The Transformations of Trig Functions section covers:
 TCharts for the Six Trigonometric Functions
 Sine and Cosine Transformations
 Sinusoidal Applications
 Secant and Cosecant Transformations
 Tangent and Cotangent Transformations
 Transformations of all Trig Functions without TCharts
 More Practice
We learned how to transform Basic Parent Functions here in the Parent Functions and Transformations section. Now we will transform the six Trigonometric Functions. Later we’ll be transforming the Inverse Trig Functions here. Some prefer to do all the transformations with tcharts like we did earlier, and some prefer it without tcharts (see here and here); most of the examples will show tcharts.
TCharts for the Six Trigonometric Functions
Here are the trig parent function tcharts I like to use (starting and stopping points may be changed, as long as they cover a cycle). Note that each covers one period (one complete cycle of the graph before it starts repeating itself) for each function. Also note that “undef” means the function is undefined for that \(x\) value; there is a vertical asymptote there.
Note also that when the original functions (like sin, cos, and tan) have 0’s as \(y\) values, their respective reciprocal functions are undefined at those points (because of division of 0).
Trig Function TCharts  
\(y=\sin \left( x \right)\)

\(y=\cos \left( x \right)\)

\(y=\tan \left( x \right)\)

\(y=\csc \left( x \right)\)

\(y=\sec \left( x \right)\)

\(y=\cot \left( x \right)\)

Sin and Cos Transformations
Here’s a general formula in order to transform a sin or cos function, as well as the remaining four trig functions. Note that sometimes you’ll see the formula arranged differently; for example, with “\(a\)” being the vertical shift at the beginning.
Trig Transformation Formula 
Explanation 
\(\begin{array}{l}y=a\sin b\left( {xc} \right)+d\\\\\\y=a\cos b\left( {xc} \right)+d\end{array}\)
Others:
\(\begin{array}{l}y=a\csc b\left( {xc} \right)+d\\y=a\sec b\left( {xc} \right)+d\\y=a\tan b\left( {xc} \right)+d\\y=a\cot b\left( {xc} \right)+d\end{array}\)

\(\boldsymbol{\left a \right=}\) the amplitude.
This is how far up and down the graph goes from the middle: think “stretch” if \(a>1\) or “compression” if \(a<1\)). Without a shift, \(a=1\) (thus the sin and cos graphs go from \(y=1\) to \(y=1\), with the middle at \(y=0\). (Note that the “\(a\)” is only called an amplitude for sin and cos graphs; otherwise it’s considered a “stretch” or “compression”). For the sin and cos graphs, the amplitude is the highest \(y\) value minus the lowest \(y\) value, divided by 2. If there is a negative sign before the \(a\), the graph is flipped across the \(\boldsymbol{x}\)axis.
\(\boldsymbol{b=}\) the number of times the graph will repeat itself in the “normal” period, which is \(2\pi\) for sin, cos, csc, and sec, and \(\pi\) for tan and cot. Remember that the period is the length (\(x\)–value difference) of one complete cycle of the graph (sometimes called a frequency). It follows for the sin, cos, csc, and sec graphs that \(\displaystyle b=\frac{{2\pi }}{{\text{new period}}}\) and \(\displaystyle \text{new period}=\frac{{2\pi }}{b}\). (Normally, \(b=1\), which means that the period of the graph is \(\displaystyle b=\frac{{2\pi }}{\text{1}}=2\pi \).) For tan and cot, since normally the period is \(\pi\), we have: \(\displaystyle b=\frac{\pi }{{\text{new period}}}\) and \(\displaystyle \text{new period}=\frac{\pi }{b}\). .
\(\boldsymbol{c=}\) the horizontal shift or phase shift of the graph. Notice that it’s on the inside of the parentheses; this shifts a graph horizontally and when \(c\) is subtracted from \(\boldsymbol{x}\), it shifts to the right (opposite of what we’d think; we saw this with nontrig transformations). Normally, \(c=0\).
