Trig Functions: Reading Values From A Table

by Andrew McMorgan 44 views

Hey guys, welcome back to Plastik Magazine! Today, we're diving deep into the world of mathematics, specifically focusing on how to interpret and use tables to understand trigonometric functions. You know, those functions like sine and cosine that pop up everywhere from physics to engineering and even in understanding wave patterns. Sometimes, seeing all those Greek letters and fractions can be a bit intimidating, right? But trust me, once you get the hang of it, it's super straightforward. We've got this neat table here, which is like a cheat sheet for specific values of a function, let's call it f(x)f(x). This table shows us what happens when we plug in certain angles (represented by xx) into our function. These angles are given in radians, which is a standard way to measure angles in math and science, especially when dealing with circles and calculus. You'll notice angles like - rac{\pi}{4}, ฯ€4\frac{\pi}{4}, 3ฯ€4\frac{3\pi}{4}, 5ฯ€4\frac{5\pi}{4}, and 7ฯ€4\frac{7\pi}{4}. Each of these xx values has a corresponding f(x)f(x) value listed right below it. So, if xx is โˆ’ฯ€4-\frac{\pi}{4}, then f(x)f(x) is 0. If xx is ฯ€4\frac{\pi}{4}, f(x)f(x) is 1. See the pattern? The table is just a organized way to list these input-output pairs for our function. Understanding these specific points can help us sketch the graph of the function, predict its behavior, or solve problems where these exact values are crucial. We'll be looking at how to read this table and what it tells us about the underlying trigonometric function. So, grab your favorite beverage, get comfy, and let's break down this table like the math wizards we are!

Decoding the Table: What's Inside?

Alright, let's zoom in on this table, shall we? This isn't just a random collection of numbers and symbols; it's a powerful tool for understanding trigonometric functions. The top row, labeled 'xx', shows us the inputs to our function. These are the angles. Now, these angles aren't in degrees (like 45ยฐ, 90ยฐ, etc.) but in radians. Radians are a way of measuring angles based on the radius of a circle. A full circle is 2ฯ€2\pi radians, which is equivalent to 360ยฐ. So, ฯ€4\frac{\pi}{4} radians is the same as 45 degrees, 3ฯ€4\frac{3\pi}{4} is 135 degrees, and so on. The second row, labeled 'f(x)f(x)', shows us the outputs of the function for each corresponding input xx. It tells us the value of the function at that specific angle. For instance, when the input angle xx is โˆ’ฯ€4-\frac{\pi}{4}, the output value f(x)f(x) is 0. This means that if we were to graph this function, we'd have a point at (โˆ’ฯ€4,0)(-\frac{\pi}{4}, 0). Similarly, at x=ฯ€4x = \frac{\pi}{4}, f(x)=1f(x) = 1, giving us the point (ฯ€4,1)(\frac{\pi}{4}, 1). And at x=3ฯ€4x = \frac{3\pi}{4}, f(x)=0f(x) = 0, which is the point (3ฯ€4,0)(\frac{3\pi}{4}, 0). Moving on, when x=5ฯ€4x = \frac{5\pi}{4}, f(x)=โˆ’1f(x) = -1, so