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Precision Ballistic Charts

A Critical Aid to Long Range Shooting

 

 

There is an old saying, “Beware of the man with one gun.” Go ahead, take a big yawn and stretch - like a lot of the material published in hunting and shooting magazines, we have all heard that one.  We also know the logic behind this – the shooter who owns but one gun learns its trajectory, trigger pull, etc. as intimately as knows his wife.  At least that’s the way the story goes.  My observation has been those who own one gun don’t shoot much – you could almost say one gun, one box of ammo, for it seems most of my hunting buddies who own one gun take tremendous pride in stretching that box of ammo over the decades.  But the theory sounds good.  After all, trying to learn the trajectories and wind drifts of several different rifles is bound to lead to mistakes.

 

My cure for the ballistic chart blues is to simply tape one on each rifle that I own.  The only centerfire rifles I own that don’t have this data affixed to the stocks are my .308 Winchester, which I use for close cover deer and bear hunting in the upper Midwest, and my .416 Remington Mag, with which I have shot two Cape buffalo at 20 and 45 yards – obviously not trajectory stretching shooting.

 

I recently drew a coveted mule deer permit for the northern Kaibab plateau.  Lately I have shot a ton of animals with my .338 Winchester Magnum – it may not be the flatest-shooting cartridge, and it doesn’t drip sex appeal like a .300 Remington Ultra Mag, but it really hammers animals.  The rifle, a synthetic stocked Remington 700 SS, is deadly accurate – given good conditions and lots of time shooting sitting with a tight sling (no bipod or sticks), I can almost always keep my shots inside 4 inches at 300 yards.  On my last 300 yard practice session before leaving for Tanzania, I plunked in 3 shots in a group 1½ inches – two of which hit the 3 inch aiming circle (proving that luck isn’t always bad).  As you might guess, it is the rifle I am using for my upcoming mule deer hunt.  Obviously, I don’t think you need a .338 to shoot mule deer – this is simply a gun a feel very confident shooting.

 

The trajectory of my .338 Winchester is certainly not banjo-string tight, but flat enough.  More importantly, I know it like the back of my hand.  I know from lots of shooting that when zeroed at 200 yards I can hit something at 300 by cranking the scope up to 10X and holding the bottom post of the duplex reticle right where I want to hit. In August I whacked a Nyssiland wildebeest at 308 yards shooting standing off of shooting sticks doing exactly that.  Past that, I crank on the knobs.  And of course, the wind seems to have so many infinite possibilities, that no one could remember them all.

 

Varmint cartridges are no different. In fact, they are even worse, for two very good reasons: we tend to shoot at long range (certainly longer than big game ranges) and the tiny bullets we use are especially susceptible to wind drift.  The other day I headed out to the Arizona desert for some practice.  I brought out my .223 and the venerable .338.  The wind was blowing left to right for a combined effect that varied depending on exactly when I pulled the trigger.  At 400 yards, shooting sitting with a shooting sling, I guessed 15 inches of drift for the .223 (using the ballistics chart on my rifle) and 12 inches for the .338.  I was dead on for the .338, but the .223 bullets hit 8 inches to the left – I underestimated the wind, which is always tricky with such a light bullet.  The wind was not blowing quite so hard when I shot at 500 yards; I held 9 inches for the .338 and hit within 4 inches of my point of aim.  The .223 the chart said to hold 12 inches to the left, but I had one good hit and a miss (about a foot) to the right.  My shooting wasn’t the greatest, but it would have been pitiful if I didn’t have my ballistic charts, for even with constant shooting, who can remember the possibilities?

 

Just yesterday I went out into the desert and set up a target at 383 yards.  The wind was howling; I didn’t have my Kestrel anemometer, but it seemed to be blowing at 20 mph, which is a really strong wind.  But, while it was strong, it was blowing almost totally in my face, making the drift math a lot easier.  I scooped up some dust and released it.  I watched how the dust blew, and then judged the wind direction using an indicator on my muzzle.  I bet the wind was only 20% of full value, which was good, since a full value wind would have blown my bullets 28 inches instead of the 5 inches it really did.  Judging all of this is tough enough with comprehensive ballistics charts; I cannot imagine even coming close without one.

 

When I shoot at very long range, I even compensate for changes in temperatures using ballistic tables taped to the stock.  I also find an inclination/declination chart helpful (for shooting in mountainous country) as well as a trig chart (sin of a 90 degree angle in 10 degree increments) to calculate the net effect of winds at other than 90 degree angles.

 

John Anderson and I were discussing my use of ballistics charts the other day and he thought readers might be interested in how I create mine.  You see, I don’t use the tables supplied by ballistics programs such as RCBS.Load or QuickTARGET.  They are good applications, but they don’t have the detail I am looking for, so I use Microsoft Excel as a tool to compile the data these applications provide.

 

The first step in creating a good ballistic chart is to determine what you want.  If you merely want a drop table in standard conditions, then lots of ballistics programs will work.  One of the best I have found for those who would rather press a trigger than a keyboard is QuickTARGET. 

 

QuickTARGET allows you to specify the range increments in the drop table, as well as the zero and the maximum range.  For example, suppose we want to create a table for a .223 firing a 50 grain Nosler BT at 3200.  Suppose further that we zero for 200 yards in 80 degree temperatures and want a table out to 600 yards in 10 yard increments.  We launch QuickTARGET, then specify the bullet and muzzle velocity using the boxes provided.  Next, on the right side of the user form, we enter the zero range (200 yards), the range increment (10 yards), and the maximum range, called ”Last range for Table” (see Figure 1).  Next, we must press the “New Atmo” button; this allows us to input our zero range environmental conditions.  However, before we do this, we must select an option for under “Atmosphere for zero/sight in range.”  Select the “equals table” option, then click the “New Atmo” button.  This will show a form that allows us to input the environmental conditions experienced when we zeroed.  After that, we click the “OK” button on that form, which generates our ballistic table.