\(\boldsymbol{d=}\) the vertical shift of the graph (sometimes called a bias) Notice that it’s on the outside of the parentheses; this shifts a graph vertically in the direction we would think it would (positive \(d\) moves the graph higher). Normally, \(d=0\). 
Drawing Transformed Graphs for Sin and Cos
Here are some examples, first with the sin function, and then the cos (the rest of the trig functions will be addressed later). You will probably be asked to sketch one complete cycle for each graph, label significant points, and list the Domain, Range, Period and Amplitude for each graph.
Transforming Without Using tcharts (more, including examples, here)
Many teachers teach trig transformations without using tcharts; here is how you might do that for sin and cosine:
Since we get can get the new period of the graph (how long it goes before repeating itself), by using \(\displaystyle \frac{2\pi }{b}\), and we know the phase shift, we can graph key points, and then draw the curve based on whether it is sin or cosine, and positive or negative. We can use 5 key points for a whole period of a graph.
Let’s use the example \(\displaystyle y=2\cos \left( {\frac{1}{3}\left( {x\frac{\pi }{2}} \right)} \right)+1\) that we did above, without using a \(t\)chart.
 We see that the graph is centered at \(y=1\), because of the vertical shift. From here we go up 2 and down 2 so the \(y\) part of the graph goes from –1 to 3.
 The first (leftmost) point is \(\displaystyle \frac{\pi }{2}\) to the right, and it is “upside down” for cosine (because of the negative sign before the 2), so it will be 2 units down from the middle of the graph, which is \(y=1\). This point is \(\displaystyle \left( {\frac{\pi }{2},1} \right)\). (Without the negative, the point would be \(\displaystyle \left( {\frac{\pi }{2},3} \right)\)).
 Since the period is \(6\pi \), the middle point is \(3\pi \) farther than the start at \(\displaystyle \frac{\pi }{2}\), so the next (highest) point is at \(\displaystyle \left( {\frac{\pi }{2}+3\pi ,3} \right)=\left( {\frac{{7\pi }}{2},3} \right)\). The last (rightmost) point is again at the lowest \(y\) point at \(\displaystyle \left( \frac{7\pi }{2}+3\pi ,1 \right)=\left( \frac{13\pi }{2},1 \right)\).
 The intermediate points will be halfway in between each 2 of the 3 points that we just found. To get the point between \(\displaystyle \left( \frac{\pi }{2},1 \right)\) and \(\displaystyle \left( {\frac{{7\pi }}{2},3} \right)\), we take the average of the \(x\) values and the \(y\) again to get \(\left( 2\pi ,1 \right)\). We do the same thing for the point between \(\displaystyle \left( {\frac{{7\pi }}{2},3} \right)\) and \(\displaystyle \left( {\frac{{13\pi }}{2},1} \right)\) to get \(\left( 5\pi ,1 \right)\). Now we have the 5 points and we can draw the graph!
Note that some teachers may have you use a method that looks at the zeros of the sin and cosine functions. For the sin graph, we know the zeros are at \(0,\,\pi ,2\pi \), and so on \((\pi k)\), and for the cosine graphs, the zeros are at \(\displaystyle \frac{\pi }{2},\,\,\frac{\pi }{2}\) and so on (\(\displaystyle \frac{\pi }{2}+\pi k\)). We can set the arguments (what comes after the sin or cosine) to this value, and solve for the new “\(x\)” to get our key points, with the new “\(y\)” being any vertical shift.
Writing Equations from Transformed Graphs for Sin and Cos
You may be asked to write trig function equations, given transformed graphs. (Writing equations from trig functions other than sin and cos may be found here).
Here are the steps to do this; examples will follow.
 Write out the generic transformed Equation for sin or cos: \(y=a\sin b\left( xc \right)+d\) or \(y=a\cos b\left( xc \right)+d\). To determine if it is a sin graph or a cos graph, see if the graph seems to peak at the \(y\)axis (cos graph), or have the (horizontal) middle closest to the \(y\)axis (sin graph). Note that the graph may appear flipped across the \(x\)axis, but, by shifting the graph to the left or right, you may not have to write the equation as a flipped function (with a negative).
