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authorjaseg <git@jaseg.net>2017-06-12 13:03:18 +0200
committerjaseg <git@jaseg.net>2017-06-12 13:03:18 +0200
commit6f12a41cc6fc61d62bfd862f454e63b0652823fc (patch)
treefb859409840bb2dc471b3849a41ddef0d70ce2a0
parent6301aad16983dca0ac34c285bbeee7944075ddde (diff)
download7seg-6f12a41cc6fc61d62bfd862f454e63b0652823fc.tar.gz
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Add resistor calculation script
-rw-r--r--fw/main.c44
-rw-r--r--hw/chibi/chibi_2024/rcalc.py127
2 files changed, 149 insertions, 22 deletions
diff --git a/fw/main.c b/fw/main.c
index 6113a10..2e7b56e 100644
--- a/fw/main.c
+++ b/fw/main.c
@@ -74,32 +74,32 @@ int main(void) {
SPI1->CR2 &= ~SPI_CR2_DS_Msk;
SPI1->CR2 |= LL_SPI_DATAWIDTH_16BIT;
/* FIXME maybe try w/o BIDI */
- SPI1->CR1 = SPI_CR1_BIDIMODE | SPI_CR1_BIDIOE | SPI_CR1_SSM | SPI_CR1_SSI | SPI_CR1_SPE | (1<<SPI_CR1_BR_Pos) | SPI_CR1_MSTR | SPI_CR1_CPOL | SPI_CR1_CPHA;
+ SPI1->CR1 = SPI_CR1_BIDIMODE | SPI_CR1_BIDIOE | SPI_CR1_SSM | SPI_CR1_SSI | SPI_CR1_SPE | (0<<SPI_CR1_BR_Pos) | SPI_CR1_MSTR | SPI_CR1_CPOL | SPI_CR1_CPHA;
- int i = 0;
- int val = 0x5555;
+ int val = 0xffff;
GPIOA->BSRR = GPIO_BSRR_BR_6;
+ int j = 0;
+ int bval = 0x4000;
while (42) {
- if (i == 8) {
- i = 0;
- val = ~val;
+ for (int i=0; i<8; i++) {
+ spi_send(val);
+ spi_send(val);
+ strobe_leds();
+ spi_send(0x0200 | bval | (0xff^(1<<i)));
+ strobe_aux();
+ for(int i=0; i<10; i++)
+ tick();
+ //j++;
+ if (j == 1000) {
+ j = 0;
+ if (bval == 0x4000)
+ bval = 0x8000;
+ else if (bval == 0x8000)
+ bval = 0x0000;
+ else
+ bval = 0x4000;
+ }
}
- spi_send((i&1 ? 0xfa00 : 0xf000) | (0xff^(1<<i)));
- i++; // 1100'0100"0000'0000
- strobe_aux();
-
- spi_send(val);
- spi_send(val);
- strobe_leds();
- /*if (i == 32) {
- i = 0;
- }
- i++;
- spi_send((i&16) ? 0 : (1<<i));
- spi_send((i&16) ? (1<<(i&15)) : 0);
- strobe_leds();
- */
- LL_mDelay(200);
}
}
diff --git a/hw/chibi/chibi_2024/rcalc.py b/hw/chibi/chibi_2024/rcalc.py
new file mode 100644
index 0000000..3bba342
--- /dev/null
+++ b/hw/chibi/chibi_2024/rcalc.py
@@ -0,0 +1,127 @@
+#!/usr/bin/env python3
+"""
+ MBI5026 current set resistor calculations
+
+ The MBI5026's output current is set by a current set via a single resistor
+ connected to its R_ext pin.
+
+ To get a larger inter-frame dynamic range Megumin can switch between
+ four different current ranges. The ratio between one current range and the
+ next smaller one is r=1:8 (eq. -lg(r)=3 bit). This means at b=12bit BCM range we
+ get a minimum of
+
+ bmin = b+lg(r) = 8bit @ r=1:16, b=12bit
+
+ worst-case in the intermediate ranges using a static current setting.
+ Megumin uses BC847 small-signal NPN transistors to switch between three
+ current ranges:
+
+ ┌─────────┐
+ │ MBI5026 │
+ │ │
+ │ Rext─┼──┬──┤R1├───────────GND
+ │ │ │
+ └─────────┘ ├──┤R2├──┤BC847├──GND
+ │
+ ├──┤R3├──┤BC847├──GND
+ │
+ └──┤R4├──┤BC847├──GND
+
+ The transistors are used to select either or none of {R2, R3, R4}. This means
+ the R_ext pin sees either R1, R1||R2, R1||R3 or R1||R4. We don't do a full
+ R-2R or similar DAC configuration as we only have to maintain the ratio r
+ between ranges.