 

 

We can print this out, but there is a better option.  Instead, selecting the “Copy to...” option on the menu bar allows us to export the whole works to Excel.  Selecting this option launches Excel and pastes the data from QuickTARGET directly into Excel, which is my preferred tool for creating charts because I have total control of the font size, color, lines, etc.  For those readers who don’t know Microsoft Excel, a tutorial is outside the scope of this magazine, but let’s cover some basics quickly.  Readers familiar with this application can skip the next section.

 

Microsoft Excel is a spreadsheet program.  If you have a home PC, you probably own a copy.  In a nutshell, it lets us manipulate numbers using rows and columns.  I cannot possibly teach you how to use Excel in a few paragraphs; whole books have been written on the subject.  But, if you are reasonably intelligent (which you probably are, since you are reading The VARMINT HUNTER Magazine), then you can take the tutorial.  First, get on line.  Next, launch Excel and go to the menu bar (those commands at the top of Excel).  Select “Help,” then select “Microsoft on the Web,” then select “Tutorial.”  This is a relatively easy way to learn Excel basics.

 

Once you start using the copy to Excel feature in QuickTARGET, you will soon generate extremely comprehensive ballistics tables in a matter of minutes.

 

Getting data from other ballistics programs into Excel is not as easy as QuickTARGET.  RCBS.LOAD, my “what if” favorite, suffers from a lack of standard MS Windows functionality.  I am beta testing the next version of RCBS.Load and discussing possible improvements with Greg Mushial, the author of this application.

 

Let’s look at a very simple table – the above .223 Remington from 100 to 400 yards.  Lets assume that we have generated the drop table in 20 yard increments starting at the muzzle using QuickTARGET.  The resulting table, after we choose the “Copy to...” option is shown in Figure 3.  Incidentally, if you get a bunch of hash marks (####), that means your column is not wide enough to display the width of the number.  Just place you cursor on the right side of the column header and when you see the cursor go from a cross to a double-headed arrow with a line through it, double click your mouse.  This will reformat the column width to fit the numbers.

 

Figure 2

 

If you used QuickLOAD, you will note that Column A contains the range, formatted to three decimal places.  To save printing real estate, we want to reformat this to zero decimal places.  With the mouse, click on the “A” in the column header.  The whole column will be shaded darker, meaning you have selected it.  Now go to the menu bar (the list of options starting with “File”) and select “Format.”  A list of options will drop down; select “Cells...” and then select the number tab at the top of the form that appears (it may already be the tab selected).   Under the “Category” list, select “Number.”  To the right you will now see a box labeled “Decimal places.”  Change this to zero by either clicking on the number “2” and changing it to “0,” or clicking the down arrow (called a spinner bar) next to it twice.  Finally, press the “OK” button.  The numbers will be reformatted with zero decimal places – notice the first column, which indicates range, is now narrower.

 

If you don’t have QuickLOAD, you can generate a trajectory table in the application that you have, and then try to copy and paste it to Excel.  To do this, move your mouse pointer over the data you wish to copy, then left-mouse click.  Holding down the left mouse button, drag the mouse over the data you want to copy.  Next, right-mouse click and select “Copy.”  Then, select Excel, click the cell you want the data to start in, right-mouse click and select “Paste.”  Not all applications will allow you to copy and paste data; if not, you will have to manually type data into Excel.

 

The basic data necessary in a good trajectory table is range, bullet drop, and wind drift.  I used to enter wind drift data for a 10 mph cross-wind, but I now use 1-mph drift data, for the simple reason that I find it much easier to “do the math.”  For example, I know my .220 Swift, firing 75 grain Hornady A-Max bullets at 3185 fps, will drift 1.8 inches at 500 yards in a 1 mph wind; the drift in a 5 mph cross wind is 9 inches (1.8 multiplied by 5).  I find it easy to just memorize the one mile per hour drift at 100 yard increments.

 

Once you have the basic drop and drift data for each increment in range, the next step is to calculate the amount of clicks required to hit where you aim.  The first step is to identify how far one click moves the bullet impact at 100 yards.  Generally, one click will move the impact ¼ inch at 100 yards.  Ensure that your scope does not use MOA instead of inches; if it does, then one click moves the impact .262.”  Now, you might think that the difference, .012 inches, is not much to get fussed about, and if you never shoot at long ranges, you are right.  But at long ranges it does matter.  With a .223 50 gr Nosler BT at 3300 fps, it will result in an inch of error at 400 yards and 6.9 inches at 600, clearly something to be reckoned with.

 

Let’s clean up our ballistics table, and then add the clicks required for drop and drift compensation.  Remember the ballistics chart we created (Table 1)?  Well, it has a lot more detail than we need.  For example, we don’t need to know the trajectory at ranges less than 100 yards, so lets get rid of those rows.  To do this, simply left mouse click on the first row number label, and while holding the mouse button, press the down arrow until all rows that you want to delete are highlighted (shaded).  In the example I am using, I would delete rows 2-6.  Once the rows are highlighted, right mouse click and select “delete.”  The rows disappear.  Incidentally, I find it very useful to include the trajectory at 100 yards, for it comes in handy to check the zero after traveling to a hunting area.