 Find the amplitude (\(a\)) of the transformed function by subtracting the bottom \(y\) value from the top \(y\) value, and then dividing by 2. (Remember that for the csc, sec, tan, and cot graphs, this is just called a “stretch”, not an amplitude.)
 To get \(d\), or the vertical shift of the function, we add the amplitude to the bottom \(y\) value. Notice that this is the \(y\) value for the middle of the function (the “average” of the bottom \(y\) and the top \(y\)); we also can just observe this from the graph.
 To get \(b\): First find the period of the graph: see how long it goes before repeating itself, then subtract the two \(x\) values to get this new period. For example, if it “starts” at \(\pi \) and then starts repeating itself again at \(5\pi \) (a complete revolution), its period is \(4\pi \). Once you get this period, \(\displaystyle b=\frac{2\pi }{\text{new period}}\). In our example, \(b\) would be \(\displaystyle \frac{2\pi }{4\pi }=\frac{1}{2}\). (Remember that for the tan and cot graphs, \(\displaystyle b=\frac{\pi }{\text{new period}}\)).
 Find the phase shift of the graph by seeing how close it is to the \(y\) axis (\(x=0\)); this value is \(c\). You can actually write the graph as a cos graph or a sin graph; both will be correct, depending on what \(c\) is, but you typically want \(c\) to be the smallest it can be. Look at the \(x\) value of the \(y\) high point for cos (since cos typically starts at \(y=1\)), or middle point of graph for sin (since sin typically starts at \(y=0\)), and compare to \(x=0\). Since the formula has “\(xc\)” in it, if the graph is to the right of where it should be, \(c\) is positive; if it is to the left of where it should be, \(c\) is negative.
 Check your equation in the graphing calculator by setting the \(x\) window exactly to the leftmost point of the graph (Xmin) and to the rightmost point of the graph (Xmax). Similarly, set the \(y\) window to the lowest point on the graph (Ymin) and to the highest point on the graph (Ymax). When you graph, you should see the exact graph for that problem.
Here are some examples; note that answers may vary:
Graph  Steps to Get Equation 
1. Since the top of the graph is close to the \(y\)axis, we will use the positive cos function: \(y=a\cos b\left( {xc} \right)+d\).
2. To get the amplitude, or \(a\), we’ll subtract the lowest \(y\) point from the highest, and then divide by 2: \(2\left( {10} \right)=12\div 2=6\). So now we have \(y=6\cos b\left( {xc} \right)+d\).
3. To get the middle of the function, or the vertical shift (\(d\)), we add the amplitude to the lowest \(y\) value: \(–10+6=–4\). We can also see from the graph that the middle of the graph is at \(y=4\). So now we have \(y=6\cos b\left( {xc} \right)4\).
4. To get \(b\), we first find the period of the graph by seeing how long it goes before repeating itself (we can subtract the two \(x\) values to get this new period). We can see that the graph repeats half of a complete revolution from when \(x=100\) to when \(x=900\). So half a revolution is \(900100=800\), so a complete revolution is \(1600\). Then we use the equation \(\displaystyle b=\frac{{2\pi }}{{\text{new period}}}=\frac{{2\pi }}{{1600}}=\frac{\pi }{{800}}\). So now we have \(\displaystyle y=6\cos \frac{\pi }{{800}}\left( {xc} \right)4\).
5. To find the phase shift of the graph, let’s see how close it is to the \(y\)axis \((x=0)\); this value is \(c\). Since the top of the graph is closest to the \(y\)axis, and it’s a little bit to the right (100 to the right), we have a cos graph with an \(“xc”\) situation. So \(c=100\), and the graph is \(\displaystyle y=6\cos \frac{\pi }{{800}}\left( {x100} \right)4\).
