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.