 

Table 1 – Results After Copying Data From Quick.LOAD to Microsoft Excel

Range(yd)

V(fps)

t(s)

Energy(ft.lbs)

Path to LOS(in)

WindDefl(in)

Drop(in)

0.0000

3200.1313

0.0000

1136.8799

-1.5000

0.0000

0.0000

20.0000

3106.9214

0.0190

1071.6168

-0.6095

0.0053

-0.0693

40.0000

3015.9021

0.0387

1009.7491

0.1362

0.0214

-0.2835

60.0000

2926.9250

0.0589

951.0474

0.7288

0.0476

-0.6507

80.0000

2839.8589

0.0797

895.3080

1.1613

0.0832

-1.1780

100.0000

2754.6548

0.1011

842.3903

1.4228

0.1300

-1.8763

120.0000

2671.2100

0.1232

792.1274

1.4976

0.1904

-2.7613

140.0000

2589.4465

0.1461

744.3769

1.3731

0.2646

-3.8456

160.0000

2509.2666

0.1698

698.9926

1.0395

0.3518

-5.1391

180.0000

2430.5818

0.1941

655.8423

0.4883

0.4512

-6.6502

200.0000

2353.4121

0.2191

614.8582

-0.2873

0.5620

-8.3856

220.0000

2277.3904

0.2448

575.7765

-1.2993

0.6849

-10.3574

240.0000

2202.9221

0.2715

538.7375

-2.5973

0.8275

-12.6152

260.0000

2129.9158

0.2994

503.6210

-4.1949

0.9887

-15.1726

280.0000

2058.2891

0.3282

470.3181

-6.1041

1.1672

-18.0417

300.0000

1987.9657

0.3579

438.7294

-8.3357

1.3623

-21.2332

320.0000

1918.8774

0.3885

408.7648

-10.8989

1.5730

-24.7561

340.0000

1851.1926

0.4198

380.4365

-13.7871

1.7966

-28.6042

360.0000

1784.5448

0.4525

353.5362

-17.1075

2.0451

-32.8844

380.0000

1720.0702

0.4870

328.4515

-20.9392

2.3236

-37.6759

400.0000

1657.5693

0.5229

305.0158

-25.2950

2.6294

-42.9916

 

We probably are not particularly interested in velocity, time of flight, or energy, so let’s delete these as well.  Now we are deleting columns, so just click on the column label, which will be a letter, then right mouse click and select “delete.”  When finished, we have drop and drift.

 

We want to add two colums to translate our drop and drift from inches to clicks.  To do this, we go to the first empty cell in row 1 (it should be D1, if you follow my narration) and label it “Drop – Clicks.”  (Just type in “Drop-Clicks” and press enter.)

 

If you look at the drop from the line of sight, you will the numbers are positive out to your zero; obviously, that is because the bullet is above the line of sight.  Since we generally will never correct for drop at ranges less than our zero range, there is no need to calculate the number of correction clicks required.  Instead, move the cursor to row below the range at which you zeroed and click on the first empty cell to the right (D8 in my example).  In this cell we will enter what is called a formula; this formula will calculate the number of clicks required to correct for the drop indicated at the far left in our table.  Let’s say that the range increments appear in Column A, the drop is in Column B and we are currently in Column D.  The correct formula to calculate the amount of clicks required to correct for drop is: “=B8/((A8/100)*0.25)” where 8 is the row number (enter everything in between the quotes).  (Note: this formula is for scopes that move impact ¼ inch per click; for scopes that move impact 1/8 inch, substitute .125 for .25.)  Next, we need to copy this formula.  There are easier ways to copy than the one I will explain, but this is simple: just right mouse click on the cell with the just-entered formula, select copy, left mouse click on the cell just below it, hold the mouse button, and slide the cursor down to the last row.  Now right mouse click and select paste.  You know the formula is correct if the number of clicks at 400 yards exactly equals the drop in inches.

 

Next, we do the same thing for the wind deflection, except we use Column E and the formula is “=C8/((A8/100)*.25)”.  Again, if your scope has 1/8 inch click adjustments (meaning one click moves the bullet impact 1/8 inch at 100 yards) substitute .125 for .25 in the above formula.

 

No we have a basic ballistics table.  But wind rarely blows as a straight cross wind; more often than not, it is blowing at an angle less then 90 degrees.  Calculating the effect of wind at less than 90 degree angles is easy, but not as easy as some writers may have led you to believe, for I have occasionally read that a wind that quarters into the shooter has only a one-half value.  Such writers prove I am not the first to write something incorrect; the actual effect is 71%.  To correctly figure the net effect of wind angles less than 90 degrees, we must resort to a little trigonometry.

 

For those are interested calculating the net effect of wind angles less than 90 degrees, Excel works fine.  First, you must express the angle in radians.  To do this, use the radians formula.  For example, if I were interested in calculating the net effect of a 30 degree wind, I would enter 30 in cell A1.  In cell A2, I type in the formula “=radians(a1).”  The result displayed in cell A2 will be .523599.  To calculate the net effect of this angle, we must calculate the sine of the angle.  To do this in Excel, go to cell A3 and enter the formula “=sin(a2).  If you want, you can format this as a percentage by selecting “Format-Cells-Number-Percentage.”  In any event, the result is .5 or 50%, which means that a wind blowing in at a 30 degree angle has ½ of the drift value of a straight cross wind.  I did the math for you for angles in 10 degree increments; see Table 2. 

 

Table 2 – Correction Factor for Wind at Angles Other Than 90 Degrees

Angle

Effect

10

17%

20

34%

30

50%

40

64%

50

77%

60

87%

70

94%

80

98%

90

100%

 Note:  A 90 degree angle is one that is blowing perpendicular to the shooter.  To use this table, first identify the 90 degree (full drift) wind drift for the range that you are shooting.  Next, estimate the wind drift angle.  Then, multiply the full drift effect by the corresponding correction factor for the angle of wind.  For example, suppose that our bullet drifts 15 inches in a straight cross wind, but since most of the wind is in our face, we estimate the angle to be only 20 degrees, which means that our bullet will drift only 34% of the 15 inches, or about 5 inches.

 

To use this table, first identify the 90 degree (full drift) wind drift for the range that you are shooting.  Next, estimate the wind drift angle.  Then, multiply the full drift effect by the corresponding correction factor for the angle of wind.  For example, suppose that our bullet drifts 15 inches in a straight cross wind, but most of the wind is in our face.  Consequently, we estimate the angle to be only 20 degrees, which means that our bullet will drift only 34% of the 15 inches, or about 5 inches.