6. See the screens on the left to see how we can check this half revolution of the graph in a graphing calculator – looks good! (Note that to enter \(\displaystyle \frac{\pi }{{800}}\), I used “alpha” “Y=” “n/d” in order to input this fraction in fraction mode). 
Sinusoidal Applications
Uh oh – more word problems! These aren’t too bad, once you get the hang of them. And now that you know how to transform sin and cos functions, that’s really all we’re doing here.
A sinusoidal function, or sinusoid is a fancy name for the sin (or cos) waves that we’ve been working with. Sinusoids are quite useful in many scientific fields; sine waves are everywhere!
With sinusoidal applications, you’ll typically have to decide between using a sin graph or a cos graph. Sometimes it helps to remember that the sin graphs start in the middle of the graph, and the cos graphs start at the top of the graph. Also, sometimes, the graphs will be “upside down” which means you might need to reflect the sin or cos (using a negative coefficient).
Let’s just start with an example, and see the steps:
Roller Coaster Problem:
A part of the track of a roller coaster has the shape of a sinusoidal function.
The highest and lowest points on the roller coaster are 150 feet apart horizontally and 100 feet apart vertically. The lowest point of the roller coaster was actually built 10 feet below the ground.
Let \(y=\) the height of the track (with \(y=0\) as the ground), and \(x=\) the number of feet horizontally, with \(x=0\) at the highest point of the track.
(a) Write the sinusoidal equation of this part of the track of the roller coaster.
(b) How high is the highest point of the roller coaster? How high is the coaster at \(x=\) 15 feet? 100 feet?
(c) How long (horizontally) is the roller coaster when the track is 75 feet above the ground? 15 feet above the ground?
Solution:
(a) Let’s get the equation with these steps:
 Graph the function’s high points and low points, and figure out the coordinates of these points, given what we know. Since the track is 100 feet tall, and the lowest point is at \(y=10\), we know the highest point is at \((0,10010)=(0,90)\) (since the highest point is when \(x=0\)). Since the horizontal distance between the highest point and lowest point is 150, the lowest point is at \((150,10)\). So here’s what we can graph:
 We’ll use a cos graph, since the highest point of the graph is on the \(y\)axis: \(y=a\cos b\left( xc \right)+d\).
 To get the amplitude, or \(a\), we’ll subtract the lowest \(y\) point from the highest, and then divide by 2. So \(a=90\left( 10 \right)=100\div 2=50\). Now we have \(y=50\cos b\left( xc \right)+d\).
 To get the middle of the function, or the vertical shift (\(d\)), we add the amplitude to the lowest \(y\) value: \(10+50=40\). (We could also have just taken the average of 90 and –10). So now we have \(y=50\cos b\left( xc \right)+40\).
 To get the period of the graph, we know that the horizontal distance between the highest point and the lowest point is one half of a period. So the period of the graph is \(\left( 2 \right)\left( {150} \right)=300\) feet. Now to get \(b\), we have \(\displaystyle b=\frac{2\pi }{\text{new period}}=\frac{2\pi }{300}=\frac{\pi }{150}\). So now we have \(\displaystyle y=50\cos \frac{\pi }{150}\left( xc \right)+40\).
 Since the highest point is on the \(y\)axis (\(x=0\)), there is no horizontal phase shift. Thus the sinusoidal function is \(\displaystyle y=50\cos \frac{\pi }{150}x+40\). We could put it in a graphing calculator to check it.
(b) At the highest point, the roller coaster is 90 feet above the ground (\(\displaystyle y=50\cos \left( \frac{\pi }{150}*0 \right)+40=90\)). At \(x=15\) feet, the roller coaster is \(\displaystyle y=50\cos \left( \frac{\pi }{150}*15 \right)+40\), or 87.55 feet tall. At \(x=100\) feet, the roller coaster is \(\displaystyle y=50\cos \left( \frac{\pi }{150}*100 \right)+40\), or 15 feet tall. It’s easiest to put the function \(y=50\cos \frac{\pi }{{150}}x+40\) in the graphing calculator, and use the 2^{nd} TRACE (CALC) value function to get these values (see the WINDOW you can use below).
