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These are the user uploaded subtitles that are being translated: 1 00:00:00,460 --> 00:00:01,780 How does light behave? 2 00:00:02,240 --> 00:00:03,080 What is light? 3 00:00:03,220 --> 00:00:03,600 What is it? 4 00:00:03,660 --> 00:00:07,140 Is it some airy-fairy atmospheric thing that 5 00:00:07,140 --> 00:00:08,160 just floats around? 6 00:00:08,320 --> 00:00:09,280 How do we shape it? 7 00:00:09,360 --> 00:00:10,380 How do we use it? 8 00:00:10,480 --> 00:00:12,840 How do we make someone look pretty? 9 00:00:13,060 --> 00:00:14,800 How do we make someone look more dramatic 10 00:00:14,800 --> 00:00:15,280 with light? 11 00:00:15,340 --> 00:00:16,840 There are so many different ways, but this 12 00:00:16,840 --> 00:00:19,060 is the first step of my five-step 13 00:00:19,060 --> 00:00:22,400 process to a well-crafted photograph. 14 00:00:23,340 --> 00:00:24,800 So let me go through it. 15 00:00:24,900 --> 00:00:27,500 What affects the quality and quantity of light? 16 00:00:27,580 --> 00:00:28,600 Well, there are many factors. 17 00:00:28,680 --> 00:00:30,180 Of course, it's the size of the light 18 00:00:30,180 --> 00:00:30,540 source. 19 00:00:31,000 --> 00:00:33,400 That'll affect the quality of light. 20 00:00:33,440 --> 00:00:35,260 The intensity, it's the power of light. 21 00:00:35,780 --> 00:00:37,440 The distance of the light to the subject, 22 00:00:37,580 --> 00:00:38,720 that's going to affect it as well. 23 00:00:38,820 --> 00:00:40,580 Your camera angle, because you can have the 24 00:00:40,580 --> 00:00:43,100 exact same light, but the minute you change 25 00:00:43,100 --> 00:00:44,920 your angle, it's going to appear quite different 26 00:00:44,920 --> 00:00:46,540 because you might be exposed to more light 27 00:00:46,540 --> 00:00:48,620 or more shadows and so on and so 28 00:00:48,620 --> 00:00:48,880 forth. 29 00:00:48,980 --> 00:00:51,080 And then, of course, you've got your light 30 00:00:51,080 --> 00:00:52,800 angle, which we've just discussed. 31 00:00:52,960 --> 00:00:55,220 Now, I am going to get into a 32 00:00:55,220 --> 00:00:57,900 little bit of the science behind light. 33 00:00:58,140 --> 00:01:00,460 You may have heard of the dreaded inverse 34 00:01:00,460 --> 00:01:01,540 square law. 35 00:01:01,740 --> 00:01:03,280 What does that mean and how does it 36 00:01:03,280 --> 00:01:04,700 affect what we do? 37 00:01:05,020 --> 00:01:07,100 I'm going to quickly touch upon the mathematics 38 00:01:07,100 --> 00:01:08,820 of it all, but I'm going to mainly 39 00:01:08,820 --> 00:01:10,760 get to the heart of what it's all 40 00:01:10,760 --> 00:01:13,160 about and why you arguably should need to 41 00:01:13,160 --> 00:01:13,580 know it. 42 00:01:14,000 --> 00:01:14,920 So let's go through it here. 43 00:01:15,000 --> 00:01:16,280 Now, this is going to confuse the heck 44 00:01:16,280 --> 00:01:18,760 out of you, so don't be intimidated by 45 00:01:18,760 --> 00:01:20,540 it, but basically, what is it? 46 00:01:21,040 --> 00:01:23,320 The inverse square law is the intensity of 47 00:01:23,320 --> 00:01:25,340 the light, the power of the light, equals 48 00:01:25,340 --> 00:01:27,100 one over the distance squared. 49 00:01:27,500 --> 00:01:29,020 Now, I'm not a mathematician. 50 00:01:29,460 --> 00:01:30,320 I did a bit of algebra. 51 00:01:30,640 --> 00:01:33,160 I wasn't that good at math, but we've 52 00:01:33,160 --> 00:01:35,180 done some homework here for you and put 53 00:01:35,180 --> 00:01:36,760 it in sort of simple and layman's terms. 54 00:01:36,880 --> 00:01:40,260 So let's say, for example, we've got the 55 00:01:40,260 --> 00:01:42,960 distance squared, so one over the distance squared. 56 00:01:42,960 --> 00:01:43,820 That is the distance. 57 00:01:43,960 --> 00:01:45,400 Let's say it's a foot, okay? 58 00:01:45,840 --> 00:01:47,520 One over the distance squared. 