 

But here is tip for you that simplifies all of this trigonometry, and it is one that I have never seen in print.  If you study Table 2 you will see that the net effect of angles other than 90 degrees is approximately the angle value plus 50%.  In other words, a ten degree angle possesses about 15% of the value of a full crosswind; a 20 degree wind 30%, etc.  For angles greater than 66 degrees just use the full value.  For all intents and purposes, this lets us forget about the trigonometry, especially considering most of us do not measure wind angles with any degree of accuracy.

 

When I shoot in Minnesota, the last thing I have to worry about is the effect of firing uphill or downhill.  But in Arizona, it is as important as looking out for rattlesnakes when walking out to place a target at a quarter-mile.  Common wisdom, again regurgitated by a legion of gun writers, has it that one need only worry about the horizontal distance a bullet flies, not the line of sight distance.  Sportsfans, that is bad advice.  You see, the famous rule that a bullet’s trajectory, when fired at an angle, is only affected by gravity over the horizontal portion of its flight is just plain dead wrong.  If gravity only affected a bullet over the horizontal distance of travel, a bullet fired straight up would go into orbit.  Anyone out there believe that’s possible?  To be honest, calculating trajectories by using the equivalent horizontal distance works for shots at 500 yards to less for reasonably flat-shooting cartridges; at longer distances, the errors are horrendous.

 

Time of flight always matters, and a bullet flying through 600 yards of air, no matter what the angle, still takes longer to travel than one flying 520 yards (the horizontal distance of a 600 yard shot a 30 degree angle).  To prove my point, let’s assume that we are shooting a .223 Remington stoked with 50 grain Noslers at 3400 fps.  We click our scope up to our 600 yard zero and shoot at a target 600 yards away at a 30 degree angle.  Our bullet hits 13.7 inches high, according to RCBS.Load.  The impact at 520 yards is slightly over 20 inches – so much for the theory that gravity only affects a bullet over its corresponding horizontal distance of flight.

 

Table 3 – Comprehensive Ballistic Table for 50 gr Nosler BT @ 3400 fps (200 yd Zero) 

Range(yd)

Path in inches (clicks)

Wind Deflec-tion per 1 mph of wind inches (clicks)

Path 10 Degree Angle inches (clicks)

Path 20 Degree Angle inches (clicks)

Path  30 Degree Angle inches (clicks)

Path 45 Degree Angle inches (clicks)

Path 60 Degree Angle inches (clicks)

Path 29 Degrees F inches (clicks)

Path 89 Degrees F inches (clicks)

0

-1.5

0.0

 

0.0

0.0

0.0

0.0

-1.5

-1.5

100

1.2(-5)

0.1(-0.4)

1.3(-5)

1.3(-5)

1.4(-6)

1.7(-7)

2.1(-8)

1.2(-5)

1.2(-5)

105

1.3(-5)

0.1(-0.5)

1.3(-5)

1.4(-5)

1.5(-6)

1.8(-7)

2.2(-8)

1.3(-5)

1.3(-5)

110

1.3(-5)

0.1(-0.5)

1.3(-5)

1.4(-5)

1.6(-6)

1.9(-7)

2.3(-8)

1.3(-5)

1.3(-5)

115

1.3(-5)

0.1(-0.5)

1.4(-5)

1.5(-5)

1.6(-6)

2(-7)

2.4(-8)

1.3(-5)

1.3(-5)

120

1.3(-4)

0.2(-0.5)

1.4(-5)

1.5(-5)

1.7(-6)

2(-7)

2.5(-8)

1.3(-4)

1.4(-5)

125

1.3(-4)

0.2(-0.5)

1.4(-4)

1.5(-5)

1.7(-5)

2.1(-7)

2.7(-8)

1.3(-4)

1.4(-4)

130

1.3(-4)

0.2(-0.6)

1.4(-4)

1.5(-5)

1.7(-5)

2.2(-7)

2.8(-8)

1.3(-4)

1.3(-4)

135

1.3(-4)

0.2(-0.6)

1.4(-4)

1.5(-4)

1.7(-5)

2.2(-7)

2.9(-8)

1.3(-4)

1.3(-4)

140

1.3(-4)

0.2(-0.6)

1.3(-4)

1.5(-4)

1.7(-5)

2.3(-6)

3(-8)

1.3(-4)

1.3(-4)

145

1.2(-3)

0.2(-0.6)

1.3(-4)

1.5(-4)

1.7(-5)

2.3(-6)

3(-8)

1.2(-3)

1.3(-3)

150

1.2(-3)

0.3(-0.7)

1.2(-3)

1.4(-4)

1.7(-5)

2.3(-6)

3.1(-8)

1.2(-3)

1.2(-3)

155

1.1(-3)

0.3(-0.7)

1.2(-3)

1.4(-4)

1.7(-4)

2.3(-6)

3.2(-8)

1.1(-3)

1.1(-3)

160

1(-3)

0.3(-0.7)

1.1(-3)

1.3(-3)

1.6(-4)

2.3(-6)

3.3(-8)

1(-3)

1.1(-3)

165

1(-2)

0.3(-0.7)

1(-2)

1.2(-3)

1.6(-4)

2.3(-6)

3.3(-8)

0.9(-2)

1(-2)

170

0.9(-2)

0.3(-0.8)

0.9(-2)

1.2(-3)

1.5(-4)

2.3(-6)

3.4(-8)

0.8(-2)

0.9(-2)

175

0.7(-2)

0.3(-0.8)

0.8(-2)

1.1(-2)

1.5(-3)

2.3(-5)

3.4(-8)

0.7(-2)

0.8(-2)

180

0.6(-1)

0.4(-0.8)

0.7(-2)

1(-2)

1.4(-3)

2.3(-5)

3.5(-8)

0.6(-1)

0.7(-1)

185

0.5(-1)

0.4(-0.8)

0.6(-1)

0.8(-2)

1.3(-3)

2.3(-5)

3.5(-8)

0.4(-1)

0.5(-1)

190

0.3(-1)

0.4(-0.9)

0.4(-1)

0.7(-2)

1.2(-3)

2.2(-5)

3.6(-8)

0.3(-1)

0.4(-1)

195

0.2(0)