we have the point (5ฯ€4,โˆ’1)(\frac{5\pi}{4}, -1). Finally, at x=7ฯ€4x = \frac{7\pi}{4}, f(x)=0f(x) = 0, giving us the point (7ฯ€4,0)(\frac{7\pi}{4}, 0). Notice how the 'f(x)f(x)' values are only 0, 1, and -1? This is a huge clue about the type of trigonometric function we might be dealing with. Functions like sine and cosine typically oscillate between -1 and 1. Seeing zeros at these specific angles gives us even more information. For example, the sine function, sinโก(x)\sin(x), is 0 at x=0,ฯ€,2ฯ€x=0, \pi, 2\pi, etc. The cosine function, cosโก(x)\cos(x), is 0 at x=ฯ€2,3ฯ€2x=\frac{\pi}{2}, \frac{3\pi}{2}, etc. The tangent function, tanโก(x)=sinโก(x)cosโก(x)\tan(x) = \frac{\sin(x)}{\cos(x)}, is 0 when sinโก(x)=0\sin(x)=0 (i.e., at multiples of ฯ€\pi) and undefined when cosโก(x)=0\cos(x)=0 (i.e., at odd multiples of ฯ€2\frac{\pi}{2}). The values in our tableโ€”0, 1, -1โ€”suggest that f(x)f(x) could be a sine or cosine function, or perhaps a transformation of one. The specific angles where f(x)=0f(x)=0 (โˆ’ฯ€4-\frac{\pi}{4}, 3ฯ€4\frac{3\pi}{4}, 7ฯ€4\frac{7\pi}{4}) are quite interesting. Let's think about the unit circle. The angle โˆ’ฯ€4-\frac{\pi}{4} is in the fourth quadrant, 3ฯ€4\frac{3\pi}{4} is in the second quadrant, and 7ฯ€4\frac{7\pi}{4} is in the fourth quadrant. This pattern of zeros hints that f(x)f(x) might be related to sinโก(x)\sin(x) or cosโก(x)\cos(x) but possibly shifted or scaled. For instance, sinโก(x)\sin(x) is 0 at 00 and ฯ€\pi. cosโก(x)\cos(x) is 0 at ฯ€2\frac{\pi}{2} and 3ฯ€2\frac{3\pi}{2}. The angles in our table where f(x)=0f(x)=0 are not standard multiples of ฯ€\pi or ฯ€2\frac{\pi}{2}. This implies that f(x)f(x) might be something like Asinโก(Bx+C)+DA\sin(Bx+C)+D or Acosโก(Bx+C)+DA\cos(Bx+C)+D. The values 1 and -1 at ฯ€4\frac{\pi}{4} and 5ฯ€4\frac{5\pi}{4} are also key. If this were sinโก(x)\sin(x), then sinโก(ฯ€4)=22โ‰ˆ0.707\sin(\frac{\pi}{4}) = \frac{\sqrt{2}}{2} \approx 0.707 and sinโก(5ฯ€4)=โˆ’22โ‰ˆโˆ’0.707\sin(\frac{5\pi}{4}) = -\frac{\sqrt{2}}{2} \approx -0.707. If this were cosโก(x)\cos(x), then cosโก(ฯ€4)=22\cos(\frac{\pi}{4}) = \frac{\sqrt{2}}{2} and cosโก(5ฯ€4)=โˆ’22\cos(\frac{5\pi}{4}) = -\frac{\sqrt{2}}{2}. Since our f(x)f(x) values are exactly 1 and -1, and the zeros are at these specific intervals, it strongly suggests a connection to the sine or cosine function, possibly with a phase shift or a different frequency. The points (โˆ’ฯ€4,0)(-\frac{\pi}{4}, 0), (3ฯ€4,0)(\frac{3\pi}{4}, 0), and (7ฯ€4,0)(\frac{7\pi}{4}, 0) indicate roots or x-intercepts. The distance between โˆ’ฯ€4-\frac{\pi}{4} and 3ฯ€4\frac{3\pi}{4} is 3ฯ€4โˆ’(โˆ’ฯ€4)=4ฯ€4=ฯ€\frac{3\pi}{4} - (-\frac{\pi}{4}) = \frac{4\pi}{4} = \pi. The distance between 3ฯ€4\frac{3\pi}{4} and 7ฯ€4\frac{7\pi}{4} is 7ฯ€4โˆ’3ฯ€4=4ฯ€4=ฯ€\frac{7\pi}{4} - \frac{3\pi}{4} = \frac{4\pi}{4} = \pi. This consistent spacing of ฯ€\pi between consecutive zeros is characteristic of certain trigonometric functions. For example, the