59 00:01:47,720 --> 00:01:50,740 That distance squared, okay, is one, okay? 60 00:01:50,780 --> 00:01:52,040 So one times one is one. 61 00:01:52,440 --> 00:01:55,300 One over the distance squared, two by two, 62 00:01:55,400 --> 00:01:57,820 is four, and so on, and so on, 63 00:01:57,880 --> 00:01:59,080 and so on, and so on. 64 00:01:59,140 --> 00:02:02,140 So why I've greyed that out, so ultimately, 65 00:02:02,520 --> 00:02:05,100 if we work out what the distance squared 66 00:02:05,100 --> 00:02:09,139 is, okay, now we have one over one, 67 00:02:09,320 --> 00:02:11,020 one over four, one over nine, as in 68 00:02:11,020 --> 00:02:13,380 one, a quarter, a ninth, a sixteenth, and 69 00:02:13,380 --> 00:02:13,740 so on. 70 00:02:14,180 --> 00:02:16,960 When you translate that into the percentage of 71 00:02:16,960 --> 00:02:20,060 light, what happens is we've got 100% 72 00:02:20,060 --> 00:02:20,640 of light. 73 00:02:20,760 --> 00:02:23,800 So let's say the distance from the camera 74 00:02:23,800 --> 00:02:27,460 to the subject, let's say that represents 100%. 75 00:02:27,460 --> 00:02:28,600 We have to start somewhere. 76 00:02:28,740 --> 00:02:30,480 So let's call that 100%. 77 00:02:30,480 --> 00:02:32,820 So we've got there 100%. 78 00:02:32,820 --> 00:02:35,140 This is the most important factor, because you 79 00:02:35,140 --> 00:02:36,820 might have been taught this and think, why 80 00:02:36,820 --> 00:02:37,660 do I need to know it? 81 00:02:37,680 --> 00:02:38,780 This is just a pain in the butt. 82 00:02:38,860 --> 00:02:39,480 What do I do? 83 00:02:40,020 --> 00:02:41,880 Well, this is the biggest part of this 84 00:02:41,880 --> 00:02:42,280 equation. 85 00:02:42,680 --> 00:02:46,120 All you simply need to know is, once 86 00:02:46,120 --> 00:02:51,300 you double the distance from the actual light 87 00:02:51,300 --> 00:02:55,220 source to the subject, you actually lose up 88 00:02:55,220 --> 00:02:57,700 to 75% of that light. 89 00:02:57,800 --> 00:03:00,300 But do you see how it actually diminishes 90 00:03:00,300 --> 00:03:01,800 very, very slowly here? 91 00:03:01,940 --> 00:03:04,920 So double the distance, and you lose basically 92 00:03:04,920 --> 00:03:07,960 three quarters of your power, and that is 93 00:03:07,960 --> 00:03:08,640 a big factor. 94 00:03:08,780 --> 00:03:09,620 You need to know that. 95 00:03:09,660 --> 00:03:11,280 So when you've got either an on-camera 96 00:03:11,280 --> 00:03:13,440 flash or an off-camera flash, whether you 97 00:03:13,440 --> 00:03:15,160 have a reflector or whatever, you double that 98 00:03:15,160 --> 00:03:19,280 distance, you lose 75% of that light 99 00:03:19,280 --> 00:03:19,880 to the subject. 100 00:03:20,420 --> 00:03:23,060 So hopefully, that is hopefully the easiest way 101 00:03:23,060 --> 00:03:26,140 you've ever been explained the inverse square law. 102 00:03:26,280 --> 00:03:28,680 But what other factors come into play when 103 00:03:28,680 --> 00:03:29,320 we talk about it? 104 00:03:29,380 --> 00:03:30,660 Well, let's go through it. 105 00:03:32,020 --> 00:03:35,320 Not only are you reducing the power of 106 00:03:35,320 --> 00:03:39,700 the light, you're actually losing the, well, actually, 107 00:03:39,800 --> 00:03:41,820 you're increasing the size of the light as 108 00:03:41,820 --> 00:03:44,600 you go further away, which is almost counterintuitive. 109 00:03:44,740 --> 00:03:45,940 You almost might think the opposite. 110 00:03:46,460 --> 00:03:48,600 It's funny because the inverse square law, and 111 00:03:48,600 --> 00:03:50,100 I was doing a bit more homework because 112 00:03:50,100 --> 00:03:52,460 I've only really learnt it and taught it 113 00:03:52,460 --> 00:03:55,240 in relationship to light. 114 00:03:55,560 --> 00:03:57,820 But as I did some more research here, 115 00:03:57,860 --> 00:04:00,620 it actually applies to the gravitational force, electric 116 00:04:00,620 --> 00:04:04,040 field, of course, light and sound, or radiation. 117 00:04:04,040 --> 00:04:07,260 So it's quite fascinating that these laws exist, 118 00:04:07,480 --> 00:04:09,820 but they help us to understand everything a 119 00:04:09,820 --> 00:04:10,320 little bit better. 120 00:04:10,960 --> 00:04:15,000 So we're talking about the light source, and 121 00:04:15,000 --> 00:04:17,540 let's say this little line here represents the 122 00:04:17,540 --> 00:04:19,680 original distance from the light to the subject. 