)⋅[(t)′cos⁡(2t)+t[cos⁡(2t)]′]=et⋅cos⁡(2t)⋅[cos⁡(2t)−tsin⁡(2t)⋅(2t)′]=et⋅cos⁡(2t)⋅[cos⁡(2t)−2tsin⁡(2t)]\begin{align} y&=e^{t\cdot\cos(2t)}\\ y'&=e^{t\cdot\cos(2t)}\cdot\color{red}{[t\cdot\cos(2t)]'}\\ &=e^{t\cdot\cos(2t)}\cdot[\color{red}{(t)'}\cos(2t)+t\color{red}{[\cos(2t)]'}]\\ &=e^{t\cdot\cos(2t)}\cdot[\cos(2t)-t\sin(2t)\cdot\color{red}{(2t)'}]\\ &=\boxed{e^{t\cdot\cos(2t)}\cdot[\cos(2t)-2t\sin(2t)]} \end{align}

Problem 17

y=cos⁡(eπx)y′=−sin⁡(eπx)⋅(eπx)′=−sin⁡(eπx)⋅eπx(πx)′=−πeπxsin⁡(eπx)\begin{align} y&=\cos(e^{\pi x})\\ y'&=-\sin(e^{\pi x})\cdot\color{red}{(e^{\pi x})'}\\ &=-\sin(e^{\pi x})\cdot e^{\pi x}\color{red}{(\pi x)'}\\ &=\boxed{-\pi e^{\pi x}\sin(e^{\pi x})} \end{align}

Problem 18

y=(1+2e3x)12y′=12(1+2e3x)−12⋅(1+2e3x)′=12(1+2e3x)−12⋅2e3x⋅(3x)′=3e3x1+2e3x\begin{align} y&=(1+2e^{3x})^{\frac12}\\ y'&=\frac12(1+2e^{3x})^{-\frac12}\cdot\color{red}{(1+2e^{3x})'}\\ &=\frac12(1+2e^{3x})^{-\frac12}\cdot2e^{3x}\cdot\color{red}{(3x)'}\\ &=\boxed{\frac{3e^{3x}}{\sqrt{1+2e^{3x}}}} \end{align}

Problem 19

y=5−1x=5−x−1y′=5−x−1⋅ln⁡5⋅(−x−1)′=5−x−1⋅ln⁡5⋅(x−2)=ln⁡551xx2\begin{align} y&=5^{-\frac1x}\\ &=5^{-x^{-1}}\\ y'&=5^{-x^{-1}}\cdot\ln5\cdot\color{red}{(-x^{-1})'}\\ &=5^{-x^{-1}}\cdot\ln5\cdot(x^{-2})\\ &=\boxed{\frac{\ln5}{5^{\frac1x}x^2}} \end{align}

Problem 20

y=ln⁡(x4sin⁡2x)y′=1x4sin⁡2x⋅[x4sin⁡2x]′=1x4sin⁡2x⋅[(x4)′sin⁡2x+x4(sin⁡2x)′]=4x3sin⁡2x+2x4sin⁡x⋅(sin⁡x)′x4sin⁡2x=4x3sin⁡2x+2x4sin⁡xcos⁡xx4sin⁡2x=2x3sin⁡x(2sin⁡x+xcos⁡x)x4sin⁡2x=2(2+xcos⁡x)xsin⁡x=4x+2cot⁡x\begin{align} y&=\ln(x^4\sin^2x)\\ y'&=\frac{1}{x^4\sin^2x}\cdot\color{red}{[x^4\sin^2x]'}\\ &=\frac{1}{x^4\sin^2x}\cdot[\color{red}{(x^4)'}\sin^2x+x^4\color{red}{(\sin^2x)'}]\\ &=\frac{4x^3\sin^2x+2x^4\sin x\cdot\color{red}{(\sin x)'}}{x^4\sin^2x}\\ &=\frac{4x^3\sin^2x+2x^4\sin x\cos x}{x^4\sin^2x}\\ &=\frac{2x^3\sin x(2\sin x+x\cos x)}{x^4\sin^2x}\\ &=\frac{2(2+x\cos x)}{x\sin x}\\ &=\boxed{\frac4x+2\cot x} \end{align}