function sinโก(2x)\sin(2x) has zeros at 2x=nฯ€2x = n\pi, so x=nฯ€2x = \frac{n\pi}{2}. This gives zeros at 0,ฯ€2,ฯ€,3ฯ€20, \frac{\pi}{2}, \pi, \frac{3\pi}{2}, etc. Our zeros are not spaced like that. However, consider a function like sinโก(xโˆ’ฯ€4)\sin(x - \frac{\pi}{4}). Its zeros occur when xโˆ’ฯ€4=nฯ€x - \frac{\pi}{4} = n\pi, so x=nฯ€+ฯ€4x = n\pi + \frac{\pi}{4}. For n=0n=0, x=ฯ€4x = \frac{\pi}{4}. For n=1n=1, x=ฯ€+ฯ€4=5ฯ€4x = \pi + \frac{\pi}{4} = \frac{5\pi}{4}. For n=โˆ’1n=-1, x=โˆ’ฯ€+ฯ€4=โˆ’3ฯ€4x = -\pi + \frac{\pi}{4} = -\frac{3\pi}{4}. This doesn't quite match our table's zero locations. Let's try cosโก(x)\cos(x). cosโก(x)\cos(x) has zeros at ฯ€2,3ฯ€2\frac{\pi}{2}, \frac{3\pi}{2}, etc. What if we look at sinโก(2x)\sin(2x)? Zeros at 0,ฯ€2,ฯ€,3ฯ€20, \frac{\pi}{2}, \pi, \frac{3\pi}{2}. What if we look at cosโก(2x)\cos(2x)? Zeros at ฯ€4,3ฯ€4,5ฯ€4,7ฯ€4\frac{\pi}{4}, \frac{3\pi}{4}, \frac{5\pi}{4}, \frac{7\pi}{4}. Aha! cosโก(2x)\cos(2x) has zeros at ฯ€4\frac{\pi}{4} and 3ฯ€4\frac{3\pi}{4}, and 5ฯ€4\frac{5\pi}{4}, 7ฯ€4\frac{7\pi}{4}. But our table lists zeros at โˆ’ฯ€4-\frac{\pi}{4}, 3ฯ€4\frac{3\pi}{4}, 7ฯ€4\frac{7\pi}{4}. Let's re-examine the table: x=ฯ€4ightarrowf(x)=1x = \frac{\pi}{4} ightarrow f(x) = 1; x=5ฯ€4ightarrowf(x)=โˆ’1x = \frac{5\pi}{4} ightarrow f(x) = -1. This is consistent with cosโก(2x)\cos(2x) because cosโก(2imesฯ€4)=cosโก(ฯ€2)=0\cos(2 imes \frac{\pi}{4}) = \cos(\frac{\pi}{2}) = 0. This is NOT consistent with the table! The table says f(ฯ€4)=1f(\frac{\pi}{4})=1. Okay, let's pause and re-evaluate. The table IS the source of truth here. The xx values are โˆ’ฯ€4-\frac{\pi}{4}, ฯ€4\frac{\pi}{4}, 3ฯ€4\frac{3\pi}{4}, 5ฯ€4\frac{5\pi}{4}, 7ฯ€4\frac{7\pi}{4}. The corresponding f(x)f(x) values are 0, 1, 0, -1, 0. Let's look at the function f(x)=sinโก(x)f(x) = \sin(x). At x=ฯ€4x=\frac{\pi}{4}, sinโก(ฯ€4)=22e1\sin(\frac{\pi}{4})=\frac{\sqrt{2}}{2} e 1. At x=3ฯ€4x=\frac{3\pi}{4}, sinโก(3ฯ€4)=22e0\sin(\frac{3\pi}{4})=\frac{\sqrt{2}}{2} e 0. So it's not sinโก(x)\sin(x). Let's look at f(x)=cosโก(x)f(x) = \cos(x). At x=ฯ€4x=\frac{\pi}{4}, cosโก(ฯ€4)=22e1\cos(\frac{\pi}{4})=\frac{\sqrt{2}}{2} e 1. At x=3ฯ€4x=\frac{3\pi}{4}, cosโก(3ฯ€4)=โˆ’22e0\cos(\frac{3\pi}{4})=-\frac{\sqrt{2}}{2} e 0. So it's not cosโก(x)\cos(x) either. Let's consider a function involving 2x2x. What about f(x)=sinโก(2x)f(x) = \sin(2x)? At x=ฯ€4x=\frac{\pi}{4}, sinโก(2ร—ฯ€4)=sinโก(ฯ€2)=1\sin(2 \times \frac{\pi}{4}) = \sin(\frac{\pi}{2}) = 1. Perfect! At x=3ฯ€4x=\frac{3\pi}{4}, sinโก(2ร—3ฯ€4)=sinโก(3ฯ€2)=โˆ’1\sin(2 \times \frac{3\pi}{4}) = \sin(\frac{3\pi}{2}) = -1. The table says 0. So it's not sinโก(2x)\sin(2x). What about f(x)=cosโก(2x)f(x) = \cos(2x)? At x=ฯ€4x=\frac{\pi}{4}, cosโก(2ร—ฯ€4)=cosโก(ฯ€2)=0\cos(2 \times \frac{\pi}{4}) = \cos(\frac{\pi}{2}) = 0. The table says 1. So it's not cosโก(2x)\cos(2x) either. Hmm, this is where careful observation pays off. Let's consider the specific function f(x)=sinโก(xโˆ’ฯ€4)f(x) = \sin(x - \frac{\pi}{4}). If x=ฯ€4x = \frac{\pi}{4}, f(ฯ€4)=sinโก(ฯ€4โˆ’ฯ€4)=sinโก(0)=0f(\frac{\pi}{4}) = \sin(\frac{\pi}{4} - \frac{\pi}{4}) = \sin(0) = 0. The table says 1. This is tricky! Let's consider f(x)=cosโก(x)f(x) = \cos(x). The values of cosโก(x)\cos(x) at the given points are: cosโก(โˆ’ฯ€4)=22\cos(-\frac{\pi}{4}) = \frac{\sqrt{2}}{2}, cosโก(ฯ€4)=22\cos(\frac{\pi}{4}) = \frac{\sqrt{2}}{2}, cosโก(3ฯ€4)=โˆ’22\cos(\frac{3\pi}{4}) = -\frac{\sqrt{2}}{2}, cosโก(5ฯ€4)=โˆ’22\cos(\frac{5\pi}{4}) = -\frac{\sqrt{2}}{2}, cosโก(7ฯ€4)=22\cos(\frac{7\pi}{4}) = \frac{\sqrt{2}}{2}. None of these match the table directly. What about a transformation? Let's look at the zeros again: โˆ’ฯ€4,3ฯ€4,7ฯ€4-\frac{\pi}{4}, \frac{3\pi}{4}, \frac{7\pi}{4}. The difference between โˆ’ฯ€4-\frac{\pi}{4} and 3ฯ€4\frac{3\pi}{4} is ฯ€\pi. The difference between 3ฯ€4\frac{3\pi}{4} and 7ฯ€4\frac{7\pi}{4} is ฯ€\pi. This suggests a period of ฯ€\pi for the function or its components. Consider f(x)=Asinโก(Bx+C)+Df(x) = A\sin(Bx+C)+D. The period of sinโก(Bx)\sin(Bx) is 2ฯ€โˆฃBโˆฃ\frac{2\pi}{|B|}. If the period is ฯ€\pi, then 2ฯ€โˆฃBโˆฃ=ฯ€\frac{2\pi}{|B|} = \pi, so โˆฃBโˆฃ=2|B|=2. So maybe f(x)=Asinโก(2x+C)+Df(x) = A\sin(2x+C)+D. Let's check the values again. f(ฯ€4)=1f(\frac{\pi}{4}) = 1. f(3ฯ€4)=0f(\frac{3\pi}{4}) = 0. f(5ฯ€4)=โˆ’1f(\frac{5\pi}{4}) = -1. f(โˆ’ฯ€4)=0f(-\frac{\pi}{4}) = 0. f(7ฯ€4)=0f(\frac{7\pi}{4}) = 0. Let's try f(x)=cosโก(x)f(x) = \cos(x). The cosine function has a period of 2ฯ€2\pi. cosโก(0)=1,cosโก(ฯ€2)=0,cosโก(ฯ€)=โˆ’1,cosโก(3ฯ€2)=0,cosโก(2ฯ€)=1\cos(0)=1, \cos(\frac{\pi}{2})=0, \cos(\pi)=-1, \cos(\frac{3\pi}{2})=0, \cos(2\pi)=1. Let's try f(x)=sinโก(x)f(x) = \sin(x). The sine function has a period of 2ฯ€2\pi. sinโก(0)=0,sinโก(ฯ€2)=1,sinโก(ฯ€)=0,sinโก(3ฯ€2)=โˆ’1,sinโก(2ฯ€)=0\sin(0)=0, \sin(\frac{\pi}{2})=1, \sin(\pi)=0, \sin(\frac{3\pi}{2})=-1, \sin(2\pi)=0. The values 1, 0, -1 are definitely related to sine and cosine. Let's consider the function f(x)=cosโก(x)f(x) = \cos(x). The values are \cos(-\frac{\pi}{4}) = rac{\sqrt{2}}{2}, \cos( rac{\pi}{4}) = rac{\sqrt{2}}{2}, \cos( rac{3\pi}{4}) = - rac{\sqrt{2}}{2}, \cos( rac{5\pi}{4}) = - rac{\sqrt{2}}{2}, \cos( rac{7\pi}{4}) = rac{\sqrt{2}}{2}. These don't match. What about f(x)=sinโก(x)f(x) = \sin(x)? \sin(-\frac{\pi}{4}) = - rac{\sqrt{2}}{2}, \sin( rac{\pi}{4}) = rac{\sqrt{2}}{2}, \sin( rac{3\pi}{4}) = rac{\sqrt{2}}{2}, \sin( rac{5\pi}{4}) = - rac{\sqrt{2}}{2}, \sin( rac{7\pi}{4}) = - rac{\sqrt{2}}{2}. Still no match. Let's look closely at the pattern of outputs: 0, 1, 0, -1, 0. This pattern is highly suggestive of the sine wave, but shifted. Consider the standard sine wave sinโก(x)\sin(x). It starts at 0, goes up to 1 at ฯ€2\frac{\pi}{2}, back to 0 at ฯ€\pi, down to -1 at 3ฯ€2\frac{3\pi}{2}, and back to 0 at 2ฯ€2\pi. Our table's f(x)f(x) values hit 1 at ฯ€4\frac{\pi}{4} and -1 at 5ฯ€4\frac{5\pi}{4}. The zeros are at โˆ’ฯ€4,3ฯ€4,7ฯ€4-\frac{\pi}{4}, \frac{3\pi}{4}, \frac{7\pi}{4}. The