(c) When the track is 75 feet above the ground, \(y=75\). The easiest way to get the \(x\) at that point is to use the Intersect feature in the graphing calculator: (2^{nd} Trace (Calc), 5, ENTER, ENTER, ENTER). So when the track is 75 feet above the ground, the roller coaster is about 37.98 feet from the highest point at \(x=0\). Note the window I used to match the graph of the roller coaster.
You can use the same steps to see that when the roller coaster track is 15 feet above the ground, the roller coaster is 100 feet from the beginning point.
Bouncing Spring Problem:
The weight on a long spring bounces up and down sinusoidally with time. You are looking at a second hand on a clock and notice that when the clock reads .2 seconds, the weight first reaches a high point that is 50 centimeters (cm) above the ground. The next low point is at 30 cm above the ground, and this occurs at 1.5 seconds.
(a) Draw the graph that represents this situation, and write the sinusoidal equation that expresses the distance from the ground in terms of the numbers of seconds that has passed.
(b) What would be the approximate distance from the ground when the clock reads 18 seconds?
(c) What is the approximate distance from the ground when the clock was at \(t=\) 0 seconds?
(d) What would be the first positive value for the time when the weight is 45 cm above the ground?
Solution: (a) Let’s get the equation with these steps:
 Graph the function’s high points and low points, and figure out the coordinates of these points, given what we know. Since the high point is at 50 cm at .2 sec, we know the high point is at \((.2,50)\). We also know that the low point is at \((1.5,30)\). So here’s what we can graph:We’ll use a cos graph again, since the highest point of the graph is on the \(y\)axis: \(y=a\cos b\left( xc \right)+d\).
 To get the amplitude, or \(a\), we’ll subtract the lowest \(y\) point from the highest, and then divide by 2. So \(50\left( {30} \right)=20\div 2=10\).
 So now we have \(y=10\cos b\left( xc \right)+d\).
 To get the middle of the function, or the vertical shift (\(d\)), we add the amplitude to the lowest \(y\) value: \(30+10=40\). (We could also just taken the average of 30 and 50). So now we have \(y=10\cos b\left( xc \right)+40\).
 To get the period of the graph, we know that the horizontal distance between the highest point and the lowest point is one half of a period. So the period of the graph is \((1.52)(2)=2.6\) cm. Now to get \(b\), we have \(\displaystyle b=\frac{2\pi }{\text{new period}}=\frac{2\pi }{2.6}=\frac{10\pi }{13}\). So now we have \(\displaystyle y=10\cos \frac{10\pi }{13}\left( xc \right)+40\).
 Since the highest point is at \(x=.2\), the horizontal phase shift is .2 to the right. Thus \(c=.2\). The sinusoidal function is then \(\displaystyle y=10\cos \frac{10\pi }{13}\left( x.2 \right)+40\). We could put it in a graphing calculator to check it.
(b) When the clock reads 18 seconds, we can plug in 18 for \(x\) to get \(y\) (the distance from the ground): \(\displaystyle y=10\cos \frac{10\pi }{13}\left( 18.2 \right)+40\), which is about 45.68 cm. This is after many bounces, as you could see if you graphed the function and made the window of \(x\) larger.
(c) The approximate distance from the ground when the clock is at \(t=0\) seconds is \(\displaystyle y=10\cos \frac{10\pi }{13}\left( 0.2 \right)+40=48.85\) cm.
(d) Let’s use the graphing calculator to find the first positive value when the weight is 45 cm above the ground. After you hit GRAPH, you may have to use the TRACE button to get the cursor closer to the first point of intersection before you use intersect. This value is approximately .63 seconds:
Tidal Problem:
Let’s do one more, where we’ll use a sin function:
A tsunami or tidal wave is an ocean wave caused by an earthquake. The water first goes down from its normal level and then rises an equal distance above its normal level, and so on. Let’s say the amplitude for this particular tsunami is 12 meters, it’s period is about 20 minutes, and it’s normal depth is 10 meters. Assuming the depth of the water varies sinusoidally with time, find the sinusoidal function for this tsunami.