0.4(-0.9)

0.3(-1)

0.6(-1)

1.1(-2)

2.2(-4)

3.6(-7)

0.1(0)

0.2(0)

200

0(0)

0.5(-0.9)

0.1(0)

0.4(-1)

1(-2)

2.1(-4)

3.6(-7)

-0.1(0)

0.1(0)

205

-0.2(0)

0.5(-0.9)

-0.1(0)

0.3(-1)

0.8(-2)

2.1(-4)

3.6(-7)

-0.3(1)

-0.1(0)

210

-0.4(1)

0.5(-1)

-0.3(0)

0.1(0)

0.7(-1)

2(-4)

3.7(-7)

-0.5(1)

-0.3(1)

215

-0.6(1)

0.5(-1)

-0.5(1)

-0.1(0)

0.5(-1)

1.9(-4)

3.7(-7)

-0.7(1)

-0.5(1)

220

-0.8(1)

0.6(-1)

-0.7(1)

-0.3(1)

0.4(-1)

1.8(-3)

3.7(-7)

-0.9(2)

-0.7(1)

225

-1.1(2)

0.6(-1.1)

-0.9(2)

-0.5(1)

0.2(0)

1.7(-3)

3.6(-6)

-1.2(2)

-0.9(2)

230

-1.3(2)

0.6(-1.1)

-1.1(2)

-0.7(1)

0(0)

1.6(-3)

3.6(-6)

-1.4(3)

-1.2(2)

235

-1.6(3)

0.6(-1.1)

-1.4(2)

-0.9(2)

-0.2(0)

1.5(-3)

3.6(-6)

-1.7(3)

-1.4(2)

240

-1.8(3)

0.7(-1.1)

-1.7(3)

-1.2(2)

-0.4(1)

1.3(-2)

3.6(-6)

-2(3)

-1.7(3)

245

-2.1(3)

0.7(-1.1)

-1.9(3)

-1.4(2)

-0.6(1)

1.2(-2)

3.5(-6)

-2.3(4)

-2(3)

250

-2.4(4)

0.7(-1.2)

-2.2(4)

-1.7(3)

-0.8(1)

1(-2)

3.5(-6)

-2.6(4)

-2.3(4)

255

-2.7(4)

0.8(-1.2)

-2.6(4)

-2(3)

-1.1(2)

0.9(-1)

3.5(-5)

-2.9(5)

-2.6(4)

260

-3.1(5)

0.8(-1.2)

-2.9(4)

-2.3(4)

-1.3(2)

0.7(-1)

3.4(-5)

-3.3(5)

-2.9(4)

265

-3.4(5)

0.8(-1.3)

-3.2(5)

-2.6(4)

-1.6(2)

0.5(-1)

3.3(-5)

-3.7(6)

-3.2(5)

270

-3.8(6)

0.9(-1.3)

-3.6(5)

-3(4)

-1.9(3)

0.3(0)

3.2(-5)

-4(6)

-3.6(5)

275

-4.2(6)

0.9(-1.3)

-4(6)

-3.3(5)

-2.2(3)

0.1(0)

3.2(-5)

-4.4(6)

-4(6)

280

-4.6(7)

0.9(-1.3)

-4.4(6)

-3.7(5)

-2.5(4)

-0.1(0)

3.1(-4)

-4.9(7)

-4.4(6)

285

-5(7)

1(-1.4)

-4.8(7)

-4.1(6)

-2.9(4)

-0.3(0)

3(-4)

-5.3(7)

-4.8(7)

290

-5.5(8)

1(-1.4)

-5.2(7)

-4.5(6)

-3.2(4)

-0.6(1)

2.9(-4)

-5.7(8)

-5.2(7)

295

-5.9(8)

1.1(-1.4)

-5.6(8)

-4.9(7)

-3.6(5)

-0.8(1)

2.7(-4)

-6.2(8)

-5.6(8)

300

-6.4(9)

1.1(-1.5)

-6.1(8)

-5.3(7)

-4(5)

-1.1(1)

2.6(-3)

-6.7(9)

-6.1(8)

305

-6.9(9)

1.1(-1.5)

-6.6(9)

-5.7(8)

-4.4(6)

-1.4(2)

2.5(-3)

-7.2(9)

-6.6(9)

310

-7.4(10)

1.2(-1.5)

-7.1(9)

-6.2(8)

-4.8(6)

-1.7(2)

2.3(-3)

-7.7(10)

-7(9)

315

-7.9(10)

1.2(-1.6)

-7.6(10)

-6.7(8)

-5.2(7)

-2(3)

2.2(-3)

-8.3(11)

-7.5(10)

320

-8.4(11)

1.3(-1.6)

-8.1(10)

-7.2(9)

-5.6(7)

-2.3(3)

2(-3)

-8.9(11)

-8.1(10)

325

-9(11)

1.3(-1.6)

-8.7(11)

-7.7(9)

-6.1(8)

-2.6(3)

1.9(-2)

-9.4(12)

-8.6(11)

330

-9.6(12)

1.4(-1.6)

-9.2(11)

-8.2(10)

-6.6(8)

-3(4)

1.7(-2)

-10(12)

-9.2(11)

335

-10.2(12)

1.4(-1.7)

-9.8(12)

-8.8(10)

-7.1(8)

-3.3(4)

1.5(-2)

-10.7(13)

-9.7(12)

340

-10.8(13)

1.5(-1.7)

-10.4(12)

-9.3(11)

-7.6(9)

-3.7(4)

1.3(-2)

-11.3(13)

-10.3(12)

345

-11.4(13)

1.5(-1.7)

-11(13)

-9.9(12)

-8.1(9)

-4.1(5)

1.1(-1)

-12(14)

-10.9(13)

350

-12.1(14)

1.6(-1.8)

-11.7(13)

-10.5(12)

-8.6(10)

-4.5(5)

0.9(-1)

-12.7(14)

-11.6(13)

355

-12.7(14)

1.6(-1.8)

-12.3(14)