spacing between consecutive zeros is ฯ€\pi. This means the function has a period of ฯ€\pi. A function of the form Asinโก(Bx)A\sin(Bx) has period 2ฯ€B\frac{2\pi}{B}. If the period is ฯ€\pi, then 2ฯ€B=ฯ€\frac{2\pi}{B} = \pi, which means B=2B=2. So, we are likely looking at a function of the form f(x)=Asinโก(2x+C)f(x) = A\sin(2x+C). Let's test this. If f(x)=sinโก(2x)f(x) = \sin(2x). Then f(ฯ€4)=sinโก(2ร—ฯ€4)=sinโก(ฯ€2)=1f(\frac{\pi}{4}) = \sin(2 \times \frac{\pi}{4}) = \sin(\frac{\pi}{2}) = 1. This matches! f(3ฯ€4)=sinโก(2ร—3ฯ€4)=sinโก(3ฯ€2)=โˆ’1f(\frac{3\pi}{4}) = \sin(2 \times \frac{3\pi}{4}) = \sin(\frac{3\pi}{2}) = -1. The table says 0. So it's not sinโก(2x)\sin(2x). Let's try f(x)=cosโก(2x)f(x) = \cos(2x). f(ฯ€4)=cosโก(2ร—ฯ€4)=cosโก(ฯ€2)=0f(\frac{\pi}{4}) = \cos(2 \times \frac{\pi}{4}) = \cos(\frac{\pi}{2}) = 0. The table says 1. So it's not cosโก(2x)\cos(2x). Okay, let's go back to the zeros. The zeros are at โˆ’ฯ€4,3ฯ€4,7ฯ€4-\frac{\pi}{4}, \frac{3\pi}{4}, \frac{7\pi}{4}. The difference between โˆ’ฯ€4-\frac{\pi}{4} and 3ฯ€4\frac{3\pi}{4} is ฯ€\pi. The difference between 3ฯ€4\frac{3\pi}{4} and 7ฯ€4\frac{7\pi}{4} is ฯ€\pi. This pattern of zeros implies a period of ฯ€\pi. Let's consider the function f(x)=sinโก(x)f(x) = \sin(x). sinโก(โˆ’ฯ€4)=โˆ’22\sin(-\frac{\pi}{4}) = -\frac{\sqrt{2}}{2}. \sin( rac{\pi}{4}) = \frac{\sqrt{2}}{2}. \sin( rac{3\pi}{4}) = \frac{\sqrt{2}}{2}. \sin( rac{5\pi}{4}) = -\frac{\sqrt{2}}{2}. \sin( rac{7\pi}{4}) = -\frac{\sqrt{2}}{2}. Let's consider f(x)=cosโก(x)f(x) = \cos(x). \cos(-\frac{\pi}{4}) = rac{\sqrt{2}}{2}. \cos( rac{\pi}{4}) = rac{\sqrt{2}}{2}. \cos( rac{3\pi}{4}) = - rac{\sqrt{2}}{2}. \cos( rac{5\pi}{4}) = - rac{\sqrt{2}}{2}. \cos( rac{7\pi}{4}) = rac{\sqrt{2}}{2}. Now, let's check the function f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}). Zeros occur when x+ฯ€4=nฯ€x+\frac{\pi}{4} = n\pi. For n=0n=0, x=โˆ’ฯ€4x = -\frac{\pi}{4}. This matches! For n=1n=1, x=ฯ€โˆ’ฯ€4=3ฯ€4x = \pi - \frac{\pi}{4} = \frac{3\pi}{4}. This matches! For n=2n=2, x=2ฯ€โˆ’ฯ€4=7ฯ€4x = 2\pi - \frac{\pi}{4} = \frac{7\pi}{4}. This matches! So the zeros are perfectly explained by f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}). Now let's check the other values. If f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}): f(ฯ€4)=sinโก(ฯ€4+ฯ€4)=sinโก(ฯ€2)=1f(\frac{\pi}{4}) = \sin(\frac{\pi}{4} + \frac{\pi}{4}) = \sin(\frac{\pi}{2}) = 1. This matches the table! f(5ฯ€4)=sinโก(5ฯ€4+ฯ€4)=sinโก(6ฯ€4)=sinโก(3ฯ€2)=โˆ’1f(\frac{5\pi}{4}) = \sin(\frac{5\pi}{4} + \frac{\pi}{4}) = \sin(\frac{6\pi}{4}) = \sin(\frac{3\pi}{2}) = -1. This also matches the table! So, the function represented by this table is indeed f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}). The table provides specific points that allow us to identify this trigonometric function. It's a standard sine function, but it's been phase-shifted to the left by ฯ€4\frac{\pi}{4} radians. This means the whole graph is moved ฯ€4\frac{\pi}{4} units to the left compared to the basic sinโก(x)\sin(x) graph. The amplitude is 1 (since the maximum is 1 and minimum is -1), and the period is 2ฯ€2\pi (since the coefficient of xx is 1). The zeros, peaks, and troughs occur at shifted locations compared to the basic sine function.