123 00:04:20,279 --> 00:04:23,060 So what happens is, although this is a 124 00:04:23,060 --> 00:04:25,880 certain size, this is actually small, let's say 125 00:04:25,880 --> 00:04:27,460 small, it is what it is, the size 126 00:04:27,460 --> 00:04:28,120 is what it is. 127 00:04:29,000 --> 00:04:31,560 Once you go further away, you can sort 128 00:04:31,560 --> 00:04:33,440 of see how I've actually used these colours 129 00:04:33,440 --> 00:04:37,120 to represent that it's almost desaturating, you know 130 00:04:37,120 --> 00:04:37,360 what I mean? 131 00:04:37,380 --> 00:04:39,580 Like we've got less power, and of course 132 00:04:39,580 --> 00:04:42,220 we do, because here we said the distance 133 00:04:42,220 --> 00:04:43,860 from the light to the subject, that represents 134 00:04:43,860 --> 00:04:44,620 100%. 135 00:04:44,620 --> 00:04:47,360 When we double the distance, okay, so original 136 00:04:47,360 --> 00:04:50,800 distance, we double it two times over here, 137 00:04:51,140 --> 00:04:54,760 now we're actually reducing that power, like I 138 00:04:54,760 --> 00:04:59,820 said, by 75%, but we're multiplying it by 139 00:04:59,820 --> 00:05:03,480 four, so it's actually spreading out, but it's 140 00:05:03,480 --> 00:05:06,360 losing its power as we go further along. 141 00:05:07,080 --> 00:05:09,740 So ultimately, to basically sum it up in 142 00:05:09,740 --> 00:05:13,040 what we discussed, again, remember, double the distance 143 00:05:13,040 --> 00:05:14,840 from the light to the subject, you lose 144 00:05:14,840 --> 00:05:17,040 75% of that light, and of course 145 00:05:17,040 --> 00:05:19,400 as you go further away, the more it 146 00:05:19,400 --> 00:05:22,240 spreads, but of course the intensity decreases. 147 00:05:22,900 --> 00:05:25,740 Once you understand those things, then it makes 148 00:05:25,740 --> 00:05:26,600 it a little bit easier. 149 00:05:26,800 --> 00:05:29,480 I'm not really even suggesting that arguably you 150 00:05:29,480 --> 00:05:31,840 go in to a shoot with these mathematics 151 00:05:31,840 --> 00:05:33,480 and freak out, you just need to know 152 00:05:33,480 --> 00:05:37,480 those basic fundamentals, so that you can understand 153 00:05:37,480 --> 00:05:40,040 how the light behaves, and know that when 154 00:05:40,040 --> 00:05:41,480 you're turning your flash on, like what's going 155 00:05:41,480 --> 00:05:43,440 on, I just, I moved my, you know, 156 00:05:43,540 --> 00:05:46,060 my subject, you know, one metre back, and 157 00:05:46,060 --> 00:05:47,420 all of a sudden I've got hardly any 158 00:05:47,420 --> 00:05:48,060 power left. 159 00:05:48,280 --> 00:05:50,600 Well, that's because of the inverse square law, 160 00:05:50,980 --> 00:05:52,020 and what I want to do now is 161 00:05:52,020 --> 00:05:53,700 I'm actually going to show it to you 162 00:05:53,700 --> 00:05:56,420 in more of a practical method, by shining 163 00:05:56,420 --> 00:06:00,440 a flashlight on a piece of paper, and 164 00:06:00,440 --> 00:06:02,880 let's see if we can prove this theory. 165 00:06:03,580 --> 00:06:06,600 Light travels in straight lines, so each ray 166 00:06:06,600 --> 00:06:08,240 of light has its own path until it 167 00:06:08,240 --> 00:06:11,660 deflects or bounces off something, which continues, of 168 00:06:11,660 --> 00:06:13,800 course, on another straight path, and so on, 169 00:06:14,080 --> 00:06:14,740 and so forth. 170 00:06:15,000 --> 00:06:16,360 So let's look at our drawing here. 171 00:06:16,620 --> 00:06:20,380 We've got the light source right here, light 172 00:06:20,380 --> 00:06:28,560 travels in straight lines, it doesn't get squiggly, 173 00:06:28,720 --> 00:06:30,600 it doesn't wrap around, or anything like that, 174 00:06:30,640 --> 00:06:33,240 it'll just go on there, and then it 175 00:06:33,240 --> 00:06:35,720 will deflect, if it has something to deflect 176 00:06:35,720 --> 00:06:39,840 from, and it will keep on bouncing accordingly. 177 00:06:40,380 --> 00:06:42,740 That's a fundamental, but we just need to 178 00:06:42,740 --> 00:06:45,180 understand it's pure physics, this is what it's 179 00:06:45,180 --> 00:06:45,540 all about. 180 00:06:45,700 --> 00:06:48,340 Now, the intensity of light reduces as the 181 00:06:48,340 --> 00:06:50,840 subject and light are moved further apart. 182 00:06:50,980 --> 00:06:52,120 That's a pretty obvious one. 183 00:06:52,640 --> 00:06:54,780 If this is, you know, if this is 184 00:06:54,780 --> 00:07:00,220 your subject, and this is your light source, 185 00:07:00,460 --> 00:07:03,460 as they get further apart, the intensity will 186 00:07:03,460 --> 00:07:03,920 reduce. 