-11.1(13)

-9.2(10)

-4.9(6)

0.6(-1)

-13.4(15)

-12.2(14)

360

-13.4(15)

1.7(-1.8)

-13(14)

-11.8(13)

-9.7(11)

-5.3(6)

0.4(0)

-14.1(16)

-12.9(14)

365

-14.1(16)

1.7(-1.9)

-13.7(15)

-12.4(14)

-10.3(11)

-5.8(6)

0.2(0)

-14.8(16)

-13.5(15)

370

-14.9(16)

1.8(-1.9)

-14.4(16)

-13.1(14)

-10.9(12)

-6.2(7)

-0.1(0)

-15.6(17)

-14.2(15)

375

-15.6(17)

1.8(-1.9)

-15.2(16)

-13.8(15)

-11.5(12)

-6.7(7)

-0.4(0)

-16.4(17)

-14.9(16)

380

-16.4(17)

1.9(-2)

-15.9(17)

-14.5(15)

-12.2(13)

-7.1(8)

-0.6(1)

-17.1(18)

-15.7(16)

385

-17.1(18)

1.9(-2)

-16.7(17)

-15.2(16)

-12.8(13)

-7.6(8)

-0.9(1)

-18(19)

-16.4(17)

390

-18(18)

2(-2)

-17.4(18)

-15.9(16)

-13.5(14)

-8.1(8)

-1.2(1)

-18.8(19)

-17.2(18)

395

-18.8(19)

2(-2.1)

-18.3(18)

-16.7(17)

-14.2(14)

-8.7(9)

-1.5(2)

-19.7(20)

-18(18)

400

-19.6(20)

2.1(-2.1)

-19.1(19)

-17.5(17)

-14.9(15)

-9.2(9)

-1.8(2)

-20.6(21)

-18.8(19)

405

-20.5(20)

2.1(-2.1)

-20(20)

-18.3(18)

-15.6(15)

-9.8(10)

-2.2(2)

-21.5(21)

-19.6(19)

410

-21.4(21)

2.2(-2.2)

-20.9(20)

-19.2(19)

-16.4(16)

-10.4(10)

-2.5(2)

-22.5(22)

-20.5(20)

415

-22.4(22)

2.3(-2.2)

-21.8(21)

-20(19)

-17.2(17)

-11(11)

-2.9(3)

-23.5(23)

-21.4(21)

420

-23.4(22)

2.3(-2.2)

-22.8(22)

-20.9(20)

-18(17)

-11.6(11)

-3.3(3)

-24.5(23)

-22.3(21)

425

-24.4(23)

2.4(-2.3)

-23.7(22)

-21.9(21)

-18.8(18)

-12.2(12)

-3.6(3)

-25.6(24)

-23.3(22)

430

-25.4(24)

2.5(-2.3)

-24.8(23)

-22.8(21)

-19.7(18)

-12.9(12)

-4(4)

-26.7(25)

-24.2(23)

435

-26.5(24)

2.5(-2.3)

-25.8(24)

-23.8(22)

-20.6(19)

-13.6(12)

-4.5(4)

-27.8(26)

-25.2(23)

440

-27.6(25)

2.6(-2.4)

-26.9(24)

-24.8(23)

-21.5(20)

-14.3(13)

-4.9(4)

-28.9(26)

-26.3(24)

445

-28.7(26)

2.7(-2.4)

-28(25)

-25.9(23)

-22.4(20)

-15(13)

-5.4(5)

-30.1(27)

-27.3(25)

450

-29.8(27)

2.8(-2.4)

-29.1(26)

-26.9(24)

-23.4(21)

-15.8(14)

-5.8(5)

-31.3(28)

-28.4(25)

455

-31(27)

2.8(-2.5)

-30.2(27)

-28(25)

-24.4(21)

-16.5(15)

-6.3(6)

-32.6(29)

-29.5(26)

460

-32.2(28)

2.9(-2.5)

-31.4(27)

-29.1(25)

-25.4(22)

-17.3(15)

-6.8(6)

-33.9(29)

-30.7(27)

465

-33.4(29)

3(-2.6)

-32.6(28)

-30.3(26)

-26.4(23)

-18.1(16)

-7.3(6)

-35.2(30)

-31.9(27)

470

-34.7(30)

3.1(-2.6)

-33.9(29)

-31.5(27)

-27.5(23)

-19(16)

-7.8(7)

-36.5(31)

-33.1(28)

475

-36(30)

3.1(-2.6)

-35.2(30)

-32.7(28)

-28.6(24)

-19.8(17)

-8.4(7)

-37.9(32)

-34.3(29)

480

-37.3(31)

3.2(-2.7)

-36.5(30)

-33.9(28)

-29.7(25)

-20.7(17)

-8.9(7)

-39.3(33)

-35.5(30)

485

-38.7(32)

3.3(-2.7)

-37.8(31)

-35.2(29)

-30.9(25)

-21.6(18)

-9.5(8)

-40.7(34)

-36.8(30)

490

-40.1(33)

3.4(-2.8)

-39.2(32)

-36.5(30)

-32(26)

-22.5(18)

-10.1(8)

-42.2(34)

-38.1(31)

495

-41.5(34)

3.5(-2.8)

-40.6(33)

-37.8(31)

-33.2(27)

-23.4(19)

-10.7(9)

-43.7(35)

-39.5(32)

500

-42.9(34)

3.6(-2.8)

-42(34)

-39.1(31)

-34.5(28)

-24.4(20)

-11.3(9)

-45.2(36)

-40.8(33)

505

-44.4(35)

3.6(-2.9)

-43.4(34)

-40.5(32)

-35.7(28)

-25.4(20)

-11.9(9)

-46.8(37)

-42.2(33)

510

-45.9(36)

3.7(-2.9)

-44.9(35)

-41.9(33)

-37(29)

-26.4(21)

-12.6(10)

-48.4(38)

-43.7(34)

515

-47.5(37)

3.8(-3)

-46.4(36)