Problem 21

y=ln⁡5x−12x+3=ln⁡(5x−12x+3)12=12[ln⁡(5x−12x+3)]=12[ln⁡(5x−1)−ln⁡(2x+3)]y′=12[15x−1⋅(5x−1)′−12x+3⋅(2x+3)′]=12[55x−1−22x+3]=12[5(2x+3)−2(5x−1)(5x−1)(2x+3)]=12[10x+15−−10x+210x2+13x−3]=12[1710x2+13x−3]=1720x2+26x−6\begin{align} y&=\ln\sqrt{\frac{5x-1}{2x+3}}\\ &=\ln\bigg(\frac{5x-1}{2x+3}\bigg)^{\frac12}\\ &=\frac12\bigg[\ln\bigg(\frac{5x-1}{2x+3}\bigg)\bigg]\\ &=\frac12[\ln(5x-1)-\ln(2x+3)]\\ y'&=\frac12[\frac{1}{5x-1}\cdot\color{red}{(5x-1)'}-\frac{1}{2x+3}\cdot\color{red}{(2x+3)'}]\\ &=\frac12\bigg[\frac{5}{5x-1}-\frac{2}{2x+3}\bigg]\\ &=\frac12\bigg[\frac{5(2x+3)-2(5x-1)}{(5x-1)(2x+3)}\bigg]\\ &=\frac12\bigg[\frac{10x+15--10x+2}{10x^2+13x-3}\bigg]\\ &=\frac12\bigg[\frac{17}{10x^2+13x-3}\bigg]\\ &=\boxed{\frac{17}{20x^2+26x-6}} \end{align}

Problem 22

y=t3−3ty′=3t2−3t⋅ln⁡3=3t2−3tln⁡3\begin{align} y&=t^3-3^t\\ y'&=3t^2-3^t\cdot\ln3\\ &=\boxed{3t^2-3^t\ln3} \end{align}

Problem 23

y=ln⁡(sec⁡x+tan⁡x)y′=1sec⁡x+tan⁡x⋅[sec⁡x+tan⁡x]′=1sec⁡x+tan⁡x⋅[sec⁡x⋅tan⁡x+sec⁡2x]=sec⁡xtan⁡x+sec⁡2xsec⁡x+tan⁡x\begin{align} y&=\ln(\sec x+\tan x)\\ y'&=\frac{1}{\sec x+\tan x}\cdot\color{red}{[\sec x+\tan x]'}\\ &=\frac{1}{\sec x+\tan x}\cdot[\sec x\cdot\tan x+\sec^2x]\\ &=\boxed{\frac{\sec x\tan x+\sec^2x}{\sec x+\tan x}} \end{align}

Problem 24

y=log⁡10(2xx−1)=log⁡10(2x)−log⁡10(x−1)y′=12xln⁡10⋅(2x)′−1(x−1)ln⁡10⋅(x−1)′=22xln⁡10−1(x−1)ln⁡10=1xln⁡10−1(x−1)ln⁡10\begin{align} y&=\log_{10}\bigg(\frac{2x}{x-1}\bigg)\\ &=\log_{10}(2x)-\log_{10}(x-1)\\ y'&=\frac{1}{2x\ln10}\cdot\color{red}{(2x)'}-\frac{1}{(x-1)\ln10}\cdot\color{red}{(x-1)'}\\ &=\frac{2}{2x\ln10}-\frac{1}{(x-1)\ln10}\\ &=\boxed{\frac{1}{x\ln10}-\frac{1}{(x-1)\ln10}} \end{align}

Problem 25

y=ln⁡xx2y′=(ln⁡x)′(x2)−(ln⁡x)(x2)′[x2]2=1x(x2)−2x(ln⁡x)x4=x−2x(ln⁡x)x4=1−2ln⁡xx3\begin{align} y&=\frac{\ln x}{x^2}\\ y'&=\frac{\color{red}{(\ln x)'}(x^2)-(\ln x)\color{red}{(x^2)'}}{[x^2]^2}\\ &=\frac{\frac1x(x^2)-2x(\ln x)}{x^4}\\ &=\frac{x-2x(\ln x)}{x^4}\\\\ &=\boxed{\frac{1-2\ln x}{x^3}} \end{align}

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