Solution: Let’s first draw a graph, assuming that the water is at its regular depth when \(t=0\), and then goes down to its lowest point, and then up to its highest point. (Notice that the water technically goes below the surface of the ocean; we won’t worry about the scientific consequences of this.)
We know the lowest point is at 5 minutes, and the period is 20 minutes, we can figure out that the highest point is at half the distance of the period (10 minutes) from that lowest point. So we can plot the following points and draw the graph:
Now for this graph, we will use the sin function since the middle of the function goes through the \(y\)axis (\(x=0\)). But notice how the graph is flipped, so we will use –sin.
We are already given the amplitude (12 meters), vertical shift (normal depth is at 10 meters), and period (20 minutes), so \(\displaystyle b=\frac{2\pi }{\text{new period}}=\frac{2\pi }{20}=\frac{\pi }{10}\). There is no horizontal phase shift, so the sinusoidal function is \(\displaystyle y=12\sin \frac{\pi }{10}x+10\).
Secant and Cosecant Transformations
The reciprocal functions secant (sec) and cosecant (csc) are transformed the same way as the sin and cos, yet the “\(a\)” part of the transformation is not called an amplitude, but a stretch, as we are used to with “regular” transformed functions.
Remember, again, like the sin and cos transformations, the \(\displaystyle \text{new period}=\frac{{2\pi }}{b}\). If asked for asymptotes of transformed functions, you’ll perform the same transformations on them as you would the \(x\) values of the graph.
You can look at one of the new asymptotes of the transformed graph, and then add \(\displaystyle \left( {\frac{{\text{new period}}}{2}} \right)k\), since there are two asymptotes per period for the csc and sec graphs.
We have the parent graph tcharts from above, so let’s go right to examples.
Tangent and Cotangent Transformations
The reciprocal functions tangent (tan) and cotangent (cot) are transformed the same way as the csc and sec, (with “\(a\)” part of the transformation a stretch and not an amplitude). The difference however is that, since the period of the tan and cot functions (how long the graph goes before repeating itself) is \(\pi\) instead of \(2\pi\), we have \(\displaystyle \text{new period}=\frac{\pi }{b}\).
If asked for asymptotes of transformed functions, you’ll perform the same transformations on them as you would the \(x\) values of the graph. You can look at one of the new asymptotes of the transformed graph, and then add \((\text{new period})k\), since there is one asymptote per period for the tan and cot graphs.
We have the parent graph tcharts from above, so let’s go right to examples.
Writing Equations from Transformed Graphs for Sec, Csc, Tan, and Cot
Here are a few examples where we get the equations of trig functions other than sin and cos from graphs. Note that there may be varying answers for these equations:
Graph  Steps to Get Equation 



Transformation of all Trig Functions without TCharts
Let’s go over once again how to transform trig functions without tcharts. Note that in order to perform the transformations accurately and quickly, you must know your 6 trig functions graphs inside out!
Here are the steps for sin and cos graphs:
 Put the trig function in the \(y=a\sin b\left( {xc} \right)+d\,\,\,\text{or}\,\,\,y=a\cos b\left( {xc} \right)+d\) format.
 The new domain will still be \(\left( {\infty ,\,\infty } \right)\).
 The new range will be \(\left[ {\text{vertical shift (}d\text{)}\left a \right\,\text{,}\,\,\text{vertical shift (}d\text{)}+\left a \right} \right]\). (\(\left a \right\) is amplitude)
 New period will be \(\displaystyle \frac{{2\pi }}{b}\).
 Phase shift will be \(c\); start graph at this point, and if \(a\) is negative, make graph upside down.
 First draw line where vertical shift is, and lines where lower and upper ranges are. Graph will be centered vertically at the vertical shift, go up to the top line, and down to the bottom line.