-43.3(34)

-38.3(30)

-27.4(21)

-13.2(10)

-50(39)

-45.1(35)

520

-49(38)

3.9(-3)

-48(37)

-44.8(34)

-39.6(30)

-28.5(22)

-13.9(11)

-51.7(40)

-46.6(36)

525

-50.7(39)

4(-3)

-49.6(38)

-46.3(35)

-41(31)

-29.5(23)

-14.6(11)

-53.4(41)

-48.1(37)

530

-52.3(39)

4.1(-3.1)

-51.2(39)

-47.8(36)

-42.4(32)

-30.6(23)

-15.3(12)

-55.2(42)

-49.7(37)

535

-54(40)

4.2(-3.1)

-52.8(39)

-49.4(37)

-43.8(33)

-31.7(24)

-16(12)

-56.9(43)

-51.2(38)

540

-55.6(41)

4.3(-3.2)

-54.5(40)

-51(38)

-45.2(34)

-32.9(24)

-16.8(12)

-58.7(44)

-52.8(39)

545

-57.4(42)

4.4(-3.2)

-56.2(41)

-52.6(39)

-46.7(34)

-34(25)

-17.5(13)

-60.6(44)

-54.5(40)

550

-59.2(43)

4.5(-3.3)

-57.9(42)

-54.2(39)

-48.2(35)

-35.2(26)

-18.3(13)

-62.5(45)

-56.1(41)

555

-61(44)

4.6(-3.3)

-59.7(43)

-55.9(40)

-49.7(36)

-36.4(26)

-19.1(14)

-64.5(46)

-57.8(42)

560

-62.8(45)

4.7(-3.3)

-61.5(44)

-57.6(41)

-51.3(37)

-37.7(27)

-19.9(14)

-66.5(47)

-59.5(43)

565

-64.7(46)

4.8(-3.4)

-63.4(45)

-59.4(42)

-52.9(37)

-39(28)

-20.8(15)

-68.6(49)

-61.3(43)

570

-66.7(47)

4.9(-3.4)

-65.3(46)

-61.2(43)

-54.6(38)

-40.3(28)

-21.6(15)

-70.7(50)

-63.1(44)

575

-68.7(48)

5(-3.5)

-67.3(47)

-63.1(44)

-56.3(39)

-41.6(29)

-22.5(16)

-72.9(51)

-64.9(45)

580

-70.7(49)

5.1(-3.5)

-69.3(48)

-65(45)

-58.1(40)

-43(30)

-23.4(16)

-75.1(52)

-66.8(46)

585

-72.9(50)

5.2(-3.6)

-71.4(49)

-67(46)

-59.9(41)

-44.5(30)

-24.4(17)

-77.4(53)

-68.8(47)

590

-75(51)

5.3(-3.6)

-73.5(50)

-69(47)

-61.7(42)

-45.9(31)

-25.4(17)

-79.7(54)

-70.8(48)

595

-77.2(52)

5.4(-3.6)

-75.7(51)

-71.1(48)

-63.6(43)

-47.4(32)

-26.4(18)

-82.1(55)

-72.8(49)

600

-79.5(53)

5.5(-3.7)

-77.9(52)

-73.2(49)

-65.5(44)

-49(33)

-27.4(18)

-84.6(56)

-74.9(50)

605

-81.8(54)

5.7(-3.7)

-80.2(53)

-75.4(50)

-67.5(45)

-50.5(33)

-28.4(19)

-87.1(58)

-77(51)

610

-84.1(55)

5.8(-3.8)

-82.5(54)

-77.6(51)

-69.5(46)

-52.1(34)

-29.5(19)

-89.6(59)

-79.2(52)

615

-86.6(56)

5.9(-3.8)

-84.8(55)

-79.8(52)

-71.6(47)

-53.8(35)

-30.6(20)

-92.2(60)

-81.4(53)

620

-89(57)

6(-3.9)

-87.3(56)

-82.1(53)

-73.6(48)

-55.4(36)

-31.7(20)

-94.9(61)

-83.7(54)

625

-91.5(59)

6.1(-3.9)

-89.7(57)

-84.4(54)

-75.8(49)

-57.1(37)

-32.8(21)

-97.6(62)

-86(55)

630

-94.1(60)

6.3(-4)

-92.2(59)

-86.8(55)

-78(50)

-58.9(37)

-34(22)

-100.3(64)

-88.4(56)

635

-96.7(61)

6.4(-4)

-94.8(60)

-89.2(56)

-80.2(51)

-60.7(38)

-35.2(22)

-103.1(65)

-90.8(57)

640

-99.3(62)

6.5(-4.1)

-97.4(61)

-91.7(57)

-82.4(52)

-62.5(39)

-36.4(23)

-106(66)

-93.2(58)

645

-102(63)

6.6(-4.1)

-100(62)

-94.2(58)

-84.8(53)

-64.3(40)

-37.6(23)

-108.9(68)

-95.7(59)

650

-104.7(64)

6.8(-4.2)

-102.7(63)

-96.8(60)

-87.1(54)

-66.2(41)

-38.9(24)

-111.9(69)

-98.3(60)

655

-107.5(66)

6.9(-4.2)

-105.5(64)

-99.4(61)

-89.5(55)

-68.1(42)

-40.2(25)

-115(70)

-100.9(62)

660

-110.4(67)

7(-4.3)

-108.3(66)

-102.1(62)

-91.9(56)

-70(42)

-41.5(25)

-118.2(72)

-103.5(63)

665

-113.3(68)

7.2(-4.3)

-111.2(67)

-104.8(63)

-94.5(57)

-72.1(43)

-42.9(26)

-121.4(73)

-106.2(64)

670

-116.3(69)

7.3(-4.4)

-114.1(68)

-107.6(64)

-97(58)

-74.1(44)

-44.3(26)

-124.7(74)

-108.9(65)

675

-119.4(71)

7.4(-4.4)

-117.1(69)

-110.5(65)

-99.6(59)