Key Takeaways from the Data

So, what can we really learn from this table? First off, key points matter. The table highlights specific inputs (xx) and their corresponding outputs (f(x)f(x)). We see that the function f(x)f(x) hits zero at three different points: x=โˆ’ฯ€4x = -\frac{\pi}{4}, x=3ฯ€4x = \frac{3\pi}{4}, and x=7ฯ€4x = \frac{7\pi}{4}. These are the roots or x-intercepts of the function's graph. This tells us where the function crosses the x-axis. The fact that it hits zero at these particular values, and not at, say, 00 or ฯ€\pi, tells us that this isn't just a simple sinโก(x)\sin(x) or cosโก(x)\cos(x) function. It's been transformed in some way, likely with a phase shift. We also see that the function reaches a maximum value of 1 at x=ฯ€4x = \frac{\pi}{4} and a minimum value of -1 at x=5ฯ€4x = \frac{5\pi}{4}. These points, (ฯ€4,1)(\frac{\pi}{4}, 1) and (5ฯ€4,โˆ’1)(\frac{5\pi}{4}, -1), are crucial for understanding the amplitude and range of the function. The amplitude is the distance from the midline (which appears to be y=0y=0 here, as the max is 1 and min is -1) to the maximum or minimum value. So, the amplitude is 1. The range of the function, meaning all possible output values, is [โˆ’1,1][-1, 1]. This is typical for basic sine and cosine functions. The spacing between these points is also super important. Let's look at the distance between the zeros: 3ฯ€4โˆ’(โˆ’ฯ€4)=4ฯ€4=ฯ€\frac{3\pi}{4} - (-\frac{\pi}{4}) = \frac{4\pi}{4} = \pi. And the distance between the next two zeros: 7ฯ€4โˆ’3ฯ€4=4ฯ€4=ฯ€\frac{7\pi}{4} - \frac{3\pi}{4} = \frac{4\pi}{4} = \pi. This consistent spacing of ฯ€\pi between consecutive zeros tells us that the period of this function is ฯ€\pi. Remember, the period is the length of one complete cycle of the function. For the basic sinโก(x)\sin(x) or cosโก(x)\cos(x) function, the period is 2ฯ€2\pi. Since our period is ฯ€\pi, this means the function completes two cycles in the same interval where sinโก(x)\sin(x) or cosโก(x)\cos(x) would complete only one. This suggests that the coefficient of xx inside the trigonometric function is 2 (because the period of sinโก(Bx)\sin(Bx) or cosโก(Bx)\cos(Bx) is 2ฯ€โˆฃBโˆฃ\frac{2\pi}{|B|}, so if 2ฯ€โˆฃBโˆฃ=ฯ€\frac{2\pi}{|B|} = \pi, then โˆฃBโˆฃ=2|B|=2). Combining these observations (amplitude of 1, range of [โˆ’1,1][-1, 1], period of ฯ€\pi, and specific zero/peak/trough locations), we can deduce that the function is likely of the form f(x)=sinโก(2x+C)f(x) = \sin(2x+C) or f(x)=cosโก(2x+C)f(x) = \cos(2x+C). As we identified earlier, the function f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}) fits all these points perfectly, indicating a phase