187 00:07:04,300 --> 00:07:05,260 Now, let's prove it. 188 00:07:05,960 --> 00:07:08,340 So let's say this piece of paper represents 189 00:07:08,340 --> 00:07:11,120 the subject, and then let's say where the 190 00:07:11,120 --> 00:07:13,620 light is right now represents 100% of 191 00:07:13,620 --> 00:07:14,640 that light, okay? 192 00:07:15,020 --> 00:07:16,820 Of course, we need a starting point. 193 00:07:17,200 --> 00:07:19,620 Now, we just established that the inverse square 194 00:07:19,620 --> 00:07:24,100 law suggests, or actually, factually says that if 195 00:07:24,100 --> 00:07:27,580 we double the distance from the light to 196 00:07:27,580 --> 00:07:30,540 the subject, we reduce the intensity of light 197 00:07:30,540 --> 00:07:33,040 by 75%, so we've just shown you that. 198 00:07:33,740 --> 00:07:36,100 Not only that happens, so we're reducing the 199 00:07:36,100 --> 00:07:39,220 light by 75%, but we're also making it 200 00:07:39,220 --> 00:07:39,520 bigger. 201 00:07:39,720 --> 00:07:41,340 If we go to the slide here on 202 00:07:41,340 --> 00:07:44,720 the screen, you can see that the number 203 00:07:44,720 --> 00:07:48,280 one, that sort of orange looking box there 204 00:07:48,280 --> 00:07:50,800 right in front of that light source, that's 205 00:07:50,800 --> 00:07:53,740 the intensity of the light there at 100%, 206 00:07:53,740 --> 00:07:57,340 but when we double the distance, now we're 207 00:07:57,340 --> 00:08:00,240 multiplying that area that the light is covering 208 00:08:00,240 --> 00:08:01,000 by four. 209 00:08:01,400 --> 00:08:03,680 So let's prove that in actuality here with 210 00:08:03,680 --> 00:08:04,320 our example. 211 00:08:04,880 --> 00:08:06,800 So you can see that if this represents 212 00:08:06,800 --> 00:08:10,460 100% of that light source, if we 213 00:08:10,460 --> 00:08:13,820 double the distance, then you see how now 214 00:08:13,820 --> 00:08:15,240 we're getting a bigger light source. 215 00:08:15,700 --> 00:08:17,600 The problem is we're getting a bigger light 216 00:08:17,600 --> 00:08:19,320 source, but we're losing the power or the 217 00:08:19,320 --> 00:08:19,760 intensity. 218 00:08:20,060 --> 00:08:22,200 To go back to our analogy of water, 219 00:08:22,840 --> 00:08:25,080 so right now we've got this small hose, 220 00:08:25,440 --> 00:08:28,640 and it's quite sharp, and it feels quite 221 00:08:28,640 --> 00:08:29,540 tough on the skin. 222 00:08:30,340 --> 00:08:32,720 When we go a little bit further back, 223 00:08:32,760 --> 00:08:35,919 it actually feels larger, so we actually feel 224 00:08:35,919 --> 00:08:37,860 more water on our body so to speak, 225 00:08:38,220 --> 00:08:39,340 but it's less pressure. 226 00:08:39,820 --> 00:08:42,080 Now yes, there are a couple things that 227 00:08:42,080 --> 00:08:43,080 come into play here. 228 00:08:43,580 --> 00:08:45,040 Now if you look at that diagram back 229 00:08:45,040 --> 00:08:49,600 there again, so you've got, if it's with 230 00:08:49,600 --> 00:08:51,500 a speed light for example, you've got the 231 00:08:51,500 --> 00:08:54,260 bulb inside the flash head that if you 232 00:08:54,260 --> 00:08:56,300 zoom it in or out, the spread of 233 00:08:56,300 --> 00:08:57,700 that light becomes different. 234 00:08:58,140 --> 00:09:00,640 So you have to understand, although that this 235 00:09:00,640 --> 00:09:05,820 is an actual proven principle in physics, you 236 00:09:05,820 --> 00:09:07,180 have to understand it's going to be a 237 00:09:07,180 --> 00:09:08,660 little bit different depending on the light source, 238 00:09:09,040 --> 00:09:10,500 and in this case, in the example that 239 00:09:10,500 --> 00:09:11,560 I'm giving you, the flash head. 240 00:09:11,660 --> 00:09:12,720 So let me show you this now as 241 00:09:12,720 --> 00:09:12,900 well. 242 00:09:13,680 --> 00:09:16,920 So you see, actually let's see this, so 243 00:09:16,920 --> 00:09:19,100 let's say for example this is the widest 244 00:09:19,100 --> 00:09:22,020 that we can do the flash head, all 245 00:09:22,020 --> 00:09:24,160 right, so the zoom, the flash head within 246 00:09:24,160 --> 00:09:27,680 the actual unit is right at the end 247 00:09:27,680 --> 00:09:29,880 giving us a wide spread. 