 Then start graph (first point) where phase shift starts and count over (to right) an amount that is the new period (make complete revolution or cycle of the sin or cos). Draw the last point here.
 Draw middle point halfway between; this will be at the halfway mark of the complete cycle. So we’ll have a total of five points.
(Note that there’s an example of this here).
Here are the steps for tan and cot graphs:
 Put the trig function in the \(y=a\tan b\left( {xc} \right)+d\,\,\,\text{or}\,\,\,y=a\cot b\left( {xc} \right)+d\) format.
 Remember that asymptotes for tan are at \(\displaystyle \frac{\pi }{2}+\pi k\) and for cot are \(\pi k\) (the \(c\)’s (cot and csc) have the “easier” ones). To get the new asymptotes, set the trig argument to asymptotes, and solve for \(x\). For example, if we have \(\displaystyle \tan \left( {3x+\pi } \right)\,\,(\text{which would be}\,\,\tan \left( {3\left( {x+\frac{\pi }{3}} \right)} \right))\), we would solve: \(\displaystyle 3x+\pi =\frac{\pi }{2}+\pi k;\,\,\,\,\,\,3x=\left( {\frac{\pi }{2}\pi } \right)+\pi k;\) \(\displaystyle 3x=\frac{\pi }{2}+\pi k;\,\,\,\,x=\frac{{\frac{\pi }{2}}}{3}+\frac{{\pi k}}{3};\,\,\,\,x=\frac{\pi }{6}+\frac{{\pi k}}{3}\).
 The new range will still be \(\left( {\infty ,\,\infty } \right)\).
 Draw asymptotes first; phase shift will take care of itself. (To get an asymptote starting point, you can set \(k=0\) in your new asymptote equation, \(k=1\) for one to the left, \(k=1\) for one to the right). Right in between the asymptotes (you can take average of the \(x\)’s), draw the middle of the graph (but make sure it is shifted up or down according to the vertical shift, or \(d\)).
 New period will be \(\displaystyle \frac{\pi }{b}\) (since tan and cot have periods of \(\pi\)). This should be the distance between asymptotes (the coefficient of “\(k\)” in the asymptote equations).
 If trig function is negative, make sure you flip the graph.
 New domain will be all \(x\) values except for the asymptotes.
 To get two more points on either side of the center point, take the center or average again of the middle point of the asymptotes for the \(x\)’s. To get the \(y\) value for these points (since these are normally at \(y=1\) and \(y=1\)), shift the y according according to the vertical stretch, or “slope” (for example, if the function is \(3\tan \left( {x+\pi } \right)4\), the \(y\)’s would be \(3(1)4=1\) for one of the points, and \(3(1)4=7\) for the other one.
Here are the steps for csc and sec graphs:
 Put the trig function in the \(y=a\csc b\left( {xc} \right)+d\,\,\,\text{or}\,\,\,y=a\sec b\left( {xc} \right)+d\) format.
 Remember that asymptotes for sec are at \(\displaystyle \frac{\pi }{2}+\pi k\) and asymptotes for csc are \(\pi k\) (the \(c\)’s (cot and csc) have the “easier” ones). To get the new asymptotes, set the trig argument to asymptotes, and solve for \(x\). For example, if we have \(\displaystyle \csc \left( {3x\frac{\pi }{6}} \right)\), we would solve: \(\displaystyle 3x\frac{\pi }{6}=\pi k;\,\,\,3x=\frac{\pi }{6}+\pi k;\,\,\,x=\frac{\pi }{{18}}+\frac{{\pi k}}{3}=\frac{\pi }{{18}}+\frac{{6\pi k}}{{18}}\)
 The new range will be \(\left( {\infty ,\,\,\text{vertical shift (d)}\left a \right} \right]\cup \left[ {\text{vertical shift (d)}+\left a \right,\infty } \right)\). (\(\left a \right\) is amplitude)
 Draw asymptotes first; the “cups” will fall into these areas. (To get an asymptote starting point, you can set \(k=0\) in your new asymptote equation, \(k=1\) for one to the left, \(k=1\) for one to the right). The center of the “cups” will fall halfway between the asymptotes.