shift. The period is 2ฯ€2\pi for this function, not ฯ€\pi. Let's re-evaluate the period deduction. The sequence of values is 0, 1, 0, -1, 0. If we plot these points: (โˆ’ฯ€4,0)(-\frac{\pi}{4}, 0), (ฯ€4,1)(\frac{\pi}{4}, 1), (3ฯ€4,0)(\frac{3\pi}{4}, 0), (5ฯ€4,โˆ’1)(\frac{5\pi}{4}, -1), (7ฯ€4,0)(\frac{7\pi}{4}, 0). The distance between (โˆ’ฯ€4,0)(-\frac{\pi}{4}, 0) and (3ฯ€4,0)(\frac{3\pi}{4}, 0) is ฯ€\pi. The distance between (3ฯ€4,0)(\frac{3\pi}{4}, 0) and (7ฯ€4,0)(\frac{7\pi}{4}, 0) is ฯ€\pi. This indicates that these are not consecutive zeros of a standard sine/cosine function with period 2ฯ€2\pi and coefficient of x=1x=1. Ah, I see the mistake in my reasoning about the period. The points given are specific points, and we should not assume they are consecutive zeros of a period 2ฯ€2\pi function without further evidence. The function f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}) has zeros at โˆ’ฯ€4,3ฯ€4,7ฯ€4-\frac{\pi}{4}, \frac{3\pi}{4}, \frac{7\pi}{4}. Let's check the distance between consecutive cycles. For sinโก(x+ฯ€4)\sin(x + \frac{\pi}{4}), the period is 2ฯ€2\pi. The zeros are at x = n\pi - rac{\pi}{4}. For n=0,x=โˆ’ฯ€4n=0, x=-\frac{\pi}{4}. For n=1,x=3ฯ€4n=1, x=\frac{3\pi}{4}. For n=2, x= rac{7\pi}{4}. For n=3, x= rac{11\pi}{4}. The distance between n=0n=0 and n=1n=1 is 3ฯ€4โˆ’(โˆ’ฯ€4)=ฯ€\frac{3\pi}{4} - (-\frac{\pi}{4}) = \pi. The distance between n=1n=1 and n=2n=2 is 7ฯ€4โˆ’3ฯ€4=ฯ€\frac{7\pi}{4} - \frac{3\pi}{4} = \pi. Okay, so the zeros are indeed separated by ฯ€\pi. This implies that the function repeats its pattern every ฯ€\pi units. This points towards a period of ฯ€\pi. If the period is ฯ€\pi, and the function is Asinโก(Bx+C)A\sin(Bx+C), then 2ฯ€โˆฃBโˆฃ=ฯ€\frac{2\pi}{|B|} = \pi, so โˆฃBโˆฃ=2|B|=2. So the function should be of the form f(x)=Asinโก(2x+C)f(x) = A\sin(2x+C) or f(x)=Acosโก(2x+C)f(x) = A\cos(2x+C). Let's recheck f(x)=sinโก(2x)f(x) = \sin(2x). We found f(ฯ€4)=1f(\frac{\pi}{4})=1, f(3ฯ€4)=โˆ’1f(\frac{3\pi}{4})=-1. Table: (ฯ€4,1)(\frac{\pi}{4}, 1), (3ฯ€4,0)(\frac{3\pi}{4}, 0). Not sinโก(2x)\sin(2x). Let's try f(x)=cosโก(2x)f(x) = \cos(2x). We found f(ฯ€4)=0f(\frac{\pi}{4})=0, f(3ฯ€4)=0f(\frac{3\pi}{4})=0. Table: (ฯ€4,1)(\frac{\pi}{4}, 1), (3ฯ€4,0)(\frac{3\pi}{4}, 0). Not cosโก(2x)\cos(2x). There must be a mistake in my initial assumption or calculation. Let's go back to the points: (โˆ’ฯ€4,0)(-\frac{\pi}{4}, 0), (ฯ€4,1)(\frac{\pi}{4}, 1), (3ฯ€4,0)(\frac{3\pi}{4}, 0), (5ฯ€4,โˆ’1)(\frac{5\pi}{4}, -1), (7ฯ€4,0)(\frac{7\pi}{4}, 0). Consider f(x)=sinโก(x)f(x) = \sin(x). The values were ยฑ22\pm \frac{\sqrt{2}}{2}. Not matching. Consider f(x)=cosโก(x)f(x) = \cos(x). The values were ยฑ22\pm \frac{\sqrt{2}}{2}. Not matching. Let's consider f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}). We found zeros at โˆ’ฯ€4,3ฯ€4,7ฯ€4-\frac{\pi}{4}, \frac{3\pi}{4}, \frac{7\pi}{4}. These match! We found f(ฯ€4)=1f(\frac{\pi}{4})=1. This matches! We found f(5ฯ€4)=โˆ’1f(\frac{5\pi}{4})=-1. This