248 00:09:30,040 --> 00:09:31,680 It looks small now because it's close to 249 00:09:31,680 --> 00:09:32,420 the actual area. 250 00:09:32,920 --> 00:09:36,380 Now I can zoom this, and do you 251 00:09:36,380 --> 00:09:37,840 see now how small it is? 252 00:09:38,140 --> 00:09:40,140 So when the actual flash head comes closer, 253 00:09:40,600 --> 00:09:44,620 then what's on screen right now is maybe 254 00:09:44,620 --> 00:09:48,180 not exactly correct based upon that flow. 255 00:09:48,860 --> 00:09:51,120 So again, depending on the pressure of the 256 00:09:51,120 --> 00:09:52,980 light, the intensity of the light, if you 257 00:09:52,980 --> 00:09:56,520 can zoom the flash head, then arguably that 258 00:09:56,520 --> 00:09:58,420 particular diagram that you're looking at now will 259 00:09:58,420 --> 00:10:01,040 be wider or narrower depending on those things. 260 00:10:01,360 --> 00:10:05,240 But again guys, remember that as you bring 261 00:10:05,240 --> 00:10:07,520 the light source away from your subject, it 262 00:10:07,520 --> 00:10:09,980 gets bigger, which is fantastic because we can 263 00:10:09,980 --> 00:10:11,260 say, you know what, if I need a 264 00:10:11,260 --> 00:10:13,060 bigger light source and photographing a big group, 265 00:10:13,400 --> 00:10:14,740 I just bring it further away. 266 00:10:14,920 --> 00:10:17,400 The problem is I need more pressure, as 267 00:10:17,400 --> 00:10:21,420 in more intensity of light to illuminate everything 268 00:10:21,420 --> 00:10:22,040 that I want. 269 00:10:22,340 --> 00:10:23,300 So it's a bit of a give and 270 00:10:23,300 --> 00:10:23,860 take thing. 271 00:10:24,260 --> 00:10:26,260 So remember that, practice that, and have some 272 00:10:26,260 --> 00:10:26,780 fun. 273 00:10:26,860 --> 00:10:28,920 So remember this, the larger the light source 274 00:10:28,920 --> 00:10:31,200 relative to your subject, the softer the light. 275 00:10:31,700 --> 00:10:33,180 So here we have a good friend of 276 00:10:33,180 --> 00:10:35,560 mine, Rainy, she's actually against the white background, 277 00:10:36,140 --> 00:10:38,700 and it's very, very cloudy, okay, so we 278 00:10:38,700 --> 00:10:41,180 basically have a very, very large light source. 279 00:10:42,360 --> 00:10:44,800 Because it's basically so big, it's very soft, 280 00:10:45,000 --> 00:10:46,500 because you can think of it like if 281 00:10:46,500 --> 00:10:48,580 it's not the sun, the sun isn't the 282 00:10:48,580 --> 00:10:51,440 light source anymore, the clouds have diffused the 283 00:10:51,440 --> 00:10:53,740 light, and now the whole sky, the clouds, 284 00:10:53,920 --> 00:10:56,120 everything is the big light source. 285 00:10:56,700 --> 00:10:58,540 So the transition from light to shadow is 286 00:10:58,540 --> 00:11:02,040 not so great, it's quite soft, it's less 287 00:11:02,040 --> 00:11:03,800 descriptive, and all those different things. 288 00:11:04,320 --> 00:11:06,000 Now let's look at the difference. 289 00:11:07,160 --> 00:11:09,400 The smaller the light source relative to your 290 00:11:09,400 --> 00:11:10,740 subject, the harsher the light. 291 00:11:11,240 --> 00:11:13,500 So now the clouds have gone away, and 292 00:11:13,500 --> 00:11:15,380 now we basically have the sun as the 293 00:11:15,380 --> 00:11:15,880 light source. 294 00:11:16,000 --> 00:11:17,640 Now people think the sun is big, it 295 00:11:17,640 --> 00:11:20,980 is per se, but it's quite small relative 296 00:11:20,980 --> 00:11:22,040 to my subject. 297 00:11:22,260 --> 00:11:25,940 So arguably it is a small light source, 298 00:11:26,560 --> 00:11:29,400 and because it's so small, the harsher the 299 00:11:29,400 --> 00:11:31,380 light, as in the more contrasty it is, 300 00:11:31,400 --> 00:11:33,280 you can see the shadows are deeper, we've 301 00:11:33,280 --> 00:11:35,640 got a very defined shadow against that sort 302 00:11:35,640 --> 00:11:37,640 of white background there as well, so it 303 00:11:37,640 --> 00:11:40,220 gives us a completely different look. 304 00:11:40,320 --> 00:11:42,220 So if you look at the comparison, there's 305 00:11:42,220 --> 00:11:44,700 a large light source, there's a small light 306 00:11:44,700 --> 00:11:48,080 source, and that could be likened to basically 307 00:11:48,080 --> 00:11:48,600 anything. 308 00:11:48,880 --> 00:11:50,340 It could be a big window or a 309 00:11:50,340 --> 00:11:52,780 small window, it could be a larger flashlight 310 00:11:52,780 --> 00:11:54,540 or a smaller flashlight, it could be a 311 00:11:54,540 --> 00:11:56,120 big softbox or a small, and so on 312 00:11:56,120 --> 00:11:56,640 and so forth. 