-76.2(45)

-45.7(27)

-128(76)

-111.7(66)

680

-122.5(72)

7.6(-4.5)

-120.2(71)

-113.4(67)

-102.3(60)

-78.3(46)

-47.1(28)

-131.4(77)

-114.5(67)

685

-125.7(73)

7.7(-4.5)

-123.3(72)

-116.4(68)

-105(61)

-80.5(47)

-48.6(28)

-134.9(79)

-117.4(69)

690

-128.9(75)

7.9(-4.6)

-126.5(73)

-119.4(69)

-107.8(62)

-82.8(48)

-50.1(29)

-138.5(80)

-120.4(70)

695

-132.2(76)

8(-4.6)

-129.8(75)

-122.5(71)

-110.7(64)

-85(49)

-51.7(30)

-142.1(82)

-123.4(71)

700

-135.6(77)

8.2(-4.7)

-133.1(76)

-125.7(72)

-113.5(65)

-87.4(50)

-53.3(30)

-145.8(83)

-126.5(72)

705

-139.1(79)

8.3(-4.7)

-136.5(77)

-128.9(73)

-116.5(66)

-89.7(51)

-54.9(31)

-149.6(85)

-129.6(74)

710

-142.6(80)

8.5(-4.8)

-139.9(79)

-132.2(74)

-119.5(67)

-92.1(52)

-56.5(32)

-153.4(86)

-132.8(75)

715

-146.1(82)

8.6(-4.8)

-143.4(80)

-135.5(76)

-122.6(69)

-94.6(53)

-58.2(33)

-157.3(88)

-136.1(76)

720

-149.8(83)

8.8(-4.9)

-147(82)

-138.9(77)

-125.7(70)

-97.1(54)

-59.9(33)

-161.3(90)

-139.4(77)

725

-153.5(85)

8.9(-4.9)

-150.7(83)

-142.4(79)

-128.9(71)

-99.7(55)

-61.6(34)

-165.4(91)

-142.8(79)

730

-157.2(86)

9.1(-5)

-154.4(85)

-145.9(80)

-132.1(72)

-102.3(56)

-63.4(35)

-169.5(93)

-146.3(80)

735

-161.1(88)

9.2(-5)

-158.2(86)

-149.5(81)

-135.4(74)

-104.9(57)

-65.2(35)

-173.8(95)

-149.8(81)

740

-165(89)

9.4(-5.1)

-162(88)

-153.2(83)

-138.8(75)

-107.6(58)

-67.1(36)

-178.1(96)

-153.3(83)

745

-169(91)

9.6(-5.1)

-166(89)

-156.9(84)

-142.2(76)

-110.4(59)

-69(37)

-182.5(98)

-156.9(84)

750

-173(92)

9.7(-5.2)

-169.9(91)

-160.7(86)

-145.7(78)

-113.2(60)

-70.9(38)

-186.9(100)

-160.6(86)

Note:

To calculate wind drift in the field estimate  the angle of wind (a straight crosswind is 90 degrees), add 50% to that angle, then multiply that number by the wind velocity times the drift for 1 mph.  Be sure to multiply the clicks by the wind speed as well.

 

 

Nevertheless, at distances of 500 yards or less, you can get pretty accurate using the corresponding horizontal distance theory.  The easiest way to do this is to estimate the angle to the target and then multiply the distance to the target by the correction factor in Table 3, which is simply the cosine of the angle to the target.  The result is the corresponding horizontal distance, which you then use to estimate drop using your ballistic chart.

 

Finally, while temperature corrections are not normally important until the range gets long, they are worth including.  Obviously, including every temperature from –20 to 120 would result in 140 additional columns.  Instead, I include one column 30 degrees less than the standard temperature (59 degrees F) and one column 30 degrees warmer.  I use this to estimate the effects at all temperatures.

 

Since I would imagine a 50 grain Nosler BT at 3400 fps is representative of something a lot of readers shoot, I constructed a trajectory table in 5 yard increments from 100 to 750 yards.  It includes wind drift for a 1 mph wind and the effect of uphill/downhill angles at 10, 20, 30, 45, and 60 degrees.  (Note:  technically, a bullet fired at a downhill angle impacts slightly higher than one fired uphill, due to a slight reduction on the time of flight, but I simplified matters and ignored this effect.)  The numbers in parentheses indicate the number of clicks required to correctly compensate.  It took me about 30 minutes to construct.  Combine it with the wind angle correction chart mentioned previously and you a comprehensive ballistic chart. 

 

To use this chart, you have to combine the effects of range, wind, temperature, and shooting angle.  For example, suppose we have the following shooting conditions: range – 435 yards; temperature - 78 degrees; angle – 0; wind – 8 mph at 45 degree angle.  Tackle temperature first.  The drop at 435 yards when the temperature is 59 degrees requires 24 clicks; at 89 degrees, it is 23 clicks.  Since 78 is closer, dial in 23 clicks for elevation.  The wind deflection at 435 yards is 2.3 clicks per mile per hour of wind, or 18 clicks for a full value 8 mph wind.  But the angle is 45 degrees, so we use only 70% of 18 clicks.  We dial in 12 clicks of windage and get ready to shoot.  If you prefer, you can use inches and hold off. 

 

If you have a mil-dot scope, you can calculate drop and windage in mils.  (Actually, after a lot of practice, you will just “know” where to hold with a mil-dot reticle.)

 

When John Anderson first suggested this article, I had to admit I questioned whether readers would really learn anything.  If my detailed descriptions on Excel were a little tedious, my apologies.  But in the end, I think this piece gave a few a hints and tricks on how to quickly calculate trajectories at long range in various conditions. I am lucky to be able to shoot a lot at long range, and my hope is to share my observations with readers who share my passion but who might not be able to shoot as much.  My personal goal in writing for this magazine is to impart at least one piece of knowledge with every submission that might help you hit the target at what you are aiming.  I know I am not always right, but hopefully, this piece keeps that charter intact.

 
 

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