matches! So, the function is indeed f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}). My deduction about the period being ฯ€\pi based only on the spacing of the given zeros was flawed. The function sinโก(x+ฯ€4)\sin(x + \frac{\pi}{4}) has a period of 2ฯ€2\pi, not ฯ€\pi. The points provided just happen to include zeros that are ฯ€\pi apart. This table is a fantastic example of how specific data points can help us identify a function, even if it's a transformed version of a basic one. It highlights the importance of checking all provided points against a hypothesized function.

Applying the Table in Practice

So, you've got this table, and you've figured out that f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}). What now? This isn't just an academic exercise, guys. Knowing the function represented by the table allows you to do a bunch of cool stuff. For starters, you can now predict the value of f(x)f(x) for any xx, not just the ones in the table. Need to know f(ฯ€)f(\pi)? Just plug it into the formula: f(ฯ€)=sinโก(ฯ€+ฯ€4)=sinโก(5ฯ€4)=โˆ’22f(\pi) = \sin(\pi + \frac{\pi}{4}) = \sin(\frac{5\pi}{4}) = -\frac{\sqrt{2}}{2}. Easy peasy! This is super useful if you're working with data that follows a sinusoidal pattern โ€“ maybe it's sound waves, light waves, or even the oscillation of a spring. You can use these specific points to model the behavior. Furthermore, you can use these points to sketch an accurate graph of the function. You already have five points plotted: (โˆ’ฯ€4,0)(-\frac{\pi}{4}, 0), (ฯ€4,1)(\frac{\pi}{4}, 1), (3ฯ€4,0)(\frac{3\pi}{4}, 0), (5ฯ€4,โˆ’1)(\frac{5\pi}{4}, -1), and (7ฯ€4,0)(\frac{7\pi}{4}, 0). You know the amplitude is 1 and the midline is y=0y=0. You also know the period is 2ฯ€2\pi. With this information, you can draw a smooth curve connecting these points, extending it to cover the desired domain. This visual representation can help you understand the function's behavior over a wider range. In more advanced contexts, like calculus or physics, identifying the function from a table of values is a common problem. It could be part of finding the equation of motion, analyzing signals, or solving differential equations. For example, if you were given these points as measurements of a vibrating system, identifying f(x)=sinโก(x+ฯ€4)f(x) = \sin(x + \frac{\pi}{4}) would allow you to model that system mathematically and make predictions about its future behavior. You could determine when the system reaches its highest or lowest points, or when it passes through its equilibrium position. Itโ€™s like having a secret decoder ring for mathematical patterns! The table is essentially a snapshot, and by understanding the underlying trigonometric principles, we can reconstruct the whole movie. So, next time you see a table of numbers like this, don't just see numbers โ€“ see a function waiting to be discovered! Itโ€™s all about connecting the dots, literally and figuratively.