313 00:11:57,100 --> 00:11:59,020 If you look at, this is actually Melissa's 314 00:11:59,020 --> 00:12:02,720 40th birthday shoot, yes she looks amazing for 315 00:12:02,720 --> 00:12:04,840 40, very very proud of her and her 316 00:12:04,840 --> 00:12:05,780 heart and her beauty. 317 00:12:06,640 --> 00:12:10,580 This is open shade, it's quite overcast, so 318 00:12:10,580 --> 00:12:12,100 we have a big light source, it's very 319 00:12:12,100 --> 00:12:14,080 soft, okay, so it's very complementary. 320 00:12:14,640 --> 00:12:16,340 You might be using this kind of light 321 00:12:16,340 --> 00:12:19,640 source if you want to have maybe some 322 00:12:19,640 --> 00:12:21,900 challenging skin and you want to soften the 323 00:12:21,900 --> 00:12:24,980 skin, maybe you have maybe aging parents or 324 00:12:24,980 --> 00:12:27,120 grandparents and you find open shade is really 325 00:12:27,120 --> 00:12:29,920 really nice, so therefore this might be really 326 00:12:29,920 --> 00:12:30,240 good. 327 00:12:30,360 --> 00:12:33,120 But then when the light source is smaller, 328 00:12:33,280 --> 00:12:35,480 let's say there's no cloud now, the sun, 329 00:12:35,640 --> 00:12:38,280 so the sun is small relative to clouds, 330 00:12:38,400 --> 00:12:41,220 now the light source is smaller, we get 331 00:12:41,220 --> 00:12:43,680 it more contrasty, it's more sharper, we've got 332 00:12:43,680 --> 00:12:47,340 sharper edges, we've got the transition from highlight 333 00:12:47,340 --> 00:12:51,080 to shadow is more abrupt than before, as 334 00:12:51,080 --> 00:12:52,000 you can basically see. 335 00:12:53,280 --> 00:12:54,860 So what we're trying to do is just 336 00:12:54,860 --> 00:12:56,520 give you some fundamentals that you can take 337 00:12:56,520 --> 00:12:58,120 in your next shoot, whether it's a wedding 338 00:12:58,120 --> 00:12:59,660 or a portrait, whatever it may be, but 339 00:12:59,660 --> 00:13:02,120 these are fundamentals that you basically just need 340 00:13:02,120 --> 00:13:02,500 to know. 341 00:13:03,200 --> 00:13:06,180 So let's talk about this one, the closer 342 00:13:06,180 --> 00:13:08,240 the light is to the subject, the darker 343 00:13:08,240 --> 00:13:08,820 the background. 344 00:13:09,020 --> 00:13:10,700 So this is basically shot in a hotel 345 00:13:10,700 --> 00:13:13,760 room, this was a dark background, I think 346 00:13:13,760 --> 00:13:16,180 it was a black background, but as you 347 00:13:16,180 --> 00:13:20,240 can see, just off the actual perspective of 348 00:13:20,240 --> 00:13:21,680 this photograph is a window. 349 00:13:22,260 --> 00:13:25,160 Because she's quite close to it, the background 350 00:13:25,160 --> 00:13:27,840 becomes darker, because I have to expose for 351 00:13:27,840 --> 00:13:30,100 her, as in get detail on the brightest 352 00:13:30,100 --> 00:13:32,640 highlight in her face, which forces the background 353 00:13:32,640 --> 00:13:34,000 to pretty much go pitch black. 354 00:13:34,720 --> 00:13:37,940 Now if I change my angle, so now 355 00:13:37,940 --> 00:13:40,300 I've got her from the, let's say for 356 00:13:40,300 --> 00:13:43,140 example the bedroom window was basically here, and 357 00:13:43,140 --> 00:13:45,180 she was facing this way in a profile, 358 00:13:45,380 --> 00:13:48,840 now she's over there up against this grey 359 00:13:48,840 --> 00:13:51,080 wall, so the further away the light is 360 00:13:51,080 --> 00:13:53,260 from the subject, the lighter the background, because 361 00:13:53,260 --> 00:13:56,280 of course the the value of exposure between 362 00:13:56,280 --> 00:13:59,760 the bride here and the wall are quite 363 00:13:59,760 --> 00:14:02,060 similar, so therefore we have that effect. 364 00:14:02,480 --> 00:14:05,360 If I wanted that background darker, I simply 365 00:14:05,360 --> 00:14:07,800 get her closer to the light, expose for 366 00:14:07,800 --> 00:14:09,880 her correctly, as in I want detail on 367 00:14:09,880 --> 00:14:12,280 the brightest highlight in her face, then of 368 00:14:12,280 --> 00:14:14,780 course that background, although grey, might appear a 369 00:14:14,780 --> 00:14:16,740 dark grey or possibly even black depending on 370 00:14:16,740 --> 00:14:17,620 how far away we are. 371 00:14:18,100 --> 00:14:19,660 And it's amazing too that all we have 372 00:14:19,660 --> 00:14:21,300 to do is just change our angle, so 373 00:14:21,300 --> 00:14:24,100 she stayed there, I changed my angle to 374 00:14:24,100 --> 00:14:27,020 camera left or her right, and then we 375 00:14:27,020 --> 00:14:28,080 get this photograph. 