 New period will be \(\displaystyle \frac{{2\pi }}{b}\) (since csc and sec have periods of \(2\pi \)). (This should be the distance between every other asymptote).
 To get where graphs start (“cup up” or “cup down”), shift the graph according to the phase shift (\(c\)) (using the \(y\)axis as the starting point), and draw the graph according to the original trig function (csc or sec) and whether or not it’s negative (if negative, you flip it vertically).
 New domain will be all \(x\) values except for the asymptotes.
It’s a good idea to graph your answers on a graphing calculator (radians) with window of one period (with the Xmin and Xmax) and range (with Ymin and Ymax) to check your graphs.
Here are some examples:
Transformation 
Graph and Notes 
\(\displaystyle y=2\cos \left( {3x+\frac{\pi }{2}} \right)+4\) \(\displaystyle y=2\cos \left( {3\left( {x+\frac{\pi }{6}} \right)} \right)+4\) (First factor out the 3).
Domain: \(\left( {\infty ,\,\,\infty } \right)\) Range: \(\left[ {42,4+2} \right]=\left[ {2,6} \right]\) Period: \(\displaystyle \frac{{2\pi }}{3}\) Amplitude: 2 Phase Shift: \(\displaystyle \frac{\pi }{6}\) Flip?: Yes 
To get the range, start with the vertical shift, and add and subtract the amplitude. You can see graph is shifted up 4 (vertical shift), and goes up and down by 2 (amplitude).
Start graph \(\displaystyle \frac{\pi }{6}\) to the left of the \(y\)axis (low point, since graph is flipped) and next cycle starts at \(\displaystyle \frac{\pi }{6}+\frac{{2\pi }}{3}=\frac{\pi }{2}\), since \(\displaystyle \frac{{2\pi }}{3}\) is the period. To get the high point, take the middle (average) of \(\displaystyle \frac{\pi }{6}\text{ and }\frac{\pi }{2}\), which is \(\displaystyle \frac{\pi }{6}\). 
\(\displaystyle y=3\tan \left( {\frac{\pi }{2}x+\pi } \right)3\) \(\displaystyle y=3\tan \left( {\frac{\pi }{2}\left( {x+2} \right)} \right)3\) (First factor out the \(\displaystyle \frac{\pi }{2}\)).
Asymptotes: \(\displaystyle 1+2k\) Domain: \(\displaystyle x\ne 1+2k\) Range: \(\left( {\infty ,\,\,\infty } \right)\) Period: \(2\) Phase Shift: \(2\) Flip?: Yes 
To get the asymptotes, start with the regular tan asymptotes, set to the new tan argument, and solve for \(x\): \(\displaystyle \frac{\pi }{2}x+\pi =\frac{\pi }{2}+\pi k;\,\,\,\,\frac{\pi }{2}x=\left( {\frac{\pi }{2}\pi } \right)+\pi k;\,\,\,\frac{\pi }{2}x=\frac{\pi }{2}+\pi k;\,\,\,x=1+2k\). Let’s draw the asymptotes for \(k=1, 0, 1\), which are \(3,1,\,\text{and}\,\,\text{1}\). Graph will be flipped because of the negative sign.
To get the period, take the regular tan period of \(\pi\) and divide by \(\displaystyle \frac{\pi }{2}\); period is 2 (distance between asymptotes). To get middle of each tan graph, look at vertical shift; graph will be shifted down 3 units, and the \(x\) value will be halfway between the asymptotes.
To get two more points on either side of the center point, go halfway between the center point and the asymptotes; these \(x\) values will be \(2.5,\,1.5,\,\,.5,\,\,\text{and}\,\,\text{.5}\). To get the \(y\) value for these points, apply the vertical stretch of 3 (starting with the middle points) by going up 3 and down 3.

Here’s one more with csc:
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