+
+ Megumin's smallest BCM period is tb=250ns resulting in a base BCM rate of
+ 4MHz minus control overhead. This results in a BCM period and frame rate of
+
+ Tm = tb*(2**b) = 1.024ms @ tb=250ns, b=12bit.
+ fm = 1/Tm ≈ 1kHz
+
+ Now, if we want to modulate the display at a current range in between two
+ of the preset ranges, we can switch between both ranges with a ratio of
+ sqrt(r)=1:4 and still get a frame rate of
+
+ f = fm/sqrt(r) = 250Hz @ fm=1kHz, r=1:16
+
+ Normalized to the larger of the two ranges (here r1=1) we get the following
+ equation for the ratio of the resulting modulated range:
+
+ r_im1 = sqrt(r)*r1 = 0.25 @ r=1:16, r1=1
+ r_im_tot = r_im1 + (1-sqrt(r))*r2 = 0.297 @ r2=r*r1
+
+ Including the 2 bit gained by inter-frame modulation this results in the
+ following basic ranges at framerate f=250Hz with a slight mid-range
+ discontinuity at the mixed ranges:
+
+ Range max │ Total bits
+ ───────────┼──────────────────────
+ 1.000 │ 14
+ 0.297 | 16 (14 at mid-range)
+ 0.250 | 14
+
+ The resistances of the resistors R1, R2, R3, R4 used are calculated in this
+ script.
+"""
+
+prefixes = {' ': 1, 'k': 1e3, 'M': 1e6, 'm': 1e-3, 'μ': 1e-6, 'n': 1e-9}
+def format_unit(val):
+ for prefix, magnitude in prefixes.items():
+ if 1.0 <= val/magnitude < 1000.0:
+ return val/magnitude, prefix
+ else:
+ if val<1:
+ return val/10e-9, 'n'
+ else:
+ return val/10e6, 'M'
+
+def print_var(name, val, unit, **kwargs):
+ scaled, prefix = format_unit(val)
+ print('{} = {: >7.3f}{}{}'.format(name, scaled, prefix, unit), **kwargs)
+
+r = 1/16
+stages = 3
+mod_r = 1/8
+I_max_led = 0.01
+n_boards = 20
+n_digits_per_board = 8*4
+n_leds = n_boards*n_digits_per_board*8
+V_fw = 1.9 # V
+
+print('r = 1:{:.0f}'.format(1/r))
+
+I_min_led = I_max_led*(r**(stages-1)) # A
+I_max_mod = I_max_led/mod_r
+I_min_mod = I_min_led/mod_r
+print_var('I_max_led', I_max_led, 'A')
+print_var('I_max_mod', I_max_mod, 'A')
+print_var('I_min_mod', I_min_mod, 'A')
+if (I_max_mod > 0.09):
+ print('\033[91mError: The MBI5026 has a maximum output current of 90mA!\033[0m')
+
+Vrext = 1.26 # V
+# Iout = 15 * Vrext/Rext | acc. to MBI5026 datasheet
+R1 = 15*Vrext/I_min_mod
+Itot_1 = n_leds * mod_r * I_min_mod
+Ptot_1 = Itot_1 * V_fw
+print_var('R1', R1, 'Ω', end='\t')
+print_var('I1', I_min_mod, 'A', end='\t')
+print_var('Itot_1', Itot_1, 'A', end='\t')
+print_var('Ptot_1', Ptot_1, 'W')
+
+for i in range(stages-2, -1, -1):
+ # Rpar = 15*Vrext/(I_max_mod*r)
+ # R1||R2 = 1/(1/R1 + 1/R2) =!= Rpar = 15*Vrext/(I_max_mod*r)
+ # ⇒ 1/R1 + 1/R2 = 1/(15*Vrext/(I_max_mod*r))
+ # ⇒ 1/R2 = 1/(15*Vrext/(I_max_mod*r)) - 1/R1
+ # ⇒ R2 = 1/((I_max_mod*r)/(15*Vrext) - 1/R1)
+ In = I_max_mod*(r**i)
+ Rn = 1/(In/(15*Vrext) - 1/R1)
+ Itot_n = n_leds * mod_r * In
+ Ptot_n = Itot_n * V_fw
+ scaled, prefix = format_unit(Rn)
+ print_var('R{}'.format(stages-i), Rn, 'Ω', end='\t')
+ print_var('I{}'.format(stages-i), In, 'A', end='\t')
+ print_var('Itot_{}'.format(stages-i), Itot_n, 'A', end='\t')
+ print_var('Ptot_{}'.format(stages-i), Ptot_n, 'W')
+