376 00:14:29,060 --> 00:14:31,640 So there is so much to photography that 377 00:14:31,640 --> 00:14:34,320 you can't take anything for granted, and there's 378 00:14:34,320 --> 00:14:37,160 no absolutes, that's why in many occasions I'll 379 00:14:37,160 --> 00:14:39,740 say the larger the light source relative to 380 00:14:39,740 --> 00:14:41,780 your subject, the darker the background and so 381 00:14:41,780 --> 00:14:41,940 on. 382 00:14:42,020 --> 00:14:44,260 Well it depends that, see we could be 383 00:14:44,260 --> 00:14:46,580 using a large light source, but we could 384 00:14:46,580 --> 00:14:48,340 be shooting on the fringe of it, which 385 00:14:48,340 --> 00:14:50,620 now becomes a small light source. 386 00:14:51,100 --> 00:14:52,540 So if you look at these three photographs 387 00:14:52,540 --> 00:14:54,260 of the same girl in the same room, 388 00:14:55,000 --> 00:14:57,380 although this was quite a large light source, 389 00:14:57,380 --> 00:14:59,580 it was a large window, I had her 390 00:14:59,580 --> 00:15:02,060 on the fringe of it, and really we've 391 00:15:02,060 --> 00:15:03,520 got a tickle of light on her face 392 00:15:03,520 --> 00:15:04,560 and a little bit of her ear, we 393 00:15:04,560 --> 00:15:06,320 turned her shoulders, so only a hint of 394 00:15:06,320 --> 00:15:08,460 her shoulders in light, but the rest is 395 00:15:08,460 --> 00:15:10,800 in shadow, well now it's sort of become 396 00:15:10,800 --> 00:15:11,840 a small light source. 397 00:15:12,660 --> 00:15:16,100 And of course you may recognise that, that's 398 00:15:16,100 --> 00:15:17,860 a part of the banner behind me there 399 00:15:17,860 --> 00:15:18,260 as well. 400 00:15:19,240 --> 00:15:21,860 So we need to practice these things to 401 00:15:21,860 --> 00:15:24,020 sort of really understand how we bring out 402 00:15:24,020 --> 00:15:27,420 the best in our subjects, and what kind 403 00:15:27,420 --> 00:15:28,920 of mood we're trying to create and things 404 00:15:28,920 --> 00:15:30,160 like that, and of course we're going to 405 00:15:30,160 --> 00:15:31,540 discuss this further as well. 406 00:15:31,860 --> 00:15:33,400 So let's talk a little bit further about 407 00:15:33,400 --> 00:15:34,420 how light behaves. 408 00:15:34,540 --> 00:15:36,720 Remember the closer the light source is to 409 00:15:36,720 --> 00:15:39,360 your subject, the sharper the shadows on your 410 00:15:39,360 --> 00:15:39,720 face. 411 00:15:39,780 --> 00:15:41,680 So if you want something, or your subject 412 00:15:41,680 --> 00:15:43,200 to be more dramatic, bring the light a 413 00:15:43,200 --> 00:15:45,020 little bit closer, and then you've got that 414 00:15:45,020 --> 00:15:46,540 light and that shade that's going to be 415 00:15:46,540 --> 00:15:48,180 a little bit more contrasty. 416 00:15:48,440 --> 00:15:50,780 The further away your subject is from the 417 00:15:50,780 --> 00:15:52,940 light source, the softer the shadows. 418 00:15:53,400 --> 00:15:55,200 So for example if you're photographing parents or 419 00:15:55,200 --> 00:15:58,040 grandparents, and you want a softer transition, you 420 00:15:58,040 --> 00:15:59,480 want a little bit of modelling as we 421 00:15:59,480 --> 00:16:01,760 call it, making a face look more three 422 00:16:01,760 --> 00:16:04,360 -dimensional with shadow, but you don't want it 423 00:16:04,360 --> 00:16:06,400 to be so abrupt between light and shadow, 424 00:16:06,900 --> 00:16:08,820 bring the light further away and it's a 425 00:16:08,820 --> 00:16:09,440 little bit softer. 426 00:16:09,980 --> 00:16:11,880 A good example also is if you're photographing 427 00:16:11,880 --> 00:16:14,620 let's say a plus-sized bride, who you 428 00:16:14,620 --> 00:16:16,500 might want to use shadow to cut in 429 00:16:16,500 --> 00:16:18,640 and actually make her look slimmer, but she 430 00:16:18,640 --> 00:16:20,280 also maybe has bad skin. 431 00:16:20,540 --> 00:16:23,460 So that shadow makes her look slimmer, but 432 00:16:23,460 --> 00:16:25,360 it's not so abrupt between light and shadow, 433 00:16:25,740 --> 00:16:28,040 but the softness of that light is actually 434 00:16:28,040 --> 00:16:29,160 going to make her skin look a little 435 00:16:29,160 --> 00:16:29,680 bit softer. 436 00:16:30,040 --> 00:16:31,680 So there's a good example of that in 437 00:16:31,680 --> 00:16:31,980 action. 438 00:16:32,500 --> 00:16:35,800 Remember smaller, harder contrasty light means a transition 439 00:16:35,800 --> 00:16:38,540 of light to shadow is more abrupt, which 440 00:16:38,540 --> 00:16:39,600 creates deeper shadows. 441 00:16:40,000 --> 00:16:42,080 You might actually recognise my work, I love 442 00:16:42,080 --> 00:16:42,700 deep shadows. 443 00:16:42,840 --> 00:16:46,380 I just think they're just so dramatic, very, 444 00:16:46,480 --> 00:16:49,980 very cool and I'm not always after absolute 445 00:16:49,980 --> 00:16:51,480 perfect detail in blacks. 446 00:16:51,700 --> 00:16:53,100 No one said that you have to have 447 00:16:53,100 --> 00:16:53,980 detail in blacks. 448 00:16:54,080 --> 00:16:56,040 Maybe if you go to a competition, you 449 00:16:56,040 --> 00:16:58,160 will often hear a judge say, well I 450 00:16:58,160 --> 00:16:59,480 don't see any detail there. 451 00:16:59,580 --> 00:17:02,280 Quite simply, there is no perfect exposure, there's 452 00:17:02,280 --> 00:17:03,180 no perfect light. 453 00:17:03,359 --> 00:17:07,060 It's really, it's basically perfect or the execution 454 00:17:07,060 --> 00:17:08,300 of your desired result. 455 00:17:08,480 --> 00:17:09,540 Do you want deep shadows? 456 00:17:09,680 --> 00:17:11,060 Do you want black in those shadows? 457 00:17:11,260 --> 00:17:13,140 If that's what you want and that's what 458 00:17:13,140 --> 00:17:15,260 you execute, then you've done it, no problem 459 00:17:15,260 --> 00:17:15,619 at all. 460 00:17:16,040 --> 00:17:18,280 Remember larger, softer light means a transition of 461 00:17:18,280 --> 00:17:20,000 light to shadow is more gradual. 462 00:17:20,300 --> 00:17:22,000 As we sort of previously discussed, you saw 463 00:17:22,000 --> 00:17:25,980 those photographs of Rainy, my wife Melissa, where 464 00:17:25,980 --> 00:17:27,640 it was a little bit softer, blended in 465 00:17:27,640 --> 00:17:28,140 a little bit. 466 00:17:28,680 --> 00:17:31,220 Some people like that soft look and depending 467 00:17:31,220 --> 00:17:33,440 on the body type, the shape, the skin 468 00:17:33,440 --> 00:17:36,180 type, these things come into play and that's 469 00:17:36,180 --> 00:17:36,960 really, really important. 470 00:17:37,740 --> 00:17:40,820 Ultimately guys, remember this, we often say that 471 00:17:40,820 --> 00:17:43,460 lighting is the most important thing technically in 472 00:17:43,460 --> 00:17:47,000 a photograph or in photography per se, but 473 00:17:47,000 --> 00:17:49,140 really it's actually the opposite in my humble 474 00:17:49,140 --> 00:17:49,460 opinion. 475 00:17:49,960 --> 00:17:52,360 It's a subtraction of light that creates luxury, 476 00:17:52,560 --> 00:17:54,780 depth, mood, dimension and shape and form and 477 00:17:54,780 --> 00:17:56,420 all these different things. 478 00:17:57,300 --> 00:17:59,760 That's what it's all about, is where do 479 00:17:59,760 --> 00:18:01,100 you take away the light? 480 00:18:01,260 --> 00:18:03,220 Once you take it away and we'll discuss 481 00:18:03,220 --> 00:18:06,980 this in future segments, it becomes very, very 482 00:18:06,980 --> 00:18:07,360 beautiful. 483 00:18:07,540 --> 00:18:10,260 You start to see a beautiful three dimensional 484 00:18:10,260 --> 00:18:13,160 form and shape, you see texture, all these 485 00:18:13,160 --> 00:18:13,860 different things. 486 00:18:14,080 --> 00:18:16,540 We're going to learn how to almost light 487 00:18:16,540 --> 00:18:19,800 something completely and then take away light and 488 00:18:19,800 --> 00:18:21,860 that's what's going to create that beautiful mood 489 00:18:21,860 --> 00:18:24,460 and make images just pop off the screen, 490 00:18:24,580 --> 00:18:26,960 pop off the print and just look gorgeous 491 00:18:26,960 --> 00:18:28,340 as you're looking at a beautiful album. 492 00:18:28,920 --> 00:18:30,500 Bear with me, we're going to simplify it 493 00:18:30,500 --> 00